Abstract
Cement production is currently the largest single industrial emitter of CO2, accounting for ∼8% (2.8 Gtons/y) of global CO2 emissions. Deep decarbonization of cement manufacturing will require remediation of both the CO2 emissions due to the decomposition of CaCO3 to CaO and that due to combustion of fossil fuels (primarily coal) in calcining (∼900 °C) and sintering (∼1,450 °C). Here, we demonstrate an electrochemical process that uses neutral water electrolysis to produce a pH gradient in which CaCO3 is decarbonated at low pH and Ca(OH)2 is precipitated at high pH, concurrently producing a high-purity O2/CO2 gas mixture (1:2 molar ratio at stoichiometric operation) at the anode and H2 at the cathode. We show that the solid Ca(OH)2 product readily decomposes and reacts with SiO2 to form alite, the majority cementitious phase in Portland cement. Electrochemical calcination produces concentrated gas streams from which CO2 may be readily separated and sequestered, H2 and/or O2 may be used to generate electric power via fuel cells or combustors, O2 may be used as a component of oxyfuel in the cement kiln to improve efficiency and lower CO2 emissions, or the output gases may be used for other value-added processes such as liquid fuel production. Analysis shows that if the hydrogen produced by the reactor were combusted to heat the high-temperature kiln, the electrochemical cement process could be powered solely by renewable electricity.
Keywords: cement, electrolysis, decarbonization, hydrogen, carbon dioxide
As discussed at the 2018 Sackler Colloquium “Status and Challenges in Science for Decarbonizing our Energy Landscape” and in other recent analyses (1–4), deep decarbonization of today’s energy system will require addressing not only energy generation (24% of global greenhouse gas emissions) and transportation (14% of global greenhouse gas emissions) but also difficult-to-decarbonize sectors such as large industry, which today is responsible for about 21% of global greenhouse gas emissions (5). Industry uses fossil fuels for heat and to drive chemical and thermochemical reactions but may become less reliant on fossil fuel if 1) electrical alternatives become available and 2) the cost and reliability of renewable electricity continues to improve (6, 7). The rise of very low-cost renewable electricity has already motivated the search for electrochemical methods to innovate industrial processes (1, 8, 9). Among these, electrochemical pathways to the production of cement have heretofore been limited; 1 previous example is high-temperature electrochemical decarbonation using molten salts, operating in the same temperature range as thermal calciners (10, 11). Here, we propose and demonstrate proof of concept for an ambient-temperature electrochemically based process that decarbonates CaCO3, precipitates solid Ca(OH)2 from which desired calcium silicates are synthesized, and produces concentrated gas streams of H2 and O2 + CO2 that are amenable to CO2 capture and sequestration, and/or used in other value-added processes (Fig. 1).
Portland cement (12) is the most widely produced man-made material in the world, produced at a rate of 4 billion metric tons per year (13). Excluding agriculture, cement production is the largest industrial source of greenhouse gases (steelmaking follows closely), accountable today for 8% of global greenhouse gas emissions (14). About one-half of the emitted CO2 is due to the use of CaCO3 (generally, limestone) as a key component, with the balance being mainly due to combustion of fossil fuels in the cement kiln (15). Demand for cement is growing as the world’s population increases and becomes more urban, and as emerging economies develop infrastructure (16). By 2060, the number of buildings on Earth is expected to double; this is equivalent to building a New York City each 30 days for the next 40 years (17). Since each kilogram of cement produced emits nearly 1 kg of CO2 (15), several gigatons of CO2 per year will be released from new infrastructure, highlighting the urgency of decarbonizing cement production.
Current efforts to reduce cement’s carbon footprint include carbon capture from flue gases, use of alternative fuels, or development of supplementary cementitious materials (14, 18–21). Currently, the flue gas from cement plants is too impure for economical carbon capture through amine scrubbing; use of alternative fuels (such as used tires) does not alleviate the primary emissions from CaCO3; and use of supplementary materials in the concrete has limited impact on the carbon emissions from Portland cement and may simultaneously compromise the physical properties (14, 19–21). Another family of approaches uses the cement to capture and sequester more CO2, producing a carbonate-enriched cement or concrete product (22–25). In contrast with the above approaches, we were motivated to seek electrochemically based approaches that have the potential to produce the most widely accepted and used cements, thereby minimizing adoption risk, while taking advantage of emerging very low-cost renewable electricity to alleviate both the chemical and thermal sources of CO2. As we show, our process can work synergistically with other scientific and technological tools of a sustainable energy system discussed in the Sackler Colloquium, including wind and solar electricity, water splitting and fuel creation, and chemical and electrical energy storage.
Our reactor takes advantage of the inherent pH gradients in an electrolysis cell to carry out CaCO3 decarbonation and Ca(OH)2 precipitation and collection (Fig. 2). We show that the Ca(OH)2 produced in this manner, which requires less energy to dehydrate to CaO than is required to calcine CaCO3, is readily reacted with SiO2 to produce alite, the major active phase (50 to 70% by weight) in Portland cement (12). Near-stoichiometric operation, where every 2 protons electrolytically produced at the oxygen-generating anode decarbonates 1 CaCO3 formula unit, is demonstrated at laboratory scale. We propose several pathways by which this electrochemical decarbonation reactor can be integrated into a low- or zero-carbon-emission cement plant (Fig. 1), including powering by renewable electricity and using the gases produced in any of several alternative functions such as 1) direct capture and sequestration of the inherently concentrated CO2 stream, 2) generation of electricity or heat from the H2 (and optionally the O2) via fuel cells or combustors, 3) providing oxy-fuel for cleaner combustion in the cement sintering cycle, and 4) liquid fuel production. A first-order technoeconomic analysis of the energy consumption and fuel cost of such a process as a function of the cost of renewable electricity is presented.
Results
Our decarbonation cell simultaneously functions as an electrolyzer as well as chemical reactor to convert solid CaCO3 to solid Ca(OH)2, illustrated schematically in Fig. 2 and demonstrated experimentally in Fig. 3 and SI Appendix, Figs. S2 and S3. An electrolyzer operating with near-neutral water has the following anode and cathode half-cell reactions:
[1] |
[2] |
At steady state, the electrolyzer produces a pH gradient that is readily visualized upon addition of universal pH indicator to an operating H-cell, as shown in Fig. 3 and Movies S1 and S2. In such an electrolyzer, H+ and OH− will normally recombine to form water:
[3] |
Our reactor replaces this reaction with a decarbonation reaction. When CaCO3 is added to the acidic solution produced in the vicinity of the anode during electrolysis, chemical decarbonation occurs via the following sequence of reactions (26):
[4] |
[5a] |
[5b] |
[5c] |
Dissolved Ca2+ (Eq. 4) is drawn towards the anode and then precipitates from solution as Ca(OH)2 upon reaction with OH−; this reaction is favored above pH 12.5:
[6] |
The sum of the electrochemical and chemical reactions occurring in the cell is
[7] |
We define stoichiometric operation of this reactor as the condition where every 2 mol of protons produced during electrolysis (Eq. 1) converts 1 mol of CaCO3 to 1 mol of Ca(OH)2 as shown in Eq. 7; this represents the maximum possible yield and coulombic efficiency. At stoichiometric operation, the ratio of gases produced is also given by Eq. 7: each mole of Ca(OH)2 produced results in the generation of 1 mol of H2 at the cathode and 1 mol of O2 and 2 mol of CO2 at the anode.
Previously, Rau, along with others (27–30), proposed using electrolytic decarbonation, powered by renewable electricity, as a means of mitigating ocean acidification. Their concept is in turn similar to the operation of a calcium reactor used to maintain alkalinity in reef aquariums: CaCO3 is reacted with acid (in Rau’s case, the acid is made from the oxidation of seawater) to produce dissolved Ca(HCO3)2 and Ca(OH)2 at the cathode. The resulting solution of Ca(HCO3)2 and Ca(OH)2 is alkaline and captures CO2 from the atmosphere to reform CaCO3 and can be returned to the saltwater body to mitigate acidification. Here, instead of using electrolytic decarbonation for CO2 capture, we liberate the CO2 as a gaseous product to be captured and sequestered, or used in other processes, and precipitate the Ca(OH)2 for use in cement production. Note that in addition to cement production, Ca(OH)2 is an important component in the manufacture of refined sugar, pulp and paper, alkali carbonates, for wastewater remediation, and as a fluxing agent in steel refining (31). Typically the Ca(OH)2 is produced by slaking of CaO obtained by calcination of CaCO3; using our decarbonation reactor, Ca(OH)2 could be produced directly for these applications as well, while allowing direct capture of the CO2 produced.
A series of laboratory H-cell reactors was constructed to test the proposed scheme. Fig. 3 A–E shows time-lapse images of a reactor assembled with platinum electrodes and using an electrolyte consisting of 1 M NaNO3 in distilled water, to which a few drops of universal pH indicator have been added. The color scale correlating color to pH is shown at the bottom of the figure. The anode chamber contains CaCO3 powder, and in contrast to the cell in Fig. 3 F–J, no porous separator is used between the chambers. Initially, in Fig. 3A the yellow tint shows that the electrolyte is at pH ∼6 everywhere except immediately above the bed of CaCO3 powder, where the purple tint shows that partial dissolution of the carbonate has raised the pH to >10. Fig. 3 B–E show the cell at different times after electrolysis commences, under potentiostatic conditions (2.5-V cell voltage, ∼6-mA current). The color gradients show that over time a steeper pH gradient develops, reaching more extreme pH values in each chamber, consistent with the half-cell reactions (Eqs. 1 and 2). However, close examination of the solution within the cross-tube shows a distinct stratification, with the acidic (pink) solution above and the alkaline (purple) solution below, which we attribute to a density difference between the 2 solutions. Movie S1 shows the development of the pH gradient and stratified liquid layers in this cell over time. In this cell configuration, Ca(OH)2 was observed to precipitate across the length of the cell including directly on the platinum wire cathode, which it eventually passivates. As shown in SI Appendix, Fig. S1, passivation leads to a sharp drop in cell current after a few hours of operation.
Fig. 3 F–I show the same cell design but with a porous paper separator placed at the intersection of each chamber with the cross-tube in order to limit convection. In addition, the CaCO3 powder source in this cell is contained within a removable cup so that the dissolution of CaCO3 as a function of time could be measured by removing and weighing the remaining powder (after drying). Note the lack of stratification; in the absence of convective mixing the cells could be operated for >12 h without Ca(OH)2 passivation of the cathode (SI Appendix, Fig. S1). In this cell the alkaline solution diffuses as a uniform front across the cell, and at steady-state operation the pH within the cross-tube is high enough that Ca(OH)2 precipitation occurs predominantly between the separators, where it is readily collected for analysis. Note also that in this configuration the pH around the anode is far less acidic (i.e., no pink tint), and in fact the yellow color indicates pH ∼6. This is significant because 6 is approximately the pH at which HCO3− and CO2(aq) are in equilibrium. The observation suggests that essentially all of the protons produced in the oxygen evolution reaction (Eq. 1) are consumed by reaction with the carbonate ion (Eq. 5). We confirm this through independent measurements discussed later. In addition, the composition of the output gases was confirmed by gas chromatography.
Using the cell design in Fig. 3 F–I, we collected significant amounts of white precipitate on the porous paper separator directly in front of the cathode, as shown in Fig. 3J. Upon drying, the precipitate was confirmed using powder X-ray diffraction (XRD) to be predominantly Ca(OH)2 with a small amount of CaCO3 (6%, based on Rietveld refinement) (Fig. 4A). Brunauer–Emmett–Teller (BET) analysis showed that the precipitate has a specific surface area of 0.8 m2/g. The impurity CaCO3 may have formed upon exposure of the Ca(OH)2 to air when preparing samples for XRD, or when some of the soluble HCO3− deprotonates on contact with OH− to reform CaCO3. Scanning electron microscopy (SEM) shows that the Ca(OH)2 particles are crystallized with 3 different characteristic length scales. The largest isolated crystallites (Fig. 4B) have dimensions of tens of micrometers and show a hexagonal prism morphology characteristic of Ca(OH)2 (32). Next in size scale are aggregates of much finer crystallites having dimensions of a few micrometers (Fig. 4 C and D) but of similar hexagonal-prism morphology. Finally, there exist precipitates with a rounded nodule morphology, which at higher magnification reveals submicrometer-scale crystallites (Fig. 4 E and F). The appearance of 3 different morphologies of Ca(OH)2 precipitates suggests that nucleation and growth conditions vary widely within the reactor. The origin of these variations is a topic for future study. However, essentially all of the particles produced fall below the <90-μm specification typical for raw mixes in cement production (12). Composition analysis by energy-dispersive X-ray analysis (SI Appendix, Fig. S2) showed no impurities above background levels in the Ca(OH)2 except for trace amounts of Na, likely resulting from the Na salt used in the reactor electrolyte. Thus, the present approach appears to be capable of producing fine, high-purity Ca(OH)2 particulates.
A series of experiments was conducted to characterize the coulombic efficiency of the reactor compared to the stoichiometric limit. In each experiment, an H-cell reactor was assembled with fresh electrolyte, using 1 M of either NaClO4 or NaNO3 salt, and the same starting amount of CaCO3 powder. The reactor was operated under potentiostatic conditions (3.5 V) for times from 1 to 14 h, after which the CaCO3-containing cup was removed from the reactor, dried, and weighed to obtain the amount of CaCO3 lost to chemical dissolution. Results from 13 experiments are plotted in Fig. 5 as the moles of dissolved CaCO3 against the coulombs passed (upper abscissa), obtained by integrating the current over the duration of the experiment, and the H2 gas equivalent (lower abscissa), calculated assuming that the rate of electrolysis is equal to the cell current (i.e., no side reactions). The red dashed line in Fig. 5 represents the stoichiometric reaction wherein every 2 protons produced at the anode in the oxygen-evolving reaction protonates 1 carbonate ion. The error bars for each data point correspond to cumulative weighing error based on the precision of the scale. A least-squares fit through all of the data points yields a ratio of chemical reaction rate to electrolysis rate of 0.85, relative to a maximum value of 1. This demonstrates that a high coulombic efficiency is possible, even using an unoptimized laboratory-scale reactor. For both electrolytes the longest-time data (far right data points) show a fall-off in efficiency, which other experiments (SI Appendix, Fig. S1) suggest is due to passivation of the cathode with Ca(OH)2 at long reactor run times. Note that some of the data points lie above the line of maximum theoretical efficiency. We attribute this deviation to some inadvertent loss of CaCO3 during removal of the CaCO3-containing cup from the reactor. We also attempted to measure directly the amount of Ca(OH)2 produced in these experiments but were not able to recover all of the Ca(OH)2 precipitated in the cells (e.g., from the cell walls) or to efficiently remove all of the precipitate on the paper separator. Clearly, more advanced reactors can be designed in which there is greater control over convection and chemical gradients, and in which the precipitated Ca(OH)2 is collected more efficiently, including continuously. Such reactor design improvements are beyond the scope of the current paper. Even so, the present efficiency is close to the thermal efficiency of a conventional cement precalciner, which decarbonates about 90% of the incoming CaCO3.
Having demonstrated the efficacy of the proposed decarbonation reactor, we turned our attention to evaluating the suitability of its solid Ca(OH)2 product as a precursor to Portland cement. The most abundant mineral in Portland cement, constituting 50 to 70% by weight, is alite, 3CaO·SiO2. We prepared mixtures of the Ca(OH)2 and a fine SiO2 powder, as well as a control sample using purchased CaCO3 powder mixed with the same SiO2, in the 3:1 alite molar ratio. The mixed powders were subjected to heat treatment over a wide range of temperatures. Fig. 6 A and B show the XRD pattern and SEM image of the Ca(OH)2 + SiO2 mixture after heating to 600 °C for 2 h in air. Unlike CaCO3, which does not decompose until 898 °C (at 1 atm PCO2), Ca(OH)2 has a thermodynamic decomposition temperature of 512 °C (at 1 atm PH2O) and here has already decomposed to CaO upon firing at 600 °C, although the CaO has not yet reacted with SiO2 to form alite. After heating for 2 h at 1,500 °C, a typical cement kiln temperature, and cooling by turning off the furnace power, the mixture has reacted to form the low-temperature T1 polymorph of alite (ICSD:4331), as shown by the XRD pattern in Fig. 6C. The polymorphism of alite is known to depend on the nature and amount of impurities in the raw material as well as the cooling rate from kiln temperature (33). While the high-temperature M1 and M2 polymorphs are more commonly obtained in commercial processes, the T1 polymorph we obtained in slow-cooled samples is considered just as cementitious (33–35). Fig. 6D shows that the alite particles produced from our precursors are less than 30 µm in size, which is within the range desired for commercial Portland cements (12). Fig. 6 E and F show calcium and silicon composition maps, from which the compositional homogeneity of the alite is evident. Fig. 7 A and B show the XRD pattern and SEM image of the corresponding CaCO3 and SiO2 mixture after heating to 600 °C for 2 h in air, and Fig. 7 C and D show the results after heating to 800 °C for 2 h in air. At 600 °C, no significant decomposition has occurred, whereas at 800 °C the CaCO3 has decomposed to CaO but reaction to alite has not commenced. After heating to 1,500 °C for 2 h (Fig. 7 E and F), the XRD shows that the alite phase has formed. However, there remains some unreacted CaO, 6% according to Rietveld refinement of the XRD spectra. The SEM image in Fig. 7F, when compared to Fig. 6D, shows that the Ca(OH)2- and CaCO3-derived alites ultimately reach similar particle morphologies and sizes. These results show that the electrochemically produced Ca(OH)2 from our decarbonation reactor is a suitable precursor for synthesizing the main hydrating calcium silicate phase in Portland cement. Moreover, due to the fine precipitate morphology (compared to, for example, ground limestone) and its >300 °C lower decomposition temperature, it appears to have improved reactivity compared to CaCO3, which could translate to reduced firing times and/or temperatures that lower energy consumption in the high-temperature reaction step.
Discussion
In addition to producing a reactive Ca(OH)2 suitable for cement synthesis, our electrolysis-based decarbonation reactor produces concentrated gas streams of H2 at the cathode and O2 and CO2 (in a 1:2 molar ratio when operating at high coulombic efficiency) at the anode. These gases are important components in a wide range of sustainable technologies that are currently being pursued worldwide and open up several possible synergies between cement production and these technologies, which we now discuss.
Carbon capture and sequestration (CCS) at the cement plant level has to date focused on postcombustion capture of CO2, combined with the use of oxy-fuel combustion. The O2/CO2 stream from our decarbonation reactor can make these processes simpler and more efficient. Postcombustion capture refers to technologies that capture CO2 from the kiln exhaust, such as calcium looping, amine scrubbing, and membrane filtration (36–38). Oxy-fuel, or oxygen-enhanced combustion, refers to the burning of fossil fuels (here, primarily coal) with oxygen instead of air (37, 39). Oxy-combustion first results in improved fuel efficiency, since the nitrogen content of air does not have to be heated. Second, the absence of nitrogen permits higher flame temperatures without emitting nitrous oxides (NOx), which have a global warming potential 298 times that of CO2 on a per-mass basis (40) and also contribute to smog, acid rain, and ozone depletion. Third, the flue gas from oxy-fuel combustion has a higher concentration of CO2 and fewer NOx impurities (37, 41), making carbon capture more efficient. In a cement plant using our decarbonation reactor, the O2/CO2 gas mixture could therefore be used as oxy-fuel in the high-temperature kiln to lower energy consumption and NOx emissions. Among other benefits of oxygen enrichment, 1 commercial-scale experiment using 30 to 35% oxygen enrichment resulted in a 25 to 50% increase in cement kiln production (42). Also, oxy-fuel combustion has negligible, if not beneficial, effects on Portland cement clinker quality (39, 43–47).
The concentration of CO2 in the flue gas from conventional cement kilns is ∼25% (48). For chemical absorption with amines, the most technologically mature postcombustion capture method for a combined stream (37, 38), increasing the concentration of CO2 up to 60% has been shown to decrease heat requirements, solvent regeneration energy, and steam costs of capture (49–53). The gas stream from our decarbonation cell is higher still (67%), which should make amine scrubbing more efficient. However, a greater benefit may be the ability to avoid expensive CCS processes like amine scrubbing altogether. Since here the CO2 is delivered in a highly concentrated form mixed only with O2 (and some H2O vapor), direct capture using the same simple compression processes (54, 55) now used for purified and concentrated CO2, could be used.
The hydrogen gas produced at the cathode in our decarbonation cell has value as a feedstock in major industries such as ammonia and fertilizer production, oil and gas refining, and process metallurgy and is considered a key component of developing technologies that could decarbonize heavy-duty transportation, aviation, and heating (56, 57). The combined gas streams could also be used in CO2 utilization processes that produce liquid fuels, such as those that also use hydrogen and produce alcohols.
The hydrogen could also be looped back to support the cement process (Fig. 1). It could be directly combusted to provide heat or electric power back to the cement operation, or the H2 and O2/CO2 gas streams could supply a fuel cell that generates on-site electricity to power the electrochemical reactor or other plant operations such as grinding, mixing, and handling. By using a solid oxide fuel cell (SOFC) (58), which has the highest electrical efficiency of all fuel cell types (60 to 80%) (59), the deleterious effects of the CO2 on proton exchange membrane fuel cells (60, 61) is averted, and typical SOFC operating temperatures of 500 to 1,000 °C could be readily maintained using heat from the cement kiln (which typically operates at 1,450 to 1,500 °C). Simultaneously, oxygen would be removed from the O2/CO2 gas stream, further purifying the CO2 and simplifying sequestration. Note that this combination of an electrochemical reactor and SOFC creates a regenerative fuel cell (62), which has the ability to store energy if storage of the reactants is provided, and could thereby smooth the intermittency of renewable electricity used to power the cement plant.
The CO2 stream produced from the decarbonation cell may also have value in applications that up-cycle captured CO2. CO2 is already used to enhance oil recovery (EOR) (63, 64) and to make chemicals such as urea, salicylic acid, methanol, carbonates (65), synthetic fuel (via the Fischer–Tropsch process) (66), and synthetic natural gas (via the Sabatier reaction) (67). There is growing interest in finding ways to react CO2 electrochemically or photochemically to create chemicals and fuels from captured CO2 using renewable electricity (68). For example, a model plant that uses captured CO2 to make synfuel has been demonstrated (69).
We also considered the feasibility of operating an electrochemically based cement manufacturing process purely with renewable electricity. Perhaps the least capital-intensive way to use the output gases of the decarbonation reactor is through combustion to heat the cement kiln. We analyzed the energy flows in this configuration; details are given in SI Appendix. Assuming a decarbonation reactor operating with 85% coulombic efficiency, an electrolyzer operating at 60 to 75% efficiency, and combustion of the resulting H2 and O2 to heat the sintering kiln with 60 to 80% efficiency, the input electrical energy required to make 1 kg of cement is 5.2 to 7.1 MJ. This assumes no energy benefit from the substitution of Ca(OH)2 for CaCO3 in the high-temperature sintering process or other potential benefits such as reduction of capital and energy cost for grinding limestone (given that this function is replaced by chemical dissolution). At 80% efficient combustion of the H2 and O2 produced from the decarbonation cell, the thermal energy produced slightly exceeds that required for sintering. If combustion is only 60% efficient, 90% of the thermal energy required for sintering can be supplied from the electrolyzer gases (i.e., ∼0.5 MJ/kg of supplemental energy is required). This energy deficit, as well as electric power for supporting operations, could be made up with an excess of electrolyzer capacity above that stoichiometrically needed for decarbonation. This analysis suggests that a renewables-powered electrochemical cement process would not require large amounts of supplemental energy, if any.
An important related question is, of course, the cost of the electrochemically based process. Given the numerous possible configurations discussed above, a complete techno-economic analysis is beyond the scope of this paper. The lifetime cost and economic return for a complete system or any of its subunits depends on capital cost, efficiency, and durability, as well as the value of the cement and gaseous byproducts. Many of the cost factors are currently unknown; for example, the lifetime cost of the decarbonation reactor will depends on its specific design and performance, none of which have yet been optimized. We therefore limit our techno-economic analysis to a comparison of the energy cost of the electrochemical process with its coal-fired counterpart. The 5.2 to 7.1 MJ/kg cement estimated for the electrochemical process does exceed the energy required for the conventional cement process in the average US kiln, which is 4.6 MJ/kg (70). At a coal price of $61 per ton (for bituminous coal) (71), the energy cost for the conventional process is ∼$28 per ton of cement, which is 25% of the average US cement selling price of $113 per metric ton (13). The corresponding cost for the electrochemical process naturally depends on the price of electricity and could in some instances be zero or even negative if obtained from renewable resources. However, for electricity costs of $0.02, $0.04, and $0.06 per kW⋅h, and assuming an energy requirement for the electrochemical process of 6 MJ/kg, which is in the middle of our estimated range, the energy cost is $35, $60, and $100 per ton of cement, respectively. This suggests that, in the absence of other considerations, the electrochemical process would be cost-competitive with conventional plants (∼$28 per ton of cement) if electricity is available at <$0.02 per kW⋅h. Note that the wholesale cost of wind electricity is now at or slightly below $0.02 per kW⋅h across much of the interior of the United States (72). We assume that wind electricity will be available at this price for the proposed cement plants, for example from a colocated wind farm.
However, this cost comparison neglects the cost of carbon capture and sequestration, which for amine scrubbing of conventional cement flue gas has been estimated to be on the order of $91 per ton (50). In the electrochemical sequence modeled above, where electrolytic H2 is combusted to heat the kiln, the cost of directly capturing CO2 from the O2/CO2 stream exhibiting the decarbonation reactor should be less than $40 per ton (50). This would swing net energy costs in favor of the electrochemical process, in an environment where policies require carbon remediation, and where low-cost renewable electricity is available.
Finally, the water intensity of such an electrolyzer-based process should be considered. Each kilogram of cement made using the proposed decarbonation cell would require 0.4 kg of water; this means that the average US kiln, producing 1,800 tons of cement per day, would require ∼760 tons of water per day. However, half of this water would be recovered upon the dehydration of Ca(OH)2. If H2 was used to fuel the kiln, the other half of the water could be condensed from the flue gas. In principle, all of the water used for electrolysis could be recycled.
Conclusions
We propose and demonstrate an electrochemically based cement synthesis process in which CaCO3 is decarbonated and Ca(OH)2 is precipitated in the pH gradient produced by a neutral-water electrolyzer, while concentrated gas streams of H2 and O2/CO2 are simultaneously produced. The fine powder Ca(OH)2 is used to synthesis phase-pure alite, the majority cementitious phase in ordinary Portland cement. The concentrated gas streams from this process may be used synergistically with other processes under development for sustainable industrial technologies. Among several alternatives, the CO2 may be directly captured and sequestered; the H2 and/or O2 may be used to generate electric power via fuel cells or combustors; the O2 may be used as a component of oxy-fuel to further lower CO2 and NOx emissions from the cement kiln; or the output gases may be used to synthesize value-added products such as liquid fuels. Our laboratory-scale prototype decarbonation reactors are shown to be capable of operating with near-theoretical coulombic efficiency, wherein every 2 protons produced at the anode during electrolysis dissolves 1 CaCO3 formula unit. Under such conditions, the electrolytic hydrogen produced, if combusted, can supply most or all of the thermal energy required in high-temperature sintering of the cement. These results suggest a pathway to cost-competitive emissionless cement manufacturing wherein all energy is supplied by renewable electricity.
Materials and Methods
Decarbonation Cells.
Custom-designed H-cells were fabricated by James Glass, Inc. The electrolyte was 1 M NaClO4 or NaNO3 (Sigma-Aldrich, ≥98%) dissolved in deionized water. These electrolytes were chosen because their calcium salts are soluble, and because they do not decompose at high voltage. Both electrodes were made from platinum: a rod at the cathode, and a wire at the anode (MW-1032; BASi). Platinum was chosen because it has a high catalytic activity for hydrogen and oxygen evolution in both acid and base. Alternative low-cost electrode materials might include Ni, Cu, or stainless steel for the cathode (pH 12.5) and Al, Sn, or Pb for the anode (pH 6). CaCO3 powder (Sigma-Aldrich, ≥99%) was added to the anode compartment. Filter paper (28310-015, particle retention 5 µm; VWR) was used as the porous separator. Potentiostatic experiments were conducted using a Bio-Logic Science Instruments VMP3 potentiostat. All tests were done at room temperature.
XRD Characterization.
XRD patterns were collected using a PANalytical X’Pert PRO XRPD, using Cu radiation and a vertical circle theta:theta goniometer with a radius of 240 mm. The default configuration of this instrument is in Bragg–Brentano geometry with a high-speed high-resolution X’Celerator position-sensitive detector, using the Open Eulerian Cradle sample stage. XRD data were analyzed using Highscore, version 4.7.
SEM Characterization.
SEM imaging and compositional analysis of the samples was conducted using a Phenom XL instrument equipped with an energy-dispersive X-ray detector (nanoScience Instruments), operating at 10-kV accelerating voltage for imaging and 15 kV for energy-dispersive X-ray spectroscopy analysis.
BET Characterization.
A Quantachrome Instruments NOVA 4000E (Anton Paar QuantaTech) was used to perform multipoint BET analysis of powder specific surface areas.
Alite Synthesis.
Electrochemically precipitated Ca(OH)2 or CaCO3 (Sigma-Aldrich, ≥99%) was mixed with SiO2 (99.5%, 2 µm; Alfa Aesar) in a 3:1 molar ratio. The powders were mixed into a slurry with ethanol then dried. The resulting well-mixed powders were pressed into pellets. The pellets were placed in platinum crucibles and heated at 2 °C per min to 1,500 °C in a muffle furnace (Thermolyne F46120-CM). The temperature was held at 1,500 °C for 2 h, then the pellets were furnace-cooled by turning off the power. The resulting powders were confirmed to be alite by XRD.
Supplementary Material
Acknowledgments
This publication is based on work funded by the Skolkovo Institute of Science and Technology (Skoltech), “Center for Research, Education and Innovation for Electrochemical Energy Storage” program under contract 186-MRA. L.D.E. acknowledges support from the Banting Postdoctoral Fellowships program, administered by the Government of Canada. We thank Isaac Metcalf, Nathan Corbin, Kindle Williams, and Karthish Manthiram (Massachusetts Institute of Technology) for experimental assistance; Muhammad Adil and 24 M Technologies, Inc., for performing the BET measurements; and Form Energy, Inc., for providing access to the Phenom XL SEM. This work made use of the Shared Experimental Facilities supported in part by the Materials Research Science and Engineering Centers Program of the National Science Foundation under award DMR-1419807.
Footnotes
Conflict of interest statement: Y.-M.C., L.D.E., and A.F.B. are inventors on patent applications filed by Massachusetts Institute of Technology in relation to certain subject matter in the paper.
This paper results from the Arthur M. Sackler Colloquium of the National Academy of Sciences, “Status and Challenges in Decarbonizing our Energy Landscape,” held October 10–12, 2018, at the Arnold and Mabel Beckman Center of the National Academies of Sciences and Engineering in Irvine, CA. NAS colloquia began in 1991 and have been published in PNAS since 1995. From February 2001 through May 2019 colloquia were supported by a generous gift from The Dame Jillian and Dr. Arthur M. Sackler Foundation for the Arts, Sciences, & Humanities, in memory of Dame Sackler’s husband, Arthur M. Sackler. The complete program and video recordings of most presentations are available on the NAS website at http://www.nasonline.org/decarbonizing.
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