

A moving coil galvanometer is an instrument used for detection and measurement of small electric currents.
The concave or cylindrical pole pieces ensure that the plane of coil is parallel to B thus (cosq = 1 and sina = 1) in the expression t = NIBA cosqand t = NIBA sina .
The whole arrangement is enclosed in non-magnetic case, which is provided with leveling screws. The torsion head is connected to terminal T1. The galvanometer can be connected to the circuit through terminals T1 and T2.
t = NIBA sina
Since the magnified field is radial the plane of the coil is parallel to the magnetic field
such that a = 90o and hence t = NIBA.
The coil rotates and the phosphor bronze strip gets twisted. As a result a restoring torque comes into play trying to restore the coil back to original position.
If f be the twist produced in the strip and C be the restoring torque per unit twist then the restoring torque = Cf.
In equilibrium,

where G is the galvanometer constant.

This shows that galvanometer has a linear scale and detects the presence of current.

The following diagram shows two spiral springs which control how far the coil turns and are made from very fine hair springs which have a weak unwinding effect. The pointer sometimes moves over a scale with evenly spaced graduations or the scale is replaced by a small mirror which deflects a ray of light falling on it.

