The present disclosure relates to a cell stack and a redox flow battery.
As a large-capacity storage battery, a redox flow battery is known. For example, redox flow batteries disclosed in Patent Literatures 1 to 4 include a cell stack in which a plurality of battery cells are stacked. Charging and discharging are performed by circulating a positive electrolyte and a negative electrolyte in the battery cells.
Each of the battery cells includes a positive electrode, a negative electrode, and a membrane disposed between the positive and negative electrodes. A bipolar plate is disposed between battery cells adjacent in a stacking direction. The electrode is a porous body including an aggregate of carbon fibers or the like. In the bipolar plate including a groove, the groove facilitates spread of the electrolyte over the entire surface of the bipolar plate.
PTL 1: Japanese Patent Laying-Open No. 2015-122230
PTL 2: Japanese Patent Laying-Open No. 2015-122231
PTL 3: Japanese Patent Laying-Open No. 2015-138771
PTL 4: Japanese Patent Laying-Open No. 2015-210849
A cell stack of the present disclosure is a cell stack in which a plurality of battery cells are stacked,
the cell stack including an electrode of a porous body, and a bipolar plate facing the electrode, in which
the bipolar plate includes
R2/R1 is 7×10−11 or more and 2×10−4 or less,
R
1=(L1/K1)×μ×(1/S1),
R
2=(32×μ×L2)/(de2×S2),
A redox flow battery of the present disclosure includes the cell stack of the present disclosure.
When flowability of an electrolyte in an electrode is low, a battery reaction in the electrode may be insufficient. As a result, reactive resistance in the electrode increases. In addition, when the flowability of the electrolyte in a groove of a bipolar plate is low, heat associated with the battery reaction tends to be trapped in the electrolyte. When temperature of the electrolyte increases, stability of the electrolyte decreases. As a result, reactive resistance in the electrode increases.
An object of the present disclosure is to provide a cell stack in which reactive resistance in an electrode is less likely to increase. Another object of the present disclosure is to provide a redox flow battery having excellent battery performance.
The present inventor has intensively studied a configuration for reducing reactive resistance in an electrode of a cell stack. As a result, the present inventor has found that an increase in the reactive resistance in the electrode can be reduced by adjusting a difficulty of a flow of an electrolyte in the electrode and a difficulty of a flow of the electrolyte in a bipolar plate. Based on this finding, aspects of the present disclosure will be described below.
<1> A cell stack according to an embodiment is a cell stack
in which a plurality of battery cells are stacked,
the cell stack including an electrode of a porous body, and a bipolar plate facing the electrode, in which
the bipolar plate includes
R2/R1 is 7×10−11 or more and 2×10−4 or less,
R
1=(L1/K1)×μ×(1/S1),
R2 is a permeation resistance indicating the difficulty of the flow of the electrolyte in each of the plurality of first grooves,
R
2=(32×μ×L2)/(de2×S2),
The present inventor has defined a new index of the permeation resistance that indicates the difficulty in the flow of the electrolyte. Aspect <1> defines permeation resistance R1 in the electrode, permeation resistance R2 in the first groove of the bipolar plate, and R2/R1 being 7×10−11 or more and 2×10−4 or less. When R2/R1 is within the above range, the electrolyte flowing through the first groove of the bipolar plate appropriately easily flows toward the electrode, and flowability of the electrolyte in the electrode is improved. As a result, an increase in a reactive resistance in the electrode is greatly reduced. Here, the range of R2/R1 in aspect <1> is 7×10−9% or more and 2×10−2% or less in percentage. Hereinafter, a value of R2/R1 may be expressed in percentage.
<2> In one aspect of the cell stack according to the embodiment, R2/R1 is 2×10−10 or more and 1×10−4 or less.
When R2/R1 is 2×10−10 or more and 1×10−4 or less, the increase in the reactive resistance in the electrode is further reduced as compared with aspect <1>. The range of R2/R1 in aspect <2> is 2×10−8% or more and 1×10−2% or less in percentage.
<3> In one aspect of the cell stack according to the embodiment, R2/R1 is 5×10−9 or more and 3×10−5 or less.
When R2/R1 is 5×10−9 or more and 3×10−5 or less, the increase in the reactive resistance in the electrode is further reduced as compared with aspects <1> and <2>. The range of R2/R1 in aspect <3> is 5×10−7% or more and 3×10−3% or less in percentage.
<4> In one aspect of the cell stack according to the embodiment, the electrode includes a plurality of materials having different permeabilities of the electrolyte.
The electrode including a plurality of materials having different permeabilities facilitates adjustment of the permeability of the electrode as a whole. It is therefore easy to obtain a cell stack satisfying the range of R2/R1 defined in aspects <1> to <3>.
<5> In one aspect of the cell stack according to the embodiment,
the electrode includes
The carbon paper is less likely to be deformed than the carbon felt and the carbon cloth. Therefore, the electrode including the carbon paper is less likely to be deformed. The electrode that is less likely to be deformed is less likely to enter the first groove of the bipolar plate in contact with the electrode. Therefore, communication of the electrolyte is prevented from being hindered by the electrode that has entered the first groove. From the viewpoint of making the electrode less likely to enter the first groove, the second layer including carbon paper is preferably disposed so as to face the bipolar plate.
<6> In one aspect of the cell stack according to aspect <5>,
the first layer has a quantity per unit area of 20 g/m2 or more and 500 g/m2 or less, and
the second layer has a quantity per unit area of 10 g/m2 or more and 100 g/m2 or less.
When the quantity per unit area of the first layer and the quantity per unit area of the second layer satisfy the above ranges, the permeability of the electrolyte of the electrode as a whole tends to be an appropriate value. It is therefore easy to obtain a cell stack satisfying the range of R2/R1 defined in aspects <1> to <3>.
<7> In one aspect of the cell stack according to the embodiment,
the bipolar plate includes a second groove, and
the second groove allows two adjacent first grooves of the plurality of first grooves to communicate with each other.
The second groove facilitates the flow of the electrolyte in the two adjacent first grooves. Therefore, the permeation resistance in the first grooves is prevented from becoming excessively high.
<8> A redox flow battery according to the embodiment includes the cell stack according to any one of aspects <1> to <7>.
The redox flow battery according to the embodiment is excellent in battery performance. This is because the redox flow battery includes the cell stack according to the embodiment in which the increase in the reactive resistance in the electrode is suppressed.
Specific examples of the cell stack and the redox flow battery of the present disclosure will be described with reference to the drawings. Hereinafter, the redox flow battery may be referred to as an “RF battery”. In the drawings, the same reference signs denote the same or corresponding parts. The present invention is not limited to the above examples but defined by the claims, and is intended to include meanings equivalent to the claims and all modifications within the scope.
An RF battery 1 according to an embodiment will be described with reference to
RF battery 1 is typically connected to a power system 90 via an AC/DC converter 80 or a transformer facility 81. RF battery 1 charges power generated by a power generation unit 91 or discharges charged power to a load 92. Power generation unit 91 is a power generation facility using natural energy such as solar power generation or wind power generation, a general power plant, or the like. RF battery 1 is used for, for example, load leveling, instantaneous voltage drop compensation, emergency power supply, and output smoothing of natural energy power generation.
RF battery 1 includes a battery cell 10, a positive electrolyte tank 12, and a negative electrolyte tank 13. Battery cell 10 is responsible for charging and discharging. Positive electrolyte tank 12 stores a positive electrolyte. Negative electrolyte tank 13 stores a negative electrolyte.
Battery cell 10 is separated into a positive electrode cell 102 and a negative electrode cell 103 by a membrane 101. Membrane 101 is an ion exchange film that does not permeate electrons but permeates hydrogen ions, for example. A positive electrode 104 is built in positive electrode cell 102. A negative electrode 105 is built in negative electrode cell 103.
A positive electrolyte and a negative electrolyte are respectively supplied to positive electrode cell 102 and negative electrode cell 103 constituting battery cell 10. RF battery 1 of this example includes a supply pipe 108 and a return pipe 110 that connect battery cell 10 and positive electrolyte tank 12. RF battery 1 of this example includes a supply pipe 109 and a return pipe 111 that connect battery cell 10 and negative electrolyte tank 13. Supply pipes 108 and 109 are provided with pumps 112 and 113, respectively. The positive electrolyte is supplied from positive electrolyte tank 12 to positive electrode cell 102 through supply pipe 108 by pump 112. The positive electrolyte discharged from positive electrode cell 102 through positive electrode cell 102 is returned to positive electrolyte tank 12 through return pipe 110. The negative electrolyte is supplied from negative electrolyte tank 13 to negative electrode cell 103 through supply pipe 109 by pump 113. The negative electrolyte discharged from negative electrode cell 103 through negative electrode cell 103 is returned to negative electrolyte tank 13 through return pipe 111. That is, supply pipes 108 and 109 and return pipes 110 and 111 constitute a circulation flow path.
As shown in
Cell frame 3 includes a bipolar plate 31 disposed between positive electrode 104 and negative electrode 105, and a frame body 32 provided around bipolar plate 31. A central region of bipolar plate 31 is exposed from a through-window 32o of frame body 32. Positive electrode 104 is disposed so as to face a first surface of bipolar plate 31. Negative electrode 105 is disposed so as to face a second surface of bipolar plate 31. The second surface is a surface opposite to the first surface. Positive electrode 104 and negative electrode 105 are accommodated inside frame body 32 with bipolar plate 31 interposed therebetween. Positive electrode 104 and negative electrode 105 are disposed between bipolar plates 31 of adjacent cell frames 3 with membrane 101 interposed therebetween to form one battery cell 10.
In frame body 32 of cell frame 3, liquid supply manifolds 33 and 34, liquid discharge manifolds 35 and 36, liquid supply slits 33s and 34s, and liquid discharge slits 35s and 36s are formed. In this example, the positive electrolyte is supplied from liquid supply manifold 33 to positive electrode 104 through liquid supply slit 33s. The positive electrolyte supplied to positive electrode 104 is discharged to liquid discharge manifold 35 through liquid discharge slit 35s. In a similar manner, the negative electrolyte is supplied from liquid supply manifold 34 to negative electrode 105 through liquid supply slit 34s. The negative electrolyte supplied to negative electrode 105 is discharged to liquid discharge manifold 36 through liquid discharge slit 36s. Liquid supply manifolds 33 and 34 and liquid discharge manifolds 35 and 36 penetrate frame body 32, and cell frames 3 are stacked to constitute flow paths of the electrolytes. Each of these flow paths communicates with supply pipes 108 and 109 and return pipes 110 and 111 shown in
One of the characteristics of cell stack 2 of this example is to adjust the flow of the electrolytes from bipolar plate 31 to positive electrode 104 and negative electrode 105 in cell stack 2. For the adjustment, the configurations of positive electrode 104, negative electrode 105, and the bipolar plate 31 are adjusted. In the following description, positive electrode 104 and negative electrode 105 are simply referred to as an electrode 4 without distinction.
The configuration of electrode 4 will be described with reference to
Electrode 4 is a porous body having conductivity. For example, electrode 4 is a porous body including at least one selected from the group consisting of carbon, titanium, and tungsten.
Electrode 4 may include a single material or a plurality of materials. In particular, electrode 4 may include a plurality of materials having different permeabilities of electrolyte. Electrode 4 including a plurality of materials having different permeabilities facilitates adjustment of the permeability of electrode 4 as a whole. By adjusting the permeability of electrode 4, it is easy to obtain cell stack 2 in which R2/R1 described later satisfies a specific range.
Electrode 4 of this example includes a first layer 41 and a second layer 42 arranged in a thickness direction. Electrode 4 including first layer 41 and second layer 42 is an example of electrode 4 including a plurality of materials having different permeabilities. The number of layers constituting electrode 4 may be three or more.
First layer 41 and second layer 42 include, for example, carbon paper, carbon felt, or carbon cloth. The carbon cloth is a carbon fiber warp and weft alternately woven. The carbon felt is entangled independent carbon fibers. The carbon paper includes a plurality of carbon fibers and a binder that binds the carbon fibers. The carbon paper may include carbon particles. A preferable fiber diameter of the carbon fibers constituting the carbon felt and the carbon paper is 1 μm or more and 20 μm or less. A preferable fiber length of the carbon fibers constituting the carbon felt and the carbon paper is 500 μm or more and 100 mm or less. Examples of the binder of the carbon paper include an organic binder such as a phenol resin. The organic binder may be carbonized by heat treatment. The carbon paper is less likely to be deformed than the carbon felt and the carbon cloth. Therefore, electrode 4 including the carbon paper is less likely to be deformed. Electrode 4 that is less likely to be deformed is less likely to enter first groove 51 of bipolar plate 5 in contact with electrode 4. Therefore, the communication of the electrolyte in first groove 51 is prevented from being hindered by electrode 4 that has entered first groove 51.
First layer 41 includes, for example, carbon felt or carbon cloth. Second layer 42 includes, for example, carbon paper. From the viewpoint of making electrode 4 less likely to enter first groove 51, second layer 42 including carbon paper is preferably disposed so as to face bipolar plate 5. Inevitably, first layer 41 faces membrane 101 (see
A quantity per unit area of first layer 41 is, for example, 20 g/m2 or more and 500 g/m2 or less. A quantity per unit area of second layer 42 is, for example, 10 g/m2 or more and 100 g/m2 or less. When the quantity per unit area of first layer 41 and the quantity per unit area of second layer 42 satisfy the above ranges, the permeability of the electrolyte of electrode 4 as a whole tends to be an appropriate value. As a result, it is easy to obtain cell stack 2 in which R2/R1 described later satisfies a specific range.
Bipolar plate 5 will be described mainly with reference to
Introduction portion 5A is a portion serving as an inlet of an electrolyte to bipolar plate 5. Discharge portion 5B is a portion serving as an outlet of the electrolyte discharged from bipolar plate 5. An overall flowing direction of the electrolyte in bipolar plate 5 of this example is a direction from the bottom to the top as indicated by a thick arrow on the right side. Therefore, introduction portion 5A of bipolar plate 5 in
First grooves 51 extend from introduction portion 5A toward discharge portion 5B in bipolar plate 5. In this example, an extending direction of first grooves 51 coincides with the overall flowing direction of the electrolyte. The electrolyte in first grooves 51 flows toward discharge portion 5B. First grooves 51 are all parallel to each other. First grooves 51 of this example is connected to both introduction portion 5A and discharge portion 5B. The electrolyte in first grooves 51 flows in a first direction from introduction portion 5A toward discharge portion 5B. Unlike this example, some first grooves 51 among the plurality of first grooves 51 may be inclined with respect to the flowing direction.
A width of first groove 51 is, for example, uniform in the extending direction of first groove 51. The width of first groove 51 is a length of an opening of first groove 51 orthogonal to the extending direction of first groove 51. The width of first groove 51 may change at different positions in the extending direction.
A depth of first groove 51 is, for example, uniform in the extending direction of first groove 51. The depth of first groove 51 is a length from the opening to a bottom of first groove 51. The bottom is the deepest portion of first groove 51. The depth of first groove 51 may change at different positions in the extending direction.
A sectional shape of first groove 51 is not limited. The sectional shape of first groove 51 is a contour shape of first groove 51 in a cross section orthogonal to the extending direction of first groove 51. The sectional shape of this example is rectangular. Examples of other sectional shapes include a V-shape, a semicircular shape, and a trapezoidal shape.
When flowability of the electrolyte in electrode 4 is low, a battery reaction in electrode 4 may be insufficient. In addition, when the flowability of the electrolyte in first groove 51 of bipolar plate 5 is low, heat associated with the battery reaction tends to be trapped in the electrolyte. When flowability of the electrolyte in first groove 51 is excessively high, the electrolyte flowing from first groove 51 toward electrode 4 decreases. That is, it is important that the flowability of the electrolyte in electrode 4 and the flowability of the electrolyte in first groove 51 of bipolar plate 5 are set in an appropriate balance. In the present embodiment, R1 and R2 are defined as indices indicating a difficulty of a flow of the electrolyte in cell stack 2.
R1 is a permeation resistance indicating the difficulty of the flow of the electrolyte in electrode 4. R2 is a permeation resistance indicating the difficulty of the flow of the electrolyte in first groove 51 of bipolar plate 5. The permeation resistance is a new index defined herein. The permeation resistance will be described later.
An object of this example is to adjust a balance between the difficulty of the flow of the electrolyte in electrode 4 and the difficulty of the flow of the electrolyte in first groove 51 of bipolar plate 5. Therefore, the present disclosure defines that R2/R1 falls within a predetermined range. Specifically, the range of R2/R1 expressed in percentage is 7×10−9% or more and 2×10−2% or less. When R2/R1 is within the above range, the electrolyte flowing through first groove 51 of bipolar plate 5 appropriately easily flows toward electrode 4, and the flowability of the electrolyte in electrode 4 is improved. As a result, the battery performance of the redox flow battery is improved. A more preferable range of R2/R1 is 2×10−8% or more and 1×10−2% or less. A still more preferable range of R2/R1 is 5×10−7% or more and 3×10−3% or less.
The permeation resistance R1 in electrode 4 is as follows.
R
1=(L1/K1)×μ×(1/S1) Equation 1-1
A procedure for obtaining R1 will be described below.
First, a relationship between a pressure loss ΔP1 of the electrolyte in electrode 4 and permeability K1 satisfies the relationship of Equation 1-2 based on the Darcy's law.
ΔP1=(L1/K1)×μ×(Q1/S1) Equation 1-2
Permeability K1 is a value unique to electrode 4 regardless of the type of fluid. Permeability K1 is obtained based on an actual measurement value using a test cell. Specifically, the test cell is produced by using the same electrode 4 as electrode 4 provided in cell stack 2. A compressed state of electrode 4 in the test cell is set to be the same as a compressed state of electrode 4 in cell stack 2. A tank is connected to the test cell via a pipe, and a fluid having a known viscosity, such as water, flows through the test cell. A flow meter and a differential pressure gauge are connected to the pipe in advance. The differential pressure gauge is a device that measures pressure loss ΔP1 based on a pressure of the electrolyte at an inlet of the test cell and a pressure of the electrolyte at an outlet of the test cell. Since a dimension of electrode 4 of the test cell can be measured, a value other than permeability K1 in Equation 1-2 is actually measured. By substituting the actual measurement value into Equation 1-2, permeability K1 is obtained.
Next, a relationship between pressure loss ΔP1 of the electrolyte in electrode 4, a flow rate Q, and permeation resistance R1 is expressed as in an equation of V=I×R in an electric circuit, and Equation 1-3 is defined.
ΔP1=Q1×R1 Equation 1-3
By substituting Equation 1-2 into Equation 1-3, Equation 1-1 is obtained. The unit of R1 is Pa·s/m3.
Permeation resistance R2 of the electrolyte in first groove 51 of bipolar plate 5 is as follows.
R
2=(32×μ×L2)/(de2×S2) Equation 2-1
L2=length (m) of first groove 51
de=equivalent diameter (m) of first groove 51
S2=sectional area (m2) of first groove 51
A procedure for obtaining R2 will be described below. First, a pressure loss ΔP2 of the electrolyte due to friction between the electrolyte flowing in a circular pipe and a pipe wall is considered. Pressure loss ΔP2 is obtained by the following Darcy-Weisbach Equation.
ΔP
2=λ×(L2/d)×ρ/2×(Q2/S2)2 Equation 2-2
Next, a Reynolds number Re indicating a flow state of a fluid is expressed by the following equation.
Re=ρ×Q
2
/S
2
×d/μ Equation 2-3
μ: Viscosity (Pa·s) of fluid
When Re is 2300 or less, the flow in the circular pipe is a layer flow. In this case, a pipe friction coefficient λ is obtained from the following equation based on the Hagen-Poiseuille's law.
λ=64/Re Equation 2-4
By substituting Equation 2-3 into Equation 2-4, the following equation is obtained.
λ=(64×S2×μ)/(ρ×Q2×d) Equation 2-5
By substituting Equation 2-5 into Equation 2-2, pressure loss ΔP2 is expressed by the following equation.
ΔP
2=(32×μ×L2×Q2)/(d2×S2) Equation 2-6
The sectional shape of first groove 51 in bipolar plate 5 is not circular. Thus, an inner diameter d to be substituted into Equation 2-6 cannot be obtained. Therefore, an equivalent diameter de obtained from a dimension of first groove 51 is obtained. Equivalent diameter de is obtained by the following Equation 2-7.
de=4×(S2/W) Equation 2-7
Here, W is a peripheral length of first groove 51 including the opening of first groove 51. How to obtain W will be described with reference to sectional views of
By substituting de of Equation 2-6 into d of Equation 2-7 and regarding the length of the circular pipe as the length of first groove 51, pressure loss ΔP2 of the electrolyte in first groove 51 of bipolar plate 5 is obtained.
ΔP
2=(32×μ×L2×Q2)/(de2×S2) Equation 2-8
Next, a relationship between pressure loss ΔP2 of the electrolyte in first groove 51 of bipolar plate 5, a flow rate Q2, and permeation resistance R2 is expressed as in an equation of V=I×R in an electric circuit, and Equation 2-9 is defined.
ΔP
2
=Q
2
×R
2 Equation 2-9
By substituting Equation 2-9 into Equation 2-8, Equation 2-1 is obtained. The unit of R2 is Pa·s/m3.
Equation 1-1 is substituted for R1 in R2/R1, and Equation 2-1 is substituted for R2. As a result, the following Equation 3-1 is obtained.
R
2
/R
1=(32×L2×S1×K1)/(de2×S2×L1) Equation 3-1
As shown in Equation 3-1, in order to obtain R2/R1, L1 and S1 in electrode 4 and L2, S2, and de of first groove 51 in bipolar plate 5 by actual measurement are required. Here, it will be described which parts of electrode 4 and bipolar plate 5 are related to variables to be substituted into Equation 3-1.
One of the objects of the present disclosure is to allow an appropriate amount of an electrolyte to flow from first groove 51 of bipolar plate 5 toward electrode 4 so that the electrolyte quickly flows in electrode 4. Therefore, in this example, the difficulty of the flow of the electrolyte from one first groove 51A of two adjacent first grooves 51 to the other first groove 51B of two adjacent first grooves 51 through electrode 4 is used as an evaluation criterion.
In the evaluation criterion, a direction of the flow of the electrolyte in electrode 4 is a direction intersecting with, or typically, orthogonal to the extending direction of first groove 51. Therefore, length L1 of electrode 4 is a distance between first groove 51A and first groove 51B adjacent to each other. This distance is also a width of a ridge between two adjacent first grooves 51A and 51B.
A direction of the electrolyte from first groove 51 toward electrode 4 is a direction intersecting with, or typically, orthogonal to the extending direction of first groove 51. Thus, length L2 of first groove 51 is a length at which two adjacent first grooves 51 overlap each other in the extending direction of first grooves 51 (see
Sectional area S1 of electrode 4 is a product of a thickness d1 (see
A method of obtaining permeability K1, equivalent diameter de, and sectional area S2 of first groove 51 is as described above.
Here, when electrode 4 includes first layer 41 and second layer 42, permeation resistance R1 of electrode 4 is obtained by the following equation.
1/R1=(1/R1-1)+(1/R1-2) Equation 4-1
R1-1: Permeation resistance of electrolyte in first layer 41
R1-2: Permeation resistance of electrolyte in second layer 42
Cell stack 2 satisfies 7×10−9%≤R2/R1≤2×10−2%. When R2/R1 satisfies the above range, the electrolyte flowing through first groove 51 of bipolar plate 5 in cell stack 2 appropriately easily flows toward electrode 4, and the flowability of the electrolyte in the electrode 4 is improved. As a result, an increase in reactive resistance in electrode 4 of cell stack 2 is greatly reduced. RF battery 1 including cell stack 2 described above is excellent in the battery performance.
In a second embodiment, a bipolar plate 5 having a configuration different from bipolar plate 5 of the first embodiment will be described with reference to
As shown in
In this example, a length L2 of first groove 51 for obtaining R2/R1 is different from length L2 in the first embodiment. Length L2 is a length at which adjacent first grooves 51A and 51B overlap each other in the extending direction of first grooves 51. Therefore, length L2 of this example is shorter than the length of bipolar plate 5 in the overall flowing direction of the electrolyte.
In a third embodiment, a bipolar plate 5 having a configuration different from bipolar plate 5 of the first and second embodiments will be described with reference to
An extending direction of first grooves 51 of this example is inclined with respect to the overall flowing direction of the electrolyte. In this case, the electrolyte in first grooves 51 also flows in the first direction from introduction portion 5A toward discharge portion 5B.
In this example, a direction of length L2 of first groove 51 of bipolar plate 5 to be substituted into Equation 3-1 to obtain R2/R1 is inclined with respect to the overall flowing direction of the electrolyte. Length L2 is a length at which two first grooves 51 overlap each other in a direction in which two adjacent first grooves 51 are arranged in parallel. Length L1 of electrode 4 (see
In a fourth embodiment, a bipolar plate 5 having a first groove 51 different from first groove 51 of the first to third embodiments will be described with reference to
Bipolar plate 5 of this example includes one meandering groove 50. A first end of meandering groove 50 is connected to introduction portion 5A, and a second end of meandering groove 50 is connected to discharge portion 5B. A flow of the electrolyte in meandering groove 50 is indicated by a thick line arrow. Meandering groove 50 of this example is constituted by connecting a first groove 51 and a second groove 52. First groove 51 is a portion of meandering groove 50 through which the electrolyte flows in a direction along the overall flow of the electrolyte. Second groove 52 is a portion of meandering groove 50 that allows adjacent first grooves 51A and 51B to communicate with each other. That is, second groove 52 is an S-shaped portion including a lateral groove closer to discharge portion 5B, a lateral groove closer to introduction portion 5A, and a longitudinal groove connecting both of the lateral grooves. The lateral groove closer to discharge portion 5B extends in a direction orthogonal to the overall flowing direction of the electrolyte, and is connected to an end of first groove 51A closer to discharge portion 5B. The lateral groove closer to introduction portion 5A extends in a direction orthogonal to the overall flowing direction of the electrolyte, and is connected to an end of first groove 51B closer to introduction portion 5A. The longitudinal groove extends along the overall flowing direction of the electrolyte, and connects the two lateral grooves. A flowing direction of the electrolyte in the longitudinal groove is a direction toward introduction portion 5A. Therefore, the longitudinal groove is not first groove 51 that allows the electrolyte to flow toward discharge portion 5B.
In this example, the presence of second groove 52 is ignored in obtaining R2/R1. Therefore, length L1 of electrode 4 to be substituted into Equation 3-1 is a distance between first groove 51A and first groove 51B at the closest position. Length L2 of bipolar plate 5 to be substituted into Equation 3-1 is a length at which first groove 51A and first groove 51B overlap each other in the extending direction of first groove 51.
In a test example, an influence of the size of R2/R1 in the cell stack on an increase of the reactive resistance in the electrode of the cell stack was examined. The superiority and inferiority of the reactive resistance in the electrode were evaluated by reactive resistivity (Ω·cm2).
Cell stacks of samples Nos. 1 to 12 were prepared. A difference between these cell stacks lies in the configuration of the electrodes. The electrode of sample No. 1 was an electrode having a single layer structure. The electrodes of samples Nos. 2 to 12 were electrodes having a two-layer structure including a first layer and a second layer. The structure of the electrodes is shown in Table 1. A quantity per unit area (g/m2) of each layer of the electrodes is also shown in Table 1.
In addition, R2/R1 in the cell stack of each sample was obtained by calculation. A method for obtaining R2/R1 is as described above. Values of R2/R1 are shown in Table 1. R2/R1 in the table is shown in percentage.
The reactive resistivities (Ω·cm2) of the cell stacks of samples Nos. 1 to 12 were determined. A measurement method is as follows. First, the cell stack of each sample was charged and discharged at a constant current with a current density of 90 mA/cm2. In this test, charge and discharge were performed for a plurality of cycles. In the test, an upper limit and a lower limit of a switching voltage were set, charge was switched to discharge when the voltage reached the upper limit during charging, and discharge was switched to charge when the voltage reached the lower limit during discharging. After charging and discharging of each cycle, the cell resistivity (Ω·cm2) was determined for each sample. An average voltage at a time of charge and an average voltage at a time of discharge in any one cycle of a plurality of cycles were obtained, and the cell resistivity was defined as {(a difference between the average voltage at the time of charge and the average voltage at the time of discharge)/(an average current/2)}×an cell effective area. The cell resistivity is determined by the sum of a conductive resistivity and a reactive resistivity. The conductive resistivity is determined by measuring an electric resistance of the cell stack with a battery high tester. Therefore, the reactive resistivity is obtained by subtracting the conductive resistivity from the cell resistivity.
3 × 10−12
As shown in Table 1, the reactive resistivities of samples Nos. 1, 2, 3, 4, 5, 6, 9, 10, and 11 in which R2/R1 were 7×10−9% or more and 2×10−2% or less was lower than the reactive resistivities of the other samples. Therefore, it has been found that the fact that R2/R1 satisfies 7×10−9% or more and 2×10−2% or less has a great influence on reducing an increase in the reactive resistance in the electrode of the cell stack.
The reactive resistivities of samples Nos. 2 to 6 in which R2/R1 were 3×10−8% or more and 1×10−2% or less was lower than the reactive resistivities of the other samples. The reactive resistivities of samples Nos. 3 to 5 in which R2/R1 was 7×10−7% or more and 3×10−3% or less were lower than the reactive resistivities of samples Nos. 2 and 6. Here, even when R2/R1 was 3×10−8% or more and 1×10−2% or less, the reactive resistance of samples Nos. 10 and 11 having a layer with an extremely small quantity per unit area tended to increase.
1: redox flow battery (RF battery)
90: power system, 91: power generation unit, 92: load
2: cell stack
3: cell frame
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/JP2020/037918 | 10/6/2020 | WO |