Table 6.
Ignition source and its temperature
| Definition | Ignition source | TIgnition source | ||
|---|---|---|---|---|
| °C | ||||
| Forced ignition | The CEG is heated locally by forced ignitions, and the local CEG ignites first, and then, the flame spreads to the others. Forced ignition sources often have high temperatures. | Spark | (1) Electric spark caused by too small electric clearance between conductive parts | 3000–6000 |
| (2) Electric arc caused by lots of sparks | 8700–9700 | |||
| (3) Static electric spark caused by invalid equipotential bonding | – | |||
| (4) Mechanical spark caused by friction between the eruption flow and the wall | ~1200 | |||
| (5) Spark from the ICE pipe | 600–800 | |||
| Hot spot | 6) High temperature surface of the cell | ~1000 | ||
| (7) High temperature cable with short circuit or overcurrent | – | |||
| (8) Cigarette butts | 250–800 | |||
| Flame | (9) Gas flame | 1600–2100 | ||
| (10) Gasoline flame | ~1200 | |||
| (11) Match flame | 500–650 | |||
| Autoignition | The CEG is heated whole by autoignition sources and then ignites. The autoignition source does not need to have a high temperature but needs to have enough energy to heat the CEG. | Self-heating | (1) Heats from the chemical reactions during the generating process of CEGs | 200–1000 |
| (2) Heats from slow chemical reactions of CEGs caused by lighting, catalytic reactions by cathode materials, etc. | – | |||
| Non-self-heating | (3) Heats from high temperature autoignition sources often with indirect contact with the CEG, such as the high temperature surface of a cell with thermal runaway, the high temperature surface of the ICE of another vehicle, a heater, etc. They can make the temperature of all the CEG be increased. | – | ||
| (4) An energy source that converts other forms of energy into heat, such as friction, compression, etc. | – | |||