3.1. Properties of the Paste Mixtures
The setting parameters measured by the Vicat apparatus are shown in
Table 6. It is obvious from the results that the dosage of borax directly affects the course of the hydration process; the higher the borax dosage, the longer the paste setting time. The shortest initial setting time was observed for MP-0-P (control mixture without a borax additive), where the length of initial setting time was only 9 min, and after another 2 min, the setting was completed. The elongation of setting time was then achieved by the application of borax retarder. By the use of 2.5 wt.% of borax, the setting start was postponed to 11:15 min after mixing dry components with water, and the setting duration was extended to 7:45 min. The use of 5 wt.% of borax addition resulted in the initial setting time being 13 min and the length of the setting period to 9 min; 7.5 wt.% of borax postponed the initial setting time to 14 min, and elongated the setting duration to 10:30 min. The longest setting, 13:30 min, started at the time 17:30, and it was achieved by the mixture MP-10-P with 10 wt.% of borax. Overall, the growing borax share in the developed pastes postponed the setting start by up to 8.5 min, and elongated duration of setting by up to 11.5 min compared to the reference sample; such achievement shows that the use of borax in MKPC pastes allows wider material application assured by the elongated setting time. Gained results exceed the set expectations based on the previously reviewed studies. The reached final setting times are longer than those ones measured by Li et al. [
30], who manufactured samples with 5% and 10% of borax (mass percentage of the used MgO) that provided the final setting time 15 min and 25 min, respectively. The obtained results are also more promising than the initial setting times obtained by Wen et al. [
39], who measured initial setting times around 2 min, 2.5 min, 2.5 min, and 3.5 min for 2.5%, 5%, 7.5%, and 10% of borax, respectively. However, it should be taken into account that the used amount of borax in the mentioned experiments was slightly lower, as it was set as the mass percentage of MgO, while in this experiment, the borax share was calculated as the mass percentage of MgO + KH
2PO
4.
The results of the rheological behavior measurement, closely connected with the aforementioned setting characteristics, are shown in
Figure 2. The performed measurement of the pastes’ shear stress development captures in detail the beginning of the transformation of the fresh mixtures into the hardened material. The presented curves show the progress of the hardening process before reaching the initial setting time; the time of measuring in each case is adjusted to the measuring range of the used apparatus. These results broaden the previously gained findings describing the setting process, and they also describe viscosity of the tested materials.
The pictured curves can be divided into two sections. The first curve section, which can be described as the period before the start of the hardening process, is characterized by a very little growth of shear stress values. Afterwards, the hydration process starts and the slight growth in shear stress changes into the rapid increase; in that period, the initial fluid mixture gradually changes into the semi-solid and later solid composite. With respect to the testing principle, the Viscotester is able to measure the mixtures only in their viscous state. Therefore, the results only provide the information about the course of the hydration process beginning, as the measurement was stopped when the maximum value of the measuring range was reached; the maximum reached shear stress value was the same for all the experiments. Theoretically, it can be expected the progressive increase in shear stress curves until the final setting time, where the curves will reach a plateau.
The curves of all the tested mixtures fully captured the start of the transition from liquid to solid state manifested by the rapid growth in viscosity. For all the cases except MP-2.5-P, similar shape of the steep part of the shear stress curve was detected independently of the borax content; however, it is obvious that the period preceding hardening was elongated based on the used borax amount. In the case of the curve describing the mixture MP-2.5-P, more moderate shear stress growth was observed compared to the other cases. Such result could be caused by reaching some specific binder to retarder ratio associated with a slower onset of hydration reaction. This finding is in agreement with the observed development of temperature and Young’s dynamic modulus (presented below). In both MP-2.5-P and MP-5-P curves there were recorded horizontal steps that were followed by further increase in the shear stress values. However, after reaching approx. 10 min, the increase in shear stress curve was much steeper in the case of M-5-P than recorded for MP-2.5-P. It was similar to those obtained for MP-0-P, MP-7.5-P, and MP-10-P. Therefore, the performance of MP-2.5-P in comparison to other research mixtures can be considered as unique and may lead to the prolongation of the hardening time and retardation of strength development.
As indicated above, the starting moment of the rapid shear stress growth is important, as it marks the start of the hydration process. In the case of the reference mixture MP-0-P (without borax), the onset of hydration was detected at the time 8 min after mixing water with binder. On the other hand, when using 10 wt.% of borax, the time reached 13 min. Using 5 wt.% provided an extension of 1 min compared to the reference mixture. Moreover, the retarder use influenced not only the timing of the hydration, but also the viscosity of fresh mixtures; higher share of borax led to the decrease in viscosity values. It is necessary to note, in the case of MP-5-P, two steep changes in the slope of shear stress curves were identified, first one at approx. 9 min and the second one at 10.2 min. The onset of MP-5-P was attributed to 9 min, the time when the first sharp increase in the shear stress values started.
Overall, the results again demonstrate the effect of retarder use and confirm that the use of borax leads to the time extension of the MKPC hydration process; it specifically shows the elongation of the first (prehydration) period. Moreover, the results reveal that while the borax addition affects the start of setting, it does not affect the shape of the steep part of the shear stress development curve. The results also mostly show (except for the case of the MP-2.5-P mixture) that the transition between the first and the second part of the shear stress curves is milder when using borax; the higher the borax dosage, the milder is the transition.
To avoid any confusion, it is necessary to emphasize that the measurement of viscosity captures the initial period of hardening preceding the initial setting time; the initial setting time occurs approximately 0.5–3 min after the end of viscosity test. Such a fact must be taken into account when setting parameters and shear stress development are compared.
The temperature evolution in the fresh paste mixtures is together with Young’s modulus shown in
Figure 3 and
Figure 4. It is another parameter describing the hydration process, and another possibility to evaluate the efficiency of the borax ratio used in the mixtures. The duration of the temperature change monitoring was for all tested materials 14 h. The values were recorded continuously, with one measured value per 10 s; later on, these values were plotted against time, generating a smooth curve and capturing the temperature changes occurring during the hydration period well.
The results show noticeable differences between the pastes in dependence on borax content. The considerable deceleration of the hydration reaction caused by the increasing borax share is manifested by a slower rate of temperature growth and lower temperature maximum, with this impact becoming more significant with the increase in borax amount. A similar trend of the MKPC paste temperature development in dependence on the borax share was previously observed, e.g., by Yang et al. [
37]. The maximum temperature reached, 64.4 °C, was measured for the sample MP-0-P at 26 min after the mixing binder with water. The temperature peaks reached by the mixtures containing borax were lower in all cases, with the lowest peak provided by paste labeled MP-10-P. Similarly, as in the shear stress results, the samples with 2.5% share of borax (MP-2.5-P) showed atypical behavior when compared to the other samples. In this case, using 2.5 wt.% of borax led to the more significant decrease in maximum temperature (43.7 °C) than using 5% of borax (48.4 °C). The use of 7.5% and 10% of borax then led to the expected temperature drop, with the mixture MP-7.5-P reaching the maximum 39.4 °C and the mixture MP-10-P providing the maximum temperature lower than 35 °C.
As for the rate of temperature growth, it might look like that the mixtures MP-2.5-P and MP-5-P reached their maximum temperature earlier than the reference mixture (
Figure 2). However, on closer inspection (
Figure 3), it is obvious that each temperature curve contains two local maxima—the main peak, and the additional (lower) peak. In the case of the reference sample, the lower maximum occurs first, while in the case of borax-containing samples, the higher maximum occurs first and the lower maximum follows. The first maximum was reached at the time 7.5 min after mixing water with binder by the reference sample. Samples with 2.5%, 5%, 7.5% and 10% of borax reached the first maximum at 15 min, 19.8 min, 27.5 min, and 43.1 min, respectively. It is obvious that the time when the first maximum is reached depends directly on the borax amount—the more borax, the later the peak. Moreover, it is apparent that the borax addition in general affects the course of the temperature vs. time curve.
Generally, borax addition lowered the temperature of hydration reaction in all cases; the highest borax share provided the mildest rate of temperature growth and reached the lowest temperature. It should be mentioned that the most significant differences in the temperature profiles were detected until 100 min after blending water with the binder. After the time of 300 min, the curves remained nearly the same, regardless of the borax ratio.
The dynamic Young’s modulus was measured by the Vicasonic apparatus alongside the temperature profiles. The Young’s modulus change was monitored continuously for 14 h in time intervals 10 s; subsequently, the measured values were plotted against time as shown in
Figure 3 and
Figure 4. The results are in agreement with the temperature development and the recorded setting times.
The measurement started approximately 4 min after mixing the binder with batch water. In the beginning phase, the values of Young’s modulus were very low and stayed nearly constant until the start of hardening. The initial stage of the hardening process was accompanied by a rapid increase in Young’s modulus values. In the case of the mixture without borax additive, the significant increase was observed from the start of the measurement (4 min). As expected, the mixtures containing borax proved to have a later Young’s modulus increase, with the longest period before increase provided by sample MP-10-P (24 min); according to the results, the time of Young’s modulus rapid increase is directly dependent on the borax amount. However, there is a remarkably small difference between samples MP-2.5-P and MP-5-P—the increase in the case of MP-5-P starts only 2 min later than in the case of MP-2.5-P, while in the case of MP-7.5-P and MP-10-P, the time difference exceeds 5 min, and an even longer time difference was observed between samples MP-0-P and MP-2.5-P. Moreover, the rate of the initial growth of MP-2.5-P elastic modulus values is notably milder; such fact is in accordance with the previous observations.
As for the final Young’s modulus values, the MP-0-P reached the final dynamic modulus (20.6 GPa) quite quickly—approximately 100 min after mixing; afterwards, it remained approximately constant until the end of the measurement. On the contrary, in the case of samples containing borax, the modulus values kept growing until the end of the measurement. The growth was rapid at first, and after 15–42 min (in dependence on the borax share), it became more moderate. The measured modulus values of the samples containing borax were overall significantly lower than those measured for the reference sample. At the age of 100 min, the values of the samples with borax reached approximately 50% of the MP-0-P Young’s modulus value. After 840 min, the values gained for mixtures with 2.5 wt.% and 5 wt.% of borax were both approximately equal to 15.5 GPa. The difference between MP-7.5-P and MP-10-P was also negligible; their Young’s modulus reached approximately 13 GPa.
The gained results show that by adding borax, the dynamic elastic modulus development is postponed, slowed down, and also elongated. Moreover, in the case of sample MP-2.5-P, a significantly milder curve increase can be observed. The values for all borax containing samples keep growing until the end of the measurement. Overall, the results of the dynamic elastic modulus time development are in agreement with the aforementioned temperature development. The rapid increase in temperature is accompanied by the significant dynamic elastic modulus growth. In
Figure 4, it can be observed that the duration of the rapid Young’s modulus growth corresponds with the time necessary to reach the first temperature peak, especially in the case of samples MP-5-P, MP-7.5-P, and MP-10-P. Moreover, it should be noted that in both cases, the irregular behavior of the samples containing 2.5% of borax can be observed in the form of slower growth of values and also lower and later peaks. As for the comparison with the setting characteristics, the initial setting time that indicates the start of hardening corresponds well with the start of dynamic elastic modulus growth. The slight deviations may be caused by the experiment setup and the laboratory conditions (temperature and relative humidity).
The basic structural properties, namely bulk density, specific density, and total open porosity were measured on fully dried hardened samples; the obtained results are summarized in
Table 7. It can be seen that the borax influence on these properties is very little in most cases. The values of bulk density were approximately equal to 2000 kg·m
−3, the measured values or specific density were close to 3000 kg·m
−3, and the total open porosity was approximately 35% in most cases. Only sample MP-5-P provided considerably higher bulk density, 2179 kg·m
−3, and consequently a lower total open porosity, 26%. This specific borax dosage enabled to uniformly distribute paste components which led to the optimum workability of fresh paste and thus formation of more dense hydrated products. The highest value of specific density, 3103 kg·m
−3, was obtained for MP 0-P.
The addition of borax reduced both examined mechanical parameters. The lowest mechanical strength yielded MP-10-P, paste with the highest borax dosage. On the contrary, MP-5-P exhibited a moderate drop in mechanical parameters only what was compensated by prolonged workability. In this case, the drop in compressive strength was ~9.8% and ~7.6% for flexural strength, respectively.
The part of the research presented above includes the design and testing of MKPC paste mixtures with the intention to choose an ideal share of borax for the use in MKPC-based mortars. Except for the basic structural and mechanical properties, the testing was focused on determining properties of the fresh mixtures. Overall, the gained results show that the use of a varying share of borax retarder causes significant material changes. The increase in borax content caused the elongation of the hardening period demonstrated by longer initial setting time, changes in viscosity trends, and a slower rise in hydration temperature together with lower temperature peaks. The obtained values of Young’s modulus in time only prove the borax’s impact on setting. Thus, it may seem to be obvious that the highest borax share is the most advantageous one, providing the slowest setting and the lowest temperatures reached within the material at the same time.
However, it is necessary to mention that the use of a higher borax dosage, namely in the case of samples MP-7.5-P and MP-10-P, led to the separation of a thin surface layer of the manufactured samples that may have been caused by an inhomogeneity of the samples and their segregation is molds; the separation was accompanied by the crack development in the surface layer. The cracks were continuously expanding during the hardening process (see
Figure 5). Such effect disrupted the material integrity. If this effect of borax addition persisted in mortars, it could cause a significant worsening of the mechanical properties. Therefore, to avoid cracking development, the use of 0–5 wt.% of borax was considered to be suitable for the use in mortars.
Based on the rheological performance, the samples MP-2.5-P and MP-5-P were considered as the potential reference borax-containing binders for the MKPC-based mortar design. The efficiency of 2.5 wt.% of borax was surprisingly high; the experiments revealed that the samples with the mentioned retarder amount can provide a slower rate of the change in viscosity, temperature, and Young’s modulus in time in comparison to the samples with a different (higher) borax amount. However, the mixture containing 5 wt.% of borax was chosen in the end, as it provided a longer setting time than MP-2.5-P, and managed to maintain a good integrity without visible defects. Additionally, the lower initial modulus of elasticity growth rate in the case of MP-2.5-P may be a disadvantage, as high initial mechanical properties are important for the materials used for repair purposes. Accordingly, taking into consideration mechanical parameters of pastes, material MP-5-P exhibited the best mechanical resistance among borax-enriched materials. For these reasons, the next part of this study uses the composition of MP-5-P and combines it with different aggregates to manufacture mortars with a wide range of desirable properties.
3.2. Properties of the Hardened Mortars
The results of mortar testing are summarized in the following paragraphs. Unlike the paste-focused part of this study, the mortar testing was aimed mainly at the properties of mortars in the hardened state.
The first part of mortar results, the basic material characteristics of the hardened mortars and workability of the fresh mortars, are summarized in
Table 8. All the mortars containing borax addition showed higher spread diameter than the control mortar MP-REF-0. The measured spread values showed that the set W/C ratio equal to 0.25 was high for all the borax-containing mortars, as the borax application led to a significant decrease in viscosity. Such behavior was responsible for the rise in the spread values—in the case of reference mortar with 5 wt.% of borax, the borax addition caused the increase in the spread diameter value by 70 mm compared to the reference sample. This finding is in agreement with a study concluded by Yang et al. [
37], who noticed that the increase in borax share enhances the MKPC paste fluidity.
Moreover, the impact of the aggregate type was observed. The full replacement of silica sand by Liaver (MP-L) even increased the obtained spread values to 250/260 ± 5 mm; such a fact may have been caused by the oval shape and smooth surface of the Liaver particles. On the contrary, the use of rubber granulate partly served as a counterweight to the borax effect, and slightly lowered the spread value to 210/220 ± 5 mm. In that case, the spread value was again affected by the aggregate shape—the used rubber aggregate was characteristic by particles with rough surface and sharp edges. In the case of the mortars containing a combination of Liaver and rubber aggregate, the spread value was almost as high as the one measured for the mortars containing Liaver only. Overall, for a practical use, it would be necessary to decide a specific fitting ratio for each aggregate type a planned application.
The basic structural properties measured for the dried samples also reported noticeable material differences in dependence on the type of used aggregate. In the case of the reference samples, both specific and bulk density of the mortar proved to be relatively high; the bulk density was slightly higher than in the case of the reference paste, and the specific density was slightly lower. The reference sample containing 5 wt.% of borax showed basically the same specific density, but a higher value of bulk density, and therefore lower total open porosity compared to the sample without borax. The same effect of borax addition was observed for the MKPC pastes in the first part of the research; the denser structure and therefore the lower porosity is likely the result of the less viscous consistency of the fresh mixture.
As for the properties of mortars containing different aggregates, those considerably depend on the parameters of the applied aggregates. The less dense and visibly non-compact structure of the used rubber granulate (see
Figure 6) resulted in quite low bulk density of the final composite MP-R, but also low specific density resulting in total open porosity even lower than the one obtained for the reference sample without the borax addition. Meanwhile, the highly porous expanded glass as a sand substitution caused a very low bulk density of the Liaver-containing mortar and as a consequence that mortar also reached the highest open porosity. This feature is typical when lightweight porous aggregate is used as silica sand substitution. Based on the obtained results it is possible to claim that the Liaver incorporation outweighs the effect of borax addition in terms of total open porosity—even with a huge spread value, and the high total open porosity is achieved. This observation is supported by the previous research conducted by Pavlíková et al. [
53], where the growing share of Liaver in MOC-based mortars caused the increase in open porosity.
The thermal properties measured on dried mortar samples are introduced in
Table 9. Those results show that while the borax addition basically does not affect thermal conductivity of the materials, it causes a slight decrease in thermal diffusivity and an increase in volumetric heat capacity. On the other hand, the aggregate substitution affects all the measured thermal parameters. The incorporation of both crumb rubber and expanded glass aggregate and also their combination resulted in the lowering of the thermal conductivity of the mortars. The lowest thermal conductivity was measured for the sample MP-L, the highest was measured for the sample MP-R; however, both values were considerably lower than the thermal conductivity of both reference mortars. Overall, the highly porous Liaver structure enhanced the thermal behavior, and Liaver-containing mortars ended up being the best thermal insulation material of all the examined possibilities. However, the gained thermal conductivity was still high in comparison to the standard thermal insulation materials [
67,
68].
The thermal diffusivity values measured for samples containing Liaver and rubber were comparable and lower than the thermal diffusivity values of the reference samples. The lowest value, 0.53 m2·s−1, was measured for the MP-R composite. The heat storage ability represented by the volumetric heat capacity oscillated around 1.60 × 106 J·m−3·K−1 for the samples containing rubber and Liaver, with the reported lowest value 1.29 × 106 J·m−3·K−1.
The experimentally assessed heat transport and storage parameters reflect the arrangement of the mortar inner structure formed from dense magnesia-phosphate binder and aggregates with variable porosity, shape and morphology. The inverse proportionality between the calculated open porosity and measured thermal conductivity can be observed—e.g., the sample containing Liaver aggregate showed the highest open porosity and the lowest thermal conductivity. Thus, higher porosity is connected with higher thermal insulation ability and also with slower heat transport. Overall, the use of lightweight aggregates enhances the thermal insulation ability of MKPC-based mortars. A similar effect of rubber and expanded glass aggregate incorporation on thermal parameter of MOC-base mortars was also reported by Pavlíková et al. [
53].
The obtained water transport parameters of the hardened MKPC-based mortars are shown in
Table 10. These parameters determine the rate of water transport and storage and thus clearly affect the water resistance against liquid water penetration and the consequential water-induced damage. Except the water absorption coefficient, which was very similar for all examined mortars, the highest values of 24 h water absorption
Wa and
W were observed for the reference mortar MP-REF 0, showing that the composite containing silica sand aggregate and not using the setting retarder is the most susceptible to water-induced damage of all manufactured samples. The use of borax provided the other reference sample, MP-REF 5, with more compact structure that showed noticeably lower water absorption potential. Obviously, the borax use is advantageous in terms of water resistance improvement.
The acquired data further indicate that water transport parameters of MKPC-based mortars depend on the type of the used aggregate. The considerable differences in parameters between the samples containing different aggregates can be observed. Although the expanded glass is classified as a highly porous material which gives high porosity value of the hardened mortar, it provides the samples with moderate moisture transport ability and hygric parameters only slightly higher than received for mortar with silica sand aggregate. The high porosity is probably balanced by a non-absorbing repellent character, which partially reduced the effect of high porous inner structure. From the point of view of moderation of water ingress, the most advantageous hygric parameters were measured for the samples containing crumb rubber, which was due to its hydrophobic nature recently reported by Chen et al. [
69].
Table 11 shows the mechanical parameters represented by compressive and flexural strength measured for mortars at the age of 14 days. Trends of both values are in agreement. The highest mechanical resistance (compressive strength 34.57 MPa, flexural strength 7.2 MPa) was detected in the case of the reference composite MP-REF 0. The incorporation of borax into the reference mixture caused a decrease in the 14 days flexural value, but the compressive strength remained unaffected. The drop in mechanical strength on a larger scale was observed when silica sand aggregate was replaced by expanded glass and rubber granulate. The worst mechanical properties were measured for the composite containing 100% of rubber aggregate, despite the rubber granulate samples had lower porosity compared to Liaver. This issue may be caused by an insufficient bond between the hydrated magnesia-phosphate structure and rubber particles that is likely affected by the rough surface of the used rubber aggregate; a closer look at this issue is presented in
Figure 6.
Reference mortar MP-REF 0 as well as MP-REF 5 were characterized in terms of time dependent strength development. The results (
Figure 7) showed the gradual increase in strength values. The differences between the early strength values (after 2 and 5 days) were quite low. However, it should be noticed that while the higher compressive strength at the age of 2 days was observed for MP-REF 0, the higher flexural strength at the same age was provided by MP-REF 5. As for the compressive strength, at 14 days it reached the same and final value for both reference samples. Meanwhile, the flexural strength of MP-REF 0 reached the final value at 14 days and on the contrary, flexural strength of MP-REF 5 kept growing until the age of 28 days. The maximal measured flexural strengths were basically the same for both reference mortars.