By S. Hussain Ather, Updated Mar 24, 2022
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The ammeter is the standard instrument for measuring electrical current, the SI unit of which is the ampere. Understanding its operation is essential for accurate circuit analysis.
Ammeters determine current by passing the flow through a coil with very low resistance and inductive reactance, creating minimal impedance. This design ensures that the meter does not disturb the circuit it is measuring.
In a moving‑coil ammeter, the current generates a magnetic field that opposes the fixed field produced by permanent magnets. The resulting torque moves a calibrated armature over a scale, displaying the current in amperes.
To measure current, an ammeter must be connected in series with the load. Its low internal resistance means it draws negligible power, preserving the circuit’s operation. Connecting it in parallel would short‑circuit the circuit, redirecting most current through the meter.
A galvanometer is a sensitive detector that can sense tiny currents and their direction. It relies on a magnetic field to convert current into a mechanical displacement. While highly precise, a galvanometer’s range is limited, and it typically measures only direct current (DC).
Ammeters extend the galvanometer’s principle. DC ammeters employ the moving‑coil method, whereas AC ammeters measure the deflection caused by the time‑varying magnetic field acting on a piece of iron. Consequently, ammeters can handle both AC and DC.
To adapt a galvanometer to larger currents, it is placed in parallel with a small shunt resistor. The shunt diverts most of the current away from the galvanometer, allowing only a fraction to pass through it. The shunt protects the galvanometer from damage and enables accurate readings of high currents.
Let G be the galvanometer resistance and Ig the maximum current for full‑scale deflection. For a total current I, the shunt resistance S is calculated as:
S = (Ig · G) / (I – Ig)
The effective resistance of the combined ammeter is:
Reff = (G · S) / (G + S)