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Article

Experimental and Numerical Study on the Effect of the Temperature-Control Curtain in Thermal Stratified Reservoirs

State Key Laboratory of Hydraulic Engineering Simulation and Safety, Tianjin University, Tianjin 300072, China
*
Author to whom correspondence should be addressed.
Appl. Sci. 2019, 9(24), 5354; https://doi.org/10.3390/app9245354
Submission received: 2 November 2019 / Revised: 30 November 2019 / Accepted: 5 December 2019 / Published: 8 December 2019
(This article belongs to the Special Issue Water-Energy-Environment Nexus (WEEN-2019))

Abstract

:
The impoundment and power generation of dams cause the temperature of released water much lower than the original rivers in the thermal stratified reservoirs. In addition, the released low-temperature water would damage the downstream habitats of fish and other biological groups seriously. Available facilities, such as stop log gate intakes and multi-level intakes, are built to alleviate the problem. For overcoming the limitations of traditional facilities on construction conditions and the improved effect of water temperature, a new facility of the temperature control curtain (TCC), with the advantages of convenient regulation and no hydropower loss, has been proposed recently. However, to the author’s knowledge, the theory of TCC is not abundant, with incomplete experimental tests and few numerical simulations. In this paper, a rectangular tank is designed specifically to conduct experimental tests to verify the effects of TCC and explore its potential impacts on released water temperature (RWT) under four major influencing factors. The study results show that TCC has significant effects on improving RWT, with a maximum increase of 8.3 °C. In addition, a three-dimensional hydrodynamic model with the same size of experimental model is established for further research. The results show that RWT is mainly related to the temperature distribution of a reservoir and the water-retaining proportion of the curtain. Finally, a basic principle for TCC construction is proposed and all these laid an important theory foundation for its application in engineering practice.

1. Introduction

Hydraulic engineering projects aim to achieve efficient utilization of water resources. While generating economic benefits, they also change the natural properties of rivers and have significant impacts on the reservoir ecology [1,2,3,4]. Due to the construction of hydraulic structures, large amounts of water are stored behind dams, which results in deep water with low-velocity flow. These conditions mean that vertical temperature stratification frequently occurs in these deep reservoirs [5,6,7]. Water temperature impacts the transportation of oxygen and other nutrients, as well as biological and chemical reaction rates [8,9,10]. For example, temperature is closely related to the concentration of dissolved oxygen, nitrogen, and phosphorus in water [11,12]. Spawning and growing of fish depend on the water temperature also. Thus, cooler temperatures can change or potentially destroy the downstream habitats of fish and other biological groups, pushing them to the verge of extinction [13,14]. In addition, using cooler temperatures to irrigate can directly reduce the crop yields. Many hydropower engineering projects are affected by low-temperature released water like Glen Canyon Dam and Cherokee Dam in America and the Three Gorges Dam and San Ban Xi Dam in China [15,16,17,18]. Especially in China during the last decade, every large hydraulic project should pass the Environmental Protection Assessment of the China Ministry of Environmental Protection to evaluate the impacts of cool released water from the reservoir on the downstream ecology before its construction. Therefore, increasing the released water temperature (RWT) is extremely significant and imperative for reducing the impacts of hydraulic engineering and promoting efficient utilization of water resources.
To resolve this issue, the principle of selective withdrawal was proposed. This involves drawing from a specific layer (thickness determined by a range in depth) of water in the reservoir [19,20]. From 1966, the U.S. Army Corps of Engineers initiated a laboratory to research the characteristics of the withdrawal zone in stratified reservoirs [21,22]. Several facilities adopted practices to regulate the outflow temperature, including a stop log gate [15] and side-type orifice outlet [23]. However, these facilities are severely limited and are subject to malpractice. Most importantly, such practices can only be used in the planning or construction stage; once hydropower stations are in operation, reducing the water level in reservoirs seriously degrades power generation and irrigation efficiency. Secondly, facilities such as stop log gates cause the loss of water head [24]. Taking the Guangzhao Hydropower Station as an example, a set of stop log gates cause a 1~2 m head loss, with an annual power loss of about 26 million kW·h [25]. Therefore, as alternative temperature control measures, some flexible structures have recently been adopted in some hydraulic projects. Focusing on a reservoir which has impounded water, the temperature-control curtain (TCC) is an effective facility of selective withdrawal [26,27,28,29,30]. The TCC is made of an impermeable fabric that can block water flow, forcing water to move above or below it. The TCC can be constructed either on dry land or in a restrained reservoir; moreover, it costs less than other facilities. In summary, compared with other selective withdrawal structures, TCC has the advantages of simpler structure, more convenient construction, and lower requirements for maintenance related to water flow [31].
The previous studies of TCC have showed the effect on raising the RWT [32], and simulated the changed thermal stratification structure of reservoirs influenced by TCC. But most of the previous studies on TCC were based on numerical simulation, resulting in a lack of validation by experimental tests. Thus, an experimental test was carried out in this study, as well as a numerical simulation test, for verifying the effect of TCC and exploring its potential impacts on RWT under different influence factors. In addition, the experimental test and numerical simulation test are all based on a model where the topography and temperature structure are generalized instead of focusing on a specific project. Through the analysis of flow and temperature fields observed and simulated, a basic principle for TCC construction is proposed at last. This paper is divided into five sections. The descriptions for experimental tests and numerical tests are, respectively, in Section 2 and Section 3. Section 4 shows the Results and Analysis; the conclusions are presented in Section 5.

2. Experimental Test

2.1. Test Methods

A rectangular tank which is 7.2 m long, 0.6 m wide, and 1.3 m high was specially designed for the tests. It was composed of three parts: the steady-flow zone, test zone, and outflow zone (Figure 1). The photos of experimental model are shown in Figure A1. There were two intakes, respectively, sitting on the top and the bottom in front of the steady-flow zone, which can pump water from different places to maintain a specific water stratification of the test zone. Several diversion tubes and a breakwater were used to represent the outlets with different heights, and each outlet was equipped with a sensor to measure the RWT. A nylon fabric curtain can be placed a certain distance from the outlet, with the bottom side fixed, the left and right top corners dragging fixed by ropes, and the top side opening.
High-power electric heat tubes were used to form the thermal stratification before the test at the same time digital temperature sensors, electromagnetic flowmeters, and graduated scales were, respectively, used to measure the water temperature, flow rates, and water level. In order to observe the vertical distribution of water during the test, the digital temperature sensors were set as follow: there were 3 temperature sensors groups and 13 sensors in each group. The sensors were set vertically with intervals of 0.05 m between the depth of 0.05 and 0.65 m below the surface in each group.
Before the tests, each electric heat tube was dipped into water by ropes, one end of the ropes was tied to the tubes and the other tied to the top of tank. The tubes’ immersion depth can be adjusted artificially by changing the length of ropes until the thermal structure of water was the same as target stratification. During the test, the high temperature water flowed into the steady-flow zone from the top intake, as the target thermal stratification, while the lowest from the bottom intake one. Thus, the steady thermal stratification can be maintained for more than 25 min according to repeated experiments, which was enough for a set of the scenario. For every test, flow and water temperature fields need approximately 5~10 min to stabilize, and the continuous monitoring was carried out for 20 min.

2.2. Generalization of Thermal Stratification

Based upon previous studies, thermal stratification influences the effect of TCC mostly. However, it is complicated owing to a variation of the topography and climates of a reservoir. To generalize the most representative thermal stratification, five hydraulic engineering projects which have the low-temperature released water problems were selected. They are all river-type reservoirs, with the dam heights more than 150 m, including Sanbanxi, Nuozhadu, Ertan, and Xiluodu projects in China and the Glen Canyon Dam in America. As shown in Figure 2a, May and August were chosen to represent the spring and summer, respectively, when the lower RWT was obvious.
The thermal stratification characteristics of these reservoirs can be generalized into two types: single thermocline and double thermocline. Single thermocline (S1) distribution refered to a clear vertical thermal stratification with a three-layer structure, comprising an upper mixed layer, a middle thermocline layer, and the hypolimnion layer at the bottom of the reservoir. This stratification was more stable and the thermocline had uniform temperature gradients. Double thermoclines (S2) included two thermoclines, upper and lower. There was a mixed layer between the two areas with more sharp gradients.
Considering the size of tank, two curves with the characteristics of S1 and S2 stratification were designed, respectively, and the curves were shown in Figure 2b. Through adjusting the depth and location of high-power electric heat tubes, the vertical temperature measured in the tank at the beginning of tests were almost the same as the designed curves (Figure 2b).

2.3. Model Scenarios

The factors influencing RWT mostly in a reservoir are the property of curtains and the discharge rules besides thermal structure [31,32]. Thus, four characteristic variables were proposed to represent the main influencing factors.
  • Curtain position (CP), means the distance from the curtain to the outlet, with the unit of m.
  • The water-retaining proportion (Pr), means the proportion of retaining water depth of TCC to the overall depth of the water, with the unit of %.
  • Outlet submerged depth (OSD), means the depth from the water surface to the centerline of the outlet, with the unit of cm.
  • Released flow quantity (RQ), means the flow quantity released from the outlet, with the unit of m3/h.
By comprehensive consideration of the possible flow fields of the real flow fields, model similarity scales, and conditions of construction sites for the typical reservoirs with low released temperature water problems, a series of scenarios were designed in Table 1. Three typical distances of CP were selected, which were 1.0, 2.5, and 3.5 m. From an engineering view, for most of reservoirs the closer to upstream the larger river cross-section is, the more difficult the construction is, thus the place of TCC will not be very far from the outlet. Our discussion about the influence of curtain position on TCC was carried out on this basis. Pr can be set from 55% to 90%. During summer and autumn, when the lower RWT is obvious, the spillway outlet is the usual way of discharge, thus OSDs were set from 24 to 40 cm, while the water level maintains 90 cm during all the tests. General outflow discharged from reservoirs has a large range, the range of released water quantity we discussed should be in the suitable range of a thermal stratification reservoir troubled by low released water temperature. Thus, take the example of the Sanbanxi project, outflow changes between 125 to 870 m3/s [33], and so the RQ was set from 1.6 to 11 m3/h. The tests were carried out inside a laboratory, so only air temperature was considered in meteorological conditions with a daily measurement.

3. Three-Dimensional Numerical Simulation

3.1. Model Description

At the meantime, Flow-3D was used to build a three-dimensional hydrodynamic and temperature numerical model with the same size of the experimental test model (Figure 3a), for the further research of TCC. The model was divided into 145 longitudinal segments, 45 vertical layers, and 20 lateral segments. Based upon the phenomenon of the experimental test, TCC appeared arc-shaped because of the thrust force by flow and its flexibility, and the fields around the curtain were the most concerned. Thus, for the test zone, 45 segments were set in the upstream forebay zone and 25 segments were set in the curtain zone to give a better show of the arc-shaped curtain for obtaining more details (Figure 3b).
The grid-independence tests were taken before the numerical simulation. For working condition A1, the RWT with different grid sizes were compared, as shown in Table 2. It can be concluded that variation in RWT basically did not with the grid size increase and decrease, both vertical and longitudinal; however, the water temperature of the outflow changes by up to 2%. Therefore, the mesh generation method described in this paper was determined by considering the calculation precision and calculation amount comprehensively.
Since the mechanical characteristics were not concerned, the curtain was simplified as a rigid arc-shaped structure without regard to flexibility.
The boundary conditions and scenarios were set the same as the experimental tests. After repeated adjustment, the bottom Manning coefficient was set as 0.01, the coefficient of bottom heat exchange was set as 0.3 W/(m2 °C), and dynamic viscosity and thermal conductivity of fluid were set according to water properties at different temperatures.
In order to cover the shortage of experimental tests, the numerical model’s scenarios were as a supplement and improvement to experimental tests. Thus, each variable set multiple scenarios; taking Pr as an example, the numerical model scenarios were set the same as model tests and with 95%, 92%, 80%, 62%, 50%, and 48% added at the same time. Through a lot of numerical simulation, the accuracy of the physical model was verified and the principle of TCC was summarized as well.

3.2. Model Verification

To verify the accuracy of the numerical model, simulated vertical temperature distributions before and after TCC were extracted and compared with the values measured in experimental tests under the same scenario. The scenarios selected were A1 and B1, and results were shown in Figure 4 and Figure 5. The root mean square error (RMSE) and coefficient of determination (R2) were used to evaluate the matching degree [34,35]. The goodness-of-fit tests and the statistic error labeled in figures showed that the 3-D numerical model matched the experimental model well and can accurately simulate the temperature fields.

4. Results and Analysis

4.1. The effect of TCC and Cause Analysis

The comparison of the RWT results under different scenarios from physical models were shown in Table 1 and Figure 6. For different Pr values, RWTs were increased by 6.8~8.3 °C under S1 thermal distribution and 2.3~3.5 °C for S2 distribution. TCC had a significant effect on RWT, but the degree of improvement was related closely to the thermal stratification of the reservoir.
In order to reveal the reason why TCC has a good effect on RWT, baseline scenarios A0 and A1 were analyzed primarily to make a contrast with others. The water upstream of the dam was subjected to a pulling force as a function of the discharge through the power station and to buoyancy differences caused by density stratification [36]. When the thermal stratification of water was strong, vertical mixing was inhibited, and the flow field in front of the dam was characterized by stratified water intake. As shown in Figure 7a, the water flow was stratified, and the pulling due to discharge of water only drove the water within a certain vertical range. However, when the TCC was set as shown in Figure 7b, the flow field changed dramatically. The flow of the water in front of and above the TCC was strengthened and the longitudinal velocity of all sections were enhanced. Then the major plume of the faster water from upstream flowed across the top of the TCC and plunges (mainly) into the layers level with the outlet. Between the outlet and the TCC, the water pulled by the discharge was still on the same horizontal line as the outlet, with an enlarged range of influence. However, it could also be concluded from the results of the physical model tests and numerical simulation that the lateral gradient of the water temperature and lateral flow velocity in the water were small and negligible. Therefore, the analysis below was focused on the action in the longitudinal and vertical directions.

4.2. Analysis of Influencing Factors

The comparisons between numerical simulation results and physical model tests in different scenarios were shown in Figure 8a, Figure 9a and Figure 10a. The flow and temperature fields of the different scenarios were shown in Figure 8b, Figure 9b and Figure 10b.

4.2.1. Effect of CP

From the results of A1~A3 and B1~B3 (Table 1), the change of the curtain’s position had little effect on RWT, and it only had influence on the stable-time of water after the set of TCC. Thus, in practical engineering, the position of TCC should be determined after considering the complex terrains, economic condition, waterway transport, and other specific cases in actual engineering.

4.2.2. Effect of Pr

Under the difference of thermal stratifications, both experimental tests and numerical simulation results had the same trend—that increasing Pr will increase the RWT dramatically (Figure 8a).
The flow velocity distributions of the water modelled with different Pr values were partly shown in Figure 8b. It can be seen that the flow velocity of the water above the TCC was significantly higher than that of the water in the lower layer. The curtain prevented the lower section of the water column from flowing downstream, thus separating it from the warmer upper water stratum. In addition, the water flow over the TCC was drawn by the tractive action of outlet. The increase of Pr caused the flow area above the TCC to decrease, which increased the flow velocity. As seen from the temperature field (Figure 8b), with the increase of Pr, higher temperature surface water flowed into the plume downstream of the curtain; therefore, the average temperature of this water was higher.
Meanwhile, there were critical values of Pr; we can see from the line graph in Figure 9a that the trend lines levelled off at both ends. There was a sensitive zone where the changes of Pr and RWT were positively correlated, and out of the zone the change of Pr had no effect on RWT; the critical value of Pr was 90% and 65%. This indicated that only the top of TCC was in the thermocline; its ability to regulate RWT was explicit.
As a result, the Pr obviously influenced the surface velocity and had a significant effect on the flow field. Most significantly, the increase of Pr blocked the flow of lower layers, allowing only high-temperature layers to flow around the curtain, thus increasing the RWT.

4.2.3. Effect of OSD

As the OSD increased, the RWT decreased, but the range of variation was less than 1 °C, as shown in Figure 9a.
The OSD values of 44 and 28 cm in the numerical simulation were compared and the flow field distribution was shown in Figure 9b. It was concluded that the change of OSD had little effect on the flow field upstream of the curtain, and the change mainly affected the outflow position of curtain-downstream water. Thus, all else equal, as the OSD increased, the RWT decreased. But the change was not that obvious. It can be explained at this point that the released water mainly gathered by the nearby layer of the outlet, so RWT mainly depended on the thermal stratification of the forebay. As previously seen in Figure 5, the vertical temperature was very close when the depth from the water surface was between 2 and 40 cm. Thus, during the OSD value range set in this study, the change of OSD had little effect on RWT.

4.2.4. Effect of RQ

Under both the S1 and S2 distribution, RWT increased as the RQ increased (Figure 10a). The maximum and minimum values of RQ (11 and 1.6 m3/h) were compared and the resulting flow field distributions and temperature field distribution were shown in Figure 10b. The factor of RQ had a great influence on the flow field. For the upstream waters, increasing RQ enlarged the range of current water and caused an increase in mean velocity. For the downstream waters, with the increase of RQ, the pulling force resulting from the discharge of water strengthened and a light eddy appeared between the main downstream flow and the curtain. For the temperature field shown in Figure 10b, the increase of RQ accelerated the flow of higher-temperature water at the top of the curtain, thus reducing the time of water after TCC reached stability. But the influence of RQ on RWT was small. The difference of RWT in experimental tests and numerical simulation was less than 1 °C.
In practical engineering, the RQs were decided with the consideration of downstream flood control capacity, power generation capacity, the benefit of the eco-environment, and so on. RQ may have a large variation range, but the final RWT would not change a lot.

4.2.5. Construction Principle of TCC

To sum up, construction principles for the application of TCC in practice are proposed as follows. First of all, the position of TCC had little influence on the improvement effect of RWT. So it should be determined after considering the complex terrains, economic condition, waterway transport, and other specific cases. Secondly, Pr should be set between 65% and 90%, whereby the larger the Pr chosen, the higher RWT was. Thirdly, the OSD and RQ had little effect on RWT, so in practical engineering its variation will not influence the improving effect of TCC on RWT.

5. Conclusions

The use of TCC is an effective and practical method to raise the RWT in thermal stratified reservoirs. To provide the theoretical basis for the engineering application of TCC, experimental tests are carried out, whose results fully demonstrated the effectiveness of the TCC in increasing the RWT. For its further research, a 3-D numerical hydrodynamic and water temperature model is built with the same size of the physical model, whose accuracy is verified through comparing with experimental test results. In contrast with previous simulations of TCC, this study describes an arc-shaped curtain, which is closer to reality. Then the influences of different factors on increasing the RWT are studied.
According to the analysis of experimental tests and numerical simulation, the conclusions are summarized as follows:
  • The regulating effects of TCC on the RWT is closely related to the temperature structure of waters. In S1 distribution, the maximum temperature increased by up to 8.3 °C, while this is only 3.5 °C under the S2 distribution.
  • The CP has a little difference on RWT, the position of TCC should be determined after considering the complex terrains, economic condition, waterway transport, and other specific cases in actual engineering.
  • The Pr directly affects the vertical range of water entering the discharge water. As the Pr increases, more upper, high-temperature water flows to the downstream of TCC drawn by the force of outlet. But there are critical values of Pr: When the value is out of the range 90%~65%, the impacts of Pr on RWT is negligible.
  • When the water is released by spillway, variation of OSD has little effect on the thermal stratification of the forebay, which causes little impact on improving RWT.
  • The change of RQ has a great influence on the flow field, and reduces the time that the forebay water takes to reach stability. But the effect of RQ on RWT is small; thus, in practical engineering, the variation of RQ can be decided by other complex factors and will not influence the improvement effect of RWT.
Based upon the above conclusions, the following principles are proposed for the application of TCC in thermal stratified reservoirs. The position of the curtain should be decided with comprehensive consideration of complex terrains, economic condition, waterway transport, and other specific cases. In spring and summer, maximize the Pr of the TCC to achieve the best effect on RWT without influencing the flow, and increase the RQ of the water to achieve the final (raised) RWT as soon as possible. The change of OSD and RQ can be decided by actual demand, which will not influence the effect of TCC on improving RWT. For those thermal stratified reservoirs troubled with the problem of RWT, the application of TCC is an effective solution.
Meanwhile, there are many points worth further study. For example, the paper is carried out based on a model with the generalized topography and temperature structure; the influence of real terrains on RWT should be studied in future. In addition, in winter, some reservoirs have the problem of high-temperature of released water, which is the opposite of our focus; the feasibility of TCC’s in this condition is worth researching. Furthermore, the impact of secondary flow on wall-bounded turbulence have obtained some achievements [37], and the role of data uncertainties in identifying the logarithmic region of turbulent boundary layers have been researched [38]; the further research on the secondary flow’s impact on the flow field of reservoir within TCC can be expected.
The research results presented herein, as well as those of future research for more complex terrains and construction methods, will offer powerful support for the application of TCC to regulate the RWT.

Author Contributions

All the authors made contributions to the concept and design of the article. Conceptualization, J.L. and Y.Y.; methodology, W.H. and N.S.; software, P.L. and W.H.; validation, J.L.; formal analysis Y.Y. and P.L.; data curation, P.L. and N.S.; writing—original draft preparation, P.L. and Y.Y.; writing—review and editing, P.L. and Y.Y.; visualization, P.L. and Y.Y.; supervision, J.L. and Y.Y.; funding acquisition, J.L. and Y.Y.

Funding

This research was supported by the National Key Research and Development Program of China (2016YFC0401701), the National Natural Science Foundation of China (51609167, 51809192), and the Program of Introducing Talents of Discipline to Universities (B14012). The authors acknowledge the assistance of anonymous reviewers.

Conflicts of Interest

The authors declare no conflicts of interest. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results.

Appendix A

The photos of experimental model tests are shown in Figure A1.
Figure A1. Photos of physical model tests: (a) Physical model test experimental configuration; (b) temperature sensor experimental set-up; (c) TCC in the tests.
Figure A1. Photos of physical model tests: (a) Physical model test experimental configuration; (b) temperature sensor experimental set-up; (c) TCC in the tests.
Applsci 09 05354 g0a1aApplsci 09 05354 g0a1b

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Figure 1. Arrangement of experimental test.
Figure 1. Arrangement of experimental test.
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Figure 2. Reference and generalization of thermal stratification: (a) Vertical temperature distributions of typical reservoirs; (b) Generalized target temperature distributions and comparison with observed distributions.
Figure 2. Reference and generalization of thermal stratification: (a) Vertical temperature distributions of typical reservoirs; (b) Generalized target temperature distributions and comparison with observed distributions.
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Figure 3. Description of the 3-D numerical model: (a) Longitudinal section of the numerical model; (b) meshes of the numerical model.
Figure 3. Description of the 3-D numerical model: (a) Longitudinal section of the numerical model; (b) meshes of the numerical model.
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Figure 4. Comparison of measured and simulated temperature distributions in front of the TCC. (1 m from TCC). (a) S1 distribution; (b) S2 distribution.
Figure 4. Comparison of measured and simulated temperature distributions in front of the TCC. (1 m from TCC). (a) S1 distribution; (b) S2 distribution.
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Figure 5. Comparison of measured and simulated temperature distributions in front of outlet (0.3 m from the outlet). (a) S1 distribution; (b) S2 distribution.
Figure 5. Comparison of measured and simulated temperature distributions in front of outlet (0.3 m from the outlet). (a) S1 distribution; (b) S2 distribution.
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Figure 6. Results of physical model tests. (a) S1 distribution; (b) S2 distribution.
Figure 6. Results of physical model tests. (a) S1 distribution; (b) S2 distribution.
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Figure 7. Velocity distribution of the basic scenario and the scenario with TCC. The red line represents the TCC (the x-axis represents the distance from the outlet while the colour bar represents the velocity magnitude): (a) The basic scenario (A0); (b) the scenario with TCC (A1).
Figure 7. Velocity distribution of the basic scenario and the scenario with TCC. The red line represents the TCC (the x-axis represents the distance from the outlet while the colour bar represents the velocity magnitude): (a) The basic scenario (A0); (b) the scenario with TCC (A1).
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Figure 8. Analysis of different values of Pr: (a) Comparison of calculated and tested data of different Pr; (b) distribution of velocity at different values of Pr (the red line represents the TCC).
Figure 8. Analysis of different values of Pr: (a) Comparison of calculated and tested data of different Pr; (b) distribution of velocity at different values of Pr (the red line represents the TCC).
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Figure 9. Analysis of different values of outlet submerged depth (OSD): (a) Comparison of calculated and tested data of different OSD; (b) distribution of velocity at different values of OSD (the red line represents the TCC).
Figure 9. Analysis of different values of outlet submerged depth (OSD): (a) Comparison of calculated and tested data of different OSD; (b) distribution of velocity at different values of OSD (the red line represents the TCC).
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Figure 10. Analysis of different values of released flow quantity (RQ): (a) Comparison of calculated and tested data of different RQ; (b) distribution of velocity at different values of RQ (the red line represents the TCC).
Figure 10. Analysis of different values of released flow quantity (RQ): (a) Comparison of calculated and tested data of different RQ; (b) distribution of velocity at different values of RQ (the red line represents the TCC).
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Table 1. Scenarios and results of experimental tests.
Table 1. Scenarios and results of experimental tests.
NumberCP (m)Pr (%)OSD (cm)RQ (m3/h)Vertical Temperature DistributionRWT (°C)
A0406.4S127.5
A13.585406.4S135.3
A22.585406.4S135.4
A31.085406.4S135.3
A43.590406.4S135.9
A53.575406.4S134.5
A63.565406.4S134.3
A73.555406.4S134.3
A83.585366.4S135.6
A93.585326.4S135.7
A103.585286.4S135.8
A113.585246.4S135.8
A123.585401.6S135.2
A133.585404.0S135.3
A143.585408.8S135.6
A153.5854011S135.6
B0406.4S229.7
B13.585406.4S232.9
B22.585406.4S232.8
B31.085406.4S232.9
B43.590406.4S233.1
B53.575406.4S232.5
B63.565406.4S232.3
B73.555406.4S232.2
B83.585366.4S233.0
B93.585326.4S233.0
B103.585286.4S233.2
B113.585246.4S233.2
B123.585401.6S232.7
B133.585404.0S232.8
B143.585408.8S233.1
B153.5854011S233.1
Notes: Curtain position (CP); water-retaining proportion (Pr); water-retaining proportion (Pr); released flow quantity (RQ); released water temperature (RWT).
Table 2. The released water temperature (RWT) with different grid meshing.
Table 2. The released water temperature (RWT) with different grid meshing.
ParametersThe Size of GridRWT (°C)Variation in RWT
VerticalOriginal × 0.535.4+0.3%
Original × 234.8−1.5%
LongitudinalOriginal × 0.535.5+0.6%
Original × 234.6−2.0%

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Lian, J.; Li, P.; Yao, Y.; He, W.; Shao, N. Experimental and Numerical Study on the Effect of the Temperature-Control Curtain in Thermal Stratified Reservoirs. Appl. Sci. 2019, 9, 5354. https://doi.org/10.3390/app9245354

AMA Style

Lian J, Li P, Yao Y, He W, Shao N. Experimental and Numerical Study on the Effect of the Temperature-Control Curtain in Thermal Stratified Reservoirs. Applied Sciences. 2019; 9(24):5354. https://doi.org/10.3390/app9245354

Chicago/Turabian Style

Lian, Jijian, Peiyao Li, Ye Yao, Wei He, and Nan Shao. 2019. "Experimental and Numerical Study on the Effect of the Temperature-Control Curtain in Thermal Stratified Reservoirs" Applied Sciences 9, no. 24: 5354. https://doi.org/10.3390/app9245354

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