1. Introduction
In recent decades, the worldwide construction industry rapidly developed, leading to environmental degradation and the gradual scarcity of sand and stone resources. Many types of wastes, such as demolished construction waste [
1,
2], glass [
3,
4], marble [
5,
6], PET [
7], coal bottom ash [
8], and waste tires [
9], can be converted to recycled aggregate through crushing treatments. Recycled aggregate can replace natural aggregate and can be used in the casting of new concrete, and this concrete is called recycled aggregate concrete (RAC). This application contributes to sustainable development and environmental conservation.
The carrying capacity of RAC structures is greatly affected by the mechanical properties of steel reinforcement and RAC [
10,
11], and the bond performance of steel reinforcement and RAC also have a significant effect on the carrying capacity of RAC structures [
12,
13]. Additionally, the bond performance is the foundation of practical design, the basis of numerical simulation, and is of great value to engineering and academic research [
12]. Hence, the bond performance of steel reinforcement and RAC has become a global research hotspot, and the results of previous research showed that the bond performance is affected by many factors, such as the replacement ratio and quality of recycled coarse aggregate (RCA) [
14,
15], the concrete cover [
16,
17], the diameter of steel reinforcement [
18,
19], the anchoring length [
20], and the types of additives (such as fibers and polymers) [
21,
22,
23,
24].
RAC structures inevitably experience freeze–thaw cycles due to the cold climate in frigid regions, which leads to the deterioration of the physical and mechanical properties of RAC [
25]. Consequently, the determination of the freeze–thaw resistance of RAC before the construction of RAC structures in frigid regions is necessary, and some research has aimed at evaluating the mechanical properties of RAC after freeze–thaw cycles and the freeze–thaw resistance of RAC [
26,
27,
28]. The bond performance of steel reinforcement and RAC is also influenced by freeze–thaw cycles. Hence, several investigations have assessed the bond performance of steel reinforcement and RAC after freeze–thaw cycles using the pull-out test [
29,
30,
31,
32,
33,
34,
35,
36], which demonstrated that the bond strength decreases with the increase in freeze–thaw cycles, but there is disagreement about the relationship between the slip and the freeze–thaw cycles in these investigations. Most scholars think that the slip between steel reinforcement and RAC increases with the increase in freeze–thaw cycles [
29,
30,
31,
32,
33,
34,
35], but Shang et al. [
36] found that the slip at the free end of plain steel reinforcement decreased with the increase in freeze–thaw cycles in seawater before 25 freeze–thaw cycles, which was different from the test results of Ren et al. [
32] and Su et al. [
33,
34,
35] on RAC specimens after freeze–thaw cycles in a salt solution. In addition, the bond strength of steel reinforcement and RAC after freeze–thaw cycles was not only affected by the number of freeze–thaw cycles but also affected by the anchoring parameters. In the above investigations, both Jiang et al. [
29] and Liu et al. [
30] considered the effect of the replacement ratio of RCA; Liu et al. [
30] thought the deterioration rate of the bond strength after freeze–thaw cycles accelerated as the replacement ratio of RCA increased, while Jiang et al. [
29] found that the replacement ratio of RCA affected the bond strength slightly. This was because all specimens had the same cubic compressive strength due to a lower water/cement ratio and larger cement consumption, which reduced the effect of the replacement ratio of RCA on the bond strength. Both Shang et al. [
31,
36] and Ren et al. [
32] studied the influence of the steel reinforcement diameter on bond strength after freeze–thaw cycles and revealed that the bond strength decreased as the steel reinforcement diameter increased, regardless of freeze–thaw cycles, which closely corroborated the test results of Cao et al. [
37] in beam-type tests. Additionally, the test results of Cao et al. [
37,
38] and Wang et al. [
39] demonstrated that the bond strength after freeze–thaw cycles decreased as the anchoring length increased.
The preceding research has focused on the bond performance of steel reinforcement and RAC after freeze–thaw cycles. Nevertheless, in a frigid marine environment, due to the cold climate and high concentration of chloride ions in the seawater, RAC structures not only experience freeze–thaw cycles but also experience steel reinforcement corrosion due to seawater. As is well-known, the cross-sectional area of the steel reinforcement was reduced with an increase in the steel reinforcement corrosion rate [
40]; meanwhile, the steel reinforcement corrosion products, which had volume expandability, increased gradually with an increase in the steel reinforcement corrosion rate [
41]. The mechanical properties of the steel reinforcement decreased due to a reduction in the cross-sectional area of the steel reinforcement, which led to the deterioration of the durability and bearing capacity of the structure [
42,
43]. The steel reinforcement corrosion products induced swelling stress on the concrete, which led to cracking and spalling of the concrete cover, and thus the bond performance decreased with a reduction in horizontal restraint provided by the concrete cover [
44,
45]. Therefore, the bond performance of corroded steel reinforcement and RAC needed to be studied adequately, and some scholars likewise conducted relevant investigations. Alhawat et al. [
46,
47] indicated that the bond performance increased slightly and then decreased pronouncedly with an increase in the steel reinforcement corrosion rate, which was in accord with the test results of Zhao et al. [
13]. Additionally, Zhao et al. [
13] observed that the tendency of the bond performance degeneration between RAC and natural aggregate concrete (NAC) structures was similar, and the difference in the bond performance between RAC and NAC structures could be decreased by the installation of stirrups. The effects of the replacement ratio of RCA on the bond performance of corroded steel reinforcement and RAC were investigated, and Yang et al. [
48] showed that the bond performance reduced as the replacement ratio of RCA increased, while the effects were slight. However, Fernandez et al. [
49] presented a different opinion; they indicated that the effects of the replacement ratio of RCA on the bond performance of RAC structures with a 50% replacement ratio of RCA were slight, while the effects became great for RAC structures with a 100% replacement ratio of RCA.
The majority of the above research focused on the separate effect of steel reinforcement corrosion or freeze–thaw cycles on the bond performance of steel reinforcement and RAC, but little research has focused on the coupled effect of both two factors on bond performance. Some research has focused on the coupled effect of steel reinforcement corrosion and freeze–thaw cycles on the bond performance of steel reinforcement and NAC [
50,
51], and the test results demonstrate that bond performance was influenced by a superimposed damage effect. Liu et al. [
50] proposed an empirical formula of the ultimate bond strength considering the stirrup corrosion rate, freeze–thaw cycles, and stirrup ratio and established a bond–slip prediction model considering the stirrup spacing, stirrup corrosion rate, and freeze–thaw cycles based on the eccentric pull-out test results. Zhang et al. [
51] revealed that freeze–thaw cycles increased the pore structure damages of concrete and accelerated steel reinforcement corrosion based on microscopic tests and center pull-out tests and proposed a bond strength damage model considering the steel reinforcement corrosion rate and freeze–thaw cycles. However, both research studies focused on the bond performance of NAC structures under the coupled effect of steel reinforcement corrosion and freeze–thaw cycles and could not provide data supporting the investigation of the bond performance of RAC structures under the coupled effect of steel reinforcement corrosion and freeze–thaw cycles, and should therefore only be a reference for analysis.
The bond performance of RAC structures is necessarily affected by the coupled effect of steel reinforcement corrosion and freeze–thaw cycles in a frigid marine environment, but little research has focused on this topic. Therefore, the objective of this research was to investigate the bond performance of corroded steel reinforcement and RAC after freeze–thaw cycles using the center pull-out test and combining the evolution of mechanical properties parameters after freeze–thaw cycles (e.g., mass loss, cubic compressive strength, and dynamic elastic modulus loss). The relationships between the ultimate bond strength and different freeze–thaw cycles and steel reinforcement corrosion rates are presented through the relativity analysis, and the pull-out energy of RAC specimens with different steel reinforcement corrosion rates after freeze–thaw cycles is presented. Additionally, a modified bond–slip prediction model of corroded steel reinforcement and RAC after freeze–thaw cycles is established. This bond–slip prediction model’s result was compared with other research, indicating its rationality and applicability. The test results provide new supporting data for the evaluation of freeze–thaw resistance and bond performance of RAC structures in a frigid marine environment.
3. Results and Analysis
3.1. Corrosion Performance of the Steel Reinforcement Embedded in RAC
In the early stages of the process of the corrosion test, lots of tiny bubbles got away from the copper sheet, and then a stratum of bronze bubbles existed at the surface of the NaCl solution. Subsequently, the steel reinforcement corrosion products located in the anchoring interfaces between the steel reinforcement and the concrete were produced, and the color of the steel reinforcement corrosion products changed from dark green to reddish-brown. This is because at the early stages of the process of the corrosion test, due to a lack of oxygen, the steel reinforcement corrosion products occur incomplete oxidation leading to the dark green color of steel reinforcement corrosion products. However, a complete oxidation reaction of the steel reinforcement corrosion products is achieved later, resulting in the reddish-brown color of steel reinforcement corrosion products [
60].
The corrosion specimens were divided into two sections after the pull-out test, and then the corroded steel reinforcement was removed and treated. Treatment of the corroded steel reinforcements included cleaning with dilute hydrochloric acid, acid neutralization with alkali, and rinsing with fresh water. Finally, the steel reinforcements were dried and weighed. Each corroded steel reinforcement and two non-corroded steel reinforcements of the same kind as the corroded steel reinforcement were treated together after the same freeze–thaw cycles to avoid the effects of the treatment on the measurement of the corrosion rate. The corrosion rate of the corroded steel reinforcements can be calculated using Equation (4) according to the China specification JTS/T 236-2019 [
61].
where
η is the actual steel reinforcement corrosion rate;
m01 and
m02 are the mass of two non-corroded steel reinforcements before the treatment, respectively;
m1 and
m2 are the mass of two non-corroded steel reinforcements after the treatment, respectively;
m0 is the initial mass of the corroded steel reinforcement;
m is the mass of the corroded steel reinforcement after the treatment.
The appearances of corroded steel reinforcements after the treatment are plotted in
Figure 7. It could be observed that the quantity and depth of corrosion pits and the corrosion degree of steel reinforcements with a higher steel reinforcement corrosion rate were more pronounced compared to that with a low steel reinforcement corrosion rate.
A comparison of actual and target steel reinforcement corrosion rates is tabulated in
Table 6, and the difference between actual and target steel reinforcement corrosion rates of most steel reinforcements was small, while some actual steel reinforcement corrosion rate was slightly higher than the target steel reinforcement corrosion rate with increasing freeze–thaw cycles, which can be explained by the enhancing effect of freeze–thaw cycles on the deterioration of steel reinforcement corrosion.
3.2. Freeze–Thaw Resistance of the Concrete
3.2.1. Appearances of Pull-Out Specimens after Freeze–Thaw Cycles
The appearance of the concrete specimens with a 1% steel reinforcement corrosion rate after freeze–thaw cycles is shown in
Figure 8. The surface of specimens showed slight spallation after 50 freeze–thaw cycles. Half of the RAC specimens showed the exposure and spallation of RCA after 100 freeze–thaw cycles and obtained a rougher surface. Coarse aggregate exposure and more severe aggregate spallation occurred on the surfaces of all specimens after 150 freeze–thaw cycles and the corners of 70% of the specimens were damaged.
The surface damage of RAC specimens was more severe than that of NAC specimens after the same freeze–thaw cycles, which revealed that the freeze–thaw resistance of RAC was inferior to that of NAC. Su et al. [
33] and Li et al. [
12] also came to similar conclusions. The reason is that the amount of the interfacial transition zone (ITZ) in the interior of RAC is larger, and the ITZ is weaker and more easily damaged by freeze–thaw cycles [
27]. Additionally, the quantity of infiltrating water was larger in RAC compared to that in NAC after fewer freeze–thaw cycles due to the higher porosity of RAC, which leads to faster damage to RAC.
3.2.2. Mass Loss
The mass loss, the cubic compressive strength, and the dynamic elastic modulus loss of the concrete specimens after freeze–thaw cycles were measured to assess the freeze–thaw resistance of the concrete (RAC and NAC).
The mass of concrete specimens initially increased and subsequently decreased with increasing freeze–thaw cycles, which was similar to the conclusions reached by Liu et al. [
26], Wu et al. [
27], and Su et al. [
33]. This can be explained by the combined effects of water infiltrates and cement mortar spalling on the mass of the concrete. Water infiltrates the concrete with increasing freeze–thaw cycles due to the disruption of the pore structure by the freeze–thaw stress, which contributes to the concrete hydration and aggregate water absorption, increasing the concrete mass. In addition, the freeze–thaw stress caused by the repeated freezing and thawing of the infiltrating water causes cracking in the interior of the concrete. The quantity and size of these cracks constantly increase with increasing freeze–thaw cycles, causing the cement mortar to loosen and spall, which leads to a reduction in the mass of the concrete. The mass of the specimens increases from 0 to 50 freeze–thaw cycles because the mass of the infiltrating water is greater compared to that of the cement mortar spalling, while the mass of the specimens decreases after 100 freeze–thaw cycles because the mass of the infiltrating water is less than that of the cement mortar spalling.
Figure 9 demonstrates that the mass loss of RAC was more influenced by freeze–thaw cycles than that of NAC; the mass increase of RAC after 50 freeze–thaw cycles was 1.8 times that of NAC, while the mass loss of RAC after 150 freeze–thaw cycles was 1.2 times that of NAC. This can be explained by the inferior freeze–thaw resistance of RAC to that of NAC.
3.2.3. Cubic Compressive Strength
The cubic compressive strength of RAC and NAC after different freeze–thaw cycles is shown in
Figure 10, and the cubic compressive strength followed an almost straight-line downward tendency with increasing freeze–thaw cycles. The cubic compressive strength loss of RAC (NAC) after every 50 freeze–thaw cycles was close to 17.05% (14.93%), which is similar to the test results of Wu et al. [
27]. This is because the quantity of deleterious pores and cracks increases due to the repeated freeze–thaw stress, which causes a large decrease in the cubic compressive strength of concrete [
62].
Figure 10 reveals that the cubic compressive strength of RAC was less than that of NAC before freeze–thaw cycles with the same water–cement ratio, and the initial cubic compressive strength of RAC (NAC) was 32.3 MPa (35.2 MPa). This can be explained by the incomplete hydration of the cement due to high water absorption and more defects in RCA, leading to a low cubic compressive strength of RAC. Additionally, the cubic compressive strength of RAC decreased slightly faster after freeze–thaw cycles compared to that of NAC in terms of the comparison of the slopes of the fitting curves between the cubic compressive strength after freeze–thaw cycles of RAC and NAC. This is because the lower initial cubic compressive strength of RAC means that the compactness of RAC is poorer than that of NAC, which leads to poorer freeze–thaw resistance of RAC compared to that of NAC. Therefore, the cubic compressive strength deterioration after freeze–thaw cycles of RAC is more rapid than that of NAC.
3.2.4. Dynamic Elastic Modulus Loss
The dynamic elastic modulus loss is calculated by Equation (5) based on the measured results of the dynamic elastic modulus of the concrete (RAC and NAC) after freeze–thaw cycles.
where Δ
E(
N) is the dynamic elastic modulus loss after
N freeze–thaw cycles;
E0 is the dynamic elastic modulus before freeze–thaw cycles;
EN is the dynamic elastic modulus after
N freeze–thaw cycles.
The dynamic elastic modulus is tabulated in
Table 7, and the dynamic elastic modulus loss is displayed in
Figure 11. The dynamic elastic modulus loss of RAC and NAC gradually increased with increasing freeze–thaw cycles, and the dynamic elastic modulus loss after 150 freeze–thaw cycles of RAC (NAC) reached 42.8% (33.5%).
Furthermore, the dynamic elastic modulus loss of RAC increased more rapidly than that of NAC from 0 to 100 freeze–thaw cycles, while the dynamic elastic modulus loss of RAC increased more slowly than that of NAC after 100 freeze–thaw cycles. The reason for this is that the concrete completeness of NAC is severely destroyed after 100 freeze–thaw cycles, resulting in a rapid increase in the dynamic elastic modulus loss. Due to the crack-free cement paste of NAC before 100 freeze–thaw cycles, the concrete completeness of NAC is better than that of RAC, which leads to less freeze–thaw damage [
12]. However, cracks not only exist at the interface between the cement paste and NCA but also appear in the interior of the cement paste of NAC after 100 freeze–thaw cycles, which causes poorer concrete completeness of NAC and more severe freeze–thaw damage to NAC than that to RAC. Therefore, the increase in the dynamic elastic modulus loss of NAC becomes more rapid compared to that of RAC after 100 freeze–thaw cycles.
The cubic compressive strength and the dynamic elastic modulus loss of RAC and NAC after freeze–thaw cycles are displayed in
Figure 12.
Figure 12 shows the cubic compressive strength deceased as the dynamic elastic modulus loss increased, which demonstrates an increase in damage for concrete causes a decrease in cubic compressive strength of RAC and NAC after freeze–thaw cycles.
3.3. Failure Pattern of Pull-Out Specimen
Figure 13 shows the failure pattern of the pull-out specimens, and the failure patterns of all specimens were pull-out failures. The coupled effect of freeze–thaw cycles and steel reinforcement corrosion did not alter the failure pattern, and the difference in the failure pattern between RAC and NAC was minimal. All pull-out specimens with stirrups exhibited the same failure pattern, the pull-out of the embedded steel reinforcement from the concrete, which was identical to the test result of Su et al. [
33]. This can be explained by the cracking of the concrete prevented by the lateral restraint contributed by the stirrups.
3.4. Ultimate Bond Strength
The ultimate bond strength of corroded steel reinforcement and RAC after freeze–thaw cycles are plotted in
Figure 14, and the ultimate bond strength of RAC specimens with a 0% corrosion rate of the previous study by Su et al. [
33] after freeze–thaw cycles was used as a reference to investigate the coupled effect of freeze–thaw cycles and steel reinforcement corrosion on the ultimate bond strength.
Figure 14 shows that the ultimate bond strength reduced with increasing freeze–thaw cycles, indicating the deterioration of the bond performance of RAC specimens after freeze–thaw cycles. This is because the pore structure is destroyed by the freeze–thaw stress caused by the repeated freezing and thawing of the infiltrating water, and then the emergence and expansion of the cracks destroy the horizontal restraint provided by the concrete cover, which causes the ultimate bond strength to reduce. The cracks then extend to the interface of steel reinforcement and RAC with increasing freeze–thaw cycles, resulting in a reduction in the chemical adhesion and friction of steel reinforcement and RAC. The freeze–thaw cracks interact with the pull-out cracks, which causes a more severe reduction in the ultimate bond strength [
26].
Moreover, the ultimate bond strength decreased with an increase in the steel reinforcement corrosion rate. The ultimate bond strength of RAC specimens with 0%, 1%, 2%, and 3% steel reinforcement corrosion rates was reduced by 4.46%, 12.77%, and 20.61%, respectively, before freeze–thaw cycles, compared with RAC specimens with a 0% corrosion rate. The mass loss of steel reinforcement and deposition of steel reinforcement corrosion products at the interface between steel reinforcement and RAC are caused due to steel reinforcement corrosion. The steel reinforcement corrosion products, which have volume expansibility, induce hoop stress in the interior of the concrete. The concrete cover cracks due to the hoop stress, causing a reduction in the horizontal restraint provided by the concrete cover. On the other hand, the cracking of the concrete also can also induce a reduction in chemical adhesion and friction. Localized pitting corrosion and rib damage of the steel reinforcement are induced when the steel reinforcement corrosion rates arrive at a high level, leading to a deterioration of the interlocking between steel reinforcement and RAC.
Linear regression was performed on the ultimate bond strength of RAC specimens with different steel reinforcement corrosion rates after freeze–thaw cycles in
Figure 14. The ultimate bond strength after freeze–thaw cycles with a 3% steel reinforcement corrosion rate decreased most rapidly, which means that the ultimate bond strength under the coupled effect of freeze–thaw cycles and steel reinforcement corrosion decreased more rapidly than that under separate effects. This is because the interaction of the corrosion-induced crack and the freeze–thaw cracks accelerates the deterioration of the ultimate bond strength.
3.5. Relativity Analysis
Relativity indicates the direction and degree between two related variables, and Pearson’s product–moment relative coefficient is a practical application of relativity in concrete research [
63]. Pearson’s product–moment relative coefficient was employed in this analysis to assess the relationships between the ultimate bond strength and different freeze–thaw cycles and steel reinforcement corrosion rates, expressed as Equation (6), and the assessment results are tabulated in
Table 8.
where
r is the Pearson’s relative coefficient;
x and
y are independent values; and
and
are average values of
x and
y, respectively. The range of
r is −1 to +1, and
y is positively related to
x when
r is a non-zero positive number; meanwhile,
y is negatively related to
x when
r is a non-zero negative number.
The assessment results in
Table 8 show the strong negative relativity between the ultimate bond strength and the freeze–thaw cycles and the steel reinforcement corrosion rates, with relative coefficients of −0.9988 and −0.7872, respectively. The relative coefficient between the freeze–thaw cycles and the steel reinforcement corrosion rates was zero, meaning no relativity. A comparison of these relative coefficients was made, demonstrating that the effect of freeze–thaw cycles on the ultimate bond strength is more pronounced compared to that of the steel reinforcement corrosion rates.
3.6. Bond–Slip Curve
The bond–slip curves are depicted in
Figure 15, which proposes the variation law of the same steel reinforcement corrosion rate after different freeze–thaw cycles. The bond–slip curves were compared and found to be similar to the tendency for the typical bond–slip curve plotted in
Figure 16, where
τ1,
τu,
su, and
τr are the initial bond strength, ultimate bond strength, peak slip, and residual bond strength, respectively. The bond–slip curves can be divided into four sections: the micro-slip section (OA), the slip section (AB), the descent section (BC), and the residual section (CD).
The micro-slip section (OA): the micro-slip section was a steep ascent until the bond strength reached the initial bond strength, and the bond strength was approximately linear, increasing up to about 0.34–0.98 of the ultimate bond strength, as illustrated in
Figure 15. During this section, the bond strength experienced very rapid growth while the slip increase was negligible, and the bond strength was supplied by the static friction and chemical adhesion between RAC and deformed steel reinforcement.
The slip section (AB): as the pull-out force increased, the steel reinforcement would start to slip, and the static friction changed to dynamic friction. Moreover, chemical adhesion was gradually lost, and interlocking began to play an essential role in the balance of the pull-out force until the ultimate bond strength was reached. This phenomenon was the same for all specimens with different corrosion rates until reaching 50 freeze–thaw cycles. However, the interlocking reduced pronouncedly after 100 freeze–thaw cycles, which led to a marked reduction in the slope of the slip section and the ultimate bond strength after 100 freeze–thaw cycles. This phenomenon can be explained by the occurrence of brittle damage in the concrete after 100 freeze–thaw cycles, which severely damages the bond of the steel reinforcement and the concrete, resulting in a rapid reduction in the ultimate bond strength after 100 freeze–thaw cycles.
The descent section (BC): the bond strength failed to maintain a relatively stable value after the pull-out force arrived at the value of the ultimate bond strength and began a rapid decline. In this section, the pull-out force was still balanced by dynamic friction and interlocking. However, due to the crushed mortar between the steel reinforcement ribs and the development of cracks in the RCA surface and cement matrix, the interlocking rapidly decreased, resulting in a rapid deterioration of the bond strength.
The residual section (CD): the bond–slip curve followed an approximately horizontal line when the bond strength exceeded a critical value, the residual bond strength. The pull-out force was balanced mainly by dynamic friction due to the pronounced reduction in interlocking. The range of residual bond strength was 0.21 to 0.41 times the ultimate bond strength.
3.7. Pull-Out Energy Analysis
The energy consumption of the pull-out force was obtained by calculating the area under the pull-out force–slip curves from its origin to the peak, and that can be referred to as the pull-out energy. The pull-out energy of RAC specimens with 1%, 2%, and 3% steel reinforcement corrosion rates is depicted in
Figure 17. Moreover, based on the test data of Cao [
54], the pull-out energy of RAC specimens with a 0% steel reinforcement corrosion rate after freeze–thaw cycles was calculated and used as a reference. The pull-out energy decreased with increasing freeze–thaw cycles for all steel reinforcement corrosion rates, and the pull-out energy loss with 0%, 1%, 2%, and 3% steel reinforcement corrosion rates was 16.97%, 23.11%, 15.63%, and 12.22%, respectively, after 100 freeze–thaw cycles. Moreover, the pull-out energy reduced with an increase in the steel reinforcement corrosion rate after the same number of freeze–thaw cycles, which is consistent with the tendency of variation in the bond strength shown in
Figure 14. Compared to the pull-out energy with a 0% steel reinforcement corrosion rate, the pull-out energy was reduced by 6.45–26.18% with an increase in the steel reinforcement corrosion rate from 1% to 3% after 0 freeze–thaw cycles and the pull-out energy was reduced by 12.62–21.46% after 100 freeze–thaw cycles. The RAC surrounding the steel reinforcement hardened and became brittle due to steel reinforcement corrosion.
3.8. Bond–Slip Prediction Model under Coupled Effect of Freeze–Thaw Cycles and Steel Reinforcement Corrosion
A bond–slip prediction model under the coupled effect of freeze–thaw cycles and steel reinforcement corrosion is required to assess the bond–slip performance of RAC structures in a frigid marine environment. For more convenient modeling, normalization of bond strength and slip was performed and the normalized bond–slip (
−
) curves are displayed in
Figure 18.
Based on the normalized bond–slip curves in
Figure 18 and a previous prediction model proposed by Xiao et al. [
64], a modified prediction model was proposed to assess the bond performance under the coupled effect of freeze–thaw cycles and steel reinforcement corrosion, which is expressed as Equation (7).
where
α and
β are parameters obtained in the ascend and descend sections of the normalized bond–slip curve of RAC severally, and the optimum values were estimated by Equation (7) and tabulated in
Table 9.
Table 9 indicates that the values of
α were randomly distributed in the range of 0.29 to 0.34; thus, the average value of 0.32 was selected as the modified value. Furthermore,
β increased with increasing freeze–thaw cycles, while that decreased with an increase in the steel reinforcement corrosion rate. The parameter
β was fitted with the freeze–thaw cycles, and the steel reinforcement corrosion rates, and the fitting result is expressed by Equation (8).
Equations (7) and (8) were superimposed, and the expression of the modified bond–slip prediction model under the coupled effect of freeze–thaw cycles and steel reinforcement corrosion can be obtained and expressed as Equation (9).
Measured curves and curves fitted by the modified bond–slip prediction model for Equation (9) of 12 specimens were compared in
Figure 19, and fitted curves agree well with measured curves.
The test data of other researchers were collected and aimed to verify the correctness of the modified bond–slip prediction model, which was presented in this paper.
Table 10 tabulates details of collected pull-out test results. Measured curves of other researchers and curves fitted by the modified bond–slip prediction model for Equation (9) were compared in
Figure 20, and fitted curves agree well with measured curves.