Complex waveforms are most accurately measured with an RMS voltmeter. This instrument produces a meter indication by sensing waveform heating power which is proportional to the square of the rms value of the voltage. This can be measured by amplifying and feeding it to a thermocouple, whose output voltages are proportional to the Erms.
However, thermocouples are non-linear devices. This difficulty can be overcome in some instruments by placing two thermocouples in the thermal environment.
The effect of non-linear behavior of the thermocouple in the input circuit is cancelled by similar non-linear effects of the thermocouple in the feedback circuit. The two couples form a bridge in the input circuit of a dc amplifier. The unknown ac voltage is amplified and applied to the heating element of the thermocouple. The application of the heat produces an output voltage that upsets the balance of a bridge.
The dc amplifier amplifies the unbalanced voltage; this voltage is fed back to the heating element of the balancing thermocouple, which heats the thermocouple, so that the bridge is balanced again, i.e., the outputs of both the thermocouples are same. At this instant, the ac current in the input thermocouple is equal to the dc current in the heating element of the feedback thermocouple. This dc current is directly proportional to the effective or rms value of the input voltage, and is indicated by the meter in the output circuit of the dc amplifier. If the peak amplitude of the signal does not exceed the dynamic range of the ac amplifier, the true rms value of the ac signal can be measured independently.
However, thermocouples are non-linear devices. This difficulty can be overcome in some instruments by placing two thermocouples in the thermal environment.
The dc amplifier amplifies the unbalanced voltage; this voltage is fed back to the heating element of the balancing thermocouple, which heats the thermocouple, so that the bridge is balanced again, i.e., the outputs of both the thermocouples are same. At this instant, the ac current in the input thermocouple is equal to the dc current in the heating element of the feedback thermocouple. This dc current is directly proportional to the effective or rms value of the input voltage, and is indicated by the meter in the output circuit of the dc amplifier. If the peak amplitude of the signal does not exceed the dynamic range of the ac amplifier, the true rms value of the ac signal can be measured independently.
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