151012-1553 EDT
domnic:
"how do I eliminate capacitance coupling ?"
Consider a stiff AC voltage source (meaning a constant voltage relatively independent of the load on the voltage source), a reference electode (a big flat sheet of copper), a hot wire a substantial distance from the copper reference plate, a floating isolated wire close to the hot wire, and the voltage source connected between the hot wire and the copper plate. You can call the copper plate ground if you want, I will.
There is capacitance between the hot wire and ground, This is effectively a shunt across the voltage source, and its current is of little concern in this discussion at this point.
There is capacitance between the hot wire and the floating wire. Also there is capacitance between the floating wire and ground, but this second value is much lower than between hot and the floating wire because of the relative spacings. The two capacitors form a voltage divider across the voltage source. Use an infinite input impedance meter and the voltage of the floating wire will be closer to that of the hot wire than ground if measured relative to ground.
You can reduce the effect of capacitive coupling by connecting a low impedance between the floating electrode, and ground. GoldDigger mentioned this. This lowers the voltage on the floating conductor relative to ground.
If you assume 1000 pfd for the hot to float capacitance, capacitive reactance is about 2.7 megohms at 60 Hz, then a 10 megohm meter would read about 10/10.36 = 0.96 times the source voltage. This calculation is from a right angle vector diagram.
A Simpson 260 is today 5000 ohms per volt or 250,000 ohms on the 50 V scale. Earlier models were 1000 ohms per volt on AC. For 5000 ohms per volt this would have a voltage reading to ground of 0.25/2.72 = 0.092 times the source voltage. At 120 V source this is 11 V, on the 50 V scale. In an actual experiment I read 11 V from 125 V. On the 250 V range the calculation is 1.25 meghoms, and thus 1.25/2.975 = 0.42 times source voltage. At 120 calculates to 50.4 V. Measured value at 125 is 45 V.
Now to elimination of the capacitive coupling. GoldDigger mentioned a conduit with the hot wire running inside the conduit. So to our above example add the conduit enclosing the hot wire with the floating wire outside the conduit, and ground spaced some distance away as before.
First, float the conduit also. Now there is capacitance from hot to conduit, conduit to ground, conduit to float, float to ground, and extremely little capacitance directly from hot to ground. But effectively there is capacitance from hot to float. Conduit will have a voltage fairly close to hot voltage relative to ground. The floating wire voltage will be somewhat less relative to ground than the conduit.
Second, connect conduit to ground. There is capacitance from hot to ground, but virtually none from hot to float. There is capacitance from float to both conduit and ground, but there is no voltage from float to ground because the conduit has now created a shield between the hot and float.
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