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Lightweight Electric/Hybrid Vehicle Design

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2<br />

Viable energy storage systems 29<br />

Viable energy storage systems<br />

2.1 Electronic battery<br />

<strong>Electric</strong> vehicles are at a historical turning point – the point where technology permits the<br />

performance of electric vehicles to exceed the performance of thermal engines 1 . Currently quality<br />

battery technology is expensive and heavy. This favours hybrids with small peaking batteries –<br />

typically 10 Ah at 300 V, with a capability of 70 kW for 2 minutes. New battery geometries have<br />

been developed for this application in the form of high performance D cells with 6 mm thick end<br />

caps and M6 terminals. A single string of cells handles 100 amps for 10 seconds. The heat is<br />

transferred to the end caps then removed by forced air cooling. It is vital to maintain an even cell<br />

state of charge in long strings. This solution has two drawbacks at present: (1) Cost – a 300 V 6.5<br />

Ah stack costs more than $10 000 in January 98; (2) reliability – with only one string a single high<br />

resistance cell disables the battery.<br />

Using the best available nickel–cadmium cells, it is possible to build a reliable peak power stack<br />

and use electronic control to maintain equal currents in strings. A later section will consider the<br />

next generation, an all electric hybrid with aluminium battery and alkaline fuel cell; this last<br />

important energy storage system is also discussed in depth in Chapter 4. A review of different<br />

battery types and performances is given in Chapter 5.<br />

2.2 Battery performance: existing systems<br />

All battery technologies can offer some solution to the peak power problem but there is only one<br />

parameter which ultimately matters, and this is the internal resistance of the cell. This is much<br />

more related to cell geometry than cell chemistry, as we shall discover. When AA, C, D and F cells<br />

were originally designed, nobody was thinking of discharging them at hundreds of amps, so it is<br />

hardly surprising that they are not ideal for the purpose. This problem will become even more<br />

extreme as power density improves:<br />

D cell characteristics<br />

Lead Acid NiCad NiMh Lithium Aluminium<br />

Amp Hr (20hr) 2.5 4.0 6.5 7.5 50<br />

Cell voltage 2.0 1.2 1.2 3.6 3.0<br />

Max C rate 40.0 25.0 11.0 40.0 Unknown<br />

Ah/25°C 0.5 3.0 5.0 6.0 Unknown

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