LOW-PRESSURE DROP STRUCTURE OF PARTICLE ADSORBENT BED FOR ADSORPTION GAS SEPARATION PROCESS
20170326494 · 2017-11-16
Assignee
Inventors
- Christoph GEBALD (Zürich, CH)
- Nicolas PIATKOWSKI (Zürich, CH)
- Tobias RUESCH (Zürich, CH)
- Jan André André WURZBACHER (Zürich, CH)
Cpc classification
B01J20/28004
PERFORMING OPERATIONS; TRANSPORTING
F28F9/26
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
B01D53/0407
PERFORMING OPERATIONS; TRANSPORTING
B01D53/0462
PERFORMING OPERATIONS; TRANSPORTING
Y02C20/40
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
B01J20/24
PERFORMING OPERATIONS; TRANSPORTING
F28F1/32
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F28F2255/12
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F28F1/126
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
B01J20/28052
PERFORMING OPERATIONS; TRANSPORTING
B01D2253/25
PERFORMING OPERATIONS; TRANSPORTING
International classification
F28F1/32
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
B01J20/24
PERFORMING OPERATIONS; TRANSPORTING
F28F9/26
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
B01J20/28
PERFORMING OPERATIONS; TRANSPORTING
Abstract
A gas separation unit for the separation of carbon dioxide from air is proposed for use in a cyclic adsorption/desorption process and using a loose particulate sorbent material. Sorbent material is arranged in at least two stacked layers, and each layer comprises two sheets of a flexible fabric material which is gas permeable but impermeable to the loose sorbent material. The sheets are arranged parallel defining an inlet face and an outlet face, are arranged with a distance in the range of 0.5-2.5 cm, and are enclosing a cavity in which the sorbent material is located. Said layers are arranged in the unit such that the inflow passes through the inlet face, subsequently through the particular sorbent material located in the cavity of the respective layer, subsequently to exit the layer through the outlet face to form the gas outflow.
Claims
1. A gas separation unit for the separation of a first gas from a mixture containing said first gas as well as further gases different from the first gas by using a cyclic adsorption/desorption process using a loose particulate sorbent material for gas adsorption wherein said particulate sorbent material is arranged in at least two stacked layers wherein each layer comprises two sheets of a flexible fabric material which is gas permeable but impermeable to the loose particulate sorbent material, which sheets: are either mounted on a stiff frame structure or which form the layer in a self-supporting way using spacers or distance elements between them, are arranged essentially parallel defining an inlet face of the layer and an outlet face of the layer, are arranged with a distance in the range of 0.5-2.5 cm, and are enclosing a cavity in which the particulate sorbent material is located, wherein the unit has a gas inlet side or gas inlet manifold through which an inflow of gas mixture enters the unit and a gas outlet side or gas outlet manifold through which a gas outflow exits the unit, the gas pathway between the inflow and the outflow being confined in the unit to pass through at least one layer; wherein said layers are arranged in the unit such that the inflow passes through the inlet face, subsequently through the particular sorbent material located in the cavity of the respective layer, subsequently to exit the respective layer through the outlet face to form the gas outflow; wherein the layers are arranged such that inlet faces of adjacent layers are facing each other enclosing gas inlet channels and such that outlet faces are facing each other enclosing gas outlet channels; wherein the mean distance between inlet faces and/or outlet faces defining said channels, measured in a direction essentially perpendicular to a main gas inflow direction and a main gas outflow direction, respectively, is in the range of 0.5-5 cm; wherein the length of the inlet face and/or of the outlet face in a direction parallel to the main gas inflow direction and the main gas outflow direction direction, respectively, is at least ten times larger than distance d between the sheets in the layer; and wherein at least one layer is provided with primary heat exchange elements.
2. The gas separation unit according to claim 1, wherein the length of the inlet face and/or of the outlet face in a direction parallel to the main gas inflow direction and the main gas outflow direction, respectively, is at least 40 times, larger than distance between the sheets in the layer.
3. The gas separation unit according to claim 1, wherein the flexible fabric material is woven or nonwoven textile material, or the flexible fabric material is made from a cellulose based material.
4. The gas separation unit according to claim 1, wherein more than 5, layers are either stacked essentially parallel to each other in the unit; and/or are stacked under relative inclination angles in the range of 0.2 15, the corresponding inlet channels converging in the main gas inflow direction and the corresponding outlet channels widening in the main gas outflow direction.
5. The gas separation unit according to claim 1, wherein the layers are essentially planar structures stacked essentially parallel to each other, or wherein the layers are essentially cylindrical structures arranged concentrically to each other.
6. The gas separation unit according to claim 1, wherein spacers are located within said layers.
7. The gas separation unit according to claim 1, wherein the at least two stacked layers, or in case of more than two layers all the layers comprising two sheets of a flexible fabric material which is gas permeable but impermeable to the loose particulate sorbent material contained in the layers, are oriented vertically, such that the plane normals of the layers are oriented horizontally.
8. The gas separation unit according to claim 1, wherein the primary heat exchange elements and/or the secondary heat exchange elements also act as frame structure supporting the sheets of flexible fabric material.
9. The gas separation unit according to claim 1, wherein the primary heat exchange elements or the secondary heat exchange elements are based an expanded material.
10. The gas separation unit according to claim 1, wherein the loose particular sorbent material is an amine-modified particular material.
11. The gas separation unit according to claim 1, wherein the frame is provided with holes into which the loose particular sorbent material is filled and the openings of which holes are closed after filling in the sorbent material.
12. The gas separation unit according to claim 1, wherein it comprises a surrounding cage, which, apart from gas inlet openings for the inflow and gas outlet openings for the outflow is gastight.
13. The gas separation unit according to claim 1, wherein the sheets of each layer are located at a distance in the range of 0.5-1.5 cm, or wherein the mean distance between adjacent inlet faces or outlet faces, measured in a direction essentially parallel to a main gas inflow direction and the main gas outflow direction, respectively, is in the range of 0.5-1.5 cm.
14. The gas separation unit according to claim 1, wherein tubing is provided in each layer, wherein there are provided stackable backbone elements, wherein means are provided in or at said stackable backbone elements for fluid transfer attachment of ends of the tubes, wherein the stackable backbone elements can be connected to each other, to transfer the heat transfer fluid to and from the tubes in individual layers.
15. Use of a gas separation unit according to claim 1 for extracting carbon dioxide from air or flue gases.
16. The gas separation unit according to claim 1, wherein the length of at least one of the inlet face or of the outlet face in a direction parallel to the main gas inflow direction and the main gas outflow direction, respectively, is at least 80 times larger than distance (d) between the sheets in the layer.
17. The gas separation unit according to claim 1, wherein the flexible fabric material is woven or nonwoven textile material, based on polymeric fibres or yarns, including those based on at least one of PET or PE, or the flexible fabric material is made from a cellulose based paper material.
18. The gas separation unit according to claim 1, wherein more than 20 layers are either stacked essentially parallel to each other in the unit, by using a stack of corresponding frames; or are stacked under relative inclination angles in the range of p 0.5-10°, the corresponding inlet channels converging in the main gas inflow direction and the corresponding outlet channels widening in the main gas outflow direction, wherein the inlet channels are closed at their downstream ends by lateral edges of adjacent layers being in contact and wherein the outlet channels are closed at their upstream end by lateral edges of adjacent layers.
19. The gas separation unit according to claim 1, wherein spacers are located within said layers, the spacers being rigid bar or rail structures, including T, H, C, or Z-bar structures, or being provided by junctures or seams between the sheets.
20. The gas separation unit according to claim 1, wherein at least one layer, or the majority of the layers, or all layers are provided with primary heat exchange elements, in the form of tubing containing a heat exchange fluid, in combination with secondary heat exchange elements for increasing the heat transfer between the sorbent material and the heat exchange elements.
21. The gas separation unit according to claim 20, wherein the primary heat exchange elements or the secondary heat exchange elements also act as frame structure supporting the sheets of flexible fabric material.
22. The gas separation unit according to claim 20, wherein the primary heat exchange elements or the secondary heat exchange elements are based an expanded metal, including a corrugated expanded metal.
23. The gas separation unit according to claim 1, wherein the loose particular sorbent material is an amine-modified particular material, based on amine-modified nanofibrilated cellulose with an average particle diameter in the range of 60 to 1200 μm, for the adsorption of carbon dioxide.
24. The gas separation unit according to claim 1, wherein it comprises a surrounding cage, made of a flexible or a stiff material, which, apart from gas inlet openings for the inflow and gas outlet openings for the outflow is gastight, and which is attached to a vacuum unit for the desorption process, wherein inlet openings and/or outlet openings are provided with controllable lids or valves for changing between adsorption and desorption stages.
25. The gas separation unit according to claim 1, wherein tubing is provided in each layer, wherein there are provided stackable backbone elements, in or as part of a frame structure, wherein means are provided in or at said stackable backbone elements for fluid transfer attachment of ends of the tubes, wherein the stackable backbone elements can be connected to each other, directly or via further tubing, involving using O-rings, to transfer the heat transfer fluid to and from the tubes in individual layers, wherein the stackable backbone elements are cylindrical elements with a diameter in the range of 1 to 5 cm and wherein the tubing of the primary heat exchange structure as well as the secondary heat exchange structure can be directly included in the frame structures during the injection molding process.
26. The gas separation unit according to claim 1, wherein the loose particular sorbent material is an amine-modified particular material, based on a weak basic ion exchange resin, with adsorbing amine groups, including polystyrene matrix materials modified with amine groups, specially primary amine groups, for the adsorption of carbon dioxide.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0096] Preferred embodiments of the invention are described in the following with reference to the drawings, which are for the purpose of illustrating the present preferred embodiments of the invention and not for the purpose of limiting the same. In the drawings,
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DESCRIPTION OF PREFERRED EMBODIMENTS
EXAMPLE 1.
Working Example of the Present Invention in the Form of a Rectangular Stack
[0118] According to one working example, the structure is composed of rectangular layers of sorbent material stacked on top of each other to form a rectangular block shaped stack comprising inlet channels, outlet channels and the sorbent layers. In this example, the fabrication and assembly of this example is described to illustrate the applicability of this invention in the form of a useful product for CO2 extraction from ambient air.
[0119] The individual sorbent material layers are formed by stiff frame structures, each comprising a rectangular frame with 0.5 m×0.6 m edge length and a height of 1 cm, made of stainless steel profiles. A top-view of such a single frame is shown in
[0138] Within the stack of this example, a total surface area of the sorbent material layers toward the gas inlet channels of about 8 m.sup.2 is accommodated. While the design air flow through the chamber is as high as 800 m.sup.3 per hour, the average velocity of the air flow through the sorbent layers is as little as 0.028 m/s. This ensures a very little pressure drop (see Example 2 below).
[0139] In
EXAMPLE 2.
Determination of the Pressure Drop Through a Stack of Sorbent Layers
[0140] The pressure drop imposed on an air flow passing through a structure essentially fabricated according to the description of Example 1 is experimentally determined for different flow rates. To this end, both butterfly valves are opened and a variable speed fan is attached to the inlet opening producing different air flow rates through the stack. The flow rate is measured with an in-pipe velocity head meter and the pressure drop over the structure is measured using a differential pressure sensor. The observed pressure drop for various volume flow rates is shown in the following table:
TABLE-US-00001 Volume flow (m.sup.3/h) Pressure drop (Pa) 200 16 400 31 600 58 800 98
[0141] It is found that up to the design flow rate of 800 m.sup.3/h, which is required to capture around 1 kg of CO2 from air per cycle (see Example 3), the pressure drop stays below 100 Pa. If the average pressure drop during the adsorption process is 100 Pa, the required pumping work to capture one ton of CO2 from atmospheric air is around 80 kWh (assuming that on average 70% of the CO2 is captured from the air stream and a fan efficiency of 70%). This energy consumption would correspond to electricity costs for air ventilation of US$ 8 per ton of CO2 (assuming an electricity price of US$ 0.1 per kWh), which is in an acceptable range. However, if the pressure drop was as high as 500 Pa, the corresponding electricity costs of US$ 40 for air ventilation would exceed the tolerable limits for an economic process.
[0142] This shows the important advantage of the structure of the present invention over conventional arrangements of particulate sorbent materials such as packed beds or fluidized beds, which are much longer than the sorbent packing of the present invention and which typically introduce pressure drops of several thousand Pascals up to several bars.
EXAMPLE 3.
Performance of Example 1 within a Cyclic Adsorption/Desorption Process
[0143] A structure essentially fabricated according to the description of Example 1 is used for a cyclic temperature-vacuum swing adsorption/desorption process to extract CO2 from ambient air. One cycle of the process takes about 6 hours and comprises the steps adsorption (3 hours) and desorption (3 hours).
[0144] During the adsorption step, according to Example 2 above, the butterfly valves are opened and air is blown through the structure by a variable speed fan, while the flow rate is recorded. Further, the CO2 content of the air flow and its relative humidity are measured before and after the vacuum chamber using an infrared detector. The relative humidity during the adsorption process is relatively constant between 35% and 40%. The air flow is 750 to 800 m.sup.3/h. The CO2 concentration before and after the chamber (“adsorption breakthrough curves”) during adsorption are shown in
[0145] It is surprisingly found that initially, during the first minutes of the adsorption process, the CO2 concentration at the outlet of the chamber drops down to almost 0 ppm. This demonstrates the very good performance of the structure of this embodiment, since the vanishing CO2 concentration indicates that substantially all of the air flow passing through the structure effectively passes through the sorbent material layers and does not by-pass them. If there had been a substantial by-pass blow, this by-pass flow, which would still contain about 400 ppm CO2, would have mixed with the portion of the flow that passes through the sorbent material layer and would have increased the CO2 concentration at the chamber outlet.
[0146] This behavior of the system is substantially superior to the behavior that was observed in experiments with a short packed bed of the sorbent material of 1 cm length in a conventional, 4 cm diameter stainless steel column, in which the outlet CO2 concentration never reached values as low as observed in this example, presumably due to flow by-passing since the bed was not fixed between two layers of fabric and by-passing could occur along the column walls.
[0147] In particular, this demonstrates that the structure disclosed in the present invention allows creating embodiments based on 3-D structures and embodiments comprising different materials, which exhibit advantageous behavior during operation and which cannot be created from prior-art extruded 2-D structures.
[0148] Further, this example illustrates that with the proposed structure, extraction of a substantial portion of the CO2 contained in a stream of atmospheric air using a particulate amine-modified sorbent material is possible at a pressure drop below 100 Pa with a structure that can be manufactured with reasonable effort.
[0149] During the subsequent desorption step, the vacuum chamber is evacuated to about 100 mbar.sub.abs and the stack is subsequently heated up to about 85° C. by circulating hot water through the plastic tubes. Thereafter, the CO2 desorbing from the sorbent material is constantly pumped off the chamber by the vacuum pump. The mass flow rate of the CO2 leaving the vacuum pump is measured using a calorimetric mass flow meter, see
EXAMPLE 4.
Example with Triangular Gas Inlet and Outlet Channels
[0150] Another structure is fabricated, in which the gas inlet and outlet channels between the sorbent material layers have a triangular cross section. To this end, 20 frame structures each defining a 2 cm thick sorbent material layer are produced by injection molding of a thermoplastic material. During the injection molding process, a heat transfer structure composed of an aluminum tube and an aluminum honeycomb structure with a cell width of .sup.1/.sub.2 inch, in which four of six side walls of each cell contain a center hole of 4 mm diameter, is integrated within the frame structure. Each frame further comprises triangular edges on its top defining the distance between two stacked frames and thereby the shape of the gas inlet and outlet channels. After the molding process, a woven fabric material made from a mixture of PET and PE fibers is glued on both sides of the frame and the frame is filled with sorbent material analog to the filling process described in Example 1. During the filling process, the sorbent material passes through the network of the cells of the aluminum honeycomb structure via the holes in the side walls of the honeycomb cells. The 20 frame structures are thereupon stacked on top of each other to form a stack with a cross section as schematically shown in
EXAMPLE 5.
Utilization for a Flue Gas CO2 Capture Process
[0151] A stack of sorbent material layers contained in a vacuum chamber similar to the stack described in Example 1 is used to capture the CO2 contained in the flue gas stream of a natural gas powered combined heat and power internal combustion engine. In this case, the CO2 concentration in the gas stream passing through the structure is approximately 6%. The gas volume flow during adsorption is substantially lower, i.e., in the range of 20 to 30 m.sup.3/h. The adsorption process takes 0.5 h, on average 90% of the CO2 contained in the gas stream are extracted.
[0152] The desorption process takes 1 h, during which the CO2 is removed from the sorbent material by heating it to 95° C. Three of the units (one unit composed of one stack contained in a vacuum chamber) are operated in tandem operation, so that at each time, one stack is in adsorption mode and two stacks are in desorption mode and CO2 can be continuously captured from the flue gas stream.
EXAMPLE 6.
Effect of Heat Exchange Structure Placed inside the Sorbent Material
[0153] In order to demonstrate the effectiveness of a heat transfer structure incorporated within the sorbent material layer in an experiment, a packed bed of 100 g of sorbent material (see Example 1) is placed in a rectangular packed bed aluminum reactor with a cross section of 60 mm×60 mm. After 3 hours of adsorption during which 20 1/min of air at 60% relative humidity are streamed through the reactor, the sample is desorbed by evacuating the reactor to 100 r mbar.sub.abs by a vacuum pump and heating the reactor walls through a water-filled jacked to 90° C. The temperature in the center of the bed is recorded during the desorption process. For this experiment, it takes 221 minutes to reach a temperature of 80° C. in the bed center.
[0154] Subsequently, the experiment is repeated with 6 g of a ¾ inch cell width aluminum honeycomb structure placed in the sorbent material bed to increase heat transfer. For this experiment, it takes 79 minutes to reach a temperature of 80° C. in the bed center.
[0155] These observation demonstrates the effectiveness of a heat transfer structure included in the sorbent material bed, resulting in significantly shorter times to heat up the sorbent material bed during the desorption step, which in turn reduces the overall cycle time and thereby the overall cost of the adsorption process.
[0156] This example further illustrates another advantage of the structure disclosed in the present invention over prior art structures, since 3-D structures increasing the heat transfer included within the sorbent material layers, such as an aluminum honeycomb, cannot be easily incorporated into prior art, extruded 2-D structures.
EXAMPLE 7.
Example in the Form of a Rectangular Stack, Describing the Possible Dimensions of Frames and Stack and Stack Assembly
[0157] Considering the requirements on pressure drop, an inlet and outlet channel length of 1 m was defined with a maximum sorbent material layer thickness of 1 cm and an inlet channel height of 1 cm. For constructive reason the vacuum chamber in which the adsorber structure is housed was defined to contain between 500 and 1000 kg of sorbent material. The resulting width of the frames was found to be 1.45 m. The frames are stacked on one another in the ‘zig-zag’ fashion with an angle of 2° between planar surface. In this fashion, the dead volume (i.e. volume of the stack not occupied by sorbent material) is decreased by 40% compared to a stack with parallel channels and the same inlet channel height. The reduction of dead volume increases the cost efficiency and process efficiency by packing more sorbent material into a given volume and thereby producing more CO2 from a given facility. The resulting stack height is 1.47 m with 88 sorbent material frames.
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[0160] The same principle of the stack layout and assembly described in this example can be applied to various other stack geometries, for example, but not limited to smaller stacks consisting of less frames, different frame dimensions, and a non-angular stacking layout, i.e. a stack in which the frames are essentially parallel to each other with no angle between the surfaces, i.e. no ‘zig-zag’ structure.
EXAMPLE 8.
Low Thermal Mass Frames
[0161] A reduction of the thermal mass of the frames per mass of contained sorbent material reduces the overall energy demand of the desorption process and is a critical parameter in the design of DAC systems. As the desorption process takes place in a vacuum structure which carries the vacuum forces, the frames themselves must only carry their own weight, the weight of the sorbent material, the weight of the heat transfer structures, and assure the desired geometry of the inlet and outlet channels and the sealing faces. An example of such a frame was constructed with four aluminum C profiles with 10×10 mm outer dimensions and 8×8 mm inner dimensions, connected with edge brackets to form the rectangular form. The primary heat transfer structure is formed by 10 passes of 8 mm OD alumium tubing which is placed into the C profiles and which pass at two places thorugh the C profiles to allow connection with water distributors. In this manner, the stability of the primary heat transfer structure is assured without additional frame components. The aluminum tubes (primary heat transfer structure) thereby make up a significant contribution to the overall stiffness of the frame. The secondary heat transfer structure is formed of expanded aluminum sheet metal, which is formed to the primary heat transfer structure as in
[0162] Decisive in the feasibility of a frame design is the thermal mass of the components which must be thermally cycled during the cyclic adsorption-desorption process. The contributions of each element and the total thermal mass of the frame per unit mass of contained sorbent material are detailed in the following table. The contained sorbent mass is 7.25 kg
TABLE-US-00002 Specific Frame Thermal Mass component Mass (kg) Material (kJ/K/kg sorbent) C Profiles & 0.37 Aluminum 0.046 Struts (Profiles) Wedge spacers and 0.158 Ultramide (PA) 0.037 sealing strips Primary heat 1.07 Aluminum 0.132 transfer structure (Tubing) Secondary heat 1.31 Aluminum 0.162 transfer structure (Expanded metal) Total 2.908 0.377
[0163] An example sorbent suitable for CO2 capture from ambient air has a specific heat capacity of 1.4 kJ/K/kg sorbent with a specific heat of desorption of CO2 and water of 211 kJ/kg sorbent material. In a typical desorption process the sorbent material must be heated from the adsorption temperature of 20° C. to 100° C. The total thermal energy demand in this typical desorption process can be determined to be 323 kJ/kg sorbent material. The thermal energy demand of the frames in this scenario is 30.2 kJ/kg sorbent material or 9.3% of the total thermal energy demand.
EXAMPLE 9.
Heat Transfer Structure and its Dimensioning
[0164] Heat transfer through a representative unit cell of a secondary heat transfer structure and sorbent material was investigated with numerical simulations. A representative unit cell composed of a heat transfer structure concentric with a sorbent cell was investigated as shown in
[0165] The 50 mm unit cell length translates into the spacing of the primary heat transfer structure in the form of bent alumium tubing. Over the 1.5 m width of the frames, there are therefore 10 passes of aluminum tubing. This solution represents a good compromise between the density of heating, structural stability, material demand and thermal mass of the frames. The selected aluminum expanded metal of the secondary heat transfer structure is firstly formed around the primary heat transfer structure to increase the contact area consistent with the form shown in
EXAMPLE 10.
Connection with Process Equipment
[0166] The stack is to be connected with a heat transfer fluid system. This is accomplished with a heat transfer fluid distributor which engages into the primary heat transfer structure at each frame as shown in
EXAMPLE 11.
Thermal Mass of Frames using Fin and Tube Heat Transfer Structure in a DAC Application
[0167] The thermal masses of a possible fin and tube heat transfer structure in a frame are determined for a 20 mm thick sorbent material layer. This is compared with a conventional frame construction with 10 mm sorbent material layer thickness. As a reference the mass and thermal mass of a 10 mm frame with planar expanded aluminum metal heat transfer structure according to the current design is calculated in the following table.
TABLE-US-00003 Specific Frame Thermal Mass component Mass (kg) Material (kJ/K/kg Sorbent) C Profiles & 0.37 Aluminum 0.046 Struts (Profiles) Wedge spacers and 0.158 Ultramide (PA) 0.037 sealing strips Primary HEX 1.07 Aluminum 0.132 (Tubing) Secondary HEX 1.31 Aluminum 0.162 (fins) (Expanded metal) Frame Mass 2.908 0.377 Sorbent mass 7.25 Ratio (kg Frame/kg 0.411 Sorbent)
[0168] A 20 mm frame with fin secondary heat transfer structure will have a doubled mass for the frame C profiles due to the doubled height. The wedge spacers 23, 26 and sealing strips 9, 8 remain the same (although their overall quantity in the stack is reduced), the primary heat exchanger structure retains the same mass as the length and diameter of the tube 11 are retained. The secondary heat transfer structure sees the main change. The results are shown in the following table for a frame with a 20 mm thick sorbent material layer with 14.1 kg sorbent material.
[0169] The following assumptions are made:
[0170] Frame width=1.5 m with 1 mm profile thickness
[0171] Frame length=1.0 m with 1 mm profile thickness
[0172] Primary HEX volume (as in a 10 mm sorbent layer)=3.964e-4 m3
[0173] Secondary HEX 100 fins with 10 mm spacing aligned with 1.5 m edge, 20 mm high, 0.5 mm thick with 50% of surface area perforated=7.5e-4m3
[0174] Mass secondary HEX=7.5e-4m3×2700 kg/m3=2.025 kg
[0175] Total volume for sorbent in frame=0.0282 m3
[0176] Sorbent material mass=sorbent density (500 kg/m3)*total volume=14.1 kg
TABLE-US-00004 Specific Frame Thermal Mass component Mass (kg) Material (kJ/K/kg Sorbent) C Profiles & 0.74 Aluminum 0.047 Struts (Profiles) Wedge spacers and 0.158 Ultramide (PA) 0.019 sealing strips Primary HEX 1.07 Aluminum 0.068 (Tubing) Secondary HEX 2.025 Aluminum 0.129 (fins) (Expanded metal) Frame Mass 3.993 0.263 Sorbent mass 14.1 Ratio (kg Frame/kg 0.283 Sorbent)
[0177] It is seen through this example that a fin and tube heat transfer structure which allows an increase in the sorbent material layer to 20 mm lowers the thermal mass per unit sorbent material of each frame by 30%. The gain is mainly seen because the primary heat transfer structure and the wedge spacers and sealing strips do not scale with the sorbent material layer thickness.
LIST OF REFERENCE SIGNS
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TABLE-US-00005 1 Inlet gas stream, gas inflow, main gas inflow direction 2 Outlet gas stream, gas outflow, main gas outflow direction 3 Gas inlet channel 4 Gas outlet channel 5 Particulate sorbent material layer 6 Sheet of fabric material enclosing the sorbent material 7 Part of a frame, defining the geometrical structure of a sorbent layer and supporting the fabric material enclosing the sorbent material 8 Structure blocking the end of a gas inlet channel 9 Structure blocking the beginning of a gas outlet channel 10 Secondary heat transfer structure inside the sorbent material layer 11 Tube containing a heat transfer fluid, being part of the primary heat transfer structure inside the sorbent material layer 12 Z-profile being part of the frame defining the geometrical structure of a sorbent layer 13 Path of a by-pass gas flow along the edge of the packed bed of sorbent material inside the sorbent material layer 14 Container, enclosing the stack of the layers of sorbent material 15 Gas outlet manifold 16 Valve/lid opening and sealing the outlet manifold with respect to the environment 17 C-profile being part of the frame defining the geometrical structure of a sorbent layer 18 inlet face 19 outlet face 20 heat transfer structure in thermal model 21 sorbent material in thermal model 22 thermal contact resistance in thermal model 23 wedge formed spacers at edges 24 mounting screw 25 mounting and orienting screw 26 wedge formed spacers on 27 heat transfer fluid distributor 28 heat transfer fluid return line d distance between 18 and 19 Tb temperature boundary in thermal model L distance between fin groups