
PORTABLE SEALED NICKEL-METAL HYDRIDE BATTERIES 29.15
at the 0.2C rate of 60 Ah /kg and 200 Ah/ L, reflecting the performance of a standard type
battery. As discussed in Sec. 3.2.6, this figure provides a convenient nomograph to determine
the approximate performance, in service hours, of a battery or to estimate the size of a
battery that will deliver the desired performance under specified discharge conditions—again
with the caveat that the battery has similar construction and characteristics to the standard
battery on which the data are based and an energy density close to the one specified.
29.4.5 Internal Resistance
The nickel-metal hydride battery has a low internal resistance because of the use of thin
plates with large surface areas and low resistance and an electrolyte having a high conduc-
tivity. Figure 29.9 shows the change in internal resistance with the depth of discharge. The
resistance remains relatively constant during most of the discharge. Toward the end of the
discharge, the resistance increases due to conversion of the active materials. The internal
resistance also increases as the temperature drops because the resistance of the electrolyte
and other components is higher at the lower temperatures. The resistance of the nickel-metal
hydride battery increases with use and cycling. This is illustrated in Fig. 29.24a which shows
the drop in midpoint voltage as the battery is cycled.
FIGURE 29.9 Internal resistance vs. discharge capacity of
sealed cylindrical nickel-metal hydride cells.
29.4.6 Polarity Reversal during Overdischarge
When a multicell series-connected battery is discharged, the lowest-capacity battery will
reach the point of full discharge before the others. If the discharge is continued, this lower-
capacity cell can be driven into an overdischarged condition through 0 V and its polarity
(voltage) reversed. This is illustrated in Fig. 29.10.
Phase 1 of the figure is the normal phase of the discharge with active material remaining
on both the positive and the negative electrodes.
During phase 2 the active material on the positive electrode has been discharged and
generation of hydrogen gas starts. Some of this gas may be absorbed by the hydrogen storage
metal alloy in the negative electrode and the remainder builds up in the cell. Active material,
however, still remains on the negative electrode and the discharge continues. The cell voltage
is dependent on the discharge current, but remains within
⫺0.2 to about ⫺0.4 V.
In phase 3 the active materials on both electrodes have been depleted and oxygen is
produced at the negative electrode. Prolonged overdischarge leads to gassing, higher internal
cell pressure, opening of the safety vent, and deterioration of the cell.