Although an analog moving-coil meter may lack the resolution and accuracy that a digital readout provides, a meter remains the display of choice for certain applications. A digital readout simply cannot provide information about a measurement's rate of change, and tracking a reading's trend is easier on an analog meter.
Large moving-coil meters may require significant amounts of current for full-scale deflection, and using a shunt resistor may prove impractical when the meter current is larger than the current you are measuring. You can solve the problem by driving the meter from a separate power supply (Figure 1). In this example, an 8-in. moving-coil meter that requires 15 mA for full-scale deflection displays a current range of 0 to 1 A dc. This technique can also simplify specifying or fabricating shunt resistors for custom current ranges. In operation, IC1 's output current, IOUT, equals VSENSE/100 Ω, where VSENSE is the voltage across RSENSE1.
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| Figure 1. | This circuit allows use of a moving-coil meter in applications for which the meter current is a substantial fraction of the current being measured. |
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This Design Idea uses IC1 rather than the many current-sense amplifiers available because it provides a separate supply-voltage terminal for the internal circuitry, whereas other devices take power from the current you are measuring. In this application, a full-scale current of 1 A develops 1 V across RSENSE1, which IC1 converts to a maximum output current of 10 mA that produces a maximum voltage of 1 V across R1. Operational amplifier IC2 and transistor Q1 form a voltage-controlled current sink that draws current through meter M1. A full-scale reading of 15 mA develops 1 V across 66 Ω resistor RSENSE2. You can adjust the resistor's value to calibrate the meter or to alter the full-scale current range.
This circuit also allows separation of the measurement point and meter location. Moving-coil meters are not intended for applications that require precision measurement, and you can use relaxed-accuracy passive components. Bypass the instrument-supply voltage with decoupling capacitors that the electrical-noise environment requires.
