Coefficient of performance
How much energy is in the gas produced, against the electrical energy it took?
- C
- Coefficient of performance
- E
- Chemical energy out
- W
- Electrical energy in
- V
- Hydrogen collected
- P
- Electrical power in
- t
- Duration, s
LaTeX
E = V \cdot h_v \qquad W = P \cdot t \qquad C = \frac{E}{W}
Method
- Take the hydrogen volume alone. The oxygen produced alongside it carries no fuel value, so valuing the mixed gas overstates the output by half.
- Multiply by the heating value: 10.783 kJ per litre for the lower figure, 12.745 for the higher. Use the lower unless the exhaust is condensed and that latent heat is actually recovered — in a flame open to the room, it is not.
- Multiply the electrical power by the run time for the energy in. The power must be true power: the mean of instantaneous voltage times instantaneous current. On a pulsed or resonant waveform, multiplying an RMS voltmeter reading by an RMS ammeter reading gives apparent power, which can be several times the real figure.
- Divide energy out by energy in.
- Also report kilojoules per litre. It is a harder number to fool, comparable across rigs, and commercial electrolysers sit around 12 to 18 kJ per litre.
Assumptions
- The input power is true power. This is where most reported figures above unity come apart: on a pulsed waveform, voltage and current are not in phase, and the product of two meter readings is apparent power rather than real power.
- The volume is dry hydrogen at the stated conditions. Gas collected over water carries vapour; mixed gas counted as hydrogen inflates the output by 50 %.
- The energy in the gas is chemical energy released on burning it, not work recovered. An engine or fuel cell then returns a fraction of it — thirty to sixty per cent — so a coefficient near 1 here is not a self-sustaining system.
- Only the electrolysis power is counted. A complete accounting includes the driver, the pump and any heating, which is why "at the wall" and "at the cell" can differ severalfold.
- The archive takes no position on whether this ratio can exceed one. It takes a position on the arithmetic being visible, which is what this page is for.