Torque on Current Loop — Explained

On this page

1. 1. Conceptual Foundation: Force on a Current-Carrying Conductor
2. 2. Key Principles and Derivation for a Rectangular Loop
3. 3. Magnetic Dipole Moment
4. 4. Potential Energy of a Magnetic Dipole in a Magnetic Field
5. 5. Real-World Applications
6. 6. Common Misconceptions
7. 7. NEET-Specific Angle

Detailed Explanation

The concept of torque on a current loop is a cornerstone of electromagnetism, explaining the operation of numerous devices from electric motors to galvanometers. It fundamentally arises from the Lorentz force acting on individual charge carriers within the current-carrying conductors that form the loop.

1. Conceptual Foundation: Force on a Current-Carrying Conductor

Before delving into torque, we must recall the force experienced by a current-carrying conductor in a magnetic field. The Lorentz force law states that a charge $q$ moving with velocity $\vec{v}$ in a magnetic field $\vec{B}$ experiences a force $\vec{F} = q(\vec{v} \times \vec{B})$.

For a current-carrying wire, which is essentially a collection of moving charges, this translates to a force on a segment of length $d\vec{l}$ carrying current $I$ as $d\vec{F} = I(d\vec{l} \times \vec{B})$.

The direction of $d\vec{l}$ is taken along the direction of current flow. The total force on a conductor is the integral of these elemental forces along its length.

2. Key Principles and Derivation for a Rectangular Loop

Consider a rectangular current loop PQRS of length $L$ (sides PS and QR) and width $b$ (sides PQ and RS), carrying a current $I$. Let this loop be placed in a uniform magnetic field $\vec{B}$. The area of the loop is $A = L \times b$. We'll analyze the forces on each side:

Side PQ (length $b$): — Current flows from P to Q. Let the angle between the normal to the plane of the loop and the magnetic field be $\theta$. The angle between the current element $d\vec{l}$ (along PQ) and $\vec{B}$ is $(90^\circ - \theta)$. The force on PQ, $\vec{F}_{PQ}$, will be $F_{PQ} = I b B \sin(90^\circ - \theta) = I b B \cos\theta$. Using the right-hand rule (or Fleming's left-hand rule), if current is along +y and B is in x-z plane, the force will be perpendicular to both. However, a simpler approach for torque is to consider the forces on the sides parallel to the axis of rotation.

Side RS (length $b$): — Current flows from R to S, opposite to PQ. The angle between $d\vec{l}$ (along RS) and $\vec{B}$ is $(90^\circ + \theta)$. The force on RS, $\vec{F}_{RS}$, will be $F_{RS} = I b B \sin(90^\circ + \theta) = I b B \cos\theta$. This force is equal in magnitude to $\vec{F}_{PQ}$ but acts in the opposite direction. Crucially, these two forces are collinear and cancel each other out, contributing nothing to the net force or torque.

Side QR (length $L$): — Current flows from Q to R. The current direction is perpendicular to the magnetic field $\vec{B}$ (assuming $\vec{B}$ is in the plane of the loop, or more generally, the component of $\vec{B}$ perpendicular to QR). The force on QR, $\vec{F}_{QR}$, has magnitude $F_{QR} = I L B \sin(90^\circ) = I L B$. By the right-hand rule, if current is along +x, and $\vec{B}$ is along +z, then $\vec{F}_{QR}$ is along -y (downwards).

Side SP (length $L$): — Current flows from S to P, opposite to QR. The force on SP, $\vec{F}_{SP}$, has magnitude $F_{SP} = I L B$. By the right-hand rule, $\vec{F}_{SP}$ is along +y (upwards).

Now, let's consider the torque. The forces $\vec{F}_{PQ}$ and $\vec{F}_{RS}$ cancel out. The forces $\vec{F}_{QR}$ and $\vec{F}_{SP}$ are equal in magnitude ($ILB$) and opposite in direction. They act on opposite sides of the loop. If the loop is free to rotate about an axis passing through the midpoints of sides PQ and RS, these two forces form a couple.

Let the axis of rotation be along the x-axis. The forces $\vec{F}_{QR}$ and $\vec{F}_{SP}$ act at a perpendicular distance from this axis. The perpendicular distance from the axis of rotation to the line of action of each force is $(b/2) \sin\theta$.

(Here, $\theta$ is the angle between the normal to the loop's plane and the magnetic field $\vec{B}$. When the plane of the loop makes an angle $\alpha$ with $\vec{B}$, then $\theta = 90^\circ - \alpha$.

The perpendicular distance from the axis to the force line is $(b/2) \cos\alpha = (b/2) \sin\theta$).

The torque due to $\vec{F}_{QR}$ is $\tau_{QR} = F_{QR} \times (b/2) \sin\theta = (ILB) (b/2) \sin\theta$. The torque due to $\vec{F}_{SP}$ is $\tau_{SP} = F_{SP} \times (b/2) \sin\theta = (ILB) (b/2) \sin\theta$.

Both torques tend to rotate the loop in the same direction (e.g., clockwise). So, the total torque is: $\tau = \tau_{QR} + \tau_{SP} = ILB (b/2) \sin\theta + ILB (b/2) \sin\theta = ILB b \sin\theta$.

3. Magnetic Dipole Moment

This expression can be simplified by introducing the concept of magnetic dipole moment, $\vec{M}$. For a current loop, the magnitude of the magnetic dipole moment is defined as $M = NIA$, where $N$ is the number of turns, $I$ is the current, and $A$ is the area of the loop.

The direction of $\vec{M}$ is given by the right-hand rule: curl your fingers in the direction of the current, and your thumb points in the direction of $\vec{M}$. This direction is perpendicular to the plane of the loop, pointing along its normal.

Using the magnetic dipole moment, the torque equation can be written in vector form as:

$$\vec{\tau} = \vec{M} \times \vec{B}$$

This vector form clearly shows that the torque is maximum when $\vec{M}$ is perpendicular to $\vec{B}$ (i.

e., $\theta = 90^\circ$, meaning the plane of the loop is parallel to $\vec{B}$), and zero when $\vec{M}$ is parallel or anti-parallel to $\vec{B}$ (i.e., $\theta = 0^\circ$ or $180^\circ$, meaning the plane of the loop is perpendicular to $\vec{B}$).

The torque always tries to align $\vec{M}$ with $\vec{B}$.

4. Potential Energy of a Magnetic Dipole in a Magnetic Field

The work done by an external agent to rotate the loop from an initial angle $\theta_1$ to a final angle $\theta_2$ is given by: $W = \int_{\theta_1}^{\theta_2} \tau_{ext} d\theta = \int_{\theta_1}^{\theta_2} MB \sin\theta d\theta = MB [-\cos\theta]_{\theta_1}^{\theta_2} = -MB (\cos\theta_2 - \cos\theta_1)$.

The potential energy $U$ of the magnetic dipole in the magnetic field is defined as the negative of the work done by the magnetic field in bringing the dipole from infinity (or a reference position where $U=0$) to its current position.

Conventionally, potential energy is taken as zero when $\vec{M}$ is perpendicular to $\vec{B}$ (i.e., $\theta = 90^\circ$). So, $U(\theta) - U(90^\circ) = - \int_{90^\circ}^{\theta} \tau d\theta = - \int_{90^\circ}^{\theta} MB \sin\theta d\theta = MB [\cos\theta]_{90^\circ}^{\theta} = MB (\cos\theta - \cos 90^\circ) = MB \cos\theta$.

Stable Equilibrium: — When $\theta = 0^\circ$, $U = -MB$ (minimum potential energy). Here, $\vec{M}$ is parallel to $\vec{B}$. The loop is in stable equilibrium, and the torque is zero.
Unstable Equilibrium: — When $\theta = 180^\circ$, $U = +MB$ (maximum potential energy). Here, $\vec{M}$ is anti-parallel to $\vec{B}$. The loop is in unstable equilibrium, and the torque is zero.

5. Real-World Applications

Electric Motors: — The continuous rotation of an electric motor is achieved by continuously reversing the direction of current in the coil (using a commutator) just as it passes the equilibrium position, ensuring that the torque always acts in the same rotational direction.
Moving Coil Galvanometer: — This device measures small currents. A coil is suspended in a radial magnetic field. The torque experienced by the coil is directly proportional to the current flowing through it. This torque is balanced by a restoring torque provided by a spring, leading to a deflection proportional to the current.

6. Common Misconceptions

Angle $\theta$: — Students often confuse the angle between the plane of the loop and the magnetic field with the angle $\theta$ used in $\tau = NIAB \sin\theta$. The angle $\theta$ in the formula is the angle between the magnetic dipole moment vector $\vec{M}$ (which is normal to the loop's plane) and the magnetic field vector $\vec{B}$. If the angle between the plane of the loop and $\vec{B}$ is $\alpha$, then $\theta = 90^\circ - \alpha$.
Net Force vs. Net Torque: — In a uniform magnetic field, the net force on a closed current loop is always zero. However, the net torque is generally non-zero, unless the magnetic moment is aligned with the field. In a non-uniform magnetic field, both net force and net torque can be non-zero.
Direction of Torque: — The direction of torque is given by the right-hand rule for cross products ($\vec{M} \times \vec{B}$). It is perpendicular to both $\vec{M}$ and $\vec{B}$.

7. NEET-Specific Angle

NEET questions often test the understanding of:

Formula application: — Direct calculation of torque given $N, I, A, B,$ and $\theta$.
Directional aspects: — Using the right-hand rule to determine the direction of $\vec{M}$ and subsequently $\vec{\tau}$.
Dependence on orientation: — Understanding when torque is maximum, minimum, or zero, and relating it to the angle $\theta$.
Equilibrium conditions: — Identifying stable and unstable equilibrium positions based on potential energy.
Comparison with force: — Differentiating between conditions for zero force and zero torque.
Effect of changing parameters: — How changing $I, A, B,$ or $N$ affects the torque.
Conceptual questions: — For example, what happens if the field is non-uniform? (In a non-uniform field, a current loop can experience a net force in addition to a torque, as the forces on opposite sides may not be equal and opposite.)
Relating to other topics: — Questions might combine torque with rotational dynamics (e.g., angular acceleration, moment of inertia) or with the working of galvanometers.

Often confused with

Side-by-side differences the NEET paper likes to test.

Torque on Current Loop vs Force on a Current Loop

Aspect	Torque on Current Loop	Force on a Current Loop
Definition	Torque on a Current Loop: The turning effect experienced by a current-carrying loop in a magnetic field, tending to rotate it.	Force on a Current Loop: The net translational push or pull experienced by a current-carrying loop in a magnetic field.
Cause	Caused by non-collinear forces acting on different segments of the loop.	Caused by the Lorentz force acting on individual charge carriers within the conductor segments.
Uniform Magnetic Field	Can be non-zero. $\tau = NIAB \sin\theta$.	Always zero. $\vec{F}_{net} = 0$ for a closed loop in a uniform field.
Non-uniform Magnetic Field	Can be non-zero.	Can be non-zero. A net force can exist if the field varies across the loop.
Effect	Causes rotation (angular acceleration).	Causes translation (linear acceleration).
Vector Representation	$\vec{\tau} = \vec{M} \times \vec{B}$	$\vec{F} = I \oint (d\vec{l} \times \vec{B})$ (which is zero for uniform B)
Alignment	Tends to align the magnetic dipole moment $\vec{M}$ with $\vec{B}$.	If non-zero, tends to move the loop towards regions of stronger magnetic field (for paramagnetic materials) or weaker field (for diamagnetic materials).

While both force and torque originate from the Lorentz force, their manifestations on a current loop differ significantly, especially in a uniform magnetic field. A current loop in a uniform magnetic field experiences a net force of zero, meaning it won't undergo translational motion.

However, the forces on its various segments can form a couple, leading to a net torque that causes rotational motion. This torque aims to align the loop's magnetic dipole moment with the external magnetic field.

In contrast, in a non-uniform magnetic field, a current loop can experience both a net force and a net torque.

Why it is tested: NEET relevance: Understanding the distinction between net force and net torque on a current loop is crucial for conceptual clarity. Questions often test this difference, especially regarding uniform versus non-uniform magnetic fields. It's fundamental to the working principles of electric motors (torque) and magnetic levitation (force in non-uniform fields).

Questions students ask

6 answered on this topic.

What is the primary condition for a current loop to experience torque in a magnetic field?

The primary condition is that the current loop must be placed in an external magnetic field, and its magnetic dipole moment vector must not be perfectly aligned or anti-aligned with the magnetic field vector. If the magnetic dipole moment $\vec{M}$ is parallel or anti-parallel to the magnetic field $\vec{B}$ (i.e., $\theta = 0^\circ$ or $180^\circ$), the torque will be zero. For any other orientation, a torque will act on the loop, tending to rotate it until $\vec{M}$ aligns with $\vec{B}$.

Why is the net force on a current loop in a uniform magnetic field zero, but the torque is not necessarily zero?

In a uniform magnetic field, for every segment of current-carrying wire in the loop, there is an equal and opposite segment (or combination of segments) experiencing an equal and opposite force. Therefore, the vector sum of all forces over the entire closed loop is zero.

However, these equal and opposite forces might not act along the same line of action. When forces form a 'couple' (equal, opposite, and non-collinear), they produce a net turning effect, or torque, even if the net translational force is zero.

How does the angle $\theta$ in the torque formula $\tau = NIAB \sin\theta$ relate to the orientation of the loop?

The angle $\theta$ in the formula $\tau = NIAB \sin\theta$ is the angle between the magnetic dipole moment vector $\vec{M}$ of the loop and the external magnetic field vector $\vec{B}$. The magnetic dipole moment vector $\vec{M}$ is defined as a vector perpendicular to the plane of the loop, with its direction determined by the right-hand rule (curl fingers in current direction, thumb points to $\vec{M}$).

Therefore, if the plane of the loop makes an angle $\alpha$ with the magnetic field, then $\theta = 90^\circ - \alpha$.

When is the torque on a current loop maximum and minimum?

The torque on a current loop is given by $\tau = NIAB \sin\theta$. It is maximum when $\sin\theta = 1$, which means $\theta = 90^\circ$. This occurs when the magnetic dipole moment vector $\vec{M}$ is perpendicular to the magnetic field $\vec{B}$, or equivalently, when the plane of the loop is parallel to the magnetic field.

The torque is minimum (zero) when $\sin\theta = 0$, which means $\theta = 0^\circ$ or $\theta = 180^\circ$. This occurs when $\vec{M}$ is parallel or anti-parallel to $\vec{B}$, meaning the plane of the loop is perpendicular to the magnetic field.

What is the significance of the magnetic dipole moment $\vec{M}$ in understanding torque on a current loop?

The magnetic dipole moment $\vec{M}$ simplifies the understanding and calculation of torque. It encapsulates the properties of the loop (number of turns $N$, current $I$, and area $A$) into a single vector quantity.

The torque can then be expressed elegantly as a vector cross product $\vec{\tau} = \vec{M} \times \vec{B}$. This formulation highlights that the torque's magnitude depends on the magnitudes of $\vec{M}$ and $\vec{B}$ and the sine of the angle between them, and its direction is perpendicular to both, tending to align $\vec{M}$ with $\vec{B}$.

Can a current loop experience a net force in a magnetic field?

Yes, but only if the magnetic field is non-uniform. In a uniform magnetic field, the net force on any closed current loop is always zero. However, if the magnetic field varies across the loop (i.e., it's non-uniform), the forces on different segments might not perfectly cancel out, leading to a net translational force in addition to a torque. This principle is used in some magnetic levitation systems.