The Ohmart patent is very interesting since it describes, confirms and characterizes one part (about one half) of the LEC effect: the possibility of generating a voltage difference and a current by using two metal electrodes and a ionized gaseous medium. In the patent there are a number of confirmations on the observations we made on the LEC, and also some information on experiments we have not made yet.
Main findings are:
- The voltage difference is due to some additional surface property and not only to the electrode potential and work function difference;
- Surface properties of materials affects the generated voltage, and some insulating or "semiconducting" compound can be used to generate the effect (such as leas oxide, copper oxide and aluminium oxide);
- The effect can be used as a sensitive detector in a number of applications, one of which is characterizing this specific material property (Ed Storm suggested something similar about the LEC);
- Some useful relationships among various parameters are reported, clarifying some of the observed data about the LEC (e.g. dependence with temperature, polarity invertions, etc);
- The effect is only obtained when the gas is ionized by external means.
The LEC makes a step forward compared to the Ohmart effect, in that it does no need an external radiation source to work: the ionization is self-generated. BTW, this is an indirect and additional confirmation that the gas inside the LEC is actually ionised.
The Ohmart effect is not explained in the patent and related documents, but now we know that it is responsible for the voltage generation in the LEC. However the LEC has an additional feature and mistery associated with it: it is able to self-ionise the gas.
The picture now is a bit more clear in that now we confidently know that there are two different, and probably unrelated, effects at play in the LEC. This suggests to avoid studying the overall LEC efficiency only by measuring the voltage (that is a compound effect), but always adding the forced current measurement, that is an indication of the ionization (and so a measurement of the first effect).