Moving Coil Galvanometer — Working Principle

medium CBSE JEE-MAIN NEET 2024 4 min read

Question

A rectangular coil of 50 turns, area 2×1042 \times 10^{-4} m², carrying a current of 1 mA, is placed in a uniform magnetic field of 0.1 T. The spring constant of the suspension is 2×1062 \times 10^{-6} N·m/rad. Find the deflection of the galvanometer and its current sensitivity.


Solution — Step by Step

The net torque on the current-carrying coil in a radial magnetic field is:

τ=nBIA\tau = nBIA

where nn = number of turns, BB = magnetic field, II = current, AA = area of coil. The radial field design ensures sinθ=1\sin\theta = 1 always — this is why deflection stays linear with current.

Substituting values:

τ=50×0.1×1×103×2×104\tau = 50 \times 0.1 \times 1 \times 10^{-3} \times 2 \times 10^{-4} τ=1×106 N⋅m\tau = 1 \times 10^{-6} \text{ N·m}

At equilibrium, deflecting torque = restoring torque:

nBIA=kθnBIA = k\theta

where kk is the spring constant (also called torsion constant or restoring couple per unit twist). So:

θ=nBIAk=1×1062×106=0.5 rad\theta = \frac{nBIA}{k} = \frac{1 \times 10^{-6}}{2 \times 10^{-6}} = 0.5 \text{ rad}

Current sensitivity is defined as deflection per unit current:

SI=θI=nBAkS_I = \frac{\theta}{I} = \frac{nBA}{k} SI=50×0.1×2×1042×106=1032×106=500 rad/AS_I = \frac{50 \times 0.1 \times 2 \times 10^{-4}}{2 \times 10^{-6}} = \frac{10^{-3}}{2 \times 10^{-6}} = 500 \text{ rad/A}

Final answers: Deflection θ=0.5\theta = 0.5 rad; Current sensitivity =500= 500 rad/A


Why This Works

The key design feature of a moving coil galvanometer is the radial magnetic field created by a cylindrical soft iron core placed inside the coil. Because the field is always parallel to the plane of the coil at every angle, the torque τ=nBIAsinθ\tau = nBIA\sin\theta reduces to τ=nBIA\tau = nBIA throughout the rotation. Without this, the relationship between current and deflection would be non-linear and calibration would be impossible.

The phosphor bronze suspension wire provides the restoring torque. A softer wire (smaller kk) gives more deflection for the same current — that’s why high-sensitivity galvanometers use very fine suspension fibres. This trade-off between sensitivity and ruggedness is a real design constraint, and NEET/JEE love asking questions about what happens to sensitivity when you change nn, BB, AA, or kk.

τdeflecting=nBIA(radial field)\tau_{deflecting} = nBIA \quad \text{(radial field)} τrestoring=kθ\tau_{restoring} = k\theta At equilibrium: θ=nBIAk\text{At equilibrium: } \theta = \frac{nBIA}{k} Current Sensitivity=θI=nBAk\text{Current Sensitivity} = \frac{\theta}{I} = \frac{nBA}{k} Voltage Sensitivity=θV=nBAkRg\text{Voltage Sensitivity} = \frac{\theta}{V} = \frac{nBA}{kR_g}

Alternative Method — Using Voltage Sensitivity

If the question gives terminal voltage VV across the galvanometer instead of current:

Since I=V/RgI = V/R_g, the voltage sensitivity is:

SV=θV=nBAkRgS_V = \frac{\theta}{V} = \frac{nBA}{kR_g}

Note the inverse dependence on RgR_g. Increasing current sensitivity by increasing nn does NOT necessarily increase voltage sensitivity — more turns means higher resistance RgR_g, so the two effects partially cancel. This specific insight appeared in JEE Main 2024 Shift 1.


Common Mistake

Students often try to improve voltage sensitivity the same way as current sensitivity — by increasing the number of turns nn. But voltage sensitivity =nBA/(kRg)= nBA/(kR_g), and RgnR_g \propto n (more turns = more wire = higher resistance). So doubling nn doubles both numerator and denominator — voltage sensitivity stays the same. Current sensitivity improves, voltage sensitivity doesn’t. Boards and NEET have both tested this distinction explicitly.

To convert a galvanometer into an ammeter: connect a low resistance shunt S=IgRgIIgS = \frac{I_g R_g}{I - I_g} in parallel.

To convert into a voltmeter: connect a high resistance R=VIgRgR = \frac{V}{I_g} - R_g in series.

The galvanometer’s full-scale deflection current IgI_g is the key starting value for both conversions — always identify it first.

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