The invention relates to a gas diffusion electrode, an electrolysis plant for the conversion of carbon oxide and also a method for operating an electrolysis plant.
To utilize the fluctuating electric power from renewable energy sources, for example wind and photovoltaics, it is possible to synthesize organic materials of value which are obtained from the carbon dioxide-containing offgases of industry and fossil fuel power station processes by means of aqueous CO2 electrolysis. One process step here is to reduce carbon dioxide to carbon monoxide with the aid of electric energy, with the carbon monoxide serving as versatile material of value and as starting material for the further synthesis of organic materials. For this purpose, electrolysis plants in the form of electrolyzers which have a gas diffusion electrode (GDE) as a central component are employed. These gas diffusion electrodes are usually produced on the basis of a silver catalyst bound in a polymer matrix, with a metal mesh, for example, also being introduced into this matrix to effect mechanical stabilization. However, a problem associated with such gas diffusion electrodes is that they have too low a long-term stability, in particular intrusion of electrolyte liquid into the gas diffusion electrode and precipitation of salts from the electrolyte solution occur. This is referred to as salting of the gas diffusion electrode, which makes the latter unusable in the long term.
It is an object of the invention to provide a gas diffusion electrode and also an electrolysis plant having a gas diffusion electrode and a method for operating an electrolysis plant which has a longer life than is the case for the conventional construction.
The object is achieved by a gas diffusion electrode as claimed and also by an electrolysis plant as claimed and the method for operating an electrolysis plant as claimed.
The gas diffusion electrode as claimed has at least two layers of which a first layer has an electrically conductive woven fabric which is at least partially embedded in a hydrophobic polymer matrix. Furthermore, the gas diffusion electrode has a second layer which has an open porosity in which catalytically active particles are present and has a thickness in the range from 1 μm to 50 μm.
The first layer having the electrically conductive woven fabric serves essentially to stabilize the gas diffusion electrode mechanically and to effect electrical contacting. This is a feature which is already known for the GDEs of the prior art. However, as a difference from the prior art, this woven fabric is surrounded by a hydrophobic polymer matrix. Hydrophobic materials are characterized in that they have a contact angle with water or the adjoining liquid electrolyte which is greater than 70°, advantageously greater than 90°. This prevents intrusion of a liquid electrolyte into the first layer of the GDE. This in turn results in “salting” by precipitation of salts from the electrolyte in the matrix of the GDE being prevented. This is additionally prevented by the presence of a second layer in which catalytically active particles, in particular or for example silver particles, are present in an open porosity of the second layer. These catalytically active particles, in particular silver particles, are, in contrast to the matrix of the first layer, hydrophilic and draw in the liquid electrolyte and lead it to an interface between the first layer and the second layer. The actual chemical reaction of a starting material occurs at or in the vicinity of this interface, with the electrons for conversion of the starting material being made available by the electrically conductive woven fabric which extends to the interface between the two layers. Further intrusion of the liquid electrolyte beyond this interface into the first, hydrophobic layer is avoided.
It has been found to be particularly advantageous for the woven fabric to consist of or comprise silver-containing, titanium-containing or carbon-containing fibers. When the woven fabric is protected against wetting by the electrolyte by the polymer matrix except for the contact points to the second layer, the fabric can also comprise nickel. Particular advantage is given to a woven fabric composed of silver fibers. A suitable matrix material for the polymer matrix of the first layer is polytetrafluoroethylene. This is sufficiently hydrophobic and is suitable for enclosing the woven fabric very well. Such an enclosure of the woven fabric by the polymer matrix is advantageous because it results in the intrinsically catalytically and hydrophilically active surface of the silver or other possible fiber materials not coming into contact with the liquid electrolyte. As mentioned above, it is undesirable for a catalytic reaction between the electrolyte and the starting material to take place in the first layer, since this could bring about salting of the first layer.
The expression polymer matrix does not refer to a closed dense matrix but instead, as mentioned above, refers to a porous matrix which allows gaseous starting materials to diffuse through this polymer matrix and get to an interface between the first layer and the second layer for reactive conversion.
The first layer of GDE advantageously has a thickness in the range from 50 μm to 1000 μm. The thickness of the first layer is essentially determined by the thickness of the individual fibers of the woven fabric. Fibers having a diameter of 100 μm are quite usual, and the mesh opening is usually 0.3 mm. Greater fiber thicknesses and thus greater layer thicknesses of the first layer are quite possible: they give greater stability to the GDE but lead to the starting materials, in particular gaseous starting materials, having to diffuse through a thicker layer, which in turn decreases the electrochemical reaction between the first layer and the second layer. A balance between the wire thickness or fiber thickness of the woven fabric and the reactivity of the GDE thus has to be achieved in selecting the thickness of the first layer. In general, the thickness of the first layer is in the range from 100 μm to 400 μm.
Furthermore, it is advantageous for the polymer matrix of the first layer to have a porosity in which 95% of the pores have a diameter in the range from 0.1 μm to 2 μm, advantageously from 0.6 μm to 0.9 μm. Pores of this size still allow gaseous starting materials to diffuse readily but, owing to their hydrophobic character, do not allow any, or barely any, liquid electrolyte to intrude, even when the electrolyte has an overpressure of 0.2 bar relative to the gas phase in the first layer, as can occur in relatively large cells and stacks.
The catalytically active particles of the second layer have a diameter which is in the range from 0.05 μm to 1 μm, advantageously from 0.1 μm to 0.5 μm. Such fine particles, in particular silver particles, in turn have a large catalytic surface area at which the desired reaction can take place. The catalytically active particles are, in particular, silver particles which firstly have a hydrophilic surface which promotes the drawing-in of the liquid electrolyte. Secondly, the surface of the silver particles is particularly catalytically active for many desired reactions, for example for the conversion of carbon dioxide into carbon monoxide, with the interfering reduction of water to hydrogen being suppressed. Furthermore, it is advantageous for the catalytically active particles to be mixed with likewise hydrophilic binders, so that a targeted porosity can be set and particular bonding between the catalytically active particles occurs. It is advantageous here for the contact angle of these hydrophilic binders to be less than 90°.
Furthermore, it is also advantageous in this composition for 95% of the pores of the second layer to have a diameter which is in the range from 0.1 μm to 5 μm or advantageously from 0.1 μm to 1 μm. In measuring the porosity in all the layers described, recourse is made to an image analysis method. Here, a cross section or plan view is imaged microscopically and the pore abundance and the diameter thereof at the largest position of the diameter is evaluated.
A further aspect of the invention is an electrolysis plant for the electrolytic conversion of carbon dioxide having a gas diffusion electrode as claimed. Such an electrolysis plant has a gas space and an electrolyte chamber. The gas diffusion electrode is installed between the gas space and the electrolyte chamber and separates these from one another at least in regions. Here, the second layer of the GDE is arranged so as to face the electrolyte chamber, while the first layer is in contact with the gas space. With this construction, the above-described action of the gas diffusion electrode can be implemented industrially. Furthermore, it is advantageous for a contact web to contact the gas diffusion electrode electronically and thus be in direct contact with uncoated parts of the woven fabric.
A further aspect of the invention is a method for operating an electrolysis plant, wherein a carbon dioxide-containing starting material is introduced into a gas space where the starting material is conveyed to a gas diffusion electrode and diffuses through a first layer of the gas diffusion electrode. Here, it arrives at an interface of the first layer and a second layer of the gas diffusion electrode and is chemically converted there. Here, the second layer is a porous layer which is impregnated by a liquid electrolyte.
As regards the method and the electrolysis plant, these have the same modes of action and advantages described above for the gas diffusion electrode. This applies particularly to the abovementioned configuration of the first and second layers, with the first layer being hydrophobic and the second layer advantageously being hydrophilic and also containing catalytically active particles. The desired reaction, in particular the reduction of carbon dioxide to carbon monoxide, occurs at an interface between the hydrophilic layer and the hydrophobic layer.
Further embodiments and further features of the invention will be illustrated with the aid of the following figures, which show:
However, it is important that the matrix 10 has an open porosity 16 with individual pores 17, so that the starting material 28, i.e. the carbon dioxide, can diffuse through the first layer 4 to the interface 30. This diffusion path is indicated by the arrow 28 next to which CO2 has been written. It is also important that the material of the polymer matrix 10 is a hydrophobic material in order to prevent liquid electrolyte 32 from passing through the interface 30 into the first layer 4 of the GDE 2. This prevents an electrochemical reaction from taking place in the first layer 4, which would, in the case of the reaction equations which apply for conversion of the carbon dioxide into carbon monoxide in conjunction with the electrolyte, lead to salting of the GDE 2 in the important regions of the first layer 4.
For the present purposes, hydrophobic means that the capillary forces which act on the liquid electrolyte 32 at the interfaces with the particles of the matrix 10 are sufficient to prevent this liquid electrolyte from intruding into the layer 4. It is usually assumed that a material surface 33 has hydrophobic properties when the contact angle, which is schematically shown in
Two important properties of the first layer 4 are thus the supporting function of the woven fabric 8 and also the fact that it is very hydrophobic and very unreactive. The second layer 6 which is generally applied to the first layer 4 by means of a further coating process is quite different therefrom. This layer comprises, in particular, catalytically active particles 9 which are, in particular, in the form of silver particles. These particles 9 can advantageously also be provided with a binder, which here is a hydrophilic binder 18 shown schematically as oval particles in
A targeted porosity is set both in the layer 4 and in the layer 6, so that the gas molecules can diffuse through the first layer 4 and the liquid electrolyte 32 can infiltrate into the second layer 6. It has been found to be advantageous here for the pore structure of the first layer 4 to be configured so that 95% of the pores have a diameter in the range from 0.6 μm to 0.9 μm. From a processing engineering point of view, it is not always possible to set such a precise pore structure without an increased engineering outlay. For this reason, larger pores up to 2 μm and also smaller pores down to 0.1 μm are also quite acceptable to a minor extent. The layer thickness of the first layer 4 is determined, in particular, by the diameter of the fibers of the woven fabric 8. It is usually in the range from 100 μm to 500 μm. Thicker layers and thus also thicker fibers of the woven fabric 8 would have a better load-bearing capability but would also result in a longer diffusion path of the gas carbon dioxide and the product 29, CO, through the first layer 4. This would possibly have an adverse effect on the efficiency and the selectivity of the GDE 2 for CO production. The second layer 6 can be made significantly thinner than the first layer 4; the second layer 6 is generally ultimately applied to the load-bearing first layer 4 by means of a particular coating process. From the purely chemical processes which proceed, the second layer 6 could be very thin; strictly speaking, one layer of catalytically active particles 9 would be sufficient. From a process engineering point of view, somewhat greater layer thicknesses are obtained, particularly when using binders 18, while the layer thickness 5 of the first layer 4 is, as mentioned above, in the range from 100 μm to 500 μm, so the layer thickness 7 of the second layer 6 is in the range from 5 μm to 50 μm. Here, each individual particle 9 of the second layer 6 has a diameter which is in the range from 0.5 μm to 3 μm, very particularly advantageously from 0.1 μm to 0.5 μm. As regards the accuracy of these values, what has been said above in respect of the first layer applies; these particle sizes are advantageously restricted so that process irregularities up to a certain extent are not damaging. The same also applies to the porosity of the second layer 6, with 95% of the pores also being in the range from 0.1 μm to 5 μm here, advantageously from 0.1 μm to 1 μm. Hollow particles 9, which are not depicted here and have an inner hollow space which is accessible from the outside and has this pore size are also advantageous. At larger external dimensions, the pores between particles are necessarily also larger and are then no longer suitable for holding the electrolyte against a gas pressure present in the pore.
The conversion of the starting material, generally carbon dioxide 28 into the product carbon monoxide 29, then proceeds at the interface 30 or in the vicinity of from 2 to 3 particle sizes into the respective layer 4 or 6. For this purpose, the following reaction equations advantageously or generally proceed:
2CO2+H2O+2e−CO+2HCO3− Equation 1
CO2+H2O+2e−CO+20H− Equation 2
The electrons required for the reaction equations are supplied via the contact web 26 and the woven fabric 8 to the interface 30. The water concerned is present in a large excess in the electrolyte which penetrates through the second layer 6 to the interface 30. The carbon dioxide is supplied along the illustrated path 28 in
The thickness of the second layer is comparatively small at from 1 μm to 50 μm. This ensures that a sufficient electronic conductivity is available within the catalyst layer in order to ensure supply to the GDE within the mesh openings of the conductive mesh 8. On the other hand, there is sufficient catalytically active surface area of the particles 9 available within the range of the diffusing and dissolved carbon dioxide in order to carry out a current density in the desired form for reduction of the carbon dioxide. The second layer 6 can consequently be in principle made of few monolayers of particles 9 having a diameter of 0.1 μm. Particles 9, in particular silver particles having a diameter of about 1 μm, are also in the region of this, which leads to successful catalysis but is not quite as suitable. However, essentially only the surfaces within a region from the interface into the layer 6 which is in the order of a diffusion length of the dissolved carbon dioxide, i.e. in the range from 0.1 to 1 μm, are electrochemically active. The regions of the second layer 6 which extend further into the electrolyte space contribute only insignificantly to the reduction of CO2 compared to those regions of the layer 6 which are close to the interface 30. The evolution of hydrogen is also possible to only a small extent, if at all, because of a low decrease in voltage in the electrolyte of the GDE 2 since virtually no concentration gradient is established in the porous second layer 6 over this small distance.
The fact that the thickness of the second layer 6 can nevertheless be larger than the abovementioned few particle layers is due to an electrical trace resistance present in the layer 6 having to be low enough to ensure supply of electronic current between the individual contact webs 26.
Furthermore, it has to be ensured that the pore diameter in the second layer 6 in the vicinity of the interface 30 is actually smaller than the above-described upper limit of 1 μm. The pores advantageously have a diameter of only from 0.1 μm to 0.5 μm, so that it is ensured that the hydrophilic surface of the catalytically active particles 9 of these pores 13 are filled with electrolyte 32, which leads to a diffusion barrier for the carbon dioxide. In this way, a stable gas-electrolyte interface is created at the boundary layer 30, which has to be stable over considerable pressure differences of at least 0.2 bar because of the hydrophobic pore structure in the first layer 4. The catalytically active particles 9 should therefore accordingly be anchored, advantageously by means of an additional binder, on the hydrophobic structure of the first layer 4 at the interface 30. It is in principle advantageous for the pore systems both in the first layer 4 which has a supporting function, and the second layer 6, which has a catalytic function, to have a very high porosity. It has been found that porosities above 25% are well suited to allowing firstly the gas transport of carbon dioxide and carbon monoxide through the first layer 4 and secondly the infiltration of the second layer 6 by the liquid electrolyte 32 to occur. Compared to conventional gas diffusion electrodes, the path which has to be covered by the liquid electrolyte 32 into the gas diffusion electrode 2 is here shortened, while the path 28 which the carbon dioxide has to cover through the first layer 4 is not appreciably increased, as a result of which the polarization of the above-described gas diffusion electrode 2 decreases compared to conventional GDEs.
A working example of the production of a gas diffusion electrode 2 as described above will now be given below. A layer of Dyneon TF 2021 is sieved onto a woven silver fabric 8 having a wire diameter of 180 μm and a mesh opening of 250 μm with the aid of 500 μm thick templates (having an opening of 60 mm×120 mm) and subsequently struck off by means of a doctor blade. The layer is rolled with a two-roll calender having a roller gap of 0.3 μm, so that the peaks of the wire mesh project from the membrane. In a further step, a 1 μm-20 μm thick second layer 6, which serves a catalyst layer, of silver nanoparticles having a primary particle diameter of 0.1 μm is sprayed onto the rear side with the aid of an air brush. The particle suspension is produced as follows: 60 mg of silver nanoparticles (purity>99.9%) and 30 mg of a hydrophilic binder (anion-exchange ionomer) are dispersed in 3 ml of n-propanol in an ultrasonic bath for 10-15 minutes. A loading of from 0.5 mg to 3 mg of catalyst/cm2 is sought. The electrode is dried under a continuous stream of argon for 12 hours. Electrical contacting of the nanoparticles is effected by percolation or via the projecting tips of the woven silver fabric 8. The electrode has a trace resistance of 0.001Ω and can advantageously be contacted from the gas side.
A particular advantage of this electrode structure is that the site of the reaction at the interface between first and second layers is fixed within certain limits independently of the pressure difference between gas side and liquid side. This is ensured by the pressure which is necessary to press the electrolyte out from the advantageously hydrophilic second layer being in the region of advantageously more than 0.2 bar and conversely an overpressure of this magnitude from the electrolyte side not being sufficient to allow the electrolyte to penetrate into the first layer. This creates very suitable operating conditions in the reaction zone without the pressure between gas side and electrolyte side having to be set carefully. The GDE described is robust against pressure fluctuations as occur due to weight in relatively large cells and cell stacks or else during flow through the cells in operation. In a conventionally constructed GDE, which consists of a single layer, the penetration depth of the electrolyte is locally different and depends on the pressure difference in the mbar range. Accordingly, the pores filled with electrolyte or gas have different lengths to the site of the reaction and there are therefore places at which the undesirable reduction of water is favored.
Number | Date | Country | Kind |
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10 2018 204 890.8 | Mar 2018 | DE | national |
10 2018 205 571.8 | Apr 2018 | DE | national |
This application is the US National Stage of International Application No. PCT/EP2019/055839 filed 8 Mar. 2019, and claims the benefit thereof. The International Application claims the benefit of German Application No. DE 10 2018 205 571.8 filed 12 Apr. 2018 and German Application No. DE 10 2018 204 890.8 filed 29 Mar. 2018. All of the applications are incorporated by reference herein in their entirety.
Filing Document | Filing Date | Country | Kind |
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PCT/EP2019/055839 | 3/8/2019 | WO | 00 |