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Separators voltage drops

Applying this to the above example for an area of 1 in2 = 6.45 cm2, the result is R= 8.8 mQ in2. Taking an example from SLI battery practice one cell with six positive and seven negative electrodes of typical 114 mm x 147 mm size with the above separator show a resistance of 28.3x10 6Q at 25°C, or close to 75xl0 Q at -18 °C. For a cold crank current of 320 A and six cells in series in a 12 V battery, the voltage drop due to the separator resistance amounts to w 0.15 V Fig. 5 shows this correlation. [Pg.249]

Doyle et al. [40] used a mathematical model to examine the effect of separator thickness for the PVDF.HFP gel electrolyte system and found that decreasing separator thickness below 52 pm caused only a minor decrease in ohmic drop across the cell. The voltage drops in the electrodes were much more significant. They state that their model predictions were confirmed experimentally. [Pg.562]

In addition to this qualitative aspect, isotachophoresis may also be used quantitatively. Once the sample zones have developed, the conductivity of each zone and hence the voltage drop across it will be related to the concentration of the ions and in order to maintain uniform conductivity the concentration (i.e. the volume occupied by each component) will alter. Hence at equilibrium, not only will the components of a mixture be separated from each... [Pg.143]

Continuous systems use the same buffer, at constant pH, in the gel, sample, and electrode reservoirs. With continuous systems, the sample is loaded directly on the gel in which separation will occur. The sample application buffer is the same as the gel and electrode buffer, but at about half the concentration. The localized voltage drop that results from decreased conductivity in the sample solution helps drive sample proteins into the gel and sharpens protein bands. Once inside a gel, proteins are separated on the basis of their individual (gel-mediated) mobility differences. Bandwidths are highly dependent on the height of the applied sample... [Pg.122]

Ohmic voltage drop Cell separator rmn nonriiiotor t... [Pg.35]

In principle, a further inexpensive method is to work at constant cell voltage. But here the potentials of the working and of the counter electrode, and all voltage drops of the electrolytes and of the cell separator are included (see Fig. 2). Thus, in most cases, clearly defined conditions at the working electrode cannot be adjusted using this operation mode (nevertheless, because of its uncomplicated realization, it is applied in most technical electrolyses to achieve approximately the desired cell current). [Pg.37]

The task of a cell separator is to impede a direct mixing of anolyte and catholyte and to decrease diffusion, but at the same time the migration of ions has to be possible without a too high voltage drop. Naturally, a compromise of these requirements has to be found. [Pg.52]

The functioning of a separator will be the more difficult, the more different both electrolytes are. With increasing concentration gradients diffusion will be enhanced. It can be reduced using a less porous and/or thicker separator, but then the voltage drop increases. A special problem, that has to be avoided, is a precipitation at the surface or within the separator if the solubility of a compound is smaller in one solution compared with the other. [Pg.52]

The most typical way to measure the in-plane electrical conductivity of a diffusion layer is through the use of the four-point probe method. A small current is applied across the sample material a separate set of voltage measuring probes that are in touch with the material are used to measure the resulting voltage drop in order to calculate the resistance. With these values, the in-plane resistivity, p, can be calculated with the following equation [9,233] ... [Pg.273]

The voltage drop across a working electrochemical cell is not uniformly distributed. This is shown schematically in Figure 1.2. A large proportion a due to the electrical resistance of the electrolyte and the separator. This, of course, can be decreased by a suitable cell design. The voltage drop across the working electrode solution interface determines the rate constant for the electrochemical reaction. It is... [Pg.3]

During CE separation, there is Joule heating due to the flow of electric current. This effect has been studied by examining the non-linearity in a plot of current vs. E [107,352]. CE current could be determined by measuring the voltage drop across a 100-ki2 resistor (typically less than 1/1000 the microchannel resistance) [193]. Deviation from linearity appeared when E was greater than 720 V/cm. At this value, the electrical power was around 2.3-3.8 W/m. This value was a twofold improvement over 1 W/m typically found in fused silica capillary [102]. [Pg.147]

Fig. 8. Voltage drop Vi, /, z) in the scattering region is presented for bias of 0.5 V applied to the left Au electrode. The electrode separation is of 11.7 A, and the C60 sits in the middle of the tunnel junction. Here, we define the voltage drop in the scattering region as Vj,(r) = Vn(r Vj,) — Vjj(r Vj, = 0). The presented Vj,(y, z) is an average over the horizontal planes, i.e., f dxV, (x,y,z)/(xt — xt>), where xt, and xt are the coordinates of the bottom and top of the computation box in the x direction. The dashed vertical lines highlight the C60 location in the molecular junction. We project the positions of the left and right electrodes and the molecule onto the surface Vf,(y, z). The corresponding edges are shown by the bold solid lines. Fig. 8. Voltage drop Vi, /, z) in the scattering region is presented for bias of 0.5 V applied to the left Au electrode. The electrode separation is of 11.7 A, and the C60 sits in the middle of the tunnel junction. Here, we define the voltage drop in the scattering region as Vj,(r) = Vn(r Vj,) — Vjj(r Vj, = 0). The presented Vj,(y, z) is an average over the horizontal planes, i.e., f dxV, (x,y,z)/(xt — xt>), where xt, and xt are the coordinates of the bottom and top of the computation box in the x direction. The dashed vertical lines highlight the C60 location in the molecular junction. We project the positions of the left and right electrodes and the molecule onto the surface Vf,(y, z). The corresponding edges are shown by the bold solid lines.
The measurement of the ohmic resistance for an electrolyte is more difficult than it is for a metal wire. A variety of chemical and physical processes occur at the electrode-solution interface that must be separated from the voltage drop associated with the migration of ions through the bulk electrolyte. [Pg.289]


See other pages where Separators voltage drops is mentioned: [Pg.418]    [Pg.418]    [Pg.196]    [Pg.78]    [Pg.275]    [Pg.88]    [Pg.90]    [Pg.109]    [Pg.338]    [Pg.259]    [Pg.472]    [Pg.178]    [Pg.400]    [Pg.146]    [Pg.156]    [Pg.239]    [Pg.174]    [Pg.364]    [Pg.143]    [Pg.35]    [Pg.2]    [Pg.201]    [Pg.219]    [Pg.147]    [Pg.266]    [Pg.27]    [Pg.168]    [Pg.200]    [Pg.14]    [Pg.849]    [Pg.34]    [Pg.315]    [Pg.410]    [Pg.73]    [Pg.199]    [Pg.79]    [Pg.20]   


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Separation voltage

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