Working of true RMS meter
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In a DC amplifier, two thermocouples form the part of the bridge in the input circuit. The input voltage is then amplified and given to the thermocouple's heating element. The heat produced by the wire is sensed using a measuring thermocouple that will produce DC voltage proportional to it. The DC voltage upsets the bridge balance. DC amplifier, amplifies the unbalanced voltage and is given to the heating element. When these two thermocouples produce the same output voltage, the reestablishment of the bridge occurs. Now the feedback thermocouple’s heating element is proportional to the AC current within the input thermocouple i.e, the RMS value of input AC signal is proportional to the DC.
DC value is indicated by metre moment in the output circuitIn the output circuit, meter moment indicates the DC value. A frequent limitation of the utility of the RMS respond voltmeter for the measuring highly nonlinear wave forms
A typical laboratory type RMS responding voltmeter has a crush factor of 10/1 (10:1). At 10% of full scale deflection it can go as high as 100/1. The crest factor of a waveform is the ratio of its peak value to the RMS value. The crest factor of a pure sine wave is 1.414 but non-sinusoidal waveforms can have much larger crest factors. The RMS level of waveforms with a crest factor of 2 or 3 can be determined by most RMS measuring instruments. Waveforms with higher crush factors are more difficult to measure. The maximum waveform crest factors is usually specified for all RMS measuring instrument.
The need for the two RMS metres has grown as possibility of non sinusoidal waves in the circuits has greatly increased in recent years.
Eg:- variable speed motor drives
Electronic ballasts
Computers
HVAC
Solid state environments
True RMS is the only AC voltage reading that does not depend on the shape of the signal which means it often is the most useful measurement for the real world waveforms.
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