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Internal cell resistance

Rc, internal resistance/cell (Q) Rtot = (m/n)Rc + Rcxt I/Rtot Etot =... [Pg.58]

Internal resistance or impedance is the resistance or impedance that a battery or cell offers to current flow. [Pg.506]

In the 2inc chloride cell, precipitated basic 2inc chloride is the primary anode product because of the low concentration of ammonium chloride in the cell. Water and 2inc chloride are consumed in equations 1 and 7 and must be provided in adequate amounts for the cell to discharge efficiendy. Usually more carbon is used in 2inc chloride cells than in Led an chit cells in order to increase the electrolyte absorptivity of the cathode and thus allow the use of a larger volume of electrolyte. Also, the use of a thin paper separator, which decreases internal resistance, allows less space for water storage than the thick, pasted separator constmction traditionally used in Leclanchn cells. [Pg.522]

Fig. 10. Power and voltage characteristics of the nickel—iron cell where the internal resistance of the cell, R, is 0.70 mQ, at various states of discharge ( )... Fig. 10. Power and voltage characteristics of the nickel—iron cell where the internal resistance of the cell, R, is 0.70 mQ, at various states of discharge ( )...
Soluble corrosion products may increase corrosion rates in two ways. Firstly, they may increase the conductivity of the electrolyte solution and thereby decrease internal resistance of the corrosion cells. Secondly, they may act hygroscopically to form solutions at humidities at and above that in equilibrium with the saturated solution (Table 2.7). The fogging of nickel in SO2-containing atmospheres, due to the formation of hygroscopic nickel sulphate, exemplifies this type of behaviour. However, whether the corrosion products are soluble or insoluble, protective or non-protective, the... [Pg.336]

Corresponding to the charge in the potential of single electrodes which is related to their different overpotentials, a shift in the overall cell voltage is observed. Moreover, an increasing cell temperature can be noticed. Besides Joule-effect heat losses Wj, caused by voltage drops due to the internal resistance Rt (electrolyte, contact to the electrodes, etc.) of the cell, thermal losses WK (related to overpotentials) are the reason for this phenomenon. [Pg.15]

The connection of AA-size cells in parallel can replace larger cells (e.g., D-size cells). Four AA cells fit into a D-size can, and six AA-cells are in equivalent weight to a D-cell [27]. The utilization of the Mn02 cathode is considerably improved because the cathode thickness is only 2 mm in a AA cell, but 5 mm in a D-cell. The internal resistance is also lower by a factor of 4 to 6. Figure 11 depicts a 5 PxlO S bundle battery five AA cells in parallel = 1 bundle, 10 bundles in series make a (nominal) 12 V battery. It is used as the power source for a transmitter/receiver service. A typical load profile is 2 A for 1 min, 0.33 A for 9 min average load, 0.5 A per bundle or 0.1 A per cell service, about 15 h. Smaller bundle batteries (with 2x9 cells) are very suitable for notebook-computers 18 AA cells weight 0.36 kg, and the total initial capacity is 32 Wh. [Pg.79]

The power of the ZEBRA cell depends on the resistance of the cell during discharge. The resistance of the ZEBRA cell rises with increasing depth of discharge (DOD). There is a contribution to the resistance from the fixed values of the solid metal components and of the/ "-alumina solid electrolyte. The variable parts of the resistance arc the sodium electrode and the positive electrode. The increase in internal resistance during discharge is almost entirely due to the positive electrode, as can be seen from Fig. 4. [Pg.568]

Figure 4. Qminbuuun.v to the internal resistance of a ZEBRA cell. Figure 4. Qminbuuun.v to the internal resistance of a ZEBRA cell.
The reduction of the internal resistance of the cell can obviously be achieved by two measures ... [Pg.569]

Figure 6. Comparison of internal resistance of cells with different /T-Al20, electrolyte geometries. Figure 6. Comparison of internal resistance of cells with different /T-Al20, electrolyte geometries.
These electrode reactions snstain a continuous flow of electrons in the external circuit. The OH ions produced by reaction (19.4) in the vicinity of the positive electrode are transported through the electrolyte toward the negative electrode to replace OH ions consumed in reaction (19.3). The electric circuit as a whole is thus closed. Apart from the OCV, the current depends on the cell s internal resistance and on the ohmic resistance present in the external circuit. Current flow will stop as soon as at least one of the reactants is consumed. [Pg.345]

Flaving had over 150 years of technical development behind them, lead-acid batteries can be custom-tailored to specific applications, such as those requiring deep discharge cycles (e.g., where the batteries are used as the sole power source for electrical equipment) and for battery backup uses such as in large uninterruptible power supply systems in data centers. Moreover, lead-acid cells not only have low internal resistance but also experience no memory effect as do some more exotic cell designs, such as NiCads. This enables these cells to produce enormous currents and have a moderately long, predictable life.1... [Pg.1313]

Relaxation methods for the study of fast electrode processes are recent developments but their origin, except in the case of faradaic rectification, can be traced to older work. The other relaxation methods are subject to errors related directly or indirectly to the internal resistance of the cell and the double-layer capacity of the test electrode. These errors tend to increase as the reaction becomes more and more reversible. None of these methods is suitable for the accurate determination of rate constants larger than 1.0 cm/s. Such errors are eliminated with faradaic rectification, because this method takes advantage of complete linearity of cell resistance and the slight nonlinearity of double-layer capacity. The potentialities of the faradaic rectification method for measurement of rate constants of the order of 10 cm/s are well recognized, and it is hoped that by suitably developing the technique for measurement at frequencies above 20 MHz, it should be possible to measure rate constants even of the order of 100 cm/s. [Pg.178]

It was shown by our investigations that such cell can be cycled with self-charging at least during 10-15 cycles. After that, the internal resistance of such cell is incremented considerably due to the accumulation of... [Pg.121]

This permits a reformulation of the cathode to include more active material and a lower internal resistance, as noted in Figure 2. The resultant lower internal resistance and higher active mass content produced a 30% increase in cell performance at high rate discharges. [Pg.178]

The proper mixing of the graphite with the Mn02 is critical for high rate performance. It is necessary to put work into the mix to uniformly coat the manganese dioxide particles with a thin layer of graphite. This provides a low resistance path from the manganese to the cell terminals to minimize the internal resistance of the cell. A similar effect can be expected if used in cathode formulations for Li-Ion cells. [Pg.178]

Ohmic losses predominate in the range of normal fuel cell operation. These losses can be expressed as iR losses where i is the current and R is the summation of internal resistances within the cell, Equation (2-2). As is readily evident from the equation, the ohmic loss and hence voltage change is a direct function of current (current density multiplied by cell area). [Pg.68]

Operating temperature has a significant influence on PEFC performance. An increase in temperature lowers the internal resistance of the cell, mainly by decreasing the ohmic resistance of the electrolyte. In addition, mass transport limitations are reduced at higher temperatures. [Pg.88]

Most modem voltmeters have such a large internal resistance that we can indeed say that a cell potential will actually be measured at zero current. [Pg.14]

If the potential of the Daniell cell is to be determined accurately, we have already seen that the measurement has to be made at zero current. In order to ensure zero current, the internal resistance of the voltmeter shown in Figure 3.1 must be vast, as discussed in the previous chapter. The voltmeter operates in much the same way as a switch or circuit breaker does reaction (in this case, cell discharge) would occur but for the incorporation of the voltmeter in the circuit. [Pg.28]


See other pages where Internal cell resistance is mentioned: [Pg.603]    [Pg.546]    [Pg.554]    [Pg.135]    [Pg.116]    [Pg.14]    [Pg.568]    [Pg.572]    [Pg.597]    [Pg.78]    [Pg.602]    [Pg.603]    [Pg.346]    [Pg.351]    [Pg.824]    [Pg.632]    [Pg.659]    [Pg.88]    [Pg.170]    [Pg.1311]    [Pg.1314]    [Pg.1317]    [Pg.120]    [Pg.513]    [Pg.305]    [Pg.194]    [Pg.67]   
See also in sourсe #XX -- [ Pg.43 ]




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