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Article

Unravelling the Relations between and Predictive Powers of Different Testing Variables in High Performance Concrete Experiments: The Data-Driven Analytical Methods

Department of Civil Engineering, National Kaohsiung University of Science and Technology, Kaohsiung 807, Taiwan
*
Author to whom correspondence should be addressed.
Buildings 2022, 12(10), 1545; https://doi.org/10.3390/buildings12101545
Submission received: 13 August 2022 / Revised: 5 September 2022 / Accepted: 20 September 2022 / Published: 27 September 2022
(This article belongs to the Special Issue Applications of (Big) Data Analysis in A/E/C)

Abstract

:
This study proposes and applies a systematic data analysis methodology to analyse experimental data for high-performance concrete (HPC) samples with different admixtures for offshore fan foundation grouting materials uses. In contrast with other relevant research, including experimental studies, the materials physics and chemistry studies, or cementitious material portfolio determination studies, this data-driven analysis provides a deep exploration of the experimental variables associated with the test data. To offer complete and in-depth perspectives, several methods are employed for the data analyses, including correlation analysis, cosine similarity analysis, simple linear regression (SLR) modelling, and heat map and heat-based tabularised visualisations; the outcome is a proposed methodology that is easily implementable. The results from these methods are validated using a pairwise comparison approach (PCA) to avoid unnecessary interference between data variables. There are several potential contributions from this work, including insights for cohered groups of variables, techniques for double check and ‘third check’, an established ‘knowledge base’ consisting of 504 SLR predictive models with their effectiveness (significance) and prediction accuracy (data-model fitness) used in practical applications, an alternative visualisations of the results, three data transforms which can be omitted in a future analysis, and three valuable theory-linking perspectives (e.g., for the relationships between destructive and non-destructive tests with respect to the variable categories). The implication that some variables are interchangeable will make future experiments less labour intensive and time consuming for pre-project HPC material testing.

1. Introduction

There are many types of experiments for testing a concrete material sample. As an example, in a study [1] involving the selection of high-performance concrete (HPC) admixtures for offshore wind farm construction, potential experiments are classified into the following three categories:
(Cat1)
fresh mechanical properties,
(Cat2)
hardened mechanical properties,
(Cat3)
the durability measures.
In the study, slump flow and the time required to flow through a V-shaped funnel were included in (Cat 1). Compressive strength (CS), ultrasound pulse velocity (USPV), and electrical resistivity on surface (ERoS) were included in (Cat 2), while anti-sulphate capability (ASC) and rapid chloride permeability (RCP) were included in (Cat 3). These categories allowed the researchers to determine the superior admixtures that included cement, fly ash, silica fume, super plasticiser, and water for grouting before building (non-floating) wind turbines with foundations constructed in the sea. One analysis, mentioned only in the paper’s Appendix, was of particular interest because it concluded that the relationship between CS and RCP could be identified (and established) as follows:
RCP = 7966.72 + (−97.76)CS.
This equation was formulated and validated through an extensive series of exploratory data analyses in that study; further details are provided in Appendix A of this study. Figure 1 provides visualisations of the final ‘effective process’ that resulted in Equation (1) using K-means (i.e., a non-supervised machine learning approach) and simple linear regression (SLR) modelling.
However, a practical benefit of the above process has not been described in the literature: such an outcome might reduce the effort to perform sample tests because with Equation (1), one of the two experimental results (e.g., RCP) can be anticipated (e.g., by CS), thereby reducing time and effort. Nevertheless, the practical benefits of this encouraging result are still limited because it was only validated for one pair of variables. Therefore, this study seeks to answer the question: Among numerous pairs of parameters tested for the HPC samples, does any other pair exist in which one parameter can be used to predict another?
In this study, a full set of data related to the experiments is sourced, and a data-driven analysis is performed following a pairwise comparison approach (PCA). To a large extent, this study identifies all pairs of concrete sample parameters in the available datasets sourced from an HPC laboratory, providing in-depth and cross-categorical views of the relationships between each variable pair and offering scientifically grounded insights about the experimental values that can be used to anticipate others.
A systematic data analysis methodology is designed and proposed utilising numerous methods, including correlation coefficient, cosine similarity, SLR modelling, and dimensional alternation (domain transform) of the variables (before estimating the parameters of the SLR model to ensure the linearity of each established model), in addition to other supplemental methods (e.g., the heatmap visualisation technique, and viewing the results from different perspectives). Using this methodology, the analysis reveals essential information about all Cat2 and Cat3 variables, the relationship between each pair of test variables, the variable’s ability to predict other variables, and the accuracy with which the variables can predict one another. The set of information obtained from the analysis (i.e., the ‘knowledge base’) can be used to benefit researchers and practitioners.
Since every pair of variables fitted with a model with sufficient predictive power (in terms of data-model fitness and model significance or effectiveness) can be summarised from the knowledge base, the results of some tests can be anticipated by using the results of other tests (if the law allows not testing every item). This could be a significant benefit to material testers whose time is valuable, and could also indirectly help reduce the cost and complexity of construction projects.
In this paper, other discussions are presented for the insights gained, particularly for the identified pairs of variables for which the results are positive (i.e., effective information). Implications are thus drawn from several aspects of the analysis, such as selecting a proper dimensional alternation method to convert the independent variable data for the established SLR model, performing both ‘double check’ and ‘third check’ by using the cosine similarity index and the relevant statistical descriptors of SLR models for the main results in the total correlation matrix, confirming theories in the existing literature or standards (between the test variables), and revealing the truth between the different destructive and non-destructive tests. Extensive discussions are also given for the utilisation of the developed knowledge base and future applications of the proposed methodological framework, as well as the time-saving effects on making material tests in each case (if the schedule for the construction project is tight). These also associate the results with theories and practices.
Section 2 reviews the literature related to the subject (i.e., the primary research question) and the methodologies to conduct this study, as well as the main data analysis methods applied. Section 3 presents the results, and Section 4 discusses the primary positive outcomes in terms of the application of methods, the practical insights gained, and the theoretical aspects of the study. Finally, Section 5 concludes this paper.

2. Literature Review and Methods

2.1. Background of the Problem

2.1.1. Renewable Energy (RE) Planning and Wind Farm Construction

For both developing and developed economies, stable and adequate supplies of energy are mandatory. However, as world’s fossil fuel-based energy resources are limited, renewable energy (RE) has emerged as a viable solution to replace conventional electric power generation [2,3]. In addition, utilising RE is also an ‘environmentally sound’ solution for a country to meet its sustainable development goals (SDGs) [4], this is also addressed by ESG (environmental, social, governance) targets that are established for business institutions [5].
Despite disagreements over the definitions of ‘RE’, ‘green energy’, ‘sustainable energy’, and ‘clean energy’, a classification of RE that is commonly accepted refers to the type of RE resource, including solar, wind, hydropower, geothermal, biomass, marine, and others [6,7,8]. This is due to the fact that the technological aspects to exploit these types of RE resource are usually totally different, thereby leading to salient ‘watersheds’ that can be told between them.
A stream of research adopting this view of classification is related to the ‘portfolios’, either in terms of selecting the optimal investment portfolio (by a company’s decision makers) [9] or determining a country’s optimal RE portfolio (by energy planners or operators within its long-term energy policy [10]. In research related to portfolios, uncertain or risky issues are also addressed [11,12]. However, in contrast to these operational management topics, more studies focus on the technologies to exploit various aspects of RE.
As an example, the technologies to exploit wind resources usually involve aspects of EE (electrical engineering), fluid dynamics/mechanics, and construction engineering (CE). Moreover, the first step in building a wind farm is typically to construct the foundations before erecting the wind turbines. For onshore or inland turbines, it is possible for the local weather conditions to be directly utilised as engineering parameters (e.g., steel structures, concrete materials, etc.). However, for offshore turbines, regardless of their working mode (i.e., fixed or floating, depending on the water depth), underwater foundations are always required, which necessitates the well-proportioned HPC material used for grouting [13].
Constructing new wind farms is necessary for a country with unique conditions to exploit its wind resources. For offshore wind farms, in the Taiwan Strait, numerous projects have taken advantage of the very shallow waters of the ‘Taiwan Bank’ [14] and the high wind availability [15]; similar projects have been developed on the edges of the Mediterranean Sea [16,17]. For on-shore or in-land wind farms, projects have been initiated near the Sahara Desert, e.g., budget has been allocated for the construction of wind farms in Algeria [18].
The motivation of this study is to explore and better understand the parameters (or the parametric performance) of the HPC materials (the numerical values for which can be obtained experimentally) used for grouting the structural bases of offshore wind turbines. This may benefit the selection process before the real admixture of the HPC is determined and applied as grouting, and it may also generate a novel knowledge set to be used for anticipating the potential outcomes of experiments.

2.1.2. The Special Weather/Sea Conditions in Taiwan and the Effects for Wind Turbines

As discussed in several studies, the soil of Taiwan is rich in sulphates and crystalline salts due to its geological features which result from frequent crustal deformation [19,20]. Osmosis of sulphate that occurs in concrete has caused serious problems for inland structures; the gypsum reaction is one such reaction, which can inflate the concrete and peel the surface off from the structure [1]. Therefore, anti-sulphate capability is typically a critical durability parameter in this context.
In addition, the high temperature and high humidity of Taiwan may accelerate these effects and decrease the life of structures. Moreover, the frequent earthquakes in the Circum-Pacific Belt and the typhoons that originated in the West Pacific region may also cause unexpected damage to structures. The damage is ‘unexpected’ because such events usually are inherently random, as is the scale of the event, e.g., the 921 Taiwan Earthquake of 1999, the Typhoon Morakot, etc. [21,22]. These types of natural disasters should be considered to be different from the damage caused by other types of unexpected events, such as fires [23].
These same conditions also apply to the Taiwan Strait, within which the Taiwan Bank is a very large but shallow continental shelf as a potential site for constructing offshore wind farms. Despite a high availability wind field above the sea all year, the land under water is susceptible to acid attacks (such as sulphates, chlorides, etc.), experiences the same extreme climate conditions discussed above (high temperature and high humidity), suffers from frequent natural disasters (earthquakes and typhoons) [24], and is scoured by the changing ocean currents throughout the year [25]. Therefore, quality HPC material is always required for wind turbines for its good workability during grouting, its beneficial mechanical properties during construction, and its long-term durability.
Thus, the parameters of an HPC sample (i.e., the experimental values from individual tests for all HPC samples which become ‘variables’ during data analysis) should be further studied and clearly understood. In addition, a suitable method is needed to determine the optimal HPC materials for construction based on the parametric data of the samples being tested during the experiments.
The parameters included in this study are organised and shown in Figure 2. It should be noted that, unlike in previous studies, electrical resistivity on surface (ERoS) is considered to be a durability property (parameter) of HPC samples in this research. This is believed to be a more reasonable consideration based on recent studies [26,27,28].
In Figure 2, the two fresh-property parameters are excluded from this study. These two tests are usually related to the workability of an HPC material during the engineering process, and their data formats are usually incompatible because the ‘data sampling periods’ of these two experiments are different than those in the other two categories. In contrast, the other eight variables have a quite large overlap in terms of their data sampling periods, so their data formats are compatible for the analysis (see Section 3.1).
In this study, the barrier between the hardened mechanical properties and durability properties is also removed intentionally. By doing so, not only can the pairs of parameters within a certain category be explored, but so can the pairs of parameters across two categories, so that relations between them and the intensities of the relations can be identified and evaluated. As will be shown later in Section 2.3, these relations include correlations, similarities, and predictive associations in terms of the ability to use one parameter to anticipate another (and how ‘safely’ it can be used).

2.2. About the Parameters

This section provides a review and discussion of the eight testing parameters of HPC analysed in this study (see Figure 2), regardless of the barrier between the hardened mechanical and durability parametric categories (see Section 2.1.2).

2.2.1. Compressive Strength (CS)

The CS of a concrete material (sample) is defined as its ability to withstand stress without failure. In concrete design and quality control, CS is the most generally specified property. The standard test method(s) for CS is (are) defined by ASTM C39 [29].

2.2.2. Tensile Strength (TS)

In this study, the splitting tensile strength (TS) of cylindrical specimens is accepted as the main tensile TS measurement for a concrete (and HPC) material (sample). Its test(s) can be performed in accordance with ASTM C496 [30].

2.2.3. Flexural Strength (FS)

The primary property for a concrete material (sample) to demonstrate is CS, but its tensile behaviours are also important. When reinforced concrete (RC) is subjected to tensile force, cracks and expansion will occur, depending largely on the TS of the concrete material. Direct tension tests of concrete are seldom performed, mainly because the device that holds the specimen may introduce secondary stresses that introduce error in the measurement. Another test for estimating the TS of a concrete material (sample) is the ASTM C78 (third point) flexural loading test, the result of which is referred to as flexural strength (FS) in this study [31].

2.2.4. Hardness (by Rebound Hammer) (HbRH)

The rebound hammer method utilises non-destructive testing techniques to measure the concrete strength. This test can be performed in accordance with ASTM C805 [32].

2.2.5. Ultrasound Pulse Velocity (USPV)

USPV is another common non-destructive index. The structural compactness in the specimen can be estimated according to the ultrasonic transferring rate (i.e., the speed of ultrasound waves going through the sample). The more complete the hydration reaction inside the concrete, the smaller the pores will be; thus, the detected USPV increases. ASTM C597 details the method(s) to test USPV [33].

2.2.6. Anti-Sulphate Capability (ASC)

Sulphate penetrates the surface of the concrete by infiltration, and a chemical reaction is produced when it combines with calcium hydroxide in the cement; when this occurs, the concrete expands, which further peels off the surface or destroys it. The experiment to measure the anti-sulphate capability of the HPC material samples can be carried out according to ASTM C1012; this method evaluates the resistance of the HPC to sulphate attack by measuring the rate of weight loss in an immersed specimen [34].

2.2.7. Rapid Chloride (Im-)Permeability (RCP)

Another indicator of the durability of concrete is its ability to resist chloride ion penetration. This can be performed by testing the concrete material samples using a rapid chloride ion rapid test (RCPT) with an applied electrical voltage. This test method can be performed in accordance with ASTM C1202 [35].

2.2.8. Electrical Resistivity on Surface (ERoS)

To evaluate concrete compactness and the durability of cement composites in an HPC sample, the ERoS can be measured. The higher the electrical resistance, the more compact the substrate, which increases durability. This study considers ERoS to be a durability variable (see Section 2.1.2), which can be tested using ASTM C876 [36].

2.3. The Methods: A Brief Review

2.3.1. Correlation Analysis

This study uses the Pearson correlation coefficient (P-Co-Co) method as the basis of the analysis to identify the correlation between each pair of experimental parameters (variables). The computation of a P-Co-Co is typically defined as the following:
P C o C o ( X , Y ) = n i n X i Y i i n X i i n Y i n i n X i 2 i n X i 2 n i n Y i 2 i n Y i 2
where X and Y are variables between which the P-Co-Co is to be calculated; n is the data size (length) of each variable; and i is the identifier for a specific data entry.
There are two primary reasons for using the P-Co-Co method:
(1)
All of the variables are continuous, so the two variables when searching for cor-relations must also be continuous; therefore, the P-Co-Co meets the analytical purpose.
(2)
Developed more than 100 years ago, P-Co-Co is the most common (and standard) method to compute and examine the correlation between two continuous variables.

2.3.2. Cosine Similarity Analysis

The cosine similarity (Cos-Sim) analysis diverges from the traditional thinking in statistics, treating experimental parameters as ‘vectors’, rather than ‘variables’; in so doing the similarity between two series of parametric values from the tests can be justified by the Cos-Sim index in the dimensional space. The standard computational process for this index can be written as:
C o s S i m ( X , Y ) = i n X i Y i i n X i 2 i n Y i 2
where X and Y are variables being treated as vectors between which the index is to be calculated (so Xi or Yi is the i-th element of vector X or vector Y); the other symbols are as defined previously.
The reasons to apply Cos-Sim in this context are as follows:
(1)
Cos-Sim has been proven to be an effective supplemental measure to P-Co-Co in real applications [37,38];
(2)
Cos-Sim also fits the data variables, i.e., the variables considered in this study are all continuous and positive, so the vectors are all meaningful in the multi-dimensional data space.

2.3.3. Simple Linear Regression

In this study, the predictive power and the relevant statistical descriptions between a pair of variables are justified by building several SLR models. Every SLR model chooses a data transform (method) to convert the independent variable (i.e., the RHS variable) prior to parameter estimation, so the model remains linear. A typical SLR model is defined as follows:
Y i = α + β X i + ε i
where α and β are the intercept and the regression coefficient associated with the only independent variable X in the model, respectively, which are to be estimated; given the i-th data tuple in the dataset, ( X i , Y i ) , ε i is the residual of this data tuple with respect to Y = α + β X ; other symbols are as defined previously.
The SLR model Y = α + β X can then be plotted as the best line fit (i.e., the ‘AB-line’) that includes all data points ( X i , Y i ) , i { 1 , 2 , , n } in the data space. This model also satisfies the requirement to identify the causal relationship and predictive power between two variables ‘pair-wisely’, i.e., the PCA used in the overall analysis (which also applies to the correlation analysis and the cosine similarity analysis).
In our analysis, every time two variables are paired, one variable becomes the dependent variable Y and the other one becomes the independent variable X. This then yields a total number of C 2 8 × 2 ! = 56 ‘base models’ of (X, Y), and in each case, the two paired variables are interchangeable (to appear on the RHS or LHS of the model, i.e., 2 ! ).

2.3.4. Data Variable Transforms

As discussed above, each of the 56 ‘basic models’ justifies the predictive relation and power between a certain pair of variables and the relevant statistical descriptions for the SLR model. However, the models are established based on the assumption that no variable is transformed, i.e., both variables on the RHS and LHS in the model use their data values in the source domain.
In this study, we transform the values of the independent variable on the RHS of each of the 56 models in nine ways in prior and build nine models by re-estimating the parameters of the SLR model that fit the independent variable in the transform domain. For comparison purpose, the models also include the initial case of ‘no transform’ (i.e., the base model), and are written as:
(1)
RHS Variable Transform: X = X 1 (no transform; the basic model)
(2)
RHS Variable Transform: X = X 2 (square)
(3)
RHS Variable Transform: X = X 3 (3 power)
(4)
RHS Variable Transform: X = e X (e power X)
(5)
RHS Variable Transform: X = 2 X (2 power X)
(6)
RHS Variable Transform: X = X (square root of X)
(7)
RHS Variable Transform: X = X 3 (triple root of X)
(8)
RHS Variable Transform: X = log ( X ) (log of X, base 10)
(9)
RHS Variable Transform: X = lg ( X ) (log of X, base 2)
With all these transforms performed prior to establishing the model, the model can be simplified as Equation (5) uniformly, and the linearity for all other SLR models derived from a basic model also holds:
Y = α + β X
For a model with (X, Y) as the RHS and LHS variables, the 56 cases already included their counterpart, i.e., (Y, X) as the RHS and LHS variables, respectively (see Section 2.3.3), meaning that all cases would be considered. As such, since there are nine models derived from each ‘basic model’ totally, there would actually be 56 × 9 = 504 SLR models in this work using the same set of data.

2.3.5. Indicators Used to Justify the SLR Modelling Results

Other than P-Co-Co and Cos-Sim which are in themselves ‘indicators’ for paired data variables, in this study, the following measures are used to tell the quality of an established SLR model. These include:
(1)
The estimated value of parameter α , α : this is the intercept of the predictive SLR model that fits the data, which is one of the two parameters defining the model in Equation (5);
(2)
The estimated value of β , β : this is the slope of the predictive SLR model, which is another parameter that defines the model in Equation (5);
(3)
The p value of the entire SLR model: this value indicates whether the model is significant or not; the significance of an SLR model usually dictates whether the model is reliable and the extent to which it can be trusted;
(4)
The p value for α : this p value indicates whether the estimated parameter α in the SLR model is significant or not;
(5)
The p value for β : this p value indicates whether the estimated parameter β in the SLR model is significant or not;
(6)
The R-square value, R 2 : this value usually connotes the data-model fitness, i.e., how well does the obtained SLR model fit the given data of ( X i , Y i ) , wherein the parameters in this case are typically estimated using the OLS (ordinal least square) method; and
(7)
The R-square value, ( R 2 ) : this is another R-square value that is adjusted based on R 2 and the sample size; we primarily observe the traditional R 2 value in this study, since the two values are usually very similar.
To visualise the summarised and tabularised computational results, they are also plotted as heat maps to provide a clear view. A heat map is a visualisation tool that is frequently used in the field of data-driven decision-making (DDDM) since Toussaint Loua provided its first application in 1873.

3. Results

3.1. Original Datasets

The experimental datasets for the eight hardened mechanical or durability parameters, i.e., the eight variables of the HPC samples to be analysed, are summarised in Table 1. The datasets are presented following the order provided in Section 2.2.

3.2. Correlation Analysis

Table 2 shows the P-Co-Cos between each pair of variables in a correlation matrix, while no variable is transformed. Figure 3 visualises the results using a heat map.
To ensure an objective basis using the adopted measures (see Section 2.3) and taking the data variables pair-wisely, every data variable should have an equal length and be tested on the same set of testing days for the same set of HPC samples. Fortunately, the collected datasets have followed these conditions. Inside the red boxes shown in Table 1, experimental data are provided for all data variables on day 28, day 56, and day 91, over all HPC samples. The result is eight variables with an equal data length of n = 36, correspondingly; these form the basis of subsequent data analyses.
Each sub table in Table 3 shows a correlation matrix produced when variable X in each pair (of variables) is transformed using one of the methods discussed in Section 2.3.4. In these sub tables, the cells are shown in different colours to visualise the results directly (which is analogous to using a separate heat map: dark green for 1, gradient green (lighter and lighter) for (less) positive values, white for 0, gradient red (heavier and heavier) for (more) negative values, full red for −1). In addition, note that the diagonal elements are white boxes with ‘---’ entries to indicate they do not contain any meaningful information.

3.3. Cosine Similarity Analysis

Table 4 shows the Cos-Sim between each pair of variables in a matrix, with no variable transformations. Figure 4 visualises the same results using a heat map.
Some studies have successfully treated variables as vectors and used the Cos-Sim between two vectors (see Section 2.3) to confirm the correlation between two variables (but not vice versa), and have observed that a higher P-Co-Co (between −1 and 1) most often indicates a higher Cos-Sim (between 0 and 1). Since in Figure 4 most variable-pairs with higher Cos-Sim indices are observed to have higher P-Co-Cos in Figure 3 (relative to other pairs), the findings from the previous studies are confirmed in terms of P-Co-Co.
Since this outcome can provide justification for performing subsequent analyses, results were not obtained in this study for the other eight transforms. Relevant tables and figures are omitted, as those outcomes are expected to be analogous.

3.4. Regression Analysis

This section summarises the results for estimating and establishing the 504 SLR models (see Section 2.3.4). The details are summarised in the web page at the following URL: http://www.DDDM.nkust.edu.tw/download/HPCStudy2_TheUltimateDataExperiments.html (accessed on 3 April 2022) (and in Appendix B), while some initial entries in Table A1 are listed in Table 5 for clarification. A guideline for reading these tables is provided below.
In Table A1, ‘X’ determines the eight ‘main phases’ defined by the eight variables used as the independent variable. In the table, the different background colours denote these phases as blocks. In each main phase fixing the independent variable, there are seven subphases defined by other variables used as the dependent variable ‘Y’. Since each subphase involves nine transforms (refer to the transform descriptions in Section 2.3.4), each block in Table A1 contains 7 × 9 = 63 SLR models, giving 63 × 8 = 504 models in total.
For each model, M# represents the unique model number assigned, with the P-Co-Co between the independent and dependent variables (X and Y) given. This is followed by the estimated model parameters: α (the estimated value of parameter α ) and β (The estimated value of β ); the p values for α , β the entire SLR model, p ( α ) and p ( β ) ; and the R square values, R 2 and ( R 2 ) .
As an example, the model with M# = 10 in Table 5 is the model established in the main phase ‘X = CS’ and in the subphase ‘Y = FS’ to identify the relationship between CS and FS of the HPC samples. Since it is the first model of the ‘X = CS, Y = FS’ subphase, transform method (1): X = X 1 is used, which means no transform is performed for the data of variable X in this model (see Section 2.3.4). From the table, the estimated parameters for this model are: α = 4.243931 (meaning the regression line intercepts with the Y axis at Y = 4.243931) and β = 0.104528 (this is the regression line’s slope, meaning one unit of increase in CS leads to an increase of 0.104528 in FS). Therefore, the established model can be written as:
F S = 4.243931 + 0.104528 × C S
For the same model, p( α ) = p( β ) = p(M) = 0. Despite the fact that in this table the p values are truncated to 4 digits past the decimal so that ‘p = 0′ may represent a very small value of p, it could still be inferred that both parameters estimated by the model are very significant, and the model itself is quite significant (i.e., it is very reliable and can be trusted to a large extent).
Moreover, for this model, R 2 = 0.679376 and ( R 2 ) = 0.669946, meaning that the data-model fitness is acceptable, since over 2/3 of the variability is explained by the established model. However, this is only slightly above the acceptability threshold of 0.6 to claim data-model fitness which was established due to this study’s scientific foundation (i.e., natural science than social science investigation, so using 0.6 than 0.4 or even 0.2 is more reasonable).
The full forms of all 504 models are provided in Table A2, which can also be accessed on the web page. For example, Equation (6) for the model with M# = 10 above is the same full form as displayed in Table A2.

3.5. Additional Information

Additional information about the SLR models is retrieved from Table A1 and rendered in terms of the transform method used to convert the data value of the independent variable, X. For the analytical targets, only the p and R 2 values for all models are considered to conserve space. The reason for considering these values is that the p value of any regression model represents its significance, and R 2 indicates the data-model fitness (or the model’s explanation power for the variations in the data), both of which are essential for qualifying SLR models.
The results for the p values of the entire model are listed in Table 6. Each sub table contains all pairs of variables (X, Y); X and Y are the RHS (independent) and LHS (dependent) variables in Equation (5), respectively. In the sub tables, the rows are identified by X and the columns are identified by Y. The significant results, indicating the SLR model is reliable and the model’s predictive power can be trusted, are shown in red font. The significance of the p values is determined using the threshold: p < 0.10, which is typically the most relaxed condition that is acceptable by statisticians. In addition, ‘p = 0′ may mean a very small value of p.
The results for the R 2 values of the entire model are listed in Table 7, where each sub table contains the R 2 values for the SLR models of all pairs of variables (X, Y) when a transform is applied for X. Similar to Table 6, the rows are identified by X and the columns are identified by Y in Table 7. However, unlike the correlation values which may range from −1 to 1 in Table 3, the R-squared values only range from 0 to 1. Therefore, the numbers in Table 7 are dyed according to the following convention: dark green for 1, gradient green (lighter and lighter) for (less) positive values, and white for 0.
To conserve space, the results of importance are shown with different shades of background colours in the table. In this manner, the SLR models with better data-model fitness can be easily identified. To evaluate the fitness, many scientific studies use the threshold: >0.4 (i.e., it has resolved more variations in the data, so using this model for prediction is therefore more accurate). The results for other observations, such as the p values of the estimated parameters α and β , as well as the adjusted R 2 value for the model, are summarised in Table A3, Table A4 and Table A5, respectively, in Appendix C. These may also be accessed on the ‘web page’.

4. Insights and Discussions

By analysing the results, many interesting insights can be gained. For the purpose of this study, only the most critical insights are discussed in this section; other advanced information may be obtained from the detailed results in the appendices.

4.1. For Method Applications

4.1.1. Insights for Data Pre-Processing Results

During data curation and pre-processing (see Section 3.1), the fresh properties of HPC are excluded because of data incompatibility, and only the hardened mechanical and durability property data at day 28, day 56 and day 91 are utilised for analysis due to data commonalities (i.e., they provide equal-sized data variables and have overlaps in testing time), despite the fact that the frequency of data recording for the experiment is typically predefined [39]. This experience will be useful for locating commensurable HPC testing data during any future analysis.

4.1.2. Insights for Correlation Analysis Results

In the correlation analysis (see Section 3.2), the main results in Table 2 and Figure 3 reveal that:
  • There are two strongly correlated groups of variables: {CS, TS, FS} form a salient group, while {ASC, RCP} form another. All of the correlations identified are either very strong (r > 0.8) or near very strong (0.6 < r < 0.8 but r~0.8).
  • Each group in 1. exists with respect to the same variable category, i.e., CS, TS and FS are hardened mechanical properties, and ASC (in terms of the weight loss percentage) and RCP (in terms of the coulombs measured) are both durability properties.
  • TS is a variable of interest because it forms a medium correlation group with USPV and ERoS. It has a strong (0.6 < 0.622967 < 0.8) positive correlation with USPV and a medium (0.4 < 0.562644 < 0.6) correlation with ERoS. Since USPV also has a strong positive correlation with ERoS (0.645174), {TS, USPV, ERoS} is another correlated group that overlaps both parametric categories of an HPC sample.
  • The observation of negative correlations is of interest, but there are no strong or very strong negative correlations (<−0.6) identified among all variables.
  • USPV has similar medium negative correlations with both ASC (−0.56893) and RCP (−0.58283); this can be explained by the fact that ASC and RCP are strongly correlated (0.817532).
  • ERoS and ASC have a medium negative correlation (−0.54312), and TS and HbRH have a medium (but near-weak) negative correlation (−0.40234). Since a negative correlation does not actually mean a ‘poor relation’ but rather a relation in the opposite ‘direction’, the observations of the above medium-negative P-Co-Cos are meaningful.
Beyond the correlations, additional information is provided. Table 3 includes eight sub tables with correlations produced when variable X (of the variable pair (X, Y)) is converted using the eight transformation methods described in Section 2.3.4. These sub tables confirm the main results in Figure 3 and Table 2 (when no data variable is transformed), and also help identify the optimal transforms to be used for each variable (this is further discussed in Section 4.1.4). In this regard, such information is valuable.

4.1.3. Insights from the Results of the Cosine-Similarity Analysis

By treating the data variables as vectors, the results obtained from the cosine-similarity analysis essentially confirm the correlations identified between pairs of variables. With few exceptions, a higher Cos-Sim index (between 0 and 1) in Table 4 indicates it has also had a relatively high P-Co-Co in Table 2 (between −1 and 1); this result can also be observed by comparing Figure 3 and Figure 4. As such, the main results of the correlation analysis are further confirmed (and ‘double checked’, in addition to the confirmations provided in Section 4.1.2 by the P-Co-Cos recalculated after different variable transforms).
Another insight of this research relates to methodology and theory. This study offers new support for the claim that a cosine-similarity analysis can be used as a supplement to the traditional correlation analysis.

4.1.4. Insights from the Established SLR Models

In this study, after successfully estimating the model parameters used in the datasets, 504 SLR models are established. The major insights gained from these analyses are summarised as follows.

The Established ‘Knowledge Base’ Is Novel and Benefits Future HPC Sample Testing

The information relating to the established models (see Table A1 and Table A2) is valuable because it can be used to create a true ‘knowledge base’ for practical applications. Given this knowledge base, if one experimental variable for the HPC sample can be used to predict another variable based on the known mathematical relationship and a guarantee of prediction accuracy, it is logical that the number of testing items that are truly necessary may be reduced. This is particularly true today as stakeholders in the construction and civil engineering industries have reduced the time and resources needed to complete a project, so the time available to test the HPC samples is limited. This should be considered as the primary and original contribution of this study.

A Method Is Provided to Explore the Insights into the Variables That Can Practically Be Used to Predict Another Variable and to Determine How Accurate the Prediction Will Be

Table A1 lists nine SLR models (where eight other models are derived from the first ‘base model’) as a group. It is critical for data analysis in such a design to utilise all opportunities to identify the optimal model that offers both better predictive power and better data-model fitness simultaneously.
Examining SLR models in which variable X is CS, for example (M# = {1, 2, 3, …, 27} in Table 5), the first nine models are established for predicting TS (Y) from CS (X). If p(M) < 0.5 is the threshold to confirm a model’s significance, the M# = 4 ( X = e X ) and M# = 5 ( X = 2 X ) models are not qualified to be effective (p(M) = 0.0558 and p(M) = 0.0540). In addition, the models are far from data-model fitness, because R 2 = 0.103447 for M# = 4 and R 2 = 0.104875 for M# = 5 (which are far below the levels of data-model fitness for seven other models), meaning that these two models may not provide good prediction accuracy. Based on these two results, it is evident that the two SLR models with the 2 ‘power X’ transforms are inadequate. A negative implication of this finding could be that the true relation between CS and TS does not exist on this basis, but a positive implication could be that there have been seven models that can be recommended (M# = {1, 2, 3, 6, 7, 8, 9}) in practice or for future research.
Investigating two subsequent (X, Y) combinations, for M# = {10, 11, …, 18}, the models are established for predicting FS (Y) from CS (X). The resulting situation is similar to using CS to predict TS: the two ‘power X’ SLR models (M# = {13, 14}) are inadequate, and “no true relation between CS and FS exists on this basis”. However, the claim can also be made that “another 7 models (M# = {10, 11, 12, 15, 16, 17, 18}) can be effective in practice or for future research”.
The M# = {19, 20, …, 27} are also established for predicting USPV (Y) from CS (X). However, no model is qualified to build a predictive relation between these two variables. Two SLR models (M# = {22, 23}) are ineffective (p > 0.1), and every model’s R 2 value is poor ( R 2 < 0.2) meaning they provide insufficient data-model fitness. Thus, we conclude that that the value of USPV from the value of CS in the experiments performed to test HPC samples cannot be anticipated, and that further research is recommended to find a method to predict USPV using CS.
This analysis is not continued throughout the entire Table A1. The above process can be repeated for all other models in Table A1 to gain other insights regarding the variables that can be used to predict other variables and the accuracy of the prediction process. In addition to these empirical insights that are expected, the experimental design to enable such explorations is the second contribution of this work.

Another Perspective to View the Model Information Is Offered to Differentiate and Recommend the Appropriate Transforms to Be Used for a Variable

An alternative method to evaluate the information relating to the established SLR models can provide additional insights. In Section 3.5 and Appendix C, the significance of the entire model (p(M)), the significance of the estimated α value (i.e., p( α )), the significance of the estimated β value (i.e., p( β )), the R square value (i.e., R 2 ), and the adjusted R square value (i.e., ( R 2 ) ) of the SLR models are systematically presented as separate tables (Table 6, Table 7, Table A1 and Table A2) according to the transform applied on the RHS variable in the SLR model. This provides another perspective for the model information which can be used in addition to the previous analytical viewpoint that presents a group of models derived from a base model at the same time (e.g., Table 5, Table A1 and Table A2). Therefore, offering two complementary perspectives is another contribution of this research. The following discussion highlights the positive outcomes of this new data-viewing perspective.
Based on the results in Table 6 and Table 7 (for the p(M) values and the R 2 values, respectively), the following insights are gained:
7.
In most of the RHS variable transformation cases (refer to the corresponding sub tables in Table 6), the SLR model’s p(M) value agrees with that of the ‘no transform’ case (shown in the ‘significant’ cells with red borders). This not only confirms that the ‘no transform’ SLR model is effective in its predictive power, but also identifies an alternative set of effective transformed SLR models.
8.
In most of the RHS variable transformation cases (refer to the corresponding sub tables in Table 7), the SLR model’s R 2 value agrees with that of the ‘no transform’ case (see the colour intensity of a cell). This not only confirms that the ‘no transform’ SLR model is able to provide accurate predictions, but also identifies an alternative set of qualified ‘having transform’ SLR models.
9.
For most of the RHS variable transforms, the SLR model’s R 2 value in Table 7 also concurs with the correlation identified in Figure 3 in terms of the equal P-Co-Co value for (X, Y) or (Y, X), and also for the counterpart model with Y and X exchanged as the RHS and LHS variables of the SLR model. In addition, the SLR model’s R 2 may also concur with the Cos-Sim index calculated for (X, Y) (and (Y, X)). In other words, if a high correlation is identified between two variables, a high data-model fitness typically exists, and vice versa. Furthermore, in such cases with high correlation and high data-model fitness, the Cos-Sim values are generally also high. These insights are critical because the relationships between these three values (P-Co-Co, Cos-Sim and R 2 ) that were previously unidentified have now been clarified for this application.
10.
The ‘lowest-performing RHS variable transforms’ can also be identified from the results, supporting the claim that the true relationship between the two variables in an SLR model (i.e., Y and the X being converted using a worse transform) is far from ‘a variable is transformed like that’. This claim further implies that some variable transformation methods can be ignored in the future.
Regarding the ‘worse variable transforms’, they can be identified by interpreting Table 6 in detail (in addition to Table A1 and Table A2, as required) to determine if, for a pair of (X, Y), a ‘no transform’ model shows good results (e.g., p(M) < 0.05 and/or R 2 > 0.6), and which model(s) with a variable transform shows poor results (e.g., p(M) > 0.1 and/or R 2 < 0.2)?
Examining the highly-correlated variable group of {CS, TS, FS} (see Section 4.1.2), the SLR models established between all pairs of these variables using every other transform (for X) offers a preferred data-model fitness for providing accurate predictions (i.e., R 2 ≥ 0.6) (shown in the dark cells in the upper left of Table 7a,b,e–h); however, this is not the case using the two ‘power X methods’ (i.e., X = e X and X = 2 X ) (shown in the light cells in the upper left part of Table 7c,d).
Further evaluating Table 7 reveals that for all pairs of variables, using these two ‘power X’ methods may depress the R 2 value in general and make it difficult to uncover the relevant information (e.g., to determine which model provides better data-model fitness). It is therefore recommended to neglect both ‘power X’ methods in future studies for all pairs of test variables.

4.1.5. Other Insights from the Research

In addition to the above insights, several other interesting findings are obtained from the data analysis in this study.
For example, the p(M) values in Table 6g,h are identical, as are the R 2 values in Table 7g,h; interestingly, the associated P-Co-Co values in Table 3g,h are also identical. By further inspecting Table 5 and A1, these can be explained by the fact that the SLR models will be identical if the transformation method is X = log ( X ) or X = lg ( X ) . That means that the base (here, 10 or 2) does not change if a logarithm is used for the RHS variable transform. Therefore, it is recommended for future studies that, for each pair of variables, keeping either SLR model is sufficient.

4.2. Theory-Linking

In this section, from three theoretical perspectives, the importance of several theory-reflexive finding and insights are discussed.
Through the numerical analysis, the relationship between FS and CS identified in this study (in its mathematical form) is found to concur with their relationship as defined in ACI 318-19 [40,41,42] and in [43] (except for the coefficients). Therefore, this result is reflexive to the existing theories; in turn, this outcome further validates the results obtained in this study.
Next to this, the measures, data variables, and tests established for the durability of concrete are critical, as durability is an important category of parameters for HPC, particularly when it is to be used in humid areas or marine environments which are prone to acid attacks [44,45,46]. However, due to the time required to obtain results, true tests for durability are difficult to perform, so other indirect tools such as ASC, RCP, and ERoS should be applied. For this, a conventional theory is that, if a correlation between a hardened mechanical (i.e., strength) property and another durability property can be identified (or if their causal relationship can be established), durability can thus be anticipated by strength properties. In this research, other than very strong or strong relationships identified for the HPC parameters in the same variable category, some significant relationships (from strong to median intensities) between variables across the two categories (see Section 3 and Section 4.1) are also found. In other words, these positive outcomes have confirmed the core theoretical logic.
Following these, another theoretical perspective relates to destructive and non-destructive tests (NDTs) [23,47]. Referring to Table 8, which is a simplified version of Table 2 with colour levels added (full red for 1, gradient red (lighter and lighter) for (less) positive values, gradient blue (heavier and heavier) for (more) negative values, dark blue for −1), the upper left cells containing the hardened mechanical properties show that, other than the very strong or near very strong correlations identified among the three destructive ‘strength’ measures, {CS, TS, FS}, USPV and HbRH are NDTs. Two interesting and important observations about these NDTs can be made.
The first observation is that USPV is an NDT that is more correlated with all destructive tests than HbRH, as evidenced by the magnitude of the P-Co-Cos, 0.43176 > 0.39808 , 0.62297 > 0.40234 , and 0.31071 > 0.30525 . Thus, USPV has a medium correlation with TS, a medium correlation with CS, and a weak correlation with FS, while HbRH has a weak negative correlation with TS, a weak negative correlation with CS, and a weak negative correlation with FS. Therefore, the test results for USPV may be more associated with the results obtained from the destructive tests than that of HbRH. This supports the recommendation to keep only one NDT (i.e., USPV, because it provides links to destructive tests more effectively), which is similar to the previous finding supporting the recommendation to keep only one destructive test (i.e., either CS, or TS, or FS, because they are interchangeable; see Section 4.1).
The second observation is that there is no significant correlation between the two NDTs for hardened mechanical properties, despite the fact that the test results for USPV may have a weak negative correlation with those of HbRH (−0.23428). This means that, for two similar HPC samples (with the same admixture) tested on the same day, these two NDTs would typically produce diversified results. An evidence-based argument can be presented that the mechanisms behind these two NDTs should be intrinsically different.
Similar observations to the destructive tests and NDTs can also be made by examining the lower right cells with respect to the durability properties. Other theory-reflexive insights of interest based on these results could be gained through future studies.

5. Conclusions

This study proposes and applies a systematic data analytic methodology to analyse the experimental data obtained from tests of HPC samples with different admixtures. In contrast with other relevant studies aimed primarily at performing experiments (and providing rationale for the experiments based on materials, physics, or chemistry) or identifying the optimal HPC admixture(s) for grouting concrete materials to be used in the sea (e.g., for the base construction of offshore wind turbines), the purpose of this study is to perform a thorough investigation of the experimental variables related to the testing data.
To achieve this purpose, a methodological framework is proposed. In order to generate comprehensive and in-depth views of the data, numerous methods are utilised, including P-Co-Co, Cos-Sim, SLR, and heatmap or heat-based tabularised visualisation. This approach is significantly different from those of other experimental-based research or admixture-selection studies. Highlights of the research activities, results, and insights gained are presented below.
  • All variables in the dataset testing the 12 HPC samples of different admixtures were previewed. The dataset was sourced intentionally to cover as many tests for HPC as possible. Among the Cat2 and Cat3 properties, the overlapping (and compatible) data for the eight variables (i.e., the data gathered at 28, 56, and 91 days for CS, TS, FS, USPV, HbRH, ERoS, ASC, and RCP) are identified and specified to support subsequent analyses.
  • Rather than providing a descriptive analysis for the testing data, the investigation began with a correlation analysis, in which the concept of PCA was applied. Within the same variable category, variable groups were identified in which the correlation between each pair of variables was very strong {CS, TS, FS} and {ASC, RCP}. Another medium-correlation variable group was {TS, USPV, ERoS}, in which the included variables overlap the two variable categories. In addition to the positive correlations, some relatively strong negative correlations were also identified between some pairs of variables. The result for P-Co-Cos in the main correlation matrix with no variable transformation was confirmed by another eight correlation matrices with variable X in Equation (2) being converted using transforms (2)–(9) described in Section 2.3.4.
  • The correlation matrix was validated using the cosine similarity analysis. With few exceptions, a higher Cos-Sim index (between 0 and 1) meant it also had a relatively high P-Co-Co.
  • This analysis generated 504 SLR models, establishing a novel ‘knowledge base’ which can benefit future HPC sample-testing. By grouping these models using the C 2 8 × 2 ! = 56 ‘base models’, each group consisted of nine models (associated with the nine types of RHS variable transform, including ‘no transform’) (see Table 5). When they are grouped using the 9 types of RHS variable transform, each stratification has 56 models. These two perspectives enabled different types of subsequent analyse.
  • With the established knowledge base, an investigation was performed to determine if a variable can be used to predict another (or not) and, if so, how accurate the prediction will be. For example, by inspecting each SLR model’s significance value, p(M), it was shown that CS test data can safely be used to predict TS and FS for an HPC sample, but it may not be used to anticipate USPV (see Section 4.1.4). By inspecting the SLR models’ R 2 values, CS was found to predict TS and FS accurately. These results were cross-validated with the very strong correlations observed among {CS, TS, TS} from the correlation analysis. Insights such as these implied that in future construction projects, valuable time and effort can be saved with respect to HPC testing.
  • By utilising a second perspective to view the model information (see #4 above), the appropriate RHS variable transforms in this analytical context were identified. It was also found that the two ‘power X’ transforms (i.e., X = e X and X = 2 X ) are both inadequate and should be omitted, and one of the ‘logarithm’ transforms (i.e., X = log ( X ) or X = lg ( X ) ) is redundant. Thus, at least three out of the nine transforms can be excluded in future analyses.
  • Some of the insights gained from the results were linked to theories, including the following: (1) The results confirmed relationships found in the existing literature or standards between the test variables; (2) The results verified that the core theoretical logic of this research is effective; (3) The results of some NDTs were more related to the destructive tests (while some NDTs were less related), and different NDTs led to different results; unlike the destructive tests (particularly strength tests), these NDTs are not interchangeable.
The methods used in this study are common, and utilising them for this study was proven to be effective. Therefore, it should also be valid to utilise the methodological framework proposed in this research for similar purposes, e.g., data analysis for other concrete samples with different admixtures. From this perspective, a future story upon taking the proposed framework is perhaps clear from scratch. When a construction project is launched, one first sees if the HPC material(s) is to be used.
As can be expected, if so (using HPC) and if the planned admixtures of the HPC samples to be tested are analogous to the ones being tested in this study, efforts related to testing the materials can be reduced considerably by either policy. The first policy is to use the direct testing results for the samples in the established knowledge base (if ‘no testing’ is allowed legally). The second is to determine the testing item to be ‘predicted’ (as desired), look up the knowledge base to know what any other testing item can predict it (and also the information about whether the prediction will be effective and/or accurate), and decide whether to really but safely save the money, and time in most of the cases, for making tests by anticipating the results for the testing item (if some regulated testing items are mandatory).
However, if so (using HPC) and the planned HPC samples to be tested are different (e.g., due to a diversified purpose of use), or if not so (using the non-HPC material), theoretically, the first step is to make similar tests for these samples, followed by using the proposed framework to conduct the thorough data experiments (in order to identify the relationship and the mutual predictive power between each pair of sample parameters). Then as can be imagined, another knowledge base for the samples included by this purpose of use can be established. Although the outcomes and the unanticipated insights gained may vary in different cases or contexts, after this one-time job, what follows is a similar policy-making problem (see the former paragraph). Anyhow, all this may support efforts to save the time required for pre-project experiments, especially when the project is urgent, which is a crucial but inevitable fact in the current A/E/C industry.
It should be noted that the applications of this framework are not limited to cases in which the source datasets for each measure are tested using conventional methods (i.e., a parameter of HPC samples may have more than one testing method). For example, the framework could be applied when a part of the data is obtained using NMR (nuclear magnetic resonance) [48,49]. In many countries, NMR equipment is legal and commercialised, and the data for some variables can be obtained [50,51]. Other than this, except for HPC, the question of ‘can similar data analysis using this framework be carried out for other construction materials?’ is also worth of exploration.
Future research directions are shown in Figure 5, wherein the aim of this study which is clearly differentiated from other relevant studies.
In the figure, the experimental-oriented studies are focused on the performance of the HPC, the inclusion of parameters for developing experiments, and statistics and variability in the data. A critical element that future research directions rely upon is the testing data sets produced by this research. Following this step, there are clear boundaries among the three research directions. The materials, physics and chemistry studies research direction involves a significant amount of opportunity for future studies. However, the knowledge base constructed for the HPC testing parameters as an outcome of the data analytics studies may benefit advance data studies in the future as well as subsequent selection decision modelling studies and current cementitious material portfolio determination studies. The selection decision modelling studies aim to rank the HPC samples with different admixtures and select the optimal candidate using the scientific decision models; therefore, the knowledge base may provide a precise numerical foundation for these models (and added value from the expert knowledge of the researchers).

Author Contributions

Conceptualization, methodology, software, visualization, Z.-Y.Z.; data curation, investigation, supervision, validation, W.-T.K.; funding acquisition, project administration, writing—original draft preparation, writing—review and editing, Z.-Y.Z. and W.-T.K. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by Ministry of Science and Technology (MOST, Taiwan, ROC), grant number MOST 110-2410-H-992-020 and 110-2637-E-992-001. The APC was funded by MDPI discount voucher and MOST 111-2410-H-992-011. Note that the institution ‘Ministry of Science and Technology (MOST)’ has been renamed as National Science and Technology Council (NSTC) in August 2022 in this area. However, we still keep the original funding number for these projects were approved before the transition.

Data Availability Statement

N/A. All related data for the results of this study are detailed in the appendix sections.

Conflicts of Interest

The authors declare no conflict of interest.

Acronyms (Alphabetic Order)

ACIAmerican Concrete Institute
A/E/CArchitect/Engineering/Construction
ASCAnti-Sulphate Capability
ASTMAmerican Society for Testing and Materials
Cat1(Property) Category 1 (Fresh Mechanical)
Cat2(Property) Category 1 (Hardened Mechanical)
Cat3(Property) Category 3 (Durability)
CEConstruction Engineering
Cos-SimCosine Similarity
CSCompressive Strength
DDDMData-Driven Decision-Making
EEElectrical Engineering
ERoSElectricity Resistivity on Surface
ESGEnvironmental, Social, Governance
FSFlexural Strength
HbRHHardness by Rebound Hammer
HPCHigh Performance Concrete
LHSLeft-Hand Side
NDTNon-Destructive Test
NMRNuclear Magnetic Resonance
OLSOrdinal Least Square
PCAPairwise Comparison Approach
P-Co-CoPearson Correlation Coefficient
RCReinforced Concrete
RCPRapid Chloride Permeability
RCPTRapid Chloride Permeability Test
RERenewable Energy
RHSRight-Hand Side
SDGSustainable Development Goals
SLRSimple Linear Regression
TSTensile Strength
USPVUltrasound Pulse Velocity

Appendix A

In that previous study, the data analytical process to obtain Equation (1) progressed as follows:
  • Each pair of (CS, ACP) data (i.e., ACP stands for accumulated charge passed for RCP) was treated as a data point (entry), considering the three testing time points (in terms of #days = 28, 56 and 91) and the 12 mixture portfolios of the concrete sample all together. This yields a data table of two variables, containing the 36 data points.
  • A rough trend was observed by plotting the data points (see Figure 1a; the data are sourced and replotted from the Appendix of (Kuo and Zhuang, 2021)). However, establishing a simple linear regression (SLR) model to fit them, the model did not provide a satisfactory explanation for the relationship between CS and RCP, i.e., the p value of the F statistic was acceptable but relatively week (p = 0.06415), and the regression coefficient of the SLR model was merely R2 = 0.09721, which is poor. Therefore, more solid clues about the relationship must be sought for.
  • The approach of ‘dimensional alternation of the variables’ was performed. The square root, square and log of the predictor variable (CS) was used as new variables, so several SLR models taking one of these predicting variables and keeping the variable being predicted (accumulated charge passed, or ACP) were reconstructed. In this process, outlier removals were also considered. However, as the case using the original data of variable CS, these trials did not give any more model that is satisfactory.
  • The second approach of ‘finding a condensed set of data points and estimating a new SLR model that fits these data points’ was then used. It used the K-means to cluster the data points (see Figure 1b), so the cluster centres form a condensed dataset. This process, in itself, removed the outliers to a certain extent, while keeping only the representative information of the data. Eventually, an effective SLR model: “ACP = 7966.72 + (−97.76)CS” was established.
  • The model in (4) was effective because the R2 (regression for data-model fitness) of the model was as high as R2 = 0.8386. The p value of the model also showed a qualified but weak result, which was p = 0.07071. However, since this was a model with one dependent variable and only one independent variable, a further scrutiny revealed that the correlation coefficient between these two data variables was as low as r = −0.9293, which could be justified as near totally negatively correlated.
From the above experiment, the last SLR model in step (5) can serve as an accurate (or, accurately calibrated) predictor when one knows a concrete sample’s CS value and would like to postulate the value of ACP that connotes the RCP of the sample. As CS is usually treated as a ‘hardened mechanical property’ but RCPT is usually a ‘durability property’ for the high-performance concrete (HPC) materials, and as this process has revealed a relationship between two experimental variables from two parametric categories, such a predictive model should be worthy of note.

Appendix B

The information in Table A1 is associated the 504 established SLR models. Table A2 lists these models in detail.
Table A1. Results from Estimating and Establishing the 504 SLR Models.
Table A1. Results from Estimating and Establishing the 504 SLR Models.
M#YXP-Co-Co α β p ( α ) p ( β ) p(M) R 2 ( R 2 )
1TSCS0.875333−3.6677130.2782090.04660.00000.00000.7662080.759331
2TSCS0.8588675.7663220.0019850.00000.00000.00000.7376520.729936
3TSCS0.8352268.9891670.0000180.00000.00000.00000.6976020.688708
4TSCS0.32163114.5688310.0000000.00000.05580.05580.1034470.077077
5TSCS0.32384414.5656440.0000000.00000.05400.05400.1048750.078548
6TSCS0.880394−22.3244744.5753310.00000.00000.00000.7750940.768479
7TSCS0.881580−40.93124013.8145830.00000.00000.00000.7771830.770630
8TSCS0.883184−62.85094142.7854090.00000.00000.00000.7800150.773545
9TSCS0.883184−62.85094112.8796920.00000.00000.00000.7800150.773545
10FSCS0.8242434.2439310.1045280.00000.00000.00000.6793760.669946
11FSCS0.8160587.7578080.0007520.00000.00000.00000.6659500.656125
12FSCS0.7996608.9628740.0000070.00000.00000.00000.6394570.628852
13FSCS0.33640611.0870360.0000000.00000.04480.04480.1131690.087086
14FSCS0.33794811.0859070.0000000.00000.04380.04380.1142090.088156
15FSCS0.824872−2.6961661.7104490.10880.00000.00000.6804140.671015
16FSCS0.824551−9.6160355.1555100.00040.00000.00000.6798840.670469
17FSCS0.823110−17.69315615.9103700.00000.00000.00000.6775100.668025
18FSCS0.823110−17.6931564.7894980.00000.00000.00000.6775100.668025
19USPVCS0.4371603.8574980.0175830.00000.00770.00770.1911080.167318
20USPVCS0.4270174.4562690.0001250.00000.00940.00940.1823440.158295
21USPVCS0.4147184.6595170.0000010.00000.01190.01190.1719910.147638
22USPVCS0.2199825.0051730.0000000.00000.19730.19730.0483920.020403
23USPVCS0.2205345.0049760.0000000.00000.19620.19620.0486350.020654
24USPVCS0.4411922.6703800.2901470.00270.00710.00710.1946510.170964
25USPVCS0.4423641.4858020.8772040.23620.00690.00690.1956860.172030
26USPVCS0.4444380.0798302.7245810.96300.00660.00660.1975250.173923
27USPVCS0.4444380.0798300.8201810.96300.00660.00660.1975250.173923
28HBRHCS−0.39807765.693972−0.3906630.00000.01620.01620.1584650.133714
29HBRHCS−0.40512552.917551−0.0028910.00000.01420.01420.1641260.139542
30HBRHCS−0.40592548.479311−0.0000270.00000.01400.01400.1647750.140210
31HBRHCS−0.17003640.1336080.0000000.00000.32150.32150.0289120.000351
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471USPVRCP−0.5218855.334800−0.0718820.00000.00110.00110.2723630.250962
472USPVRCP−0.5396865.589440−0.1133350.00000.00070.00070.2912610.270415
473USPVRCP−0.5559935.883336−0.2879370.00000.00040.00040.3091290.288809
474USPVRCP−0.5904326.890460−1.5364940.00000.00020.00020.3486100.329451
475USPVRCP−0.5912817.769025−2.4177790.00000.00010.00010.3496130.330484
476USPVRCP−0.5896485.339331−1.9980620.00000.00020.00020.3476840.328499
477USPVRCP−0.5896485.339331−0.6014770.00000.00020.00020.3476840.328499
478HBRHRCP−0.05541942.042378−1.4875820.00000.74820.74820.003071−0.026250
479HBRHRCP−0.05955441.070969−0.5153180.00000.73010.73010.003547−0.025761
480HBRHRCP−0.04927040.511711−0.1655830.00000.77540.77540.002428−0.026913
481HBRHRCP−0.04701140.997438−0.2408880.00000.78540.78540.002210−0.027137
482HBRHRCP−0.05268541.782675−0.6657510.00000.76020.76020.002776−0.026554
483HBRHRCP−0.04472943.245445−2.8401260.00270.79560.79560.002001−0.027352
484HBRHRCP−0.03964044.285542−3.9550100.02980.81850.81850.001571−0.027794
485HBRHRCP−0.02713940.148932−2.2439000.00000.87520.87520.000737−0.028654
486HBRHRCP−0.02713940.148932−0.6754810.00000.87520.87520.000737−0.028654
487ERoSRCP−0.33091499.464458−13.8232290.00000.04870.04870.1095040.083313
488ERoSRCP−0.29832688.526158−4.0172120.00000.07720.07720.0889980.062204
489ERoSRCP−0.26239084.519693−1.3723150.00000.12210.12210.0688490.041462
490ERoSRCP−0.27680989.598988−2.2073200.00000.10220.10220.0766230.049465
491ERoSRCP−0.29562295.936765−5.8133760.00000.08000.08000.0873930.060551
492ERoSRCP−0.342215119.666621−33.8160570.00000.04110.04110.1171110.091144
493ERoSRCP−0.344671139.348934−53.5168490.00000.03950.03950.1187980.092881
494ERoSRCP−0.34702585.635639−44.6518390.00000.03810.03810.1204260.094556
495ERoSRCP−0.34702585.635639−13.4415430.00000.03810.03810.1204260.094556
496ASCRCP0.817532−2.5184813.2466740.00030.00000.00000.6683590.658605
497ASCRCP0.817113−0.2034891.0460580.57360.00000.00000.6676740.657900
498ASCRCP0.7901760.6856730.3928890.02470.00000.00000.6243780.613330
499ASCRCP0.800249−0.6421950.6066660.14360.00000.00000.6403980.629821
500ASCRCP0.813711−2.1555221.5212510.00080.00000.00000.6621260.652188
501ASCRCP0.801181−6.7579527.5265140.00000.00000.00000.6418900.631358
502ASCRCP0.792474−10.89633611.6979650.00000.00000.00000.6280150.617075
503ASCRCP0.7695580.8993989.4136920.00340.00000.00000.5922190.580226
504ASCRCP0.7695580.8993982.8338040.00340.00000.00000.5922190.580226
Table A2. All SLR Models in Detail.
Table A2. All SLR Models in Detail.
M#SLR ModelM#SLR Model
1TS = −3.66771333146045 + 0.278209291384233 × CS253CS = 82.4394445799055 + −0.405631800581188 × HbRH
2TS = 5.76632220397327 + 0.0019846216045102 × CS ^2254CS = 75.4057601873381 + −0.00528600953754371 × HbRH ^2
3TS = 8.98916688640433 + 1.80409811683411e-05 × CS ^3255CS = 72.8629873306788 + −8.21782427238269e-05 × HbRH ^3
4TS = 14.5688311121099 + 2.68866314762229e-41 × e^ CS256CS = 66.9027834245253 + −5.14345524118181e-26 × e^ HbRH
5TS = 14.5656439363982 + 1.41265796681029e-28 × 2^ CS257CS = 67.1708457607848 + −7.48294418841369e-18 × 2^ HbRH
6TS = −22.3244737238133 + 4.57533122714702 × CS ^(1/2)258CS = 96.0472599467819 + −4.77054201210767 × HbRH ^(1/2)
7TS = −40.9312402935274 + 13.814582720438 × CS ^(1/3)259CS = 109.56395500385 + −12.8042675489701 × HbRH ^(1/3)
8TS = −62.8509407538376 + 42.7854090996044 × log(CS)260CS = 115.311599942547 + −31.0342296205957 × log(HbRH)
9TS = −62.8509407538376 + 12.8796915157356 × lg(CS)261CS = 115.311599942547 + −9.34223400812292 × lg(HbRH)
10FS = 4.24393079882703 + 0.104527758280078 × CS262TS = 19.9622058974958 + −0.1303029585153 × HbRH
11FS = 7.75780828627991 + 0.000752403905718667 × CS ^2263TS = 17.6543146320032 + −0.00166994242748144 × HbRH ^2
12FS = 8.96287429220537 + 6.89191529938516e-06 × CS ^3264TS = 16.83840458393 + −2.58037721938791e-05 × HbRH ^3
13FS = 11.0870361916049 + 1.12206961389585e-41 × e^ CS265TS = 15.0165743978521 + −2.03721394407596e-26 × e^ HbRH
14FS = 11.0859072057969 + 5.88205048357479e-29 × 2^ CS266TS = 15.1093101981532 + −2.84866062385744e-18 × 2^ HbRH
15FS = −2.69616622448087 + 1.71044934171127 × CS ^(1/2)267TS = 24.4677526180197 + −1.55399032698069 × HbRH ^(1/2)
16FS = −9.61603490429178 + 5.15551033198057 × CS ^(1/3)268TS = 28.9510915589449 + −4.19472168720189 × HbRH ^(1/3)
17FS = −17.6931562993013 + 15.9103695111459 × log(CS)269TS = 31.0462473657117 + −10.3012836038027 × log(HbRH)
18FS = −17.6931562993013 + 4.7894984649526 × lg(CS)270TS = 31.0462473657117 + −3.10099535858616 × lg(HbRH)
19USPV = 3.8574983286046 + 0.0175825945943531 × CS271FS = 12.7435704060995 + −0.039445290747868 × HbRH
20USPV = 4.45626900695745 + 0.000124865325500488 × CS ^2272FS = 12.0754048065075 + −0.000523213761785206 × HbRH ^2
21USPV = 4.6595172220698 + 1.13358339686721e-06 × CS ^3273FS = 11.832096250984 + −8.23893341545536e-06 × HbRH ^3
22USPV = 5.00517282814257 + 2.32706905364138e-42 × e^ CS274FS = 11.2321332373504 + −4.95164302968338e-27 × e^ HbRH
23USPV = 5.00497635203039 + 1.21736498704813e-29 × 2^ CS275FS = 11.2579775085298 + −7.20711857382233e-19 × 2^ HbRH
24USPV = 2.67038043865855 + 0.290146899587109 × CS ^(1/2)276FS = 14.0361157995126 + −0.458978534407627 × HbRH ^(1/2)
25USPV = 1.4858023636118 + 0.877204473839206 × CS ^(1/3)277FS = 15.3207207454225 + −1.22722061378818 × HbRH ^(1/3)
26USPV = 0.0798296243915567 + 2.72458142347606 × log(CS)278FS = 15.8342481716803 + −2.9508137441398 × log(HbRH)
27USPV = 0.0798296243915644 + 0.820180734095162 × lg(CS)279FS = 15.8342481716803 + −0.888283448603619 × lg(HbRH)
28HbRH = 65.6939723416543 + −0.39066291994853 × CS280USPV = 5.40527092455439 + −0.00960161616381508 × HbRH
29HbRH = 52.9175508566686 + −0.00289053323693466 × CS ^2281USPV = 5.18228451266245 + −9.23365939017983e-05 × HbRH ^2
30HbRH = 48.4793106810452 + −2.70731778165387e-05 × CS ^3282USPV = 5.105547006142 + −1.03094075674674e-06 × HbRH ^3
31HbRH = 40.1336082855694 + −4.38891161917149e-41 × e^ CS283USPV = 5.01571398268165 + 6.35172119916297e-28 × e^ HbRH
32HbRH = 40.1385314994 + −2.30412190648458e-28 × 2^ CS284USPV = 5.01761451645092 + 4.7746220119381e-20 × 2^ HbRH
33HbRH = 90.8138878413038 + −6.29176473409599 × CS ^(1/2)285USPV = 5.83782737563726 + −0.130633680633248 × HbRH ^(1/2)
34HbRH = 115.838473020169 + −18.8576275257236 × CS ^(1/3)286USPV = 6.26621225603992 + −0.367863560422559 × HbRH ^(1/3)
35HbRH = 144.146417510672 + −57.5149717946972 × log(CS)287USPV = 6.57238703587405 + −0.980912750035412 × log(HbRH)
36HbRH = 144.146417510672 + −17.3137317099717 × lg(CS)288USPV = 6.57238703587405 + −0.295284160889903 × lg(HbRH)
37ERoS = 48.638330809566 + 0.451481569206116 × CS289ERoS = 93.0915021332562 + −0.364903933321156 × HbRH
38ERoS = 63.1121233323246 + 0.00340477469183933 × CS ^2290ERoS = 85.3618387083167 + −0.00394146430058687 × HbRH ^2
39ERoS = 68.1424331649685 + 3.25053196642623e-05 × CS ^3291ERoS = 82.755136193978 + −5.23793613335234e-05 × HbRH ^3
40ERoS = 78.1544409313211 + 5.37587881956385e-41 × e^ CS292ERoS = 79.0174650656451 + −3.79940100453875e-26 × e^ HbRH
41ERoS = 78.1471425518886 + 2.83074450890616e-28 × 2^ CS293ERoS = 79.2064011656095 + −5.44974424110028e-18 × 2^ HbRH
42ERoS = 20.1584377318609 + 7.2033577129187 × CS ^(1/2)294ERoS = 108.32181180241 + −4.77082649816592 × HbRH ^(1/2)
43ERoS = −8.22243286374305 + 21.5230297614624 × CS ^(1/3)295ERoS = 123.47606121203 + −13.2894132486659 × HbRH ^(1/3)
44ERoS = −39.8009179828865 + 65.241657789968 × log(CS)296ERoS = 133.518155940357 + −34.7913378742457 × log(HbRH)
45ERoS = −39.800917982886 + 19.6396959616249 × lg(CS)297ERoS = 133.518155940357 + −10.4732362894283 × lg(HbRH)
46ASC = 4.95132054829306 + −0.0386503401063175 × CS298ASC = 2.68078131101273 + −0.00733510672804191 × HbRH
47ASC = 3.72539269504536 + −0.000294369718030655 × CS ^2299ASC = 2.60665094129842 + −0.000126382796341767 × HbRH ^2
48ASC = 3.30102796537324 + −2.84321291493011e-06 × CS ^3300ASC = 2.58769478660714 + −2.48849929099358e-06 × HbRH ^3
49ASC = 2.44093528214272 + −6.72399110323773e-42 × e^ CS301ASC = 2.44220142607004 + −4.53236511525499e-27 × e^ HbRH
50ASC = 2.44170772986293 + −3.53122466148145e-29 × 2^ CS302ASC = 2.45300492295719 + −5.49529605773755e-19 × 2^ HbRH
51ASC = 7.37026715497592 + −0.614301465019437 × CS ^(1/2)303ASC = 2.85534341592287 + −0.0747993160120245 × HbRH ^(1/2)
52ASC = 9.78274044602861 + −1.83353621086711 × CS ^(1/3)304ASC = 3.03754257943617 + −0.191963698502796 × HbRH ^(1/3)
53ASC = 12.4554180798691 + −5.54827132735972 × log(CS)305ASC = 3.06678420213484 + −0.429225020225469 × log(HbRH)
54ASC = 12.4554180798691 + −1.67019609361768 × lg(CS)306ASC = 3.06678420213485 + −0.129209605977347 × lg(HbRH)
55RCP = 2.2672230225556 + −0.0113988195146484 × CS307RCP = 1.59366458546644 + −0.00206458751119777 × HbRH
56RCP = 1.88299647072557 + −8.18219613510574e-05 × CS ^2308RCP = 1.59250269958169 + −4.7007782059367e-05 × HbRH ^2
57RCP = 1.75078592624905 + −7.4585338236417e-07 × CS ^3309RCP = 1.5940113480029 + −1.03273072317156e-06 × HbRH ^3
58RCP = 1.51818175249647 + −8.62375516317953e-43 × e^ CS310RCP = 1.53596131120061 + −2.07901551267993e-27 × e^ HbRH
59RCP = 1.51830999498204 + −4.54842382692243e-30 × 2^ CS311RCP = 1.54311874344824 + −2.70943115773082e-19 × 2^ HbRH
60RCP = 3.0251758982295 + −0.186665056505132 × CS ^(1/2)312RCP = 1.60647332079248 + −0.0152285890543703 × HbRH ^(1/2)
61RCP = 3.78074488916298 + −0.562728438143532 × CS ^(1/3)313RCP = 1.62252334316423 + −0.0328544818159167 × HbRH ^(1/3)
62RCP = 4.663140971559 + −1.73705575957867 × log(CS)314RCP = 1.5765860616204 + −0.0412065467018546 × log(HbRH)
63RCP = 4.66314097155899 + −0.522905887774061 × lg(CS)315RCP = 1.5765860616204 + −0.0124044065749873 × lg(HbRH)
64CS = 25.6010477687945 + 2.75406936542173 × TS316CS = 51.089202219025 + 0.193565839661132 × ERoS
65CS = 44.236410022525 + 0.0946888189494539 × TS ^2317CS = 56.1180779980333 + 0.00156343014265882 × ERoS ^2
66CS = 50.9063816671094 + 0.00398118874295442 × TS ^3318CS = 57.8305000886192 + 1.5170484861907e-05 × ERoS ^3
67CS = 64.102513981059 + 1.08352527227825e-08 × e^ TS319CS = 65.905973876004 + 5.56007324663602e-43 × e^ ERoS
68CS = 62.93479281879 + 9.97078792156074e-06 × 2^ TS320CS = 65.7374812451052 + 9.51622799059243e-30 × 2^ ERoS
69CS = −10.6326736740597 + 20.195416541604 × TS ^(1/2)321CS = 40.6340826309488 + 2.9192088069464 × ERoS ^(1/2)
70CS = −46.6793703465627 + 46.4175211250117 × TS ^(1/3)322CS = 30.0257116537128 + 8.53247838099428 × ERoS ^(1/3)
71CS = −29.2331517456234 + 82.8403738530719 × log(TS)323CS = 19.9860767860859 + 24.6353731468881 × log(ERoS)
72CS = −29.2331517456234 + 24.9374373817928 × lg(TS)324CS = 19.9860767860861 + 7.41598627158826 × lg(ERoS)
73FS = 6.54685987581198 + 0.313124883867076 × TS325TS = 5.57698297874872 + 0.117091719673417 × ERoS
74FS = 8.70756838739812 + 0.0105856072945152 × TS ^2326TS = 8.84882889224645 + 0.000910458534534851 × ERoS ^2
75FS = 9.48379504325131 + 0.000437165189201065 × TS ^3327TS = 9.97627368064185 + 8.60117098114261e-06 × ERoS ^3
76FS = 10.9579310971029 + 1.06591164804576e-09 × e^ TS328TS = 14.3474181010307 + 6.0953908828585e-43 × e^ ERoS
77FS = 10.8407343563029 + 9.87757373295459e-07 × 2^ TS329TS = 14.2272764535642 + 9.33570995950449e-30 × 2^ ERoS
78FS = 2.36028455472909 + 2.31370552755273 × TS ^(1/2)330TS = −1.1269089945942 + 1.80904069963451 × ERoS ^(1/2)
79FS = −1.80037496774033 + 5.33057504676748 × TS ^(1/3)331TS = −7.90186096886077 + 5.33486061240443 × ERoS ^(1/3)
80FS = 0.153469672168541 + 9.55644054219172 × log(TS)332TS = −14.7390012786689 + 15.7009205255199 × log(ERoS)
81FS = 0.153469672168538 + 2.87677525497907 × lg(TS)333TS = −14.7390012786689 + 4.72644803771776 × lg(ERoS)
82USPV = 3.8582700632675 + 0.0788332945887362 × TS334FS = 9.83395980893246 + 0.0170538323228349 × ERoS
83USPV = 4.41351597695613 + 0.00261674011715778 × TS ^2335FS = 10.3125531496547 + 0.000132286637799236 × ERoS ^2
84USPV = 4.61424167992712 + 0.000105778685478559 × TS ^3336FS = 10.486081411843 + 1.23231731631889e-06 × ERoS ^3
85USPV = 4.98138269039791 + 2.06326729117493e-10 × e^ TS337FS = 11.1527750704836 + 2.99625338895325e-44 × e^ ERoS
86USPV = 4.95689326088985 + 1.965467135128e-07 × 2^ TS338FS = 11.1479488279815 + 4.40573016768686e-31 × 2^ ERoS
87USPV = 2.78745215424647 + 0.586914035384849 × TS ^(1/2)339FS = 8.86996914221672 + 0.262067593014333 × ERoS ^(1/2)
88USPV = 1.72467454463204 + 1.35521823819063 × TS ^(1/3)340FS = 7.89844511181229 + 0.770500724179212 × ERoS ^(1/3)
89USPV = 2.21017728190999 + 2.43932132966721 × log(TS)341FS = 6.94573366509112 + 2.24915473694021 × log(ERoS)
90USPV = 2.21017728191 + 0.734308889292778 × lg(TS)342FS = 6.94573366509116 + 0.677063040708727 × lg(ERoS)
91HbRH = 58.1513390501432 + −1.24230352426858 × TS343USPV = 3.68820846972565 + 0.0169908027073602 × ERoS
92HbRH = 50.2249700104166 + −0.044770875619361 × TS ^2344USPV = 4.16938309261067 + 0.000131129610994454 × ERoS ^2
93HbRH = 47.2679048675656 + −0.00193325336213942 × TS ^3345USPV = 4.33343560349138 + 1.23579707391254e-06 × ERoS ^3
94HbRH = 40.7389382402033 + −4.66451848397386e-09 × e^ TS346USPV = 4.90797369481416 + 1.63496289148364e-43 × e^ ERoS
95HbRH = 41.3078778310346 + −4.48876900783616e-06 × 2^ TS347USPV = 4.88959412661251 + 2.26894827628225e-30 × 2^ ERoS
96HbRH = 73.3631224275738 + −8.81243566756599 × TS ^(1/2)348USPV = 2.70118294373709 + 0.2641244615984 × ERoS ^(1/2)
97HbRH = 88.4709404052577 + −19.9993370745879 × TS ^(1/3)349USPV = 1.70386942486284 + 0.780820994806742 × ERoS ^(1/3)
98HbRH = 79.8183132517281 + −34.7074847278588 × log(TS)350USPV = 0.67903797185686 + 2.31085638391061 × log(ERoS)
99HbRH = 79.8183132517281 + −10.447993977135 × lg(TS)351USPV = 0.679037971856871 + 0.695637087228694 × lg(ERoS)
100ERoS = 38.619764851316 + 2.70358942299871 × TS352HbRH = 51.6324046062446 + −0.150673692373029 × ERoS
101ERoS = 56.6412391630876 + 0.0941220459496348 × TS ^2353HbRH = 47.1704653947156 + −0.00113291769977207 × ERoS ^2
102ERoS = 63.3000205646993 + 0.00394992641131165 × TS ^3354HbRH = 45.600695422352 + −1.04038244458094e-05 × ERoS ^3
103ERoS = 77.1328153398415 + 7.09631280316041e-09 × e^ TS355HbRH = 39.9748474387209 + −2.56797542626781e-43 × e^ ERoS
104ERoS = 76.0491484044899 + 7.47562545588949e-06 × 2^ TS356HbRH = 40.0456981734223 + −4.27679705661863e-30 × 2^ ERoS
105ERoS = 4.01611935228142 + 19.5716763093765 × TS ^(1/2)357HbRH = 60.6467709227773 + −2.37198566049296 × ERoS ^(1/2)
106ERoS = −30.329978647475 + 44.7426132701713 × TS ^(1/3)358HbRH = 69.7247860734917 + −7.04081020027556 × ERoS ^(1/3)
107ERoS = −12.3728718803923 + 78.8622864433468 × log(TS)359HbRH = 79.2748060130706 + −21.0017577568586 × log(ERoS)
108ERoS = −12.3728718803923 + 23.7399137460923 × lg(TS)360HbRH = 79.2748060130704 + −6.32215904648311 × lg(ERoS)
109ASC = 4.89596300636296 + −0.16966119937039 × TS361ASC = 6.4458151840564 + −0.0516341811061645 × ERoS
110ASC = 3.87624826801362 + −0.00638384276646585 × TS ^2362ASC = 4.99563817395329 + −0.000400352711259067 × ERoS ^2
111ASC = 3.49223640961992 + −0.000285395470139084 × TS ^3363ASC = 4.50745712993463 + −3.79575450452663e-06 × ERoS ^3
112ASC = 2.53307238173374 + −7.11652324318657e-10 × e^ TS364ASC = 2.59992789799722 + −2.99484600134824e-43 × e^ ERoS
113ASC = 2.62336847692134 + −6.95199732594167e-07 × 2^ TS365ASC = 2.66261962836728 + −4.64911698183225e-30 × 2^ ERoS
114ASC = 6.86395722224124 + −1.17477367334536 × TS ^(1/2)366ASC = 9.44043438324327 + −0.802103266576792 × ERoS ^(1/2)
115ASC = 8.82414184541521 + −2.64397265299706 × TS ^(1/3)367ASC = 12.47058422184 + −2.37157285658742 × ERoS ^(1/3)
116ASC = 7.59151813198557 + −4.51149961240018 × log(TS)368ASC = 15.5963281401096 + −7.02565846862435 × log(ERoS)
117ASC = 7.59151813198557 + −1.35809670875888 × lg(TS)369ASC = 15.5963281401096 + −2.1149339383466 × lg(ERoS)
118RCP = 2.0582468256364 + −0.0369995440023129 × TS370RCP = 2.13392259412586 + −0.00792174587898038 × ERoS
119RCP = 1.8103952102763 + −0.00128284918583967 × TS ^2371RCP = 1.93360893463405 + −6.48277942505363e-05 × ERoS ^2
120RCP = 1.71859132373958 + −5.35652053686268e-05 × TS ^3372RCP = 1.86921630500704 + −6.40894224684878e-07 × ERoS ^3
121RCP = 1.53188741984192 + −1.00594344665696e-10 × e^ TS373RCP = 1.55696749364964 + −6.45133418255133e-44 × e^ ERoS
122RCP = 1.54503002030309 + −9.93922733664546e-08 × 2^ TS374RCP = 1.56902059329398 + −9.76832901653834e-31 × 2^ ERoS
123RCP = 2.53415581702009 + −0.268461007718213 × TS ^(1/2)375RCP = 2.55930807240737 + −0.11918592439322 × ERoS ^(1/2)
124RCP = 3.0066266949075 + −0.614281461688656 × TS ^(1/3)376RCP = 2.99258729570875 + −0.348402784873324 × ERoS ^(1/3)
125RCP = 2.76276107851835 + −1.08503484360649 × log(TS)377RCP = 3.40606522122726 + −1.00780487661076 × log(ERoS)
126RCP = 2.76276107851835 + −0.326628034266129 × lg(TS)378RCP = 3.40606522122725 + −0.303379497636274 × lg(ERoS)
127CS = −6.32669651116645 + 6.49948062049916 × FS379CS = 70.6776219375967 + −1.83342313666841 × ASC
128CS = 29.9785358256873 + 0.28556239381448 × FS ^2380CS = 68.2714363423197 + −0.225306775541211 × ASC ^2
129CS = 42.0916447762494 + 0.0164212042293632 × FS ^3381CS = 67.549396985626 + −0.0328026961997557 × ASC ^3
130CS = 60.4701313902147 + 2.77820273664116e-05 × e^ FS382CS = 67.1919053071617 + −0.0179652802360796 × e^ ASC
131CS = 57.7305850492271 + 0.00213782451902893 × 2^ FS383CS = 67.7103192435025 + −0.12454655051729 × 2^ ASC
132CS = −78.8618812949019 + 43.5263527058322 × FS ^(1/2)384CS = 75.0502895075756 + −6.17920002596685 × ASC ^(1/2)
133CS = −151.371735363849 + 97.5647049792941 × FS ^(1/3)385CS = 79.0740475713104 + −10.3870301811374 × ASC ^(1/3)
134CS = −107.999762435771 + 166.924543040243 × log(FS)386CS = 67.936550509068 + −8.66359978801819 × log(ASC)
135CS = −107.999762435771 + 50.2492944676166 × lg(FS)387CS = 67.936550509068 + −2.60800340662158 × lg(ASC)
136TS = −7.19991865837233 + 1.96680522970567 × FS388TS = 16.7191027509542 + −0.812996500399415 × ASC
137TS = 3.94225264358756 + 0.085188466515247 × FS ^2389TS = 15.6873265109676 + −0.10392640936173 × ASC ^2
138TS = 7.656856290228 + 0.0048301982685163 × FS ^3390TS = 15.3374234564199 + −0.014689150374878 × ASC ^3
139TS = 13.2451876094529 + 7.3023151163122e-06 × e^ FS391TS = 15.1071164105457 + −0.00663398866735903 × e^ ASC
140TS = 12.4443150069096 + 0.000582075431634922 × 2^ FS392TS = 15.3618601830077 + −0.0515731674779195 × 2^ ASC
141TS = −29.4656951691208 + 13.2662252636793 × FS ^(1/2)393TS = 18.4752766762153 + −2.61099160196387 × ASC ^(1/2)
142TS = −51.7242857085425 + 29.8074489486029 × FS ^(1/3)394TS = 20.0700807482682 + −4.30328784764094 × ASC ^(1/3)
143TS = −38.7280892344743 + 51.2417059142874 × log(FS)395TS = 15.4265286526908 + −3.43411719112025 × log(ASC)
144TS = −38.7280892344744 + 15.425290509193 × lg(FS)396TS = 15.4265286526908 + −1.03377228315253 × lg(ASC)
145USPV = 3.9220780594136 + 0.0985428823674005 × FS397FS = 11.0977464494996 + 0.031873579279226 × ASC
146USPV = 4.47728767296606 + 0.00429215529920093 × FS ^2398FS = 11.0907213145279 + 0.00949415382452752 × ASC ^2
147USPV = 4.66109666398569 + 0.000245637379412544 × FS ^3399FS = 11.1047564029815 + 0.00181183855164129 × ASC ^3
148USPV = 4.92654609777185 + 4.60706117880123e-07 × e^ FS400FS = 11.1207633178236 + 0.00106742689440128 × e^ ASC
149USPV = 4.88841164928704 + 3.36308959813418e-05 × 2^ FS401FS = 11.1016774194187 + 0.00636702684383551 × 2^ ASC
150USPV = 2.8095900623364 + 0.663750016435372 × FS ^(1/2)402FS = 11.1234296660006 + 0.0356237890342107 × ASC ^(1/2)
151USPV = 1.69679136870262 + 1.49096966175817 × FS ^(1/3)403FS = 11.1326874840045 + 0.0334964933392047 × ASC ^(1/3)
152USPV = 2.34744679463731 + 2.56255150271304 × log(FS)404FS = 11.1712737674145 + 0.0138252031036824 × log(ASC)
153USPV = 2.3474467946373 + 0.771404867750439 × lg(FS)405FS = 11.1712737674145 + 0.00416180083035513 × lg(ASC)
154HbRH = 66.1885884598235 + −2.36217666323683 × FS406USPV = 5.39967741586927 + −0.157601360131323 × ASC
155HbRH = 54.2735150191536 + −0.113846998920061 × FS ^2407USPV = 5.23018907761182 + −0.0236309154497613 × ASC ^2
156HbRH = 50.1907307977067 + −0.00705311601461987 × FS ^3408USPV = 5.16485024635992 + −0.00371278492484695 × ASC ^3
157HbRH = 42.9011476603809 + −1.48131754198992e-05 × e^ FS409USPV = 5.11372151021348 + −0.00181910156412128 × e^ ASC
158HbRH = 44.2791893797267 + −0.00111924473609312 × 2^ FS410USPV = 5.17103704429333 + −0.0130363801376633 × 2^ ASC
159HbRH = 89.7599134019201 + −14.9823912521973 × FS ^(1/2)411USPV = 5.6807412003617 + −0.464228977845544 × ASC ^(1/2)
160HbRH = 113.273550501112 + −32.9353495751625 × FS ^(1/3)412USPV = 5.94133254828393 + −0.746448185862817 × ASC ^(1/3)
161HbRH = 96.2588355860703 + −54.0764110249104 × log(FS)413USPV = 5.13201708600292 + −0.575354478791353 × log(ASC)
162HbRH = 96.2588355860704 + −16.2786217763525 × lg(FS)414USPV = 5.13201708600292 + −0.173198956255813 × lg(ASC)
163ERoS = 50.9339523136868 + 2.47332003357847 × FS415HbRH = 40.5944269259985 + −0.335108945766807 × ASC
164ERoS = 64.9117719074914 + 0.107393071702334 × FS ^2416HbRH = 40.7100131929842 + −0.104581925495593 × ASC ^2
165ERoS = 69.6091128616802 + 0.00607935520541711 × FS ^3417HbRH = 40.6632578629035 + −0.0227846026661095 × ASC ^3
166ERoS = 76.8310941676581 + 8.292501066042e-06 × e^ FS418HbRH = 40.6395211240528 + −0.0169908872975303 × e^ ASC
167ERoS = 75.8229039136237 + 0.000685638485789691 × 2^ FS419HbRH = 40.8267699220799 + −0.0910711458036205 × 2^ ASC
168ERoS = 23.0966441893402 + 16.6339398116732 × FS ^(1/2)420HbRH = 40.2047715378215 + −0.290079711211349 × ASC ^(1/2)
169ERoS = −4.70919525255609 + 37.3279849854577 × FS ^(1/3)421HbRH = 39.8328823193541 + −0.0317014234712671 × ASC ^(1/3)
170ERoS = 11.7588814417093 + 63.9854593331807 × log(FS)422HbRH = 39.6509127800971 + 0.755863068849545 × log(ASC)
171ERoS = 11.7588814417082 + 19.2615425456256 × lg(FS)423HbRH = 39.6509127800971 + 0.227537456338342 × lg(ASC)
172ASC = 1.92204377986897 + 0.0417800027959956 × FS424ERoS = 92.2180819190403 + −5.71291801262153 × ASC
173ASC = 2.18316320247149 + 0.00161753154319612 × FS ^2425ERoS = 86.2029960263802 + −0.871295867930876 × ASC ^2
174ASC = 2.27270746633942 + 7.88163424212467e-05 × FS ^3426ERoS = 83.8039817684898 + −0.137158721334941 × ASC ^3
175ASC = 2.44093390317411 + −2.48113202997887e-07 × e^ FS427ERoS = 81.593359750612 + −0.0607357705453962 × e^ ASC
176ASC = 2.41621956362761 + −6.81999208250955e-06 × 2^ FS428ERoS = 83.8162898301957 + −0.462526675987894 × 2^ ASC
177ASC = 1.40580253441745 + 0.294779993824526 × FS ^(1/2)429ERoS = 102.130604184649 + −16.6331971432884 × ASC ^(1/2)
178ASC = 0.89095417108623 + 0.671410326192849 × FS ^(1/3)430ERoS = 111.281383625304 + −26.593705666928 × ASC ^(1/3)
179ASC = 1.15276439502583 + 1.18383492977662 × log(FS)431ERoS = 82.3761104513835 + −20.1185948235959 × log(ASC)
180ASC = 1.15276439502588 + 0.356369823777509 × lg(FS)432ERoS = 82.3761104513835 + −6.05630051251246 × lg(ASC)
181RCP = 1.51812154765212 + −0.000591998745777089 × FS433RCP = 1.01973122036864 + 0.205859469380567 × ASC
182RCP = 1.51281584514026 + −1.02938718884825e-05 × FS ^2434RCP = 1.23109107218656 + 0.0320113741552666 × ASC ^2
183RCP = 1.51260094503923 + −7.42379796240544e-07 × FS ^3435RCP = 1.31420187113397 + 0.00517100383009007 × ASC ^3
184RCP = 1.5256197518961 + −6.72812668995411e-08 × e^ FS436RCP = 1.38075364835372 + 0.00262715741339878 × e^ ASC
185RCP = 1.52273012331417 + −2.80067024547618e-06 × 2^ FS437RCP = 1.30385075127291 + 0.0183094250349436 × 2^ ASC
186RCP = 1.53241072190053 + −0.0062681280895472 × FS ^(1/2)438RCP = 0.664785578422722 + 0.597777968220892 × ASC ^(1/2)
187RCP = 1.54753285970626 + −0.0161478263626681 × FS ^(1/3)439RCP = 0.331701338198878 + 0.95917456833655 × ASC ^(1/3)
188RCP = 1.5488693295213 + −0.0357822221626458 × log(FS)440RCP = 1.37132011432189 + 0.741115441374556 × log(ASC)
189RCP = 1.5488693295213 + −0.0107715221824692 × lg(FS)441RCP = 1.37132011432189 + 0.223097978103492 × lg(ASC)
190CS = 11.6998550741678 + 10.8691835328367 × USPV442CS = 79.1876086152576 + −8.52780310166127 × RCP
191CS = 40.2737226314715 + 1.02188686322694 × USPV ^2443CS = 73.2155143001305 + −2.79139452268105 × RCP ^2
192CS = 49.7955275674617 + 0.126614263542547 × USPV ^3444CS = 70.9538278880991 + −1.07403228395841 × RCP ^3
193CS = 58.3200794662332 + 0.0463658521197105 × e^ USPV445CS = 74.5394446838858 + −1.64955391286155 × e^ RCP
194CS = 53.5820935995622 + 0.368615720449898 × 2^ USPV446CS = 78.5053861753618 + −4.08652317822277 × 2^ RCP
195CS = −45.4269190022254 + 49.9062423711336 × USPV ^(1/2)447CS = 90.3023182739201 + −19.7522294845498 × RCP ^(1/2)
196CS = −102.544736756829 + 98.6873794949362 × USPV ^(1/3)448CS = 101.206498442361 + −30.737981999028 × RCP ^(1/3)
197CS = −25.625449801709 + 131.505274123587 × log(USPV)449CS = 70.2323475564202 + −24.8667652877232 × log(RCP)
198CS = −25.6254498017091 + 39.587032099214 × lg(USPV)450CS = 70.2323475564202 + −7.48564224674054 × lg(RCP)
199TS = −9.95165895269854 + 4.92289295131928 × USPV451TS = 19.0034404993042 + −2.79621405588897 × RCP
200TS = 2.94021780561976 + 0.464792876737356 × USPV ^2452TS = 17.0628654215869 + −0.922398139081904 × RCP ^2
201TS = 7.23615323870508 + 0.0578570626959677 × USPV ^3453TS = 16.3276494077446 + −0.357708176247271 × RCP ^3
202TS = 11.054729627453 + 0.0216332650123754 × e^ USPV454TS = 17.5161562873897 + −0.548248026177606 × e^ RCP
203TS = 8.91107549629212 + 0.170046021754159 × 2^ USPV455TS = 18.8166813396968 + −1.35231061799441 × 2^ RCP
204TS = −35.7255348185222 + 22.5589242403911 × USPV ^(1/2)456TS = 22.6157194894507 + −6.45016652543744 × RCP ^(1/2)
205TS = −61.4951920610503 + 44.5805803174326 × USPV ^(1/3)457TS = 26.1599023833134 + −10.0229727575101 × RCP ^(1/3)
206TS = −26.695573877673 + 59.3305417374464 × log(USPV)458TS = 16.0559054395538 + −8.08312589858581 × log(RCP)
207TS = −26.695573877673 + 17.8602727219652 × lg(USPV)459TS = 16.0559054395538 + −2.4332633542027 × lg(RCP)
208FS = 6.25268451510252 + 0.979697960884986 × USPV460FS = 11.1846550558515 + −0.00712280503711107 × RCP
209FS = 8.8968791736595 + 0.0894113658440846 × USPV ^2461FS = 11.3393422008688 + −0.0667625121783373 × RCP ^2
210FS = 9.77637198554798 + 0.0107225118544231 × USPV ^3462FS = 11.3734572783345 + −0.0460353492860872 × RCP ^3
211FS = 10.5787331781917 + 0.00345900541644401 × e^ USPV463FS = 11.4643267491817 + −0.0581305838184308 × e^ RCP
212FS = 10.1586186111251 + 0.0294317301093728 × 2^ USPV464FS = 11.4817948094672 + −0.103072169435291 × 2^ RCP
213FS = 0.963589896916147 + 4.56083275104788 × USPV ^(1/2)465FS = 10.8819830772816 + 0.240195832103802 × RCP ^(1/2)
214FS = −4.32508243714884 + 9.05905049595972 × USPV ^(1/3)466FS = 10.5923404701954 + 0.512067600446326 × RCP ^(1/3)
215FS = 2.6622701356421 + 12.1767129685834 × log(USPV)467FS = 11.0722894827807 + 0.642115587523053 × log(RCP)
216FS = 2.66227013564208 + 3.66555585213421 × lg(USPV)468FS = 11.0722894827807 + 0.19329605252784 × lg(RCP)
217HbRH = 68.5088143827834 + −5.71647747514457 × USPV469USPV = 5.99231505990734 + −0.641168070098011 × RCP
218HbRH = 53.0861857332109 + −0.52194876820546 × USPV ^2470USPV = 5.51082951115173 + −0.196770639884694 × RCP ^2
219HbRH = 47.9782012695454 + −0.0627945081108502 × USPV ^3471USPV = 5.33480011717637 + −0.0718816141889639 × RCP ^3
220HbRH = 43.4162462402041 + −0.0210529000617608 × e^ USPV472USPV = 5.58943973451332 + −0.113334749562755 × e^ RCP
221HbRH = 45.8348577834842 + −0.175122004454279 × 2^ USPV473USPV = 5.88333633268943 + −0.287937416420146 × 2^ RCP
222HbRH = 99.4128084239354 + −26.6311418511156 × USPV ^(1/2)474USPV = 6.89045968374231 + −1.53649400550554 × RCP ^(1/2)
223HbRH = 130.327235060512 + −52.9161669690371 × USPV ^(1/3)475USPV = 7.76902470819704 + −2.417778749196 × RCP ^(1/3)
224HbRH = 89.5584537535433 + −71.1931349289109 × log(USPV)476USPV = 5.33933071656506 + −1.99806201577142 × log(RCP)
225HbRH = 89.5584537535434 + −21.4312690989553 × lg(USPV)477USPV = 5.33933071656506 + −0.601476599944037 × lg(RCP)
226ERoS = −44.4898561732773 + 24.4984815259042 × USPV478HbRH = 42.0423782293484 + −1.48758153721214 × RCP
227ERoS = 18.6332502605124 + 2.35355883446629 × USPV ^2479HbRH = 41.0709689631091 + −0.515318025294051 × RCP ^2
228ERoS = 39.7125834810522 + 0.298139553955767 × USPV ^3480HbRH = 40.5117106435288 + −0.165583213312471 × RCP ^3
229ERoS = 58.2740201323325 + 0.117962114287251 × e^ USPV481HbRH = 40.9974382176738 + −0.24088810276325 × e^ RCP
230ERoS = 47.4896511762263 + 0.901006174693199 × 2^ USPV482HbRH = 41.7826752623931 + −0.665750517805537 × 2^ RCP
231ERoS = −170.590922018834 + 111.297801182333 × USPV ^(1/2)483HbRH = 43.2454450048409 + −2.8401263707606 × RCP ^(1/2)
232ERoS = −296.650864119786 + 219.314541365346 × USPV ^(1/3)484HbRH = 44.2855416269705 + −3.95501004850947 × RCP ^(1/3)
233ERoS = −124.288756274984 + 290.210321300233 × log(USPV)485HbRH = 40.1489323608852 + −2.24390039617392 × log(RCP)
234ERoS = −124.288756274984 + 87.3620117626516 × lg(USPV)486HbRH = 40.1489323608852 + −0.675481326530641 × lg(RCP)
235ASC = 12.7056584538935 + −2.05383018831603 × USPV487ERoS = 99.4644577413937 + −13.8232290332395 × RCP
236ASC = 7.42474725865513 + −0.197743106683585 × USPV ^2488ERoS = 88.526157863181 + −4.01721193944016 × RCP ^2
237ASC = 5.66197246714162 + −0.0251128822731464 × USPV ^3489ERoS = 84.5196933817461 + −1.37231471647666 × RCP ^3
238ASC = 4.11569164408351 + −0.01003606279162 × e^ USPV490ERoS = 89.5989881995607 + −2.20731976041961 × e^ RCP
239ASC = 5.01986392805905 + −0.0762694909654092 × 2^ USPV491ERoS = 95.9367653724852 + −5.81337610312006 × 2^ RCP
240ASC = 23.2575691266695 + −9.32181911366594 × USPV ^(1/2)492ERoS = 119.666620550924 + −33.8160568760288 × RCP ^(1/2)
241ASC = 33.8066223340896 + −18.3634660495521 × USPV ^(1/3)493ERoS = 139.34893446531 + −53.5168485493523 × RCP ^(1/3)
242ASC = 19.3652424955155 + −24.2863538785987 × log(USPV)494ERoS = 85.6356391257711 + −44.6518386412545 × log(RCP)
243ASC = 19.3652424955155 + −7.31092100276846 × lg(USPV)495ERoS = 85.6356391257711 + −13.4415427925656 × lg(RCP)
244RCP = 4.17276937555526 + −0.529795858393688 × USPV496ASC = −2.51848109170778 + 3.24667448853144 × RCP
245RCP = 2.8215531818394 + −0.0514416129538915 × USPV ^2497ASC = −0.203489407868408 + 1.04605755869761 × RCP ^2
246RCP = 2.36985609246673 + −0.00658572528011425 × USPV ^3498ASC = 0.685672739591328 + 0.392888626101718 × RCP ^3
247RCP = 1.97477200398597 + −0.00269246761070794 × e^ USPV499ASC = −0.642194562790037 + 0.606665572012053 × e^ RCP
248RCP = 2.2095241687276 + −0.0202348720060608 × 2^ USPV500ASC = −2.15552198342141 + 1.52125131772239 × 2^ RCP
249RCP = 6.87117560609697 + −2.39410754458009 × USPV ^(1/2)501ASC = −6.75795197625392 + 7.52651357171335 × RCP ^(1/2)
250RCP = 9.56852307231565 + −4.70927504528767 × USPV ^(1/3)502ASC = −10.8963360640752 + 11.6979653703423 × RCP ^(1/3)
251RCP = 5.85202639937843 + −6.20954309949019 × log(USPV)503ASC = 0.899397697886484 + 9.41369194818746 × log(RCP)
252RCP = 5.85202639937842 + −1.86925873231483 × lg(USPV)504ASC = 0.899397697886484 + 2.83380364634493 × lg(RCP)

Appendix C

This appendix supplements Section 3.5 by viewing the p( α ) (i.e., significance of the estimated α value), p( β ) (i.e., significance of the estimated β value) and ( R 2 ) (i.e., the adjusted R square value) of the SLR models in Table 5 from another perspective. Table A3, Table 4 and Table A5 re-sort the results by the transform method applied on the RHS independent variable in each SLR model. For each specific transform, the results for all pairs of variables are aggregated and summarised for clearer inspections.
The results are provided directly without any further marks for inspections. In addition, the order of the sub tables, from (a) to (h), follows the same order in Table 3, Table 6 and Table 7 for the different transformation method.
Table A3. SLR Models’ p( α ) Values for Each Pair of Variables, by Transform Method.
Table A3. SLR Models’ p( α ) Values for Each Pair of Variables, by Transform Method.
(a)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000010.0000000.0000000.0000000.0000000.0000920.000000
TS0.0000000.0000000.0000000.0000000.0000000.0000000.0000010.000000
FS0.0000000.0173220.0000000.0000000.0000000.0000030.0630990.000007
USPV0.0002170.2864490.0000000.0000000.0000110.1490370.0000020.000000
HbRH0.0000000.0000000.0000000.0000000.0000000.0000000.0001470.000000
ERoS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
ASC0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
RCP0.0000000.0000000.0000000.0000000.0000000.0000000.5735840.000000
(b)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0000000.0000000.0000000.0000030.000000
TS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
FS0.0000000.0000000.0000000.0000000.0000000.0000000.0069720.000000
USPV0.0000000.0004330.0000000.0000000.0000000.0000500.0000000.000000
HbRH0.0000000.0000000.0000000.0000000.0000000.0000000.0000050.000000
ERoS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
ASC0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
RCP0.0000000.0000000.0000000.0000000.0000000.0000000.0246590.000000
(c)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
TS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
FS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
USPV0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
HbRH0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
ERoS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
ASC0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
RCP0.0000000.0000000.0000000.0000000.0000000.0000000.1436160.000000
(d)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
TS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
FS0.0000000.0000000.0000000.0000000.0000000.0000000.0000010.000000
USPV0.0000000.0000030.0000000.0000000.0000000.0000000.0000000.000000
HbRH0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
ERoS0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
ASC0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
RCP0.0000000.0000000.0000000.0000000.0000010.0000000.0007690.000000
(e)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.1087510.0026710.0001000.5500160.0276120.000549
TS0.1761170.0000000.0604240.0000020.0000080.8390670.0024170.000036
FS0.0000600.0000180.0000000.0207690.0033880.6135440.7512450.175856
USPV0.2492430.0019850.8539720.0000000.0213100.0017800.0000730.000006
HbRH0.0000000.0000010.0000000.0000000.0000000.0000060.1594890.002875
ERoS0.0131460.7964160.0000970.0000070.0003960.0000000.0000400.000064
ASC0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
RCP0.0000000.0000040.0000000.0000000.0027210.0000010.0000020.000000
(f)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0004030.2362020.0006550.8703340.0491270.003082
TS0.0002650.0000000.3221550.0203860.0001310.3021750.0072080.000522
FS0.0000010.0000010.0000000.3352800.0121760.9451190.8932910.358140
USPV0.0869790.0005000.5829550.0000000.0426060.0004000.0001130.000020
HbRH0.0000010.0000250.0000000.0000000.0000000.0002210.3075280.034954
ERoS0.1906820.2187980.0102500.0284730.0036330.0000000.0001420.000813
ASC0.0000000.0000000.0000000.0000000.0000010.0000000.0000000.020166
RCP0.0000060.0001180.0001830.0000000.0297700.0000240.0000010.000000
(g)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000100.9630470.0019800.5711590.0705900.007804
TS0.0068730.0000000.9218760.0009220.0000730.6246400.0073690.000243
FS0.0000100.0000040.0000000.1011000.0084910.8304720.8288270.253466
USPV0.4194490.0037840.5308990.0000000.0111740.0044080.0000510.000003
HbRH0.0000120.0001090.0000050.0000000.0000000.0006240.3848500.081312
ERoS0.5159650.0964130.0856980.5109250.0126970.0000000.0003920.004012
ASC0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
RCP0.0000000.0000000.0000000.0000000.0000000.0000000.0033990.000000
(h)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000100.9630470.0019800.5711590.0705900.007804
TS0.0068730.0000000.9218760.0009220.0000730.6246400.0073690.000243
FS0.0000100.0000040.0000000.1011000.0084910.8304720.8288270.253466
USPV0.4194490.0037840.5308990.0000000.0111740.0044080.0000510.000003
HbRH0.0000120.0001090.0000050.0000000.0000000.0006240.3848500.081312
ERoS0.5159650.0964130.0856980.5109250.0126970.0000000.0003920.004012
ASC0.0000000.0000000.0000000.0000000.0000000.0000000.0000000.000000
RCP0.0000000.0000000.0000000.0000000.0000000.0000000.0033990.000000
Table A4. SLR Models’ p( β ) Values for Each Pair of Variables, by Transform Method.
Table A4. SLR Models’ p( β ) Values for Each Pair of Variables, by Transform Method.
(a)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0093940.0142430.0689100.0995590.067789
TS0.0000000.0000000.0000000.0000930.0099160.0002590.0132860.052104
FS0.0000000.0000000.0000000.0674510.0457920.2348880.8522310.996245
USPV0.0100630.0000900.0837750.0000000.1964460.0000280.0003360.000190
HbRH0.0096700.0101650.0478110.2805480.0000000.2240300.6846690.548015
ERoS0.0480530.0000840.1944460.0000030.1498330.0000000.0001780.023698
ASC0.2606600.0989070.7109120.0018110.5974070.0025670.0000000.000000
RCP0.0599450.0499720.7294100.0004450.7300790.0771820.0000000.000000
(b)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0119070.0140340.0629070.0883450.075272
TS0.0000000.0000000.0000000.0002370.0086120.0003170.0087750.056392
FS0.0000000.0000000.0000000.0695490.0310020.2435820.8748950.995302
USPV0.0132530.0001620.1070080.0000000.2264500.0000370.0003970.000197
HbRH0.0077690.0086330.0392530.4284300.0000000.2875370.5974160.382366
ERoS0.0318970.0000270.1781530.0000010.1407980.0000000.0000600.012067
ASC0.3538140.1885610.6878710.0061540.5130130.0078940.0000000.000004
RCP0.0625080.0503430.5383540.0010970.7753690.1221020.0000000.000000
(c)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0557660.0448460.1973400.3214620.4364680.3043120.602958
TS0.0001400.0000000.0047880.0973870.1256940.1347070.1138980.380960
FS0.0000000.0000790.0000000.0714350.0154650.4017190.7928100.777263
USPV0.0316940.0009700.2167090.0000000.3333750.0001190.0007800.000287
HbRH0.2711630.1681050.4053390.7375450.0000000.5971180.5066790.222821
ERoS0.6227990.0833280.8346750.0000550.8171840.0000000.0615800.112349
ASC0.3906760.3176730.6888280.0257750.4082850.0519720.0000000.000153
RCP0.0605090.0490790.6106540.0006810.7854200.1021840.0000000.000000
(d)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0540080.0438130.1961890.3184930.4322740.3011730.599052
TS0.0000060.0000000.0009540.0487840.0661380.0483890.0538100.282676
FS0.0000000.0000090.0000000.0708840.0117450.3405850.9211020.871662
USPV0.0206150.0004060.1549580.0000000.2771520.0000650.0005430.000228
HbRH0.1706460.0986500.3009680.8302200.0000000.5180740.4928450.174923
ERoS0.5308330.0470330.8194750.0000260.7746110.0000000.0294310.072328
ASC0.3347370.2065990.6990580.0087350.4736800.0149640.0000000.000009
RCP0.0592790.0490270.7145670.0004300.7602380.0800320.0000000.000000
(e)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0070710.0180240.0879810.1275520.063732
TS0.0000000.0000000.0000000.0000450.0204300.0005200.0382140.061495
FS0.0000000.0000000.0000000.0639280.0877510.2282180.8240970.985030
USPV0.0067260.0000370.0573420.0000000.1563940.0000190.0002780.000196
HbRH0.0233590.0198730.0906910.1305910.0000000.1464750.8135530.848792
ERoS0.1048150.0007580.2556010.0000590.1820400.0000000.0011510.068695
ASC0.0590990.0103150.9333970.0001370.9299250.0003860.0000000.000000
RCP0.0702130.0624840.8654210.0001500.7956130.0410550.0000000.000000
(f)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0069030.0187900.0910340.1315940.063793
TS0.0000000.0000000.0000000.0000450.0229410.0006100.0438040.064114
FS0.0000000.0000000.0000000.0635340.0945710.2280120.8214310.982807
USPV0.0064400.0000340.0549600.0000000.1523430.0000190.0002740.000198
HbRH0.0267390.0220830.0994470.1202530.0000000.1400530.8253410.880793
ERoS0.1146200.0009750.2656600.0000810.1870650.0000000.0014040.076639
ASC0.0470430.0081220.9608820.0001280.9952140.0003990.0000000.000000
RCP0.0730970.0656030.8181080.0001460.8184530.0395320.0000000.000000
(g)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0066150.0205900.0977970.1402590.064214
TS0.0000000.0000000.0000000.0000490.0293610.0008710.0576760.070523
FS0.0000000.0000000.0000000.0627570.1098890.2279500.8163820.977773
USPV0.0059120.0000280.0504930.0000000.1444870.0000180.0002660.000203
HbRH0.0355660.0276630.1204660.1029830.0000000.1287350.8463050.941104
ERoS0.1366670.0015940.2878370.0001530.1979020.0000000.0020560.094423
ASC0.0347890.0072370.9794970.0001930.8558840.0007430.0000000.000000
RCP0.0805360.0735750.7277050.0001540.8751530.0381170.0000000.000000
(h)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0066150.0205900.0977970.1402590.064214
TS0.0000000.0000000.0000000.0000490.0293610.0008710.0576760.070523
FS0.0000000.0000000.0000000.0627570.1098890.2279500.8163820.977773
USPV0.0059120.0000280.0504930.0000000.1444870.0000180.0002660.000203
HbRH0.0355660.0276630.1204660.1029830.0000000.1287350.8463050.941104
ERoS0.1366670.0015940.2878370.0001530.1979020.0000000.0020560.094423
ASC0.0347890.0072370.9794970.0001930.8558840.0007430.0000000.000000
RCP0.0805360.0735750.7277050.0001540.8751530.0381170.0000000.000000
Table A5. SLR Models’ ( R 2 ) Values for Each Pair of Variables, by Transform Method.
Table A5. SLR Models’ ( R 2 ) Values for Each Pair of Variables, by Transform Method.
(a)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.7299360.6561250.1582950.1395420.0673820.0506410.068132
TS0.7687820.0000000.5908710.3474190.1558700.3087170.1426900.080196
FS0.6706770.5873480.0000000.0683610.0861260.013040−0.028346−0.029411
USPV0.1552060.3486730.0584700.0000000.0205980.3904500.2985170.320593
HbRH0.1569950.1547550.0841440.0057500.0000000.015022−0.024357−0.018383
ERoS0.0839120.3510290.0210360.4633980.0323740.0000000.3230880.116357
ASC0.0087370.050938−0.0252000.230008−0.0208770.2151840.0000000.546710
RCP0.0737640.082114−0.0257420.287522−0.0257610.0622040.6579000.000000
(b)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.6887080.6288520.1476380.1402100.0715530.0560560.063348
TS0.7531090.0000000.5572780.3120800.1621800.3008340.1613420.076566
FS0.6673020.5673180.0000000.0669590.1040440.011528−0.028650−0.029411
USPV0.1428020.3265620.0473850.0000000.0145700.3799720.2919580.319156
HbRH0.1667800.1620740.093207−0.0103240.0000000.004761−0.020878−0.006231
ERoS0.1027380.3911070.0248080.5126830.0351210.0000000.3630270.147036
ASC−0.0033330.022356−0.0244650.177117−0.0163480.1660680.0000000.455422
RCP0.0718450.081774−0.0178450.250962−0.0269130.0414620.6133300.000000
(c)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0770770.0870860.0204030.000351−0.0109740.002503−0.021132
TS0.3321710.0000000.1881680.0516390.0401660.0370820.044579−0.006096
FS0.5303040.3533810.0000000.0657370.135809−0.008032−0.027294−0.026956
USPV0.1030320.2560060.0164220.000000−0.0010600.3381310.2649420.304715
HbRH0.0071260.027331−0.008356−0.0259670.000000−0.020864−0.0159530.015249
ERoS−0.0220050.058714−0.0280740.366523−0.0277710.0000000.0725300.045194
ASC−0.0070200.000814−0.0244970.112510−0.0086160.0803110.0000000.328825
RCP0.0733340.082942−0.0214780.270415−0.0271370.0494650.6298210.000000
(d)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0785480.0881560.0206540.000713−0.0106370.002914−0.020953
TS0.4394760.0000000.2567140.0832180.0692600.0835920.0787160.005445
FS0.5948530.4287160.0000000.0660910.148254−0.001882−0.029110−0.028610
USPV0.1227250.2910830.0308950.0000000.0062410.3602870.2795440.313564
HbRH0.0266780.0510560.002941−0.0280000.000000−0.016657−0.0150630.025602
ERoS−0.0174140.084898−0.0278130.392235−0.0268960.0000000.1064310.065169
ASC−0.0012170.018447−0.0248300.161547−0.0137590.1373030.0000000.426455
RCP0.0742760.082990−0.0253100.288809−0.0265540.0605510.6521880.000000
(e)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.7684790.6710150.1709640.1288480.0562430.0395120.070957
TS0.7421800.0000000.6003050.3734400.1231350.2812780.0944390.072593
FS0.6678060.6117420.0000000.0708160.0563620.014244−0.027895−0.029401
USPV0.1731870.3803830.0757990.0000000.0304890.4025930.3058910.319400
HbRH0.1170140.1243980.0548660.0384630.0000000.033374−0.027704−0.028295
ERoS0.0483180.2660890.0095410.3639490.0238740.0000000.2489630.067525
ASC0.0744160.154099−0.0291970.332853−0.0291740.2931310.0000000.697538
RCP0.0665250.071862−0.0285300.329451−0.0273520.0911440.6313580.000000
(f)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.7706300.6704690.1720300.1269530.0546950.0381220.070913
TS0.7345370.0000000.5970510.3731500.1178400.2749090.0881660.070683
FS0.6668090.6138890.0000000.0710990.0529670.014282−0.027848−0.029397
USPV0.1751080.3837370.0777460.0000000.0316430.4036350.3065040.319003
HbRH0.1108280.1195830.0506920.0421450.0000000.035356−0.027917−0.028721
ERoS0.0442950.2558250.0079600.3521570.0226990.0000000.2406970.062527
ASC0.0848880.164797−0.0293380.335491−0.0294110.2918140.0000000.699772
RCP0.0646860.069632−0.0277880.330484−0.0277940.0928810.6170750.000000
(g)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.7735450.6680250.1739230.1227790.0514490.0352910.070612
TS0.7165090.0000000.5878200.3704050.1065400.2604130.0755330.066324
FS0.6643690.6177790.0000000.0716630.0461890.014293−0.027756−0.029388
USPV0.1788900.3903150.0816370.0000000.0339770.4055200.3075960.318047
HbRH0.0977390.1092710.0420650.0491140.0000000.039100−0.028258−0.029244
ERoS0.0364410.2353840.0047190.3287810.0202820.0000000.2246510.053038
ASC0.0987530.169934−0.0293910.320016−0.0283990.2669060.0000000.672241
RCP0.0602650.064389−0.0256940.328499−0.0286540.0945560.5802260.000000
(h)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.7735450.6680250.1739230.1227790.0514490.0352910.070612
TS0.7165090.0000000.5878200.3704050.1065400.2604130.0755330.066324
FS0.6643690.6177790.0000000.0716630.0461890.014293−0.027756−0.029388
USPV0.1788900.3903150.0816370.0000000.0339770.4055200.3075960.318047
HbRH0.0977390.1092710.0420650.0491140.0000000.039100−0.028258−0.029244
ERoS0.0364410.2353840.0047190.3287810.0202820.0000000.2246510.053038
ASC0.0987530.169934−0.0293910.320016−0.0283990.2669060.0000000.672241
RCP0.0602650.064389−0.0256940.328499−0.0286540.0945560.5802260.000000

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Figure 1. Relationship between CS and RCP: (a) a rough trend was observed between CS and RCP; (b) visualising the result of clustering in the previous study. (Data source: Re-plot and New Plot).
Figure 1. Relationship between CS and RCP: (a) a rough trend was observed between CS and RCP; (b) visualising the result of clustering in the previous study. (Data source: Re-plot and New Plot).
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Figure 2. HPC Sample Parameters (Organised).
Figure 2. HPC Sample Parameters (Organised).
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Figure 3. Visualisation of the correlation matrix (no transform).
Figure 3. Visualisation of the correlation matrix (no transform).
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Figure 4. The correlation matrix visualised (no transform).
Figure 4. The correlation matrix visualised (no transform).
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Figure 5. The role of this research for HPC studies.
Figure 5. The role of this research for HPC studies.
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Table 1. Source data from experimental tests: (a) for CS and TS; (b) for FS and HbRH; (c) for USPV and ASC; (d) for RCP and ERoS.
Table 1. Source data from experimental tests: (a) for CS and TS; (b) for FS and HbRH; (c) for USPV and ASC; (d) for RCP and ERoS.
(a)
Parameter of HPC SampleCS of Sample at Days (MPa)TS of Sample at Days (MPa)
W/B Ratio% of FA and SF1728569117285691
0.28FA 0% SF 0%4265.373.9282.5495.437.3212.7416.1517.2422.05
FA 0% SF 10%31.756.368.5370.1688.045.399.8212.8615.1621.04
FA 10% SF 0%28.26068.175.3384.94.2810.2913.1315.3319.57
FA 10% SF 10%27.146.454.8867.3772.194.418.810.6914.8918.81
FA 20% SF 0%27.942.553.8860.4270.664.177.178.812.2914.95
FA 20% SF 10%25.840.552.3765.9576.743.716.948.212.3117.89
0.30FA 0% SF 0%35.750.660.570.386.595.1210.3114.1716.220.46
FA 0% SF 10%23.94857.0761.28774.888.7511.715.1620.01
FA 10% SF 0%17.749.259.6768.0373.013.089.512.1415.2718.83
FA 10% SF 10%16.138.747.7158.2560.353.317.218.7714.8718.24
FA 20% SF 0%1735.646.0253.7457.532.536.297.8112.9915.41
FA 20% SF 10%14.634.545.1755.1767.922.235.97.2213.6117.75
(b)
Parameter of HPC SampleFS of Sample at Days (MPa)HbRH of Sample at Days (MPa)
W/B Ratio% of FA and SF1728569117285691
0.28FA 0% SF 0%6.2911.6613.4913.7414.2137.6136.5833.0931.2627.92
FA 0% SF 10%3.799.7910.512.1812.4845.4142.5743.6840.3633.37
FA 10% SF 0%6.5410.6210.7712.3113.3953.4750.5144.9743.2437.17
FA 10% SF 10%4.88.799.9510.8411.7158.4755.5650.4252.2345.45
FA 20% SF 0%5.648.3710.0510.5610.8263.4865.6859.8960.7857.55
FA 20% SF 10%37.568.939.3510.1837.6136.5833.0931.2627.92
0.30FA 0% SF 0%6.1510.6112.4112.8113.3929.7829.0125.9519.523.94
FA 0% SF 10%3.388.8210.0211.8312.4144.3738.8140.9236.8330.73
FA 10% SF 0%6.249.7710.1911.9913.2652.4549.8644.2443.0134.15
FA 10% SF 10%4.458.529.410.4610.955854.4948.2448.8441.53
FA 20% SF 0%5.347.79.3710.1810.6363.3567.2658.0759.0754.52
FA 20% SF 10%2.897.478.339.1610.0129.7829.0125.9519.523.94
(c)
Parameter of HPC SampleUSPV of Sample at Days (m/s) Weight Loss at Days for ASC (%)
W/B Ratio% of FA and SF17285691285691
0.28FA 0% SF 0%4263.74794.74923.3527856535.073.350.57
FA 0% SF 10%3620.34135.34415.747814981.34.923.080.51
FA 10% SF 0%38164336.34545.74739.34859.74.812.470.27
FA 10% SF 10%3300.74380.3468547734908.72.231.320.21
FA 20% SF 0%3389.33930.34313.75454.358232.211.280.18
FA 20% SF 10%3648.74167.34634.74910.75748.31.250.790.05
0.30FA 0% SF 0%41044598469852365877.76.184.182.4
FA 0% SF 10%3442394943595078.352875.764.152.03
FA 10% SF 0%3777.343844578.34815.35386.75.213.221.04
FA 10% SF 10%3308.74407.34612.74819.753383.312.30.71
FA 20% SF 0%31283786.34231.35342.360483.811.870.61
FA 20% SF 10%3423.33905.34593.75111.359932.411.940.3
(d)
Parameter of HPC SampleCharge Passed for RCP (Coulombs)ERoS Tested at Days (kΩ-cm)
W/B Ratio% of FA and SF28569117285691
0.28FA 0% SF 0%1539.713341278.3621.432537.8977.1193.11
FA 0% SF 10%20221622.11031.6615.9624.2240.2278.7893.33
FA 10% SF 0%1893.71525.61277.9114.0325.4440.6777.7893.44
FA 10% SF 10%1569.91286.31090.0415.2726.334374.6797.45
FA 20% SF 0%1274.31093.2793.116.4820.4442.338296.78
FA 20% SF 10%1378.3990.4476.59322.0228.8947.3376.3393.33
0.30FA 0% SF 0%2051.91790.51650.6525.6746.9272.4482.7898.53
FA 0% SF 10%2541.31934.91626.5812.6344.6774.5583.6794.45
FA 10% SF 0%2315.21922.71709.1511.9646.22718290.67
FA 10% SF 10%2170.61658.21596.9610.147.1179.8985.4597.67
FA 20% SF 0%1528.61291.31019.5716.64177.2279.2298.78
FA 20% SF 10%1897.71366.8864.45527.7658.7281.4594.8998.33
Table 2. Correlation coefficients between each pair of variables (no transform).
Table 2. Correlation coefficients between each pair of variables (no transform).
CSTSFSUSPVHbRHERoSASCRCP
CS10.8753330.8242430.43716−0.398080.29562−0.2662−0.31178
TS0.87533310.7847650.622967−0.402340.562644−0.37139−0.32165
FS0.8242430.78476510.310713−0.305250.2053770.036492−0.00205
USPV0.437160.6229670.3107131−0.234280.645174−0.56893−0.58283
HbRH−0.39808−0.40234−0.30525−0.234281−0.23448−0.04958−0.05542
ERoS0.295620.5626440.2053770.645174−0.234481−0.54312−0.33091
ASC−0.2662−0.371390.036492−0.56893−0.04958−0.5431210.817532
RCP−0.31178−0.32165−0.00205−0.58283−0.05542−0.330910.8175321
Table 3. Correlation coefficients between each pair of variables, with different RHS variable transforms: (a) X = X 2 ; (b) X = X 3 ; (c) X = e X ; (d) X = 2 X ; (e) X = X ; (f) X = X 3 ; (g) X = log ( X ) ; (h) X = lg ( X ) ; (h) RHS Var. Transform: X = lg ( X ) .
Table 3. Correlation coefficients between each pair of variables, with different RHS variable transforms: (a) X = X 2 ; (b) X = X 3 ; (c) X = e X ; (d) X = 2 X ; (e) X = X ; (f) X = X 3 ; (g) X = log ( X ) ; (h) X = lg ( X ) ; (h) RHS Var. Transform: X = lg ( X ) .
(a)CSTSFSUSPVHbRHERoSASCRCP
CS---0.8588670.8160580.427017−0.405130.30664−0.27887−0.30783
TS0.880561---0.7762480.605032−0.424250.573121−0.40888−0.32631
FS0.8246740.77404---0.308186−0.335020.2030730.032173−0.00081
USPV0.4234890.6060380.292183---−0.220410.638643−0.56441−0.5831
HbRH−0.42554−0.42297−0.33213−0.18482---−0.20776−0.07007−0.10351
ERoS0.3317920.6079240.2213740.691903−0.24499---−0.58517−0.3763
ASC−0.19251−0.279380.063966−0.502−0.09105−0.48745---0.748105
RCP−0.31659−0.32915−0.05971−0.55487−0.05955−0.298330.817113---
(b)CSTSFSUSPVHbRHERoSASCRCP
CS---0.8352260.799660.414718−0.405930.313178−0.28814−0.30018
TS0.871874---0.7549350.575965−0.431410.566401−0.43047−0.32086
FS0.8226830.761367---0.30597−0.360060.1994250.027196−0.00102
USPV0.4090150.5880510.273135---−0.20670.630624−0.55874−0.5819
HbRH−0.43656−0.43129−0.34513−0.13617---−0.1822−0.09105−0.15006
ERoS0.3582930.6391430.2295010.725676−0.25038---−0.61744−0.41401
ASC−0.15917−0.224250.069324−0.44791−0.11265−0.43577---0.686281
RCP−0.31363−0.32865−0.106−0.52188−0.04927−0.262390.790176---
(c)CSTSFSUSPVHbRHERoSASCRCP
CS---0.3216310.3364060.219982−0.170040.133833−0.17608−0.08968
TS0.592665---0.4597430.280597−0.259980.254154−0.2681−0.1505
FS0.7373760.6098---0.304023−0.400630.144114−0.04536−0.04884
USPV0.3586910.5265580.211007---−0.165960.597529−0.53474−0.56972
HbRH−0.1884−0.23478−0.143020.057846---−0.09112−0.11434−0.20829
ERoS0.0848270.2925880.0360460.62018−0.03992---−0.31469−0.26921
ASC−0.14749−0.171350.0691−0.3713−0.14213−0.32648---0.589916
RCP−0.31593−0.33037−0.08779−0.53969−0.04701−0.276810.800249---
(d)CSTSFSUSPVHbRHERoSASCRCP
CS---0.3238440.3379480.220534−0.171070.135049−0.17721−0.09065
TS0.6749---0.527210.330775−0.30960.331323−0.3241−0.18401
FS0.7787350.667112---0.304588−0.415440.163534−0.01711−0.0279
USPV0.3844340.5579770.24204---−0.18610.615276−0.54784−0.57721
HbRH−0.23342−0.27959−0.177280.037031---−0.11131−0.11806−0.23117
ERoS0.107960.3332320.0394130.64−0.04944---−0.36326−0.30311
ASC−0.1655−0.215620.066715−0.4307−0.12331−0.40243---0.665464
RCP−0.31737−0.33044−0.06312−0.55599−0.05269−0.295620.813711---
(e)CSTSFSUSPVHbRHERoSASCRCP
CS---0.8803940.8248720.441192−0.3920940.288458−0.258755−0.312252
TS0.865763---0.7821280.625573−0.3849530.549375−0.346861−0.314787
FS0.8229810.789199---0.312032−0.2886580.2059330.038388−0.003242
USPV0.4436330.6309410.319695---−0.2412260.647813−0.570721−0.582105
HbRH−0.377150−0.386542−0.286130−0.256779---−0.246965−0.040729−0.032930
ERoS0.2747900.5357780.1945230.618160−0.227516---−0.520020−0.306866
ASC−0.317586−0.4222170.014438−0.593223−0.015192−0.559757---0.840345
RCP−0.305280−0.3136570.029273−0.590432−0.044729−0.3422150.801181---
(f)CSTSFSUSPVHbRHERoSASCRCP
CS---0.8815800.8245510.442364−0.3897390.285838−0.256134−0.312183
TS0.861465---0.7801050.625348−0.3782130.543715−0.337961−0.311825
FS0.8223920.790519---0.312473−0.2828870.2060230.038979−0.003723
USPV0.4457310.6335170.322639---−0.2435370.648594−0.571243−0.581773
HbRH−0.369097−0.380444−0.278953−0.263651---−0.250834−0.038112−0.025904
ERoS0.2675830.5263910.1905370.608824−0.224994---−0.512241−0.298850
ASC−0.333218−0.4343500.008473−0.595380−0.001036−0.558613---0.841635
RCP−0.302340−0.3101830.039716−0.591281−0.039640−0.3446710.792474---
(g)CSTSFSUSPVHbRHERoSASCRCP
CS---0.8831840.8231100.444438−0.3845030.280268−0.250707−0.311714
TS0.851240---0.7743360.623212−0.3634110.530608−0.319290−0.304959
FS0.8209500.792906---0.313347−0.2710000.2060500.040100−0.004813
USPV0.4498340.6385410.328445---−0.2481490.650004−0.572171−0.580974
HbRH−0.351451−0.367043−0.263505−0.276192---−0.257982−0.033478−0.012764
ERoS0.2529260.5071790.1820860.589881−0.219712---−0.496794−0.283008
ASC−0.352850−0.4400570.004440−0.5826190.031369−0.536518---0.825594
RCP−0.295152−0.3018610.060098−0.589648−0.027139−0.3470250.769558---
(h)CSTSFSUSPVHbRHERoSASCRCP
CS---0.8831840.8231100.444438−0.3845030.280268−0.250707−0.311714
TS0.851240---0.7743360.623212−0.3634110.530608−0.319290−0.304959
FS0.8209500.792906---0.313347−0.2710000.2060500.040100−0.004813
USPV0.4498340.6385410.328445---−0.2481490.650004−0.572171−0.580974
HbRH−0.351451−0.367043−0.263505−0.276192---−0.257982−0.033478−0.012764
ERoS0.2529260.5071790.1820860.589881−0.219712---−0.496794−0.283008
ASC−0.352850−0.4400570.004440−0.5826190.031369−0.536518---0.825594
RCP−0.295152−0.3018610.060098−0.589648−0.027139−0.3470250.769558---
Table 4. The Cos-Sim indices between each pair of variables (no transformation).
Table 4. The Cos-Sim indices between each pair of variables (no transformation).
CSTSFSUSPVHbRHERoSASCRCP
CS10.9917040.9947920.9868740.9230280.9700840.7660910.929148
TS0.99170410.9858010.9786040.8993980.9747610.7264420.906988
FS0.9947920.98580110.9902660.9380990.9710880.8026270.951239
USPV0.9868740.9786040.99026610.9478570.9833200.7712000.940099
HbRH0.9230280.8993980.9380990.94785710.9182750.7654500.916059
ERoS0.9700840.9747610.9710880.9833200.91827510.7128880.913845
ASC0.7660910.7264420.8026270.7712000.7654500.71288810.909864
RCP0.9291480.9069880.9512390.9400990.9160590.9138450.9098641
Table 5. Results from estimating and developing the models (some initial entries).
Table 5. Results from estimating and developing the models (some initial entries).
M#YXP-Co-Co α β p ( α ) p ( β ) p(M) R 2 ( R 2 )
1TSCS0.875333−3.6677130.2782090.04660.00000.00000.7662080.759331
2TSCS0.8588675.7663220.0019850.00000.00000.00000.7376520.729936
3TSCS0.8352268.9891670.0000180.00000.00000.00000.6976020.688708
4TSCS0.32163114.5688310.0000000.00000.05580.05580.1034470.077077
5TSCS0.32384414.5656440.0000000.00000.05400.05400.1048750.078548
6TSCS0.880394−22.3244744.5753310.00000.00000.00000.7750940.768479
7TSCS0.881580−40.93124013.8145830.00000.00000.00000.7771830.770630
8TSCS0.883184−62.85094142.7854090.00000.00000.00000.7800150.773545
9TSCS0.883184−62.85094112.8796920.00000.00000.00000.7800150.773545
10FSCS0.8242434.2439310.1045280.00000.00000.00000.6793760.669946
11FSCS0.8160587.7578080.0007520.00000.00000.00000.6659500.656125
12FSCS0.7996608.9628740.0000070.00000.00000.00000.6394570.628852
13FSCS0.33640611.0870360.0000000.00000.04480.04480.1131690.087086
14FSCS0.33794811.0859070.0000000.00000.04380.04380.1142090.088156
15FSCS0.824872−2.6961661.7104490.10880.00000.00000.6804140.671015
16FSCS0.824551−9.6160355.1555100.00040.00000.00000.6798840.670469
17FSCS0.823110−17.69315615.9103700.00000.00000.00000.6775100.668025
18FSCS0.823110−17.6931564.7894980.00000.00000.00000.6775100.668025
19USPVCS0.4371603.8574980.0175830.00000.00770.00770.1911080.167318
20USPVCS0.4270174.4562690.0001250.00000.00940.00940.1823440.158295
21USPVCS0.4147184.6595170.0000010.00000.01190.01190.1719910.147638
22USPVCS0.2199825.0051730.0000000.00000.19730.19730.0483920.020403
23USPVCS0.2205345.0049760.0000000.00000.19620.19620.0486350.020654
24USPVCS0.4411922.6703800.2901470.00270.00710.00710.1946510.170964
25USPVCS0.4423641.4858020.8772040.23620.00690.00690.1956860.172030
26USPVCS0.4444380.0798302.7245810.96300.00660.00660.1975250.173923
27USPVCS0.4444380.0798300.8201810.96300.00660.00660.1975250.173923
28HBRHCS−0.39807765.693972−0.3906630.00000.01620.01620.1584650.133714
29HBRHCS−0.40512552.917551−0.0028910.00000.01420.01420.1641260.139542
30HBRHCS−0.40592548.479311−0.0000270.00000.01400.01400.1647750.140210
31HBRHCS−0.17003640.1336080.0000000.00000.32150.32150.0289120.000351
32HBRHCS−0.17106840.1385310.0000000.00000.31850.31850.0292640.000713
33HBRHCS−0.39209490.813888−6.2917650.00010.01800.01800.1537380.128848
34HBRHCS−0.389739115.838473−18.8576280.00070.01880.01880.1518970.126953
35HBRHCS−0.384503144.146418−57.5149720.00200.02060.02060.1478430.122779
36HBRHCS−0.384503144.146418−17.3137320.00200.02060.02060.1478430.122779
Table 6. SLR models’ p values for each pair of variables, by different RHS variable transform methods: (a) X = X 2 ; (b) X = X 3 ; (c) X = e X ; (d) X = 2 X ; (e) X = X ; (f) X = X 3 ; (g) X = log ( X ) ; (h) X = lg ( X ) .
Table 6. SLR models’ p values for each pair of variables, by different RHS variable transform methods: (a) X = X 2 ; (b) X = X 3 ; (c) X = e X ; (d) X = 2 X ; (e) X = X ; (f) X = X 3 ; (g) X = log ( X ) ; (h) X = lg ( X ) .
(a)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0093940.0142430.0689100.0995590.067789
TS0.0000000.0000000.0000000.0000930.0099160.0002590.0132860.052104
FS0.0000000.0000000.0000000.0674510.0457920.2348880.8522310.996245
USPV0.0100630.0000900.0837750.0000000.1964460.0000280.0003360.000190
HbRH0.0096700.0101650.0478110.2805480.0000000.2240300.6846690.548015
ERoS0.0480530.0000840.1944460.0000030.1498330.0000000.0001780.023698
ASC0.2606600.0989070.7109120.0018110.5974070.0025670.0000000.000000
RCP0.0599450.0499720.7294100.0004450.7300790.0771820.0000000.000000
(b)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0119070.0140340.0629070.0883450.075272
TS0.0000000.0000000.0000000.0002370.0086120.0003170.0087750.056392
FS0.0000000.0000000.0000000.0695490.0310020.2435820.8748950.995302
USPV0.0132530.0001620.1070080.0000000.2264500.0000370.0003970.000197
HbRH0.0077690.0086330.0392530.4284300.0000000.2875370.5974160.382366
ERoS0.0318970.0000270.1781530.0000010.1407980.0000000.0000600.012067
ASC0.3538140.1885610.6878710.0061540.5130130.0078940.0000000.000004
RCP0.0625080.0503430.5383540.0010970.7753690.1221020.0000000.000000
(c)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0557660.0448460.1973400.3214620.4364680.3043120.602958
TS0.0001400.0000000.0047880.0973870.1256940.1347070.1138980.380960
FS0.0000000.0000790.0000000.0714350.0154650.4017190.7928100.777263
USPV0.0316940.0009700.2167090.0000000.3333750.0001190.0007800.000287
HbRH0.2711630.1681050.4053390.7375450.0000000.5971180.5066790.222821
ERoS0.6227990.0833280.8346750.0000550.8171840.0000000.0615800.112349
ASC0.3906760.3176730.6888280.0257750.4082850.0519720.0000000.000153
RCP0.0605090.0490790.6106540.0006810.7854200.1021840.0000000.000000
(d)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0540080.0438130.1961890.3184930.4322740.3011730.599052
TS0.0000060.0000000.0009540.0487840.0661380.0483890.0538100.282676
FS0.0000000.0000090.0000000.0708840.0117450.3405850.9211020.871662
USPV0.0206150.0004060.1549580.0000000.2771520.0000650.0005430.000228
HbRH0.1706460.0986500.3009680.8302200.0000000.5180740.4928450.174923
ERoS0.5308330.0470330.8194750.0000260.7746110.0000000.0294310.072328
ASC0.3347370.2065990.6990580.0087350.4736800.0149640.0000000.000009
RCP0.0592790.0490270.7145670.0004300.7602380.0800320.0000000.000000
(e)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0070710.0180240.0879810.1275520.063732
TS0.0000000.0000000.0000000.0000450.0204300.0005200.0382140.061495
FS0.0000000.0000000.0000000.0639280.0877510.2282180.8240970.985030
USPV0.0067260.0000370.0573420.0000000.1563940.0000190.0002780.000196
HbRH0.0233590.0198730.0906910.1305910.0000000.1464750.8135530.848792
ERoS0.1048150.0007580.2556010.0000590.1820400.0000000.0011510.068695
ASC0.0590990.0103150.9333970.0001370.9299250.0003860.0000000.000000
RCP0.0702130.0624840.8654210.0001500.7956130.0410550.0000000.000000
(f)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0069030.0187900.0910340.1315940.063793
TS0.0000000.0000000.0000000.0000450.0229410.0006100.0438040.064114
FS0.0000000.0000000.0000000.0635340.0945710.2280120.8214310.982807
USPV0.0064400.0000340.0549600.0000000.1523430.0000190.0002740.000198
HbRH0.0267390.0220830.0994470.1202530.0000000.1400530.8253410.880793
ERoS0.1146200.0009750.2656600.0000810.1870650.0000000.0014040.076639
ASC0.0470430.0081220.9608820.0001280.9952140.0003990.0000000.000000
RCP0.0730970.0656030.8181080.0001460.8184530.0395320.0000000.000000
(g)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0066150.0205900.0977970.1402590.064214
TS0.0000000.0000000.0000000.0000490.0293610.0008710.0576760.070523
FS0.0000000.0000000.0000000.0627570.1098890.2279500.8163820.977773
USPV0.0059120.0000280.0504930.0000000.1444870.0000180.0002660.000203
HbRH0.0355660.0276630.1204660.1029830.0000000.1287350.8463050.941104
ERoS0.1366670.0015940.2878370.0001530.1979020.0000000.0020560.094423
ASC0.0347890.0072370.9794970.0001930.8558840.0007430.0000000.000000
RCP0.0805360.0735750.7277050.0001540.8751530.0381170.0000000.000000
(h)CSTSFSUSPVHbRHERoSASCRCP
CS0.0000000.0000000.0000000.0066150.0205900.0977970.1402590.064214
TS0.0000000.0000000.0000000.0000490.0293610.0008710.0576760.070523
FS0.0000000.0000000.0000000.0627570.1098890.2279500.8163820.977773
USPV0.0059120.0000280.0504930.0000000.1444870.0000180.0002660.000203
HbRH0.0355660.0276630.1204660.1029830.0000000.1287350.8463050.941104
ERoS0.1366670.0015940.2878370.0001530.1979020.0000000.0020560.094423
ASC0.0347890.0072370.9794970.0001930.8558840.0007430.0000000.000000
RCP0.0805360.0735750.7277050.0001540.8751530.0381170.0000000.000000
Table 7. SLR models’ R2 values for each pair of variables, by different RHS variable transform methods: (a) X = X 2 ; (b) X = X 3 ; (c) X = e X ; (d) X = 2 X ; (e) X = X ; (f) X = X 3 ; (g) X = log ( X ) ; (h) X = lg ( X ) .
Table 7. SLR models’ R2 values for each pair of variables, by different RHS variable transform methods: (a) X = X 2 ; (b) X = X 3 ; (c) X = e X ; (d) X = 2 X ; (e) X = X ; (f) X = X 3 ; (g) X = log ( X ) ; (h) X = lg ( X ) .
(a)CSTSFSUSPVHbRHERoSASCRCP
CS---0.7376520.6659500.1823440.1641260.0940280.0777660.094757
TS0.775388---0.6025600.3660640.1799880.3284680.1671840.106476
FS0.6800870.599138---0.0949790.1122370.0412390.0010350.000001
USPV0.1793430.3672830.085371---0.0485810.4078650.3185590.340004
HbRH0.1810810.1789050.1103120.034157---0.0431640.0049100.010714
ERoS0.1100860.3695710.0490060.4787300.060021---0.3424280.141604
ASC0.0370590.0780540.0040920.2520080.0082910.237607---0.559661
RCP0.1002270.1083390.0035650.3078780.0035470.0889980.667674---
(b)CSTSFSUSPVHbRHERoSASCRCP
CS---0.6976020.6394570.1719910.1647750.0980800.0830260.090109
TS0.760163---0.5699270.3317350.1861180.3208100.1853040.102950
FS0.6768070.579680---0.0936180.1296420.0397700.0007400.000001
USPV0.1672930.3458030.074603---0.0427250.3976870.3121880.338609
HbRH0.1905860.1860150.1191150.018542---0.0331960.0082900.022518
ERoS0.1283740.4085040.0526710.5266060.062689---0.3812270.171407
ASC0.0253340.0502890.0048060.2006280.0126910.189895---0.470982
RCP0.0983630.1080090.0112360.2723630.0024280.0688490.624378---
(c)CSTSFSUSPVHbRHERoSASCRCP
CS---0.1034470.1131690.0483920.0289120.0179110.0310030.008043
TS0.351252---0.2113640.0787350.0675900.0645940.0718760.022650
FS0.5437240.371856---0.092430.1605010.0207690.0020570.002386
USPV0.1286590.2772630.044524---0.0275420.3570410.2859440.324581
HbRH0.0354940.0551220.0204550.003346---0.0083040.0130740.043385
ERoS0.0071960.0856070.0012990.3846230.001594---0.0990290.072474
ASC0.0217520.0293620.0047750.1378670.0202020.106588---0.348001
RCP0.099810.1091440.0077070.2912610.0022100.0766230.640398---
(d)CSTSFSUSPVHbRHERoSASCRCP
CS---0.1048750.1142090.0486350.0292640.0182380.0314020.008217
TS0.455491---0.2779510.1094120.0958530.1097750.1050390.033861
FS0.6064280.445038---0.0927740.172590.0267430.0002930.000779
USPV0.147790.3113380.058583---0.0346340.3785650.3001280.333176
HbRH0.0544870.0781680.0314280.001371---0.012390.0139390.053442
ERoS0.0116550.1110440.0015530.4095990.002444---0.1319610.091879
ASC0.027390.0464910.0044510.1855030.0152060.161951---0.442842
RCP0.1007250.1091910.0039840.3091290.0027760.0873930.662126---
(e)CSTSFSUSPVHbRHERoSASCRCP
CS---0.7750940.6804140.1946510.1537380.0832080.0669540.097501
TS0.749546---0.6117240.3913410.1481880.3018130.1203120.099091
FS0.6772980.622835---0.0973640.0833230.0424090.0014741.05 × 10−5
USPV0.196810.3980860.102205---0.058190.4196620.3257230.338846
HbRH0.1422420.1494150.081870.065935---0.0609920.0016590.001084
ERoS0.0755090.2870580.0378390.3821210.051764---0.2704210.094167
ASC0.1008610.1782680.0002080.3519140.0002310.313327---0.70618
RCP0.0931960.098380.0008570.348610.0020010.1171110.64189---
(f)CSTSFSUSPVHbRHERoSASCRCP
CS---0.7771830.6798840.1956860.1518970.0817030.0656040.097458
TS0.742121---0.6085640.391060.1430450.2956260.1142180.097235
FS0.6763280.624921---0.0976390.0800250.0424450.0015191.39 × 10−5
USPV0.1986760.4013440.104096---0.059310.4206740.3263180.33846
HbRH0.1362330.1447370.0778150.069512---0.0629180.0014530.000671
ERoS0.0716010.2770870.0363040.3706670.050622---0.2623910.089311
ASC0.1110340.188667.18 × 10−50.3544771.07 × 10−60.312048---0.70835
RCP0.0914090.0962140.0015770.3496130.0015710.1187980.628015---
(g)CSTSFSUSPVHbRHERoSASCRCP
CS---0.7800150.677510.1975250.1478430.078550.0628540.097166
TS0.724609---0.5995960.3883930.1320670.2815440.1019460.093
FS0.6739590.6287---0.0981870.0734410.0424560.0016082.32 × 10−5
USPV0.202350.4077340.107876---0.0615780.4225050.3273790.337531
HbRH0.1235180.134720.0694350.076282---0.0665550.0011210.000163
ERoS0.0639720.257230.0331550.3479590.048274---0.2468040.080094
ASC0.1245030.193651.97 × 10−50.3394450.0009840.287851---0.681605
RCP0.0871150.091120.0036120.3476840.0007370.1204260.592219---
(h)CSTSFSUSPVHbRHERoSASCRCP
CS---0.7800150.677510.1975250.1478430.078550.0628540.097166
TS0.724609---0.5995960.3883930.1320670.2815440.1019460.093
FS0.6739590.6287---0.0981870.0734410.0424560.0016082.32 × 10−5
USPV0.202350.4077340.107876---0.0615780.4225050.3273790.337531
HbRH0.1235180.134720.0694350.076282---0.0665550.0011210.000163
ERoS0.0639720.257230.0331550.3479590.048274---0.2468040.080094
ASC0.1245030.193651.97 × 10−50.3394450.0009840.287851---0.681605
RCP0.0871150.091120.0036120.3476840.0007370.1204260.592219---
Table 8. Simplified and visualised information for Table 2.
Table 8. Simplified and visualised information for Table 2.
CSTSFSUSPVHbRHERoSASCRCP
CS0.8753330.8242430.43716−0.39808
TS0.8753330.7847650.622967−0.40234
FS0.8242430.7847650.310713−0.30525
USPV0.437160.6229670.310713−0.23428
HbRH−0.39808−0.40234−0.30525−0.23428
ERoS −0.54312−0.33091
ASC −0.543120.817532
RCP −0.330910.817532
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Zhuang, Z.-Y.; Kuo, W.-T. Unravelling the Relations between and Predictive Powers of Different Testing Variables in High Performance Concrete Experiments: The Data-Driven Analytical Methods. Buildings 2022, 12, 1545. https://doi.org/10.3390/buildings12101545

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Zhuang Z-Y, Kuo W-T. Unravelling the Relations between and Predictive Powers of Different Testing Variables in High Performance Concrete Experiments: The Data-Driven Analytical Methods. Buildings. 2022; 12(10):1545. https://doi.org/10.3390/buildings12101545

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Zhuang, Zheng-Yun, and Wen-Ten Kuo. 2022. "Unravelling the Relations between and Predictive Powers of Different Testing Variables in High Performance Concrete Experiments: The Data-Driven Analytical Methods" Buildings 12, no. 10: 1545. https://doi.org/10.3390/buildings12101545

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