Encapsulation of highly viscous CO2 capture solvents for enhanced capture kinetics: Modeling investigation of mass transfer mechanisms
Introduction
Anthropogenic greenhouse gas emissions have risen sharply over the last few decades [1], [2]. Unless significant action is taken to reduce emissions, and possibly to remove CO2 from the atmosphere, significant and disruptive changes in global mean temperature will occur [3]. A prominent approach for both reducing CO2 emissions and removing CO2 from the atmosphere is Carbon Capture and Storage (CCS), in which dilute CO2 is isolated and geologically stored [4]. A large number of technologies have been investigated for carbon capture, including liquid solvents [5], solid sorbents [6], membranes [7] and various composite materials [8], [9].
Several next-generation, water-lean solvents for CCS are under active development, including reactive ionic liquids [10], CO2-Binding Organic Liquids [11], and liquid-like Nanoparticle organic hybrid materials (NOHMs) [12]. It is possible that the relatively low water content of these solvents could reduce the energy required for carbon capture, by reducing evaporative losses in the stripper, and also by reducing losses around the main cross heat exchanger associated with the large specific heat capacity of water [13] (note that these claims have been debated within the literature [14]). Unfortunately, these anhydrous solvents are often more viscous than aqueous solvents, causing handling issues and, in some cases, reduced gas flux [13].
To overcome these issues, several authors have created high-surface area composite materials, in which liquid solvent droplets are immobilized within a solid capsule or gel. Vericella et al. [15] developed microencapsulated solvents (MECS), in which 100 − 600 droplets of solvent are encased in a thin, CO2-permeable polymer shell. The very large surface area of these capsules led to 1 to 2 orders of magnitude increase in volumetric gas absorption rates [16]. To further improve the scalability of the manufacture of these materials, Moore et al. [17] developed Solvent Impregnated Polymers (SIPs), in which liquid solvents are encapsulated inside a gas permeable polymer, creating a hybrid material which can be shaped into thin strands or small particles with very large interfacial areas for CO2 capture (Fig. 1). These materials may be created via a scalable, one-pot method, and the large CO2 permeability of the polymer matrix may enhance the gas flux into the material. A similar concept was explored by Nguyen et al. [9], who manufactured composites using a solid colloidal precursor rather than the emulsion precursor used by Moore et al. [17].
In our recent study [18], the manufacture of SIP particles containing polyethylene-functionalized NOHMs (named ‘NOHM-I-PEI’) encapsulated in a CO2-permeable silicone acrylate (TEGO Rad 2650, EVONIK) matrix was reported. NOHM-I-PEI is an ideal candidate for the SIP motif. This NOHM has a low water content, is highly stable at a wide range of temperatures, has negligible vapor pressure, has an exceptionally large equilibrium CO2 capacity (up to 7 mol CO2/kg NOHMs), and its properties may be tunable for both traditional point source carbon capture, and also Direct Air Capture (DAC). However, this material is very viscous, leading to strong diffusion-limitations and slow CO2 uptake. When NOHM-I-PEI was encapsulated inside silicone acrylate, the CO2 flux into the material increased by a factor of 50, relative to a neat NOHM-I-PEI liquid with the same surface area [18]. By cryogenically grinding the NPEI-SIP film into small particles (~0.5 mm average diameter), the rate of CO2 absorption was increased by a further order of magnitude.
The 50-fold increase in gas flux observed by Rim et al. [18] was significantly larger than the 2 to 4-fold increase in flux predicted by the model of Moore et al. [17], who considered encapsulation of chemical solvents operating within the pseudo-first order regime. In order to understand this discrepancy, in this study CO2 mass transfer mechanisms within NPEI-SIP are investigated. Diffusion-limited models are developed for CO2 uptake into thin films of NPEI-SIP, and also for CO2 absorption within a packed bed of polydisperse NPEI-SIP particles. These models are validated against experimentally measured CO2 uptake and breakthrough curves, and are used to analyze the diffusion–reaction regimes in which the SIP motif is likely to lead to the greatest increase in absorption rates. Finally, mass transfer rates within SIPs containing NOHMs-PEI are compared with other chemisorbents such as amine grafted silicates, and the implications for material development and process design are discussed.
Section snippets
Synthesis of SIPs containing NOHM-I-PEI (NPEI-SIPs)
NOHM-I-PEI (polyethylenimine ionically tethered to silica nanoparticles) was synthesized as previously reported [12]. Next, a SIP film (1 mm thickness) was prepared via the emulsification of liquid-like NOHM-I-PEI in a silicone acrylate (TEGO Rad 2650, EVONIK) phase under high shear and subsequent UV curing. The mass fraction of NOHM-I-PEI was varied from 10 wt% to 60 wt%. For a fixed bed experiment, SIP particles with a mean particle size of 430 μm were prepared by cryogenic grinding of the
Absorption of CO2 into NPEI-SIP films
The absorption of CO2 into an NPEI-SIP film may be modeled via a ‘moving front’ or ‘ash-layer controlled shrinking core’ model [19], [20], in which a layer of CO2-saturated material forms at the surface and gets thicker over time as a reaction front propagates into the material, as illustrated in Fig. 2. Such a model will be valid provided the chemical reaction is fast enough for diffusion through the saturated layer to be rate-controlling. Moore [8] showed that SIPs containing concentrated K2CO
Absorption of CO2 into thin NPEI-SIP films
In Fig. 4(a), CO2 uptake into 1 mm thin films of NPEI-SIP measured using a TGA operated at 1 atm CO2 is plotted for a wide range of material compositions. The data is plotted as , and, as predicted by Eq. (1), a linear region is visible on a number of the CO2 uptake curves. The linearity is particularly clear for the more dilute SIPs (10–30 wt%), though it tends to break down as the material becomes more saturated with CO2. It is possible that the small region of slow uptake at the
Discussion
CO2 capture data from both thin film experiments and fixed bed experiments confirms our hypothesis that the absorption of CO2 into NPEI-SIP is controlled via diffusion through a growing saturated layer. This is consistent with previous studies of SIPs containing K2CO3 solutions [17]. It is likely that this assumption will also hold for absorption from more dilute CO2 streams (e.g. air), though the shrinking core model may break down if the rate of reaction decreases faster than the rate of
Conclusion
In this study, the mechanism of CO2 capture in NPEI-SIP systems (SIPs loaded with polyethylenimine functionalized silica nanoparticles) was analyzed. Mass transfer of CO2 into NPEI-SIP films was measured and shown to conform, both qualitatively and quantitatively, with a diffusion-controlled moving front model. When this model was applied to a fixed bed containing polydisperse NPEI-SIP particles, it accurately predicted experimentally measured CO2 capture breakthrough curves at multiple
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
The authors would like to acknowledge Shell’s New Energy Research and Technology (NERT) Program for providing the funding for the part of this study performed at Columbia University. We would also like to acknowledge Dr. Santhosh Shankar and Dr. Sumit Verma from the NERT’s Dense Energy Carriers team (DEC) for their useful input and discussions during the course of this work. The contribution by Dr. Thomas Moore was supported by Lawrence Livermore National Laboratory (LLNL) under Contract
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