Talha's Physics Academy
Torque on a Rectangular Coil and Working of DC Motor
Torque on a Current-Carrying Rectangular Coil
Consider a rectangular coil placed in a uniform magnetic field of strength $B$ such that it is free to rotate about an axis. When a current $I$ flows through the coil, perpendicular forces of magnitude $F = BIL$ act on the opposing conductor arms, creating a couple.
Mathematical Derivation
The basic torque ($\tau$) produced by the couple is given by the product of the force and the perpendicular distance between their lines of action:
$$\tau = F \times \text{width}$$
Since $F = BIL$ and $L \times \text{width} = A$ (area of the coil), the maximum torque when the plane of the coil is parallel to the field is:
$$\tau = BIA$$
If the plane of the coil makes an angle $\alpha$ with the magnetic field $B$, the effective perpendicular distance is reduced by a factor of $\cos\alpha$:
$$\tau = BIA \cos\alpha$$
If the coil consists of $N$ turns, the total torque is multiplied by $N$:
$$\tau = NIAB \cos\alpha$$
Note: The torque is maximum when the plane of the coil is parallel to the magnetic field ($\alpha = 0^\circ$), and zero when the plane is perpendicular to the field ($\alpha = 90^\circ$).
Working Principle of a D.C. Motor
In terms of construction, a D.C. motor is structurally similar to a D.C. generator, but it operates in reverse: electrical energy is supplied as input to produce mechanical rotation as output.
Turning Effect in a D.C. Motor
The operation relies directly on the turning effect experienced by a current-carrying coil in a magnetic field:
- Sides Parallel to Field ($BC$ and $DA$): These sides carry current in directions parallel to the magnetic field lines, so no magnetic force is exerted on them.
- Sides Perpendicular to Field ($AB$ and $CD$): These sides experience equal and opposite magnetic forces whose directions can be determined using Fleming's Left-Hand Rule or the Right-Hand Slap Rule.
- Couple Formation: The opposing forces on sides $AB$ and $CD$ form a couple, generating a continuous turning effect that rotates the coil. These forces arise from the combination of the current's magnetic field and the external permanent magnetic field, creating resultant catapult fields around the coil.

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