Hello MrAl,
I'm not quite sure if you were telling me the way you used to measure the leakage current of a cap. Sometimes I can't understand the meaning of an English sentence! For example, I have completely no idea what " the pure part of the cap is out of picture with DC current" means.
I'm very interested in knowing the principle of your method though, so please allow me to ask a few more questions. : )
Was that bridge used to charge a capacitor to a certain voltage?
Did you mean that if we can measure the current of a cap which we already know its voltage, then the resistance of the parallel resistor that was used to model the leakage (let's call it the leakage resistance and indicate it by Rp) can be calculated by Rp=V/I?
It works because if we know the cap's voltage Vo, then it's going to decay due to leakage according to
v(t)=Vo*e^(-t/Rp*C),
and if we can measure the leakage current i(t)=-C*(dv/dt)=(Vo/Rp)*e^(-t/Rp*C) at any time t=T during it's decaying,
then Rp=v(T)/i(T)?
So far, did I misunderstand your descriptions?
Hi,
The "pure" part of the capacitance is the "C" in e^(-t/(R*C)). It's the capacitance ALONE.
So if we had a capacitor of say 10uf and it had an equivalent 'leakage resistance' of 1 megohm, the pure part of the capacitance would be just the 10uf part. It is the part with units of Farads.
When we charge up a capacitor with a voltage source E in series with a resistance R, the capacitor voltage charges up as:
Vc=E*(1-e^(-t/RC))
and the current is:
Ic=E/R*(e^(-t/RC))
After a long time though, the exponential part becomes equal to zero (t very very long like 1e32 seconds) so we get:
Vc=E*1=E
and
Ic=0
That is when the resistance is in series with the cap and that is the only resistance and notice that the current is zero. But if we have the second resistance that represents the leakage current, when the cap voltage stabilizes after a long time we end up with a small current that ONLY flows through the 'leakage' resistance and since that is then just a voltage across a resistance and we know the current we can calculate the resistance from R=E/I.
So with this kind of measurement we just need to measure the DC voltage and the DC current after a long time has passed.
The old piece of equipment i had actually had a fish eye tube (dont know if they make them anymore) which gave an indication of the current through the device under test and it was very sensitive because it did not require a physical movement of anything to show current, but i later used a highly sensitive current meter in series with the cap to get a numerical reading.
To set this up, as Joe pointed out, put the DC current meter in series with the capacitor, but shunt the meter with a shorting strip so that the meter is shorted out completely. Then apply some current and wait for the cap to charge up, then remove the shorting strip to take a reading. Measuring the voltage across the cap and the current, the resistance is then:
R=E/I
and E and I are then just DC values.
This works because once the cap charges up the capacitance no longer affects the readings because they are all DC.
This provides us with an equivalent resistance for the leakage at whatever voltage we are testing with.