Isothermal tests
Thermal analysis of BOS1, BOS2 and BPD is presented in Figs. 3–5 representing the CO2 uptake (mgCO2/10 mg sample) curves in 100% CO2 atmosphere. The curves that were obtained at lower temperatures have not been added as they have shown negligible carbonation rates for the non-hydrated samples.
The non-hydrated BOS1 sample has quite similar final CO2 uptake values also at 400–500 °C, while hydrated BOS1 sample has substantial difference in CO2 uptake values at the same temperatures being much higher (see Fig. 3). Increased temperatures show increasing CO2 uptake capacities for BOS1 and all other samples as well. Changes in CO2 uptake levels with increasing temperatures are more clearly expressed for the hydrated samples (see Fig. 4) (0.58 → 0.85 mg CO2/10 mg BOS2(H), 1.1 → 1.9 mg CO2/10 mg BPD(H) at 400–500 °C) in comparison to non-hydrated samples (0.43 → 0.55 mg CO2/10 mg BOS2, 0.9 → 1.4 mg CO2/10 mg BPD at 400–500 °C). This proves that activation by hydrating (liquid to solid ratio of 0.2 w/w) of industrial residues can increase CO2 uptake potential in all samples. Approximately, 80% of the CO2max can been reached in all hydrated samples in first 2–3 min at 500 °C, and later on, the carbonation process gradually slows down and free CaO content is nearly exhausted after 30 min of treatment for hydrated samples. TG tests indicate that the carbonation process is quite fast at the first stage due to the large reaction surface available, and after 2 min, it slows down due to the decrease in surface area and increasing product layer diffusion resistance [29].
Curves of non-hydrated BPD sample show that at 500 and 600 °C CO2 uptake values are quite similar which can be interpreted so that temperature increase does not increase the CO2 uptake values at this interval anymore (see Fig. 5), and possible dehydration reaction with mass loss can also start at this temperature as it gets closer to the equilibrium temperature 500–550 °C (Eq. 2).
$${\text{Ca}}\left( {\text{OH}} \right)_{2} \to {\text{CaO}} + {\text{H}}_{2} {\text{O}} .$$
(2)
However, CO2 uptake values of non-hydrated BOS1 and BOS2 samples increase at 600 °C compared to 500 °C. Results have shown that hydrated samples have gained the ability to bind more CO2 for all the samples both at 400 and 500 °C. The non-activated samples have an initial binding rate comparable to the hydrated samples, yet the binding reaction tends to slow down at lower conversion levels which results in lower final CO2 uptake values as compared to hydrated samples.
Effect of mechanical treatment
As an additional pre-treatment method, the samples were ground in a Retsch PM 100 grinding machine (5 min) in a four-ball planetary mill. Although the BET surface area of BOS1 was increased from 2.83 to 3.06 m2 g−1, and similarly, BPD BET surface area was also increased 3.84–4.85 m2 g−1 after grinding (see Fig. 1), the ground samples that were tested at 400–500–600 °C showed an unexpected slight decrease in the reaction rates as well as in their binding capacity. For this reason, the TA curves for the ground samples have not been reproduced here.
Kinetics
Calculations for the purpose of determining the reaction mechanism of the first fast stage of the carbonation reaction up to 2 min without including the second slow stage have been made based on the isothermal data and using different well-known reaction mechanisms [30]. The experimental data from isothermal tests at different temperatures were fitted to a set of kinetic models to give the highest regression.
The general equation for solid-state reaction kinetics is shown in Eq. (3):
$$f\left( \alpha \right) = \left( {{\text{d}}\alpha /{\text{d}}t} \right)/k$$
(3)
where f(α) is a certain mechanism function, t represents time, α is the extent of the reaction or fraction converted, and k is the rate constant. By integration of Eq. (4), we get:
$$g\left( \alpha \right) = \smallint {\text{d}}\alpha /f\left( \alpha \right) = kt$$
(4)
where g(α) is the integral form of the kinetic model, the graph of g(α) versus the reaction time is a straight line, whose slope is the rate constant, k. Following this, the activation energy can be subsequently calculated from Arrhenius equation according to the graph of the logarithm of the rate constants versus the inverted temperature values (Eq. 5):
$$\ln \left( k \right) = \ln A - \frac{{E_{\text{a}} }}{RT}.$$
(5)
Based on the well-known reaction mechanisms [30] and the calculated regression coefficients, the most probable model for the carbonation process of non-hydrated BOS1 and BOS2 agrees with the three-dimensional diffusion model, D3 mechanism (Eq. 5), and the rate of CaO carbonation is mainly diffusion controlled.
$$D3{:}[1 - (1 - \alpha )^{1/3} ]^{2} = kt.$$
(6)
However, the most probable model for the carbonation process of all hydrated samples and non-hydrated BPD agrees with A2 model (Eq. 7) which is explained as random successive nucleation and nuclei growth model.
$$A2{:}[ - \ln (1 - \alpha )]^{0.5} = kt.$$
(7)
According to the selected most appropriate mechanism functions (D3, A2), the kinetic parameters have been calculated and the relationship between 1/T and lnk for BOS2 and BPD is shown in Fig. 6. According to the slopes and intercepts of the fitting straight lines, activation energy (Ea) and pre-exponential factor (A) values were obtained for all samples and are shown in Table 1.
Table 1 k values for each temperature and linear correlation coefficient (R2) for the most reasonable mechanism function, obtained Ea and A values for all samples At all selected temperatures, higher carbonation rates belong to the hydrated samples compared to non-hydrated samples. Although the rates are temperature sensitive, temperature rise is not as effective as hydration treatment even when the lowest and highest temperatures are compared in terms of the determined reaction rates. The hydration treatment is clearly more effective for BOS samples, especially, for BOS1; increasing the rates of carbonation reactions significantly at certain temperatures compared to non-hydrated cases. Due to the higher carbonation rates of hydrated BOS samples, the obtained Ea values are lower for hydrated samples, yet the hydration causes to increase in Ea value for the hydrated BPD.
Rotating tube furnace tests
Nabertherm rotating tube furnace was operated to re-evaluate the TG results with bigger amounts of samples and for bigger scale carbonation process tests. Overall, the measured mineral CO2 levels (see Fig. 7) for all the samples after carbonation treatment in the rotating tube furnace were higher than the initial levels which shows that the carbonation tests with rotating tube furnace were successful. Due to rotation of the tube which increases gas–solid contact affecting positively the CO2 diffusion in sample layer, the CO2 uptake levels are higher—up to 0.15 kg CO2 per kg of waste for BOS and 0.24 kg CO2 per kg of waste for BPD compared to the results obtained from TG tests (0.045–0.082 kg CO2 per kg of waste for BOS2 and BPD, respectively).
According to the FTIR analysis of the samples carbonated in the rotating tube furnace, the intensity of portlandite peaks (3640 cm−1) decreases and of carbonates (872, 1417 cm−1) increases after carbonation process (see Fig. 8a–f). Ca-bearing silicates (1123 cm−1) play also a role in carbonation reactions of BPD as their intensities also slightly decrease (see Fig. 8e). For hydrated BOS samples also, the intensity of Ca(OH)2 (3640 cm−1) decreases after carbonation, while Ca–silicates (980, 1120 cm−1) were not involved in carbonation process (see Fig. 8a–d). Peaks of the BOS1 and BOS2 spectra (1410–1415 cm−1) clearly show that after hydration the binding reactivity and CO2 uptake levels of BOS samples have been increased (see Fig. 8a,c).