The invention pertains to the field of generating high-purity and ultra-high-purity methane. Specifically, it involves the use of materials that both capture and convert carbon dioxide to produce hydrocarbons such as methane and ethane of sufficient purity for use in chemical vapor deposition (CVD) processes for diamond and graphene synthesis or other processes seeking high purity hydrocarbons for thermochemical processes or other applications.
Conventional processes to make high purity small hydrocarbons such as methane via atmospheric carbon capture for synthetic diamond growth are dedicated to multi-reactor processes—using one process to capture carbon dioxide and another to generate the methane. Vince et al (U.S. Pat. No. 9,994,970) highlights the multistep process required to first capture the CO2, cool, and expand the gas, before separation and hydrogenation in separate process hardware. Shearman et al (U.S. Pat. No. 11,371,162) adds to the related art by specifying the filtration steps required to purify the CO2 of any contaminants, and specifically remove nitrogen contamination from amine-based sorbents, before the methanation step. Recently, Shearman et al (U.S. Pat. No. 11,713,250) has also shown how an isotopic enrichment step between carbon capture and methanation can result in methane and a CVD product of methane with a specific isotopic signature.
In contrast to these high purity methane generation techniques, there is a growing body of methane generation technologies from a single material comprising two or more functions (DFM or dual functional materials): capturing the CO2 and catalyzing the reaction of CO2 with H2 to CH4. These processes, typified by Gonzalez-Velasco et. al. publication titled “Mechanism of the CO storage and in situ hydrogenation to CH4 Temperature and adsorbent loading effects over Ru—CaO/Al2O3 and Ru—Na2CO3/Al2O3 catalysts” and Farrauto et al publication titled “Feasibility Study of Combining Direct Air Capture of CO2 and Methanation at Isothermal Conditions with Dual Function Materials”, struggle with the fact that the same reaction chamber used for direct air capture (DAC) must then be used for methanation. Conventional teachings are that systems and reactors that regularly contact air are incapable of producing high-purity gas. The associated published works use a nitrogen purge gas for the primary purpose of preventing the safety challenge of mixing high concentrations of oxygen and hydrogen. From the standpoint of making gas for CVD application, this process utilizing a nitrogen purge introduces additional external contaminants into the product. Additionally, the catalyst in these designs is deposited only on the surface along with surface-deposited CO2-capturing sorbent. This surface-deposited arrangement of catalyst and sorbent, as well as the traditional teaching that a significant portion of the adsorbed CO2 is chemisorbed in a configuration that would be lost under vacuum, makes the use of low-pressure systems, especially vacuum systems, challenging and counterintuitive for producing high purity hydrocarbon gas.
These conventional systems typically delaminate their catalyst over time due to mechanical stress, in many cases expensive rare metals, through the use of low pressure. Finally, in Farrauto et al and said associated published works, there is no teaching to alter the process steps to selectively capture and convert carbon dioxide with ultrahigh purity or based on the isotope of carbon to produce an isotopically enriched methane that is up to ten-times or more valuable for CVD applications.
The resulting product gas in the Farrauto et al applications and publication is therefore highly contaminated with nitrogen and is of the same isotopic ratio as CO2 that exists in nature. These gases are therefore of low value to applications requiring high purity methane. Although the nitrogen contamination can be removed via a nitrogen rejection unit based on cryogenic distillation or pressure swing adsorption to the level of purity for pipeline gas using existing technologies, this mixture would require energy-intensive, slow, and expensive purifications to reach a sufficient level of purity (<1 ppm N2) for chemical vapor deposition applications. Moreover, the Farrauto et al process steps do not incorporate any downstream purification methods required for high purity methane due to both the limited applications and the batch nature of their process.
The present invention details a process for producing high-purity hydrocarbons (e.g., methane, ethane) using one or more main or “core” reactors, wherein each main reactor comprises both a sorbent and a catalyst. The initial production of hydrocarbons comprises multiple steps conducted in the same hardware: CO2 capture, reactor discharge of non-sorbed species, and hydrogenation. In most embodiments, a catalyst activation step is also conducted, after said reactor discharge of non-sorbed species, to activate the hydrogenation catalyst. This activation step comprises raising temperature to the reduction temperature of the provided catalyst, typically also causing the hydrogenation step to begin. The application of innovative vacuum steps, purge cycles, recycle loops, and/or temperature swings during these steps, in conjunction in certain embodiments with multiple main/core reactors and downstream upgrading steps, results in the generation of hydrocarbons suitable for use in chemical vapor deposition processes, such as those used in diamond and graphene growth. Preferred embodiments are capable of capturing CO2 from air to produce a feed stream to said chemical vapor deposition processes that contains hydrogen, methane and/or ethane, and preferably very low nitrogen in the range from about 0.0001 to 10 ppm, and more preferably less than 1 ppm nitrogen. Certain embodiments are capable of capturing CO2 from air to produce a feed stream to said chemical vapor deposition processes that contains hydrogen, methane and/or ethane, and less than 1 ppb nitrogen. Various embodiments of the invention overcome these challenges to efficiently generate hydrocarbons like methane potentially with enhanced isotopic purity and nitrogen contaminants less than 1 ppm in the hydrocarbon product stream.
Referring to the Figures, there are shown several, but not the only, embodiments of the invented processes and apparatus.
The Examples may be briefly summarized as follows. Example 1 features/emphasizes a simple embodiment of the system with a recycle loop, the system sending effluent methane and hydrogen into the downstream purification steps as well as the use of temperature and flow-rate swings to isotopically enrich the methane used in the CVD process. Example 2 features/emphasizes changing the substrate, support, sorbent, and catalytic portions of the system; the pairing of ruthenium with base metal catalysts capable of performing the hydrogenation reaction under similar conditions; and the use of the hydrogen/methane CVD effluent in a hydrogen fuel cell to substantially recycle the inputs (electricity, water, and CO2). Example 3 features/emphasizes using a catalyst that forms multi-carbon hydrocarbons, higher pressure and or temperature in Step 4 for hydrogenation, and combining all downstream purification steps into a single separation step. Example 4 highlights a full-scale commercial reactor operating at the current best practice for the reactor. Examples 5 and 6 highlight working bench-scale reactor operations producing high-purity methane from atmospheric carbon as detailed herein. Examples 7 and 8 highlight surprising performance of particular components of the system, the near-thermoneutral performance of sorbent-enhanced methanation catalysts and a fuel cell for selective hydrogen oxidation, respectively.
Certain embodiments of the present innovative process utilize a reactor system that combines the functions of carbon dioxide (CO2) capture and its subsequent conversion with hydrogen into hydrocarbons such as methane (CH4) within a singular operational unit where process steps are conducted at different times or as “displaced by time”. This integration is enabled by employing a unique matrix of dual-functional materials that serve both as sorbents for CO2 capture and catalysts for its conversion.
The sorbent component of the reactor is engineered with high-performing carbon capture materials, including alkali metal oxides and alkaline earth metal oxides comprising potassium (K), lithium (Li), sodium (Na), calcium (Ca), magnesium (Mg), strontium (Sr), and/or barium (Ba), and combinations thereof. Alternatives could encompass amine functionalized materials, metal-organic frameworks (MOFs), zeolites, or combinations thereof. In an ideal embodiment, these materials have a high surface area, typically exceeding about 50 m2/g, providing an enhanced adsorption capacity typically greater than about 500 μmol CO2/g and from about 300 to 5000 μmol CO2/g, thereby ensuring optimal capture efficiency of CO2 directly from ambient air.
Simultaneously, the dual function material within the reactor houses a catalyst subunit, which may comprise active metals such as ruthenium, nickel, platinum, rhodium, copper, cobalt, or group VIII transition metals, their respective oxides, and combinations thereof. Alternatively, the catalyst could be a composite of group VIII transition metals in conjunction with group I alkali metals and group VII transition metals, promoting versatile and effective conversion of the captured CO2 into useful hydrocarbons with carbon-carbon bonds. The catalyst can be applied onto the carrier material through various methods such as impregnation, ion-exchange, grafting, anchoring, post-colloidal deposition, spray coating, dip coating, or precipitation. Typically, the catalyst loading could range from about 0.25% to 30% by weight of the total coating and preferably from about 0.5 to 10 wt %, contingent upon the specific catalyst, the target reaction, and the process input conditions. The loading of the catalyst and sorbent have been combined to ensure that the reactions that occur during the desorption/methanation phase are substantially thermally balanced as defined by a gradient less than 50° C. and preferably a gradient less than about 20° C. FIG. 15 lists example reactions and their enthalpy of formation. Methanation is highly exothermic with a standard state heat of reaction at about −165 kJ/mol and about −178 kJ/mol at a reaction condition of 300° C. and desorption of CO2 is highly endothermic (estimated with a heat of desorption from about 50 to 200 kJ/mol), thus balancing the two reactions is key to optimal energy efficiency and simplification of system requirements to eliminate the need for additional heat transfer equipment, fluids, pumps, and processing and/or design complexity. Modulating the rate of desorption is done by changing the loading of the sorbent and similarly modulating the rate of methanation is done by changing the loading of the methanation catalyst.
In an embodiment, both the sorbent and the catalyst are deposited onto a carrier material to create a cohesive operational unit that may be substantially fully or partially mixed throughout the layer or disposed as sequential layers wherein one or more layers of each material may be disposed upon each other. The carrier may comprise porous ceramic-based materials such as aluminum oxide (Al2O3), ceria (CeO2), zirconia (ZrO2), silica (SiO2), or zeolites (SiO2—Al2O3), and combinations thereof, each offering distinct advantages in terms of stability, thermal tolerance, and performance enhancement. In certain embodiments, the carrier, sorbent, and/or catalyst of the DFM, and the synthesis of the DFM, are specially adapted to ensure that the coated DFM is robust against vacuum pressure.
The carrier material is deposited on a multi-channel substrate such as honeycomb type monolith made from alumina, cordierite, or other ceramic. Alternatively, the carrier material is deposited on a multi-channel substrate formed by multiple parallel plates substantially similar in structure and style to ART™ Plate Reactors or similar microchannel or millistructured plate reactors. Alternatively, the carrier material is deposited on a corrugated metal ribbon that has been bent to form a flow-through substrate made up of a series of substantially parallel open flow channels. The metal ribbon may comprise stainless steel or iron-chromium-aluminum alloys (FeCrAlY) or other metals such as anodized aluminum. Alternatively, the carrier material is deposited onto a series of mesh filters also consisting of Nichrome or FeCrAlY. Alternatively, the carrier can be deposited onto a metallic based monolith type structure that may be manufactured using 3D printing or other manufacturing methods including brazing, welding, or diffusion bonding to create a regular or irregular open pore structure for flow through the device. In an alternate embodiment, the carrier may be disposed upon a metal or ceramic foam that has an irregular or regular first macropore structure for flow substantially through the reactor.
In summary, substrates for receiving carrier material and DFM are preferably rigid or substantially rigid structures that have multiple channels running longitudinally through the structure, each channel being open at both ends and not having any significant bends or blockages so as to reduce the pressure drop from the flow across the path length. One example of monoliths that may serve in supporting the carrier material and DFM are core-drilled ceramic (cordierite) monolith pieces where the channels are square and roughly 800 microns in height and width with the wall being approximately 100 microns in width. Another example is a metal monolith as described above that is spiraled, corrugated FeCrAlloy foil. The amplitude of the corrugation is also approximately 800 microns.
At least one main reactor 20, 120, 220, 320, 420, 520, 620, 720 containing one or more of the above dual-function materials, is provided in a process flow scheme P, P1, P2, P3, P4, P5, P6, P7, such as those shown in
The initiation of the capture phase begins when the dual-function material reactor, embodying both sorbent and catalyst subunits, is exposed to an air or gas stream containing carbon dioxide (CO2). The source of this air could originate directly from the ambient atmosphere and so CO2 concentration may be about 350 to 500 ppm in dry air. Unless otherwise stated, all percentages of gas concentration stated in this text are volumetric percentages or ratios referring to the volumetric percentage or ratio of the gas in a dry gas composition. In other words, water vapor is neglected in citations of gas purity. Alternatively, the incoming stream could be partially or wholly supplemented by the emissions resulting from chemical vapor deposition process, hydrocarbon combustion, off-gas released from a fermentation process that comprises from about 1 to 99.999% CO2 by volume such as anaerobic ethanol production fermentation or aerobic fermentation used in the production of specialty biological, chemical, protein, food, or energy products, anaerobic digester, landfill gas, and/or flaring processes. Before initiating the capture phase, the gas may undergo pre-processing steps to enrich the concentration of carbon oxides or a specific isotope of carbon oxides by cryogenic distillation, membrane separation, temperature swing adsorption, pressure swing adsorption, or selective oxidation.
The sorbent component of the reactor, engineered for CO2 interaction, systematically adsorbs or absorbs CO2 molecules from the air or other gas stream until a saturation point is attained fully or partially, this point representing a state of thermodynamic equilibrium when fully sorbed. In one embodiment of the invention, the capture phase operates under conditions of ambient temperature and pressure, thereby maximizing operational simplicity and cost-effectiveness. In another embodiment of the invention, the capture phase operates under higher pressure (at or about 900 up to 3000 torr) to minimize the size of the reactor and speed at which the saturation point is reached. In a third embodiment of the system, the flow rate, pressure, and temperature of the reactor are varied across the reactor to favor adsorption of CO2 containing one specific isotope (e.g., carbon-12) over another (e.g., carbon-13).
The concentration of CO2 in the exhaust stream from the DFM reactor is an essential parameter that informs the saturation status of the sorbent. In this innovative reactor system, CO2 concentration is assessed via an integrated sensor mechanism, often employing advanced mass spectrometry, non-dispersive infrared (NDIR) sensors, or electrochemical sensors. Such sensors are typically placed strategically downstream of the reactor, where they monitor and record the concentration of CO2 in the outgoing air or gas stream. Upon initiation of the capture phase, Step 1, the sorbent in the reactor effectively adsorbs or absorbs CO2 from the incoming air or gas stream, resulting in a significantly reduced concentration (as defined by about 80% or greater reduction from the inlet composition when flowing air over the reactor at the ideal flow rate) or potentially near-zero levels of CO2 in the exhaust stream as defined below about 80 ppm, below about 50 ppm, or from at or about 0 up to 30 ppm CO2. As the sorbent approaches its saturation point, its capacity to adsorb additional CO2 decreases. This change is reflected as a gradual or rapid increase in the CO2 concentration in the exhaust air or gas stream, detected and reported by the CO2 sensors. The hardware is preferably designed with open flow channels (also “open-ended flow channels”) then coated with a carrier and the DFM material for at least a portion of the length and at least a portion of the circumscribed channel walls. The open flow channels are preferably less than 2-mm in diameter, hydraulic diameter, or in width and/or height, to improve mass transfer of CO2 from the bulk flow path to the DFM coated on the channel walls. An enlarged, detail view of the area of the reactor circled in
A critical indicator of essentially full sorbent saturation is the phenomenon known as ‘breakthrough’. This occurs when the concentration of CO2 in the exhaust stream (16) begins to approach the concentration in the incoming air or gas stream, revealing that the sorbent is no longer effectively capturing CO2. The breakthrough point, accurately detected by the system's integrated sensors, signals the need for the initiation of the reactor's purification or discharge of non-sorbed gas phase. See, for example, the CO2 concentration curve at the transition from Step 1 to Step 2 in
As part of the seamless operation, in one embodiment of process P (
In certain embodiments, the reactor purification phase, Step 2, commences with the effective clearance of residual air from the reactor, by conducting a hydrogen purge until the non-sorbed species flow out of the reactor (
It is critical that this vacuum step is conducted within an optimized temperature range, typically between at or about 10° C. and 150° C. Careful temperature control during the vacuum step is necessary to minimize thermal degradation, delamination, and/or decomposition of the sorbent and catalyst materials, thereby preserving their functional capabilities for subsequent cycles of operation. Additionally, as some sorbents are hygroscopic and will have adsorbed water during the capture phase that will be released when the reactor is put under vacuum, the temperature and vacuum condition are controlled in tandem to optimize performance of the entire system. Finally, in some embodiments, these parameters will be tuned to promote the release of some CO2 containing one carbon isotope (e.g., carbon-13) over another carbon isotope (e.g., carbon-12).
The evacuation time for this step has been calibrated, balancing the efficiency of the process and the stability of the materials. In conventional operation, the evacuation for a reactor with a volume of 1 m3 may take anywhere between at or about 3 seconds to 30 minutes, a duration based on the specific reactor design, the volume of the reactor, and the material system used. The duration of this vacuum according to preferred embodiments of the invention is between at or about 10 microseconds and 120 seconds, and in some embodiments 10 microseconds up to less than about 75 seconds, a duration optimized based on the specific reactor design, the volume of the reactor, the material system used, and the desired isotopic ratio. In some embodiments, the reactor is evacuated in two stages: first to rough vacuum with instrumentation such as a scroll pump, diaphragm pump, or rotary vane pump and later to high vacuum with instrumentation such as a turbomolecular pump, vapor jet pump, ion diffusion pump, or cryogenic pump.
Upon successful evacuation, the reactor volume is replenished with a flow of high purity hydrogen, ideally sourced from natural hydrogen wells or a sustainable method such as water electrolysis though can be delivered from any hydrogen source. This replenishment process effectively and substantially displaces remaining air in the reactor and primes the catalyst for the subsequent conversion process. The remaining content of oxygen and nitrogen in the reactor effluent after the hydrogen purge is less than at or about 1% by volume, preferably from about 0 to 0.1%, more preferably still from about 0 to 10 ppm, and most preferably less than at or about 1 ppm.
The cycle of vacuum application and hydrogen flow can be repeated as necessary, depending on the specific design of the reactor and the characteristics of the dual-function material system. In certain embodiments of the reactor, the cycle of vacuum application and hydrogen flow is done two to five times, or, in other embodiments, more than five times. The effluent of the reactor (16) is monitored for concentration of CO, CO2, H2, O2, H2O, and/or CH4.
In certain embodiments of the reactor, the hydrogen flow is conducted under conditions of ambient temperature and pressure, thereby simplifying the process, and minimizing the energy requirements. In certain other embodiments, the hydrogen flow is conducted at a pressure between at or about 1000 and 25,000 torr to quickly clear the reactor of residual air. In a preferred embodiment, hydrogen flow pressurizes the reactor to between at or about 1000 and 10000 torr, and more preferably from at or about 3000 up to 10000 torr.
The reactor purification phase is integral to the overall functionality of the reactor system, ensuring the production of high purity hydrocarbons across multiple operational cycles with minor downstream purification steps. The surprising result that the effluent of the core reactor can reach high purity on commercially viable timescales, while maintaining the structural integrity of the reactor and its internal DFM coatings of catalyst and sorbent flouts conventional teachings that regularly introducing air into porous sorbent/catalyst materials are not suitable for high-purity processes.
The process steps comprising CO2 capture at a first temperature, reactor evacuation with a vacuum step, and heating to at least one second temperature for a hydrogenation reaction to produce hydrocarbons with desorbing CO2 is conducted in the same inventive hardware as displaced in time during the process cycle. It is advantageous to minimize process hardware rather than conduct the process using separate unit operations and hardware to capture CO2 then desorb CO2, to purify the CO2, and then to react the purified CO2 with hydrogen to produce methane or other hydrocarbons. Hardware is reduced with the inventive process along with associated piping between process steps. Further the inventive process utilizes energy produced from the highly exothermic Sabatier or methanation reaction to supply necessary energy to desorb CO2 without the use of intervening complex heat transfer equipment as required with existing technology. The advantages of the inventive integrated process steps as displaced by time enable a more energy and exergy efficient compact process and system hardware for the capture and conversion of CO2 to hydrocarbons.
When the effluent of the reactor has a significant hydrogen constituent defined by a concentration greater than about 1%, as it is in the purge cycles of Step 2, the flow can be diverted to a hydrogen fuel cell or other process instrumentation to convert, separate, or utilize hydrogen. Given that the reactor could be active in CO formation which typically poisons hydrogen fuel cell catalysts, this step is counterintuitive but could provide energy to different steps of the process. The anode is composed of platinum but may also be doped with additional metals such palladium, ruthenium, gold, cobalt, or other metals that enhance the resistance to potential carbon monoxide poisoning. This fuel cell can either be a standard fuel cell, chosen from many currently available fuel cell products, which converts hydrogen into energy or a fuel cell/electrolyzer that oxidizes hydrogen at the anode and produces hydrogen at the cathode (sometimes called an electrochemical hydrogen pump). This offers the benefits of providing power, purifying and pressurizing the hydrogen for reuse, and/or altering the concentration of the hydrogen gas in the stream. Additionally, the fuel cell could be designed to collect excess gas that is not oxidized by the fuel cell's anode such as CO2 and CH4. In such a design, the anode compartment may operate between a pressure of at or about 1 PSI and 150 PSI and the gas collected from the anode gas outlet may be recycled through the reactor or collected, pressurized, and stored as its own product stream. The power load on the fuel cell may be set up as a variable load to vary the driving force of hydrogen oxidation, which allows precise control over the hydrogen removed from the stream. Traditional teachings hold that fuel cells should operate under conditions where hydrogen purity is of the utmost importance, and purposefully introducing contaminants in the anode would render a fuel cell inoperable. By carefully calibrating the fuel cell components, power draw, flow rates, and pressures, the present inventors have shown surprising results of significantly enriching the methane in the exhaust of the anodic compartment of a fuel cell while maintaining fuel cell performance.
The process of catalytic activation, Step 3, commences with a controlled increase in the reactor's temperature under the flow or presence of high-purity (>99.999% purity) hydrogen. The primary objective of this step is to enact a reduction reaction that revitalizes or “regenerates” the catalyst by increasing the number of reduced metal sites, counteracting any oxidation that may have transpired during exposure to oxygen in the air or feed gas during the capture or sorption part of the process cycle. It is recognized that the catalyst may not be fully reduced nor is this essentially required, rather, the catalyst must be sufficiently reduced such that there are enough active sites to convert the sorbed CO2 with hydrogen to methane or other hydrocarbons during the hydrogenation cycle.
Depending on DFM formulation and other process parameters, temperatures for catalytic activation and hydrogenation are expected to fall in a broad range, for example, for many but not necessarily all embodiments, a range of 50° C. to 400° C. for activation and 180° C. to 400° C. for hydrogenation. The catalytic activation step is conducted at temperatures that are elevated relative to the ambient temperature preferred for the CO2 capture and reactor purification steps, for example, between 180° C. and 350° C., between 225° C. and 300° C. (
In certain alternative embodiments, the exhaust gas resulting from this activation step is uniquely managed by directing reactor effluent/flow containing CO2, which tends to occur during activation and may also occur during hydrogenation, back to the original or sole reactor for further processing of the desorbed CO2. See
Therefore, in certain embodiments, the recycle loop may commence during the activation step (Step 3), and the recycle loop may continue into and throughout the hydrogenation step (Step 4). In certain embodiments, recycle through said recycle loop may be conducted all through the activation and/or the hydrogenation steps, or may be done intermittently in a “stop and go” pattern as desired, in other words “transiently”. In certain embodiments, said recycle is conducted transiently when the methane reactor effluent contains less than 1 percent CO2 by volume, or started again to be continuously or substantially continuously when the CO2 in said reactor effluent rises above 1 percent by volume in the effluent. While in operation, the recycle loop directs the flow from the outlet back to the inlet and is capable of directing gas at any temperature. Thus, the recycle loop is compatible with the temperature ramp of the activation step.
Redirecting the gas from the outlet via the recycle loop ensures full capture of CO2 that may be desorbed during the activation step and increases the residence time of the product gas within the reactor to achieve complete conversion. As the products are recycled in Steps 3 and 4, the recycle loop may also be used to condense water out from the reactor by decreasing the temperature of the gas below the dew point. In that case, the reactor may gradually decrease in pressure as five moles of gas are converted to one mole of gas. Thus, the recycle loop or the reactor may have additional inlet ports where the reactor can be supplemented with additional hydrogen gas as the hydrogenation reaction continues. Alternatively, the recycle loop may be used to further heat the gas, increasing the speed of the heat ramp during the activation step, which would result in the produced water remaining in the gas state. In such a case, the recycle loop or reactor could have additional hydrogen inlet, but the decrease in pressure would be approximately half of what would occur if the water were condensed within the recycle loop.
In one embodiment, a reactor with a 1000 L volume reactor interior space would have a pump recycling (also “recirculating”) the effluent during the activation step at a flow rate between about 5 SCFM and 1000 SCFM. In a preferred embodiment, the pump is recirculating the reactor gas at a flow rate between about 250 SCFM and 300 SCFM. Sec
Upon successful reduction of the catalyst, the reactor's temperature is adjusted to facilitate optimal hydrocarbon formation in Step 4. This temperature typically falls within a range of about 250° C. to 500° C., an interval that has been selected to maximize catalytic activity, selectivity, hydrocarbon yield, and/or any change to the isotopic ratio. By selectively converting CO2 containing one isotope (e.g., carbon-12) over another (e.g., carbon-13), the final hydrocarbon product will be significantly isotopically enriched.
Hydrocarbon formation by hydrogenation step employs a calibrated pressure regime, typically within a spectrum of at or about 700 torr up to 25000 torr. Operating within this pressure range ensures an optimal environment for the catalyst to facilitate the conversion of captured CO2 into the desired hydrocarbons, thus enhancing the reactor's operational efficiency. Most single carbon hydrocarbon products are generated at near atmospheric pressure of about 700 torr whereas longer hydrocarbons with higher counts of carbon-carbon bonds use progressively higher pressures through about 25000 torr. For example, methane is generated around atmospheric pressure (˜760 torr) whereas a system that favors ethane generation performs the hydrogenation step at higher pressures (from about 1000 to 5000 torr).
The exhaust gas from the reactor is monitored for the presence of hydrocarbons, employing advanced gas chromatography or mass spectrometry techniques, sensors, or other methods. This real-time monitoring aids in determining the progress and completion of the hydrocarbon formation process.
Once the monitoring system identifies that the exhaust gas stream (16) is comprised of hydrocarbons, the direction of the gas feed flow is strategically altered. For example, rather than being directed towards the recycle loop (18) (as previously described) for processing in a separate catalyst-containing reactor (B) or the purge stream (22), the hydrocarbon-rich gas stream is rerouted (26) to the primary product stream.
The hydrogenation cycle of Step 4 completes when the exhaust stream (16) displays only trace levels of hydrocarbons or is predominantly hydrogen signifying that the CO2 sorbed in a previous stage is substantially depleted. At this stage, the comprehensive four-step process-encompassing capture, reactor purification, catalytic activation, and catalytic conversion-is restarted in the main reactor. However, depending on the intended inlet/feed stream, a vacuum step may be employed prior to the CO2 capture step in some embodiments to evacuate flammable gas in the reactor without the use of an inert gas, thus maintaining a high purity environment. The dynamic monitoring of the hydrocarbon concentration in the exhaust stream, coupled with the strategic rerouting of gas flow, may ensure the continual production of hydrocarbons and the optimal utilization of the reactor system.
As described herein for the inventive process, different heating steps are used. The heat for these steps can be applied either through conventional means including resistive heating elements providing heat via convection, conduction, and radiation or less conventional mechanisms such as direct excitement and heating of the catalyst by stimulating plasma via microwave at 2450 MHz, dielectric barrier discharge (see
The main product stream (26) derived from the innovative reactor system is processed through downstream upgrading steps to ensure the generation of ultra-high purity hydrocarbons. In certain embodiments, a crucial aspect of these upgrading steps is the incorporation of a secondary, catalytic process (30). This process serves to convert residual CO2 into hydrocarbons, like CH4. The concentration of CO2 from the first reactor (26) may be between about 0.00001% and 20% by volume, but in preferred embodiments, the CO2 concentration is expected to be in the approximate range of about 0.00001%-0.0005%, when the double reactor setup, recycle/recirculation loop, switching mechanism, and temperature are all optimized for maximizing the extent of methanation reaction in the dual function materials reactor (20). The rest of the composition of stream 26 is primarily comprised of hydrogen and methane, and the methanation reactor (30) reduces the percentage of CO2 further in the effluent to less than about 0.00001% CO2, but more preferably to between about 0.00001% and 0.0005% and most preferably less than about 0.00001% (32). Recycle stream (18) may be used to prevent/minimize buildup in the reactor (20) of CO2 from the catalyst activation stage (Step 3) and reduce the CO2 concentration from the first reactor effluent (26). For example,
The secondary catalytic step (30) may be conducted under different temperature and pressure conditions compared to the main reactor (20A or B), with parameters specifically optimized to maximize conversion efficiency. This reactor can utilize similar catalytic materials for performing the CO2 hydrogenation reaction as the main reactor including nickel and/or ruthenium metal catalysts but may include additional catalyst materials such as cobalt, palladium, and rhodium or others that all have different temperatures for the methanation reaction. This step thus ensures the substantially complete utilization of CO2 as defined by greater than 95% conversion and preferably from about 98 to substantially 100% conversion, further enhancing the economic viability and environmental impact of the reactor system. Thus, the combination of the main reactor system (20A or B) and the secondary catalytic process (30) may be described as providing multiple-stage, multiple-catalyst hydrogenation of CO2.
A subsequent downstream step (40) targets the removal of trace nitrogen that may be present in the product stream, for example, by reacting N2 with H2 for subsequent NH3 removal (50) or other trace nitrogen purification techniques. One embodiment utilizes the unique chemistry of the gas mixture, which contains excess hydrogen, to convert the trace nitrogen into ammonia (NH3) or other nitrogen and hydrogen containing species. This strategic conversion not only aids in the purification of the hydrocarbon product stream but also may result in the production of ammonia (40), a valuable chemical with wide-ranging applications in sectors such as agriculture, cleaning, and industry.
In certain configurations, both the secondary catalytic conversion and the nitrogen removal steps could be performed within a single reactor. For example, iron and ruthenium catalysts have shown activity for the Haber-Bosch process and their presence in the secondary hydrogenation reaction could hydrogenate nitrogen contaminants in addition to CO2. This integrated approach to downstream processing serves to streamline the overall operation of the system, reducing complexity and energy requirements, and promoting process efficiency.
These downstream upgrading steps (30, 40) play a pivotal role in the overall process, ensuring the production of ultra-high purity hydrocarbons, and thus, contributing significantly to the commercial value and sustainability impact of the innovative reactor system.
The final phase of the reactor system process preferably encompasses a purification procedure, employing condensation (50) as a key method for the removal of water and or other liquid contaminants, such as trace ammonia, which may be present within the reactor.
Given that high purity methane serves as the principal end product, often found diluted in a hydrogen medium, several strategic measures are taken to achieve the final working concentration. One approach involves the further dilution of the product with hydrogen to the required concentration level. For example, the product (52) will likely contain 5%-40% hydrogen and high purity hydrocarbons are used in a working concentration of 1% to 10% hydrocarbon in 90% to 99% hydrogen, making dilution desirable or necessary. Alternatively, the system can employ purification techniques to eliminate excess hydrogen. In one embodiment, the full product gas could be sent through a hydrogen-air fuel cell (see
The versatility of the reactor and process design allows for co-location with chemical vapor deposition (CVD) facilities, enhancing operational synergy and efficiency. This integrated setup enables the direct flow of the product gas into the CVD chambers (58), significantly reducing the need for transportation and storage infrastructure.
In one particular embodiment, the hydrocarbons exhausted (70) from the CVD process (also, “excess” or “unused” hydrocarbons) could be treated in a combustive/oxidative process using substantially pure oxygen or steam (72), potentially sourced from the same water electrolyzer (10b) that produces the high purity hydrogen (8), to optionally recycle (80) from the combustion/oxidative process back to inlet stream 2. This procedure effectively combats any potential buildup of waste products within the system. It is generally understood that electrolyzer-produced oxygen will contain some amount of hydrogen that may be from about 0.001% to 2%.
In another embodiment, these hydrocarbons, typically with hydrogen, exhausted from CVD are reincorporated into the system after initial hydrocarbon generation (28). This strategic approach allows for the re-purification of the exhausted hydrocarbons, ensuring maximal utilization of the resources and preventing the buildup of contaminants within the system. This final phase of recycling the hydrocarbons exhausted from the CVD process, therefore, ensures the effective purification and use of product streams, exemplifying the reactor system's commitment to efficiency and sustainability.
In one potential embodiment PI of the inventive system, shown in
A reactor 20 of a volume of 1 m3 containing the above dual function material initiates the process by drawing in ambient air (102) containing about 400 ppm CO2 at a flow rate of 10 standard liters per minute (SLPM), modulated via mass flow controllers to ensure precision. The reactor is heated differentially across the bed of the reactor with the inlet (where pressure is highest) at near ambient temperatures and the bed of the reactor near the exhaust of the reactor (where pressure is lowest) heated to between about 20-50° C. based on the flow rate and pressure of the gas to differentially adsorb CO2 containing carbon-12 over CO2 containing carbon-13 based on natural phenomena such as active site specificity and kinetic isotope effects.
This gas stream is directed by the valve manifold (112) to contact the primary reactor (120A) until the Na2O sorbent portion becomes saturated with CO2, indicated by a CO2 concentration sensor which monitors the exhaust stream (116A). Upon reaching a predetermined threshold of CO2 breakthrough, the gas stream is redirected by the valve manifold (112) to a comparably equipped reactor (120B), while the original reactor (120A) undergoes a purge cycle (also discussed above as the “purification step”) to remove residual air. This purge cycle involves creating a slight vacuum within the reactor over a period of about 20 to 30 seconds at a pressure between about 10 and 100 torr at a temperature between about 15° C. and 60° C. The reactor is then purged with high-purity hydrogen at a flow rate of about 5 SLPM until at least five reactor volumes have flowed through the reactor (120A) under controlled conditions to ensure the substantially complete removal of residual air.
Next, the reactor (120A) continues to be subjected to a stream of high-purity hydrogen gas (108) at a flow rate of 5 SLPM, while the pressure within the reactor is maintained between about 700 torr and 800 torr and temperature between about 225° C. and 275° C. to ensure optimal catalyst reduction conditions. The pressure and temperature are carefully calibrated to favor the desorption of CO2 containing carbon-13 while leaving CO2 containing carbon-12 adsorbed. The temperature of the reactor is then systematically increased to between about 300° C.-350° C. to stimulate the simultaneous desorption of CO2 from the dual-function material and hydrogenation of the CO2. Once again, the temperature is finely calibrated to selectively convert CO2 containing carbon-12 to CH4 while leaving CO2 containing carbon-13 either in its original form as CO2 or catalyze its reduction to CO.
To confirm the progress and completion of the catalytic conversion, the reactor system employs a gas chromatograph mass spectrometry or commercially available syngas sensors that monitor the exhaust gas (116A) for the presence of methane. Once the monitoring system detects that the exhaust gas stream (116A) comprises predominantly methane, the flow is redirected from the recycle stream (118) to the primary product stream (126).
Finally, the product gas (126) is combined with exhausted gas (128) from the chemical vapor deposition process (CVD 158 via 170) and subjected to a series of downstream upgrading steps involving fine conversion of additional CO2 by additional hydrocarbon catalysis (130), pressure swing adsorption or temperature swing adsorption (140) to eliminate any trace impurities, such as water, residual carbon dioxide, and nitrogen. The output (152) of these multiple series process reactors (130, 140, 150), a high purity methane stream in high purity hydrogen, is then diluted further with high purity hydrogen (154) so that the high purity methane is only 1%-10% methane in 90% to 99% hydrogen ready for utilization. The contaminants (non-methane and non-hydrogen) in this final feed stream (156) to CVD (158) are expected to be less than about 0.01% by volume. This entire process P1, therefore, is an example of a unique embodiment that represents an efficient, sustainable, and reliable method for capturing and converting carbon dioxide into ultra-high purity methane stream with enriched isotopic purity used for CVD.
In another embodiment P2 of this inventive system, shown in
The reactor 220 of a volume of 1 m3 containing the above dual function material begins by mixing ambient air (206) containing CO2 supplemented with excess CO2 (280) from the exhaust of a solid oxide fuel cell (276) that is oxidizing excess hydrocarbons (272) from the effluent of a CVD reactor (264). The gas is cooled and then introduced (214A) into the reactor (220A) at a flow rate typically within the range of about 3-5 standard liters per minute (SLPM), controlled using mass flow controllers for accuracy.
The carbon dioxide laden gas stream passes through the valve manifold (212) to interact with the reactor (220A) that is uniformly at ambient temperature, in Step 1, until the zeolite sorbent portion becomes substantially saturated with carbon dioxide, which is determined by a carbon dioxide concentration sensor monitoring the exhaust stream (216A) or a reactor temperature sensor measuring any thermal events in the reactor occurring due to adsorption. Upon reaching a predetermined concentration at the reactor exit (216A) or the predetermined thermal cue, the carbon dioxide gas stream is redirected via the valve manifold (212) to another similarly equipped reactor (220B), while the initial reactor (220A) commences a purge cycle (Step 2) to eliminate residual air.
This purge cycle incorporates the generation of a slight vacuum in the reactor for about 30 seconds to 1 minute, at a pressure between about 5 and 20 torr. The reactor is then purged with high-purity hydrogen that comes both from water electrolyzers (210B) as well hydrogen purified from the main product gas (260) and CVD effluent (270). The hydrogen is introduced to the reactor at a flow rate of 2 SLPM, controlled to ensure the substantial removal of residual air. This cycle of vacuum and purge is repeated three times. The exhausted hydrogen (222) that is used to purge the reactor is sent to a recycle loop (224) that purifies out any contaminants using temperature swing adsorption and/or pressure swing adsorption to regenerate a hydrogen of greater than 99.99% purity before recycling it.
Following the purge cycle, the reactor is subjected to a hydrogen gas atmosphere at a pressure of about 1500 torr, without a continuous hydrogen flow. The reactor's temperature is then systematically increased to 275° C. to facilitate at least a portion of the reduction of the ruthenium and nickel catalysts.
Upon completion of the catalyst reduction (Step 3), the reactor temperature is brought to 325° C. and hydrogen flow (208) is resumed to facilitate the desorption of carbon dioxide from the dual-function material and catalytic conversion (Step 4) of the desorbed carbon dioxide into methane in the presence of the reducing hydrogen atmosphere.
A gas chromatograph or mass spectrometry unit continuously monitors the exhaust gas (216A) for methane. Once the exhaust gas stream (216A) is determined to consist mainly of methane, the flow is switched from 218 to the primary product stream (226) and to fine hydrogenation catalyst(s) (230). This reactor (230) can utilize similar catalytic materials for performing the CO2 hydrogenation reaction as the main reactor (220) including nickel or ruthenium metal catalysts but may include additional catalysts such as cobalt, palladium, and rhodium among others that all have different temperatures for the methanation reaction. The fine hydrogenation reactor is at similar temperatures to the main reactor (˜300° C.) but could be at higher pressures (about 700-7000 torr) to ensure complete catalytic conversion of the carbon dioxide.
In this embodiment, after fine hydrogenation (230), the product gas undergoes an additional step of nitrogen hydrogenation (240). In this step, trace nitrogen is reacted with excess hydrogen to form ammonia at 1 atm of pressure or higher and at a temperature of at least 300° C., further enhancing the purity of the resulting methane.
The final product gas undergoes condensation and additional upgrading steps (250) involving pressure swing adsorption or temperature swing adsorption to eliminate any residual impurities, such as water, residual carbon dioxide, and the newly formed ammonia.
The resulting gas (252) then undergoes filtration with membrane gas separation technology (260) to reduce the concentration of hydrogen in the product stream to approximately 10%. The high purity hydrogen that is filtered/purified out is then returned (262) to the start of the process. Effluent from the CVD process (258) is then similarly filtered/purified (270), so that the hydrogen gas returns (274) to the initial hydrogen stream (208) and a mixture containing substantial amounts of CH4 (272) is then oxidized via a hydrogen fuel cell (276) and the resulting CO2 is used to supplement the carbon capture step (280).
The reactor system 220 and process P2 thus provide a high purity methane stream in 10% H2 that can be directly used with further dilution with hydrogen before final CVD of the hydrocarbon (258). This entire process P2, therefore, is another example of a unique embodiment that represents an efficient, sustainable, and reliable method for capturing and converting carbon dioxide into ultra-high purity methane.
In a third illustrative embodiment of the invention, shown in
Notably, in process P3, the initial gas stream (302) being fed into the reactor (320) is combusted hydrocarbon and or product gas derived directly from a CVD process. The water from the combusted hydrocarbons may be recycled into the electrolyzer (310B). Under the influence of a mass flow controller, the gas (304) containing a significant concentration of carbon dioxide is introduced into the reactor at a flow rate typically in the range of about 1 to 5 SLPM. The gas stream interacts with the reactor (320) until the MOF (metal-organic framework) sorbent portion becomes substantially saturated with carbon dioxide, as determined by a carbon dioxide concentration sensor located in the exhaust stream (316).
Upon reaching a predetermined concentration of carbon dioxide in the exhaust, indicating substantial sorbent saturation, the gas stream is redirected via a valve manifold (312) to a similarly configured secondary reactor (320B). Owing to the lean-oxygen conditions under which methane is combusted after the CVD process, there is only trace surplus oxygen in the incoming gas stream. Consequently, the Fe—Ru—K catalyst is not highly oxidized, thereby allowing the process to only include a brief catalytic activation or reduction step (Step 3) that will be accomplished as the system transitions from reactor purification to hydrogenation. Step 3 therefore may not require any dedicated time and instead any trace oxidation will be removed as the temperature is increased under hydrogen flow.
As the reactor (320A) proceeds to the hydrogenation step (Step 4), hydrogen flow of 1 SLPM is commenced and the pressure of the reactor is brought to between about 5,000 torr and 15,000 torr depending on the targeted composition of hydrocarbons, as higher pressure will typically produce more C—C bonds. Also, the temperature is adjusted to a suitable range, typically 300° C. and 450° C., initiating the desorption of carbon dioxide and catalytic conversion of the desorbed carbon dioxide into light hydrocarbons, primarily methane and ethane. This step is facilitated by the reduced Fe—Ru—K catalyst, embedded in the amine-functionalized MOF, which retains its reductive potential due to the absence of excess oxygen in the initial gas stream.
A gas chromatograph or a mass spectrometer monitors the exhaust gas stream (316) for the presence of hydrocarbons. When the exhaust stream contains predominantly hydrocarbons, the flow is switched to the primary product stream.
This product stream then undergoes liquefaction to separate out CO, CO2, N2, CxHy, and H2. The trace N2 and CO is purged while the carbon dioxide is recycled back through the reactor (354). The remaining gas is hyper pure light hydrocarbons in hydrogen. The process thereby delivers an ultra-high purity stream of methane and ethane (352), which could be reintegrated into the CVD process (358) or utilized for alternative applications. Note that, in
In one potential embodiment of the inventive system, a substrate loaded with DFM-laden support for a reactor 420 is provided according to the following methods and compositions. A support layer between about 20 micrometers and 500 micrometers in average thickness of porous aluminum oxide (Al2O3) is first coated onto a FeCrAlY or FeCrAl, or similar alumina forming material when heat treated, flow-through monolith substrate with many parallel open channels coated with DFM. In a preferred embodiment, the alumina layer average thickness is between about 60 micrometers and 100 micrometers resulting in an alumina support loading of between 0.1 g/in3 and 2.5 g/in3 of flow-through substrate volume. Ruthenium (Ru) is then deposited on the alumina at a weight percent between 0.01% and 0.15% Ru resulting in a total loading of between 0.0007 g/in3 and 0.0105 g/in3 of flow through substrate. Nickel (Ni) is then deposited on the alumina at a weight percent between 0.1% and 5% Ni resulting in a total loading of between 0.007 g/in3 and 0.35 g/in3 per the flow through monolith substrate. A 1:2:0.5 mixture of sodium oxide (Na2O), calcium oxide (CaO), and potassium oxide (K20) is then loaded onto the flow-through substrate at a weight percent between 5% and 15% sorbent resulting in a total loading of between 0.01 g/in3 and 2.5 g/in3 of flow-through substrate.
The first step is started by drawing in ambient air (402, fan 410A) containing approximately 425 ppm CO2 on average at a flow rate between about 10,000 standard liters per minute (SLPM) and 1,000,000 SLPM, modulated via mass flow controllers to ensure precision. In a preferred embodiment, air is drawn into the process at a flow rate between about 400,000 and 600,000 SLPM.
This gas stream (404) contacts the reactor 420 until the Na2O sorbent portion becomes substantially saturated with CO2, indicated by a CO2 concentration sensor which monitors the exhaust stream. During this carbon capture step, CO2-lean reactor effluent 416 may be purged through purge line 422. Upon reaching a predetermined threshold of CO2, the gas stream is redirected to a comparably equipped reactor (not shown in
To confirm the progress and completion of the catalytic conversion, the reactor system may employ an infrared spectrometry and/or mass spectrometry unit, for the reactor effluent 416 or the recycle/recirculation loop 418 that may be operated during said temperature increase, to monitor the exhaust gas for the presence of methane. Once the monitoring system detects that substantially all of the hydrogen gas has been converted to methane, the reactor is evacuated with the product gas redirected to the primary product stream 426. A flow of hydrogen between about 1 SLPM and 50 SLPM is then introduced in the reactor for the remainder of the temperature ramp and temperature plateau. In a preferred embodiment, a flow of hydrogen between about 5 SLPM and 15 SLPM is introduced in the reactor 420 serving as a reactant to convert the adsorbed CO2 to CH4 and drive the product to the primary product stream 426. Once the reactor reaches 300° C., the reactor temperature is held at 300° C. until substantially all of the CO2 is desorbed and converted to CH4 with hydrogen. The molar ratio between the hydrogen introduced to the reactor during the heating step and the amount of CO2 adsorbed should be held between about 1:4 and 1:8. In a preferred embodiment, the molar ratio between the hydrogen introduced to the reactor and CO2 is between 1:4 and 1:4.1 resulting in an effluent directly from the core reactor that is greater than 90% by volume methane on a dry basis.
Finally, the product gas 426 is subjected to a series of downstream upgrading steps comprising condensation, pressure swing adsorption, membrane separation, reaction that might comprise a fuel cell to reduce the hydrogen composition, or temperature swing adsorption to eliminate or reduce trace impurities, such as water, residual carbon dioxide, hydrogen, and nitrogen. The downstream upgrading option shown in
Reactor 420 in Process P4 may be the same or similar to reactor 850 shown in
This entire process, therefore, embodies an efficient, sustainable, and reliable method for capturing and converting carbon dioxide into ultra-high purity methane used for chemical vapor deposition or other applications.
In one potential embodiment of the inventive system, flow-through monolith with DFM is provided according to the following methods and compositions. A layer between 80 micrometers and 120 micrometers in average thickness of aluminum oxide (Al2O3) is deposited onto a cordierite honeycomb monolith flow-through substrate with 400 cells per square inch (CPSI). Ruthenium (Ru) is then deposited on the alumina support at a weight percent between about 0.6% and 0.8% Ru resulting in a total loading of between 0.05 g/in3 and 0.15 g/in3 of a flow through substrate. Sodium oxide (Na2O) is then loaded or coated onto the flow-through substrate at a weight percent between about 7% and 12% Na2O resulting in a total loading of between about 0.2 g/in3 and 0.3 g/in3 of flow-through substrate. The balance between the sorbent and catalyst has been set to ensure that the combination of the desorption of the CO2 and the production of methane are balanced resulting in a process that requires minimal heating or cooling.
A single unit of the cylindric cordierite flow-through monolith with DFM is 42.5 mm in diameter and 50 mm in length. The DFM reactor piece is approximately 60 mL in volume. Thus, a reactor 520 consisting of four cordierite monoliths in series approximate a 240 mL reactor. Four cordierite pieces are loaded into a quartz tube approximately 400 mL in volume inside a tube furnace. The quartz tube is sealed by stainless steel flanges and fluorosilicone gaskets connected to a valve manifold on both sides. Downstream product gas is sampled with a residual gas analyzer with an in-line infrared CO detector. This gas sampling equipment is capable of measuring gas composition in the sub ppm regime as well as distinguishing isotopically enriched varieties of CH4.
In use, the reactor 520 with a 240 mL interior reactor volume contains primarily the flow-through monoliths with the dual function material, contained within the reactor wall. The process is initiated by performing multiple steps in the reactor: CO2 capture, reactor discharge of non-sorbed species, and hydrogenation. After reactor discharge of non-sorbed species, temperature is raised, which activates the catalyst, begins desorption of CO2, and starts hydrogenation.
In use of the above-described reactor 520, a process P5 initiated by drawing in ambient air containing approximately 425 ppm CO2 at a flow rate between about 50 standard liters per minute (SLPM) and 75 SLPM, modulated via mass flow controllers to ensure precision. The air is drawn in for about 60 minutes until the reactor is substantially saturated with CO2 as measured by the mass spectrometer. During this CO2 capture step, CO2-lean air from the reactor effluent 516 may be purged through a purge line such as illustrated by line 522.
The reactor undergoes a purge cycle to remove residual air. This purge cycle involves creating a slight vacuum within the reactor over a period of about 30 to 180 seconds at a pressure between about 0.1 torr and 10 torr at room temperature. The reactor is filled with hydrogen to approximate atmospheric pressure between about 700 and 800 torr. The purge cycle repeats by creating a vacuum and then filling the reactor 3 or more times until the substantially full removal of residual air is achieved.
Next, the reactor remains full of hydrogen at near atmospheric pressure. Valves then open gas lines to a pump compatible with flammable mixtures that circulates the hydrogen gas within the reactor at a flow rate of up to about 1.5 SLPM. Thus, the recirculation pump circulates the flow to the reactor at approximately three reactor volumes per minute. The temperature of the reactor is then systematically increased to 300° C. at a ramp rate between about 5 and 200 C/min to stimulate the substantially simultaneous desorption of CO2 from the dual-function material and hydrogenation of the CO2. During this step, CO2 containing reactor effluent 516 may be recycled to the reactor inlet by a recycle loop 518 such as portrayed in
To confirm the progress and completion of the catalytic conversion, the reactor system may employ infrared spectrometry in addition to the mass spectrometry unit within the flow recirculation loop and reactor that continually monitors the exhaust gas for the presence of methane. Once the monitoring system detects that substantially all of the initial reactor volume of hydrogen gas has been substantially converted to methane, the reactor is evacuated with the product gas redirected to the primary product stream. Evacuation of the gas usually occurs between about 180° C. and 250° C. when the ruthenium catalyst is sufficiently active for the hydrogenation reaction. A flow of hydrogen between about 0.05 SLPM and 0.5 SLPM is continually introduced in the reactor serving as a reactant to convert the adsorbed CO2 to CH4 and drive the product to the primary product stream. Once the reactor reaches 300° C., the reactor temperature is held at 300° C. until substantially all of the CO2 is desorbed and converted with hydrogen to CH4. See
Notably, during this stage the reactor requires less than 25 kJ of cooling or heating, as the endothermic desorption reaction and exothermic methanation reaction have been combined in order to approximate near thermoneutrality, as defined by a thermal gradient within the catalyst less than about 50° C. and more preferably between about 1 and 20° C. The molar ratio between the hydrogen introduced to the reactor during the heating step and the amount of CO2 adsorbed should be held between about 1:8 and 1:35.
The product gas is cumulatively about 95% high purity hydrogen with about 5% high purity methane on a dry gas basis. The output of the reactor can then be used in chemical vapor deposition processes. This entire process, therefore, embodies an efficient, sustainable, and reliable method for capturing and converting carbon dioxide into ultra-high purity methane used for chemical vapor deposition or other applications.
Reactor 520 in Process P5 may be the same or similar to reactor 750 shown in
In one potential embodiment of the inventive system, a flow-through monolith with DFM is provided according to the following methods and compositions. A support layer between 80 micrometers and 120 micrometers in average thickness of aluminum oxide (Al2O3) is deposited onto a FeCrAlloy monolith flow-through substrate with 600 cpsi. Ruthenium (Ru) is then deposited on the alumina at a weight percent between 0.6% and 0.8% Ru resulting in a total loading of between 0.05 g/in3 and 0.15 g/in3 of flow through substrate. Sodium oxide (Na2O) is then loaded onto the flow-through substrate at a weight percent between 7% and 12% Na2O resulting in a total loading of between 0.2 g/in3 and 0.3 g/in3 of flow-through substrate. The balance between the sorbent and catalyst has been set to ensure that the combination of the desorption of the CO2 and the production of methane are balanced resulting in a process that requires minimal heating or cooling.
The FeCrAlloy flow-through monolith with DFM is cylindrical measuring 120 mm in diameter and 140 mm in length. The piece is approximately 1.5 liters in volume and placed immediately upstream of the reactor in a heating coil that is approximately 150 CPSI. The heating coil may be optionally coated with additional DFM material similar to the bulk flow-through substrate. The cylindrical reactor is sealed by welded stainless steel flanges connected to a valve manifold on both sides. Downstream product gas is sampled with a residual gas analyzer with an in-line infrared CO detector. This gas sampling equipment is capable of measuring gas composition in the sub ppm regime.
In use, as in process P6 shown in
The process initiates by drawing in ambient air containing approximately 425 ppm CO2 at a flow rate between about 1000 standard liters per minute (SLPM) and 1500 SLPM, modulated via mass flow controllers to ensure precision. The air is drawn in for about 60 minutes until the reactor is substantially saturated with CO2 as measured by the mass spectrometer or other methods. During this CO2 capture step, CO2-lean air from the reactor effluent 616 may be purged through a purge line such as illustrated by line 622.
The reactor undergoes a purge cycle to remove residual air. This purge cycle involves creating a slight vacuum within the reactor over a period of about 30 to 180 seconds at a pressure between about 0.1 torr and 10 torr at room temperature. The reactor is filled with hydrogen to approximate atmospheric pressure between about 700 and 800 torr. The purge cycle repeats by creating a vacuum and then filling the reactor 2 or more times until the substantially full removal of residual air.
For the next step, the reactor remains full of hydrogen at near atmospheric pressure. Valves then open gas lines to a pump that circulates the hydrogen gas with any product within the reactor at a flow rate of up to about 30 SLPM. Thus, the recirculation pump circulates flow back through the reactor at approximately 20 reactor volumes per minute. The temperature of the reactor is then systematically increased to about 300° C. at a ramp rate from about 5 to 200° C./min to stimulate the substantially simultaneous desorption of CO2 from the dual-function material and hydrogenation of the CO2 to methane. During this step, CO2 containing reactor effluent 616 may be recycled to the reactor inlet by a recycle loop 518 such as portrayed in
To confirm the progress and substantial completion of the catalytic reaction, the reactor system may employ infrared spectrometry in addition to the mass spectrometry unit within the recirculation loop and reactor that continually monitors the exhaust gas for the presence of methane. Once the monitoring system detects that substantially all of the initial reactor volume of hydrogen gas has been converted to methane, the reactor is evacuated with the product gas redirected to the primary product stream. Evacuation of the gas usually occurs between about 180° C. and 250° C. when the ruthenium catalyst is sufficiently active for the hydrogenation reaction. A flow of hydrogen between about 0.05 SLPM and 0.5 SLPM is continually introduced in the reactor serving as a reactant to convert the adsorbed CO2 to CH4 and drive the product to the primary product stream. Once the reactor reaches about 300° C., the reactor temperature is held at 300° C. until substantially all of the CO2 is desorbed and converted to CH4. See
Notably, during this stage the reactor requires less than 25 kJ of cooling or heating as the desorption reaction and methanation reaction have been carefully calibrated in order to approximate thermoneutrality as defined by a gradient less than about 50 C. The molar ratio between the hydrogen introduced to the reactor during the heating step and the amount of CO2 adsorbed should be held between about 4:1 and 6:1 (hydrogen: CO2).
The product gas is cumulatively about 5% high purity hydrogen with about 95% high purity methane on a dry gas basis. The output of the reactor can then be used in chemical vapor deposition or other processes. This entire process, therefore, embodies an efficient, sustainable, and reliable method for capturing and converting carbon dioxide into ultra-high purity methane used for chemical vapor deposition or other processes.
Reactor 620 in Process P6 may be the same or similar to flow-through reactor 800 shown in
Further regarding reactor 800, an end view of the reactor is shown in
In one potential embodiment of the inventive system, a reactor with the same nominal dimensions and composition of DFM as in Example 5 is employed in a continuous mode to upgrade CO2-rich streams with near-thermoneutral performance. As in Example 6, the balance between the sorbent and catalyst has been set to ensure that the combination of the desorption of the CO2 and the production of methane are balanced resulting in a process that requires minimal heating or cooling.
The reactor is heated to 240° C. and held at this temperature with an external heating coil and thermocouple assembly that regulates the temperature. A stream of pure CO2 flowing at 0.2 LPM is combined with a stream of pure hydrogen produced via water electrolysis flowing at 0.8 LPM such that the two reactants are at a stoichiometric ratio for the methanation reaction. The CO2 stream is outfitted with a switching valve that can divert Argon flowing at 0.2 LPM into the reactor instead of CO2. An additional thermocouple is placed into the reactor on the face of the monolith on the downstream side. While maintaining a constant flow rate of H2, the switching valve that can select between Ar and CO2 is activated. Thus, while Ar is flowing alongside H2 no methanation is possible and the reactor will settle back to the setpoint temperature of 240 C. However, when CO2 is allowed into the reactor alongside H2 at a stoichiometric ratio, methanation proceeds with ideally over 70% conversion and the temperature in the reactor changes in response. To confirm the progress of the catalytic reaction, the reactor system may employ infrared spectrometry in addition to a residual gas analyzer unit that continually monitors the exhaust gas for the presence of CH4, CO2, Ar, and H2. Once the monitoring system detects that the continuous conversion of H2 and CO2 to CH4 has reached a steady state, or that the Ar saturation within has reached a steady state, the Ar/CO2 switching valve is actuated (see “regeneration” in
This process is schematically portrayed as process P7 in
In one potential embodiment of the inventive system, a gas with significant hydrogen and methane content such as the effluent from the core reactor in Example 4, Example 5, or Example 6 is directed to the anodic compartment of an electrochemical device as illustrated in
Referring to
The fuel cell is then connected to an electrical load either in the form of a power resistor or an electronic device that is carefully calibrated to provide a power draw that is equal to the power content of the incoming hydrogen oxidation target. The output of the anodic compartment is measured and the results from the embodiment are included in
This embodiment highlights the surprising result that by carefully calibrating the identity of the fuel cell components and power load, nearly all hydrogen can be consumed in a heterogeneous gas mixture comprising hydrogen and methane. This approach may be valid for streams produced from processes discussed herein when a reduced hydrogen feedstock is desired for a downstream user, for example, a CVD process preferring a low-hydrogen feedstock. The inventors believe that this is the first instance of fuel cell(s) being used to selectively oxidize hydrogen in a methane/hydrogen stream for purification, especially after a methanation reactor. Ethane Production:
Ethane may be beneficial or desired in CVD when manipulating the kinetics of the CVD reaction or when aiming to manipulate the properties of the product made via CVD. It may be noted that the proportions of methane and ethane produced from certain embodiments may be controlled mainly by pressure, catalyst, and sorbent composition. Pressure and sorbent composition affect the local concentration of carbon potentially leading to creating carbon-carbon bond formation. Catalysts with higher percentages of iron or cobalt or rhenium will tend to catalyze carbon-carbon bond formation.
The processes described in this document may be performed in differently sized reactors including research and development reactors and/or pilot-plant reactors, such as those portrayed in the Figures, and larger commercial-scale reactors. Commercial-scale reactors will likely contain many monoliths each between 6 inches and 12 inches in length. For example, based on an expected individual monolith length of 9-12 inches, a 12-foot reactor may contain as many as 15 monoliths. While flanges of reactors shown herein may, in certain embodiment, be adapted for use in adding or removing heat from the reactor, certain embodiments of the invention are expected not to need such adaptation or any other equipment for heating or cooling of the reactor because the reactions in the reactor are near thermoneutral. Therefore, certain embodiments need no flanges and/or comprise no heat exchanger for removing heat from the reactor being in thermal communication with the reaction chamber.
Certain embodiments of the invention may be summarized generally as encompassing novel methods, systems, and materials for the efficient capture of carbon dioxide and its conversion into ultra-high purity hydrocarbons, particularly methane. In various embodiments, the methods comprise the following steps: utilizing a reactor equipped with both a sorbent and catalyst; initiating contact between a gas stream containing carbon dioxide and the reactor until the sorbent portions reach a state of substantial saturation with carbon dioxide; diverting the stream of gas comprising carbon dioxide to a substantially similar parallel reactor; removing the residual air via vacuum and/or purge cycles with high-purity gas; introducing a stream of hydrogen gas to the low pressure reactor containing the carbon dioxide-saturated sorbent and catalyst potentially to a pressure above ambient; increasing the temperature to facilitate the desorption of carbon dioxide from the dual-function material; and catalytically transforming the carbon dioxide with the hydrogen gas into methane. Notably, the adsorption and desorption of carbon dioxide occur within the sorbent portions, while the reaction of carbon dioxide with hydrogen gas to yield methane takes place at a temperature substantially consistent with the desorption stage on the catalytic unit. Finally, the product gas undergoes downstream upgrading steps to remove or reduce impurities of water, carbon dioxide, and nitrogen. This invention represents a significant advancement in carbon capture and conversion processes, offering a highly efficient and reliable method for producing ultra-high purity methane for processes such as, but not limited to, chemical vapor deposition.
From the above description and figures, it will be understood that certain embodiments of the invention may comprise, consist essentially of, or consist of, catalyst, sorbent, and support formulation(s), and/or methods of synthesizing the formulation(s), that are specially adapted for effective performance during frequent high/low-pressure switching, for example, including vacuum/purge cycles. In preferred embodiments, said formulations are dual functional materials (DFM). Certain embodiments comprise processes for carbon dioxide capture and conversion to high purity methane and/or ethane that comprise using said formulation(s) and comprising said frequent high/low-pressure switching and vacuum/purge cycles. Certain embodiments of the formulations and processes are specially adapted for effective performance at a range of pressures from about 0.001 torr to about 25,000 torr.
Certain of these embodiments are adapted to capture CO2 from air and to produce a feed stream to a chemical vapor deposition process that contains hydrogen, methane and/or ethane, and less than about 1 ppm nitrogen. Certain of these embodiments are adapted to capture CO2 from air and to produce a feed stream for said chemical vapor deposition processes that contains hydrogen, methane and/or ethane, and less than about 1 ppb nitrogen or from about 0.1 ppb to 10 ppm nitrogen.
In certain embodiments, the carbon dioxide capture and conversion to high purity methane and/or ethane comprises a dual functional material used in a single reactor instead of having carbon capture and methanation in separate reactors/processes. In certain embodiments, the processes/materials described herein may further comprise novel purification, of the effluent of the DFM, by one or more recycle/input streams to improve environmental impacts, process efficiency and/or effectiveness, and/or to customize process effluents for particular CVD processes. Certain of the processes/materials described in this paragraph and the preceding two paragraphs may comprise methods for heating the DFM reactor in a way that maximizes CO2 capture and subsequent conversion to hydrocarbon and reactor efficiency. Certain embodiments processes/materials described in this paragraph and the preceding two paragraphs may comprise managing temperature, pressure, and flow rates to create isotopically pure methane.
In view of this disclosure and the preceding three paragraphs, it will be understood that certain embodiments will not comprise carbon capture and hydrogenation equipment and processes that are entirely separate from each other, for example, in separate reactors and/or in separate facilities. Further, it will be understood that certain embodiments do not include conventional DFM materials that are adapted substantially or entirely only for near-ambient pressure. Further, it will be understood that certain embodiments do not include a nitrogen purge of any DFM reactor, and especially certain embodiments do not include any purge of any DFM reactor that contains 80% or more nitrogen.
From the above description and the Figures, it also will be understood that certain embodiments may comprise, consist essentially of, or consist of one or more of the following items:
Although this disclosed technology has been described above with reference to particular means, materials and embodiments, it is to be understood that the disclosed technology is not limited to these disclosed particulars but extends instead to all equivalents within the broad scope of the following claims.
This application claims benefit of U.S. Provisional Application Ser. No. 63/536,039 filed Aug. 31, 2023, the entire disclosure of which is hereby incorporated by reference.
Number | Date | Country | |
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63536039 | Aug 2023 | US |