High D.C. voltages are usually measured by connecting a very high resistance (few hundreds of mega ohms) in series with a micro ammeter. Only the current flowing through the large calibrated resistance R is measured by the moving coil micro ammeter. The voltage of the source is given by
Series resistance micrometer |
The voltage drop in the meter is negligible, as the impedance of the meter is only few ohms com pared to few hundred mega-ohms of the series resistance R. A protective device like a paper gap, a neon glow tube, or a zener diode with a suitable series resistance is connected across the meter as a protection against high voltages in case the series resistance R fails or flashes over. The ohmic value of the series resistance R is chosen such that a current of one to ten microamperes is allowed for full-scale deflection. The resistance is constructed from a large number of wire wound resistors in series. The voltage drop in each resistor element is chosen to avoid surface flashovers and discharges. A value of less than 5 kv /cm in air or less than 20 kV/cm in good oil is permissible. The resistor chain is provided with corona free terminations. The material for resistive elements is usually a carbon-alloy with temperature coefficient less than 1T Carbon and other metallic film resistors are also used. A resistance chain built with ±1% carbon resistors located in airtight transformer oil filled P.V.C. tube, for 100 kV operations had very good temperature stability.
The limitations in the series resistance design are:
• Power dissipation and source loading
• Temperature effects and long time stability
• Voltage dependence of resistive elements, and
• Sensitivity to mechanical stresses
Series resistance meters are built for 500kV D.C. with accuracy better than 0.2%.
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