Animated Solution for Physics - Magnetic Effects of Current: A circular coil having N turns and radius r carries a current I. It is held in the XZ-plane in a magnetic field Bi^. The torque on the coil due to the magnetic field (in N-m) is
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Visualized Solution
Visualizing the Setup
Coil is in the XZ-plane.
Current =I
Radius =r
Turns =N
Magnetic Moment Concept
Magnetic moment, m=NIA
Area, A=πr2
Direction of A is ⊥ to XZ-plane ⇒j^
Vector Form of Magnetic Moment
m=NI(πr2)j^
External Magnetic Field
Magnetic field, B=Bi^
Torque Formula
Torque, τ=m×B
Calculating the Cross Product
τ=(NIπr2j^)×(Bi^)
τ=NIπr2B(j^×i^)
τ=−NIπr2Bk^
Magnitude of Torque
Magnitude of torque, ∣τ∣=Bπr2IN
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The Sigma Insight: Magnetic Moment of Current Loop
Solution Diagram
Visualizing the Setup
Imagine a circular coil placed flat in the XZ-plane. Let's establish our 3D coordinate system first, and then place the coil right there. We'll assume the current I flows in the anti-clockwise direction when viewed from the positive Y-axis. The coil has a radius r and consists of N turns.
The Magnetic Moment
Any current-carrying coil acts like a tiny magnet. Its strength is given by its magnetic moment, m. The formula is very simple: the number of turns, multiplied by the current, multiplied by the area of the coil.
m=NIA
And its direction? We use the right-hand thumb rule! Curl your fingers along the direction of the current, and your thumb points along the positive Y-axis. Since the area of a circle is πr2, we can write the exact vector form for the magnetic moment:
m=NI(πr2)j^
The External Field and Torque
Now, the question states that this coil is bathed in a uniform magnetic field. The field B is directed along the positive X-axis, which is represented by i^.
B=Bi^
When a magnetic dipole is placed in an external magnetic field, it experiences a twisting force, a torque. The formula for this torque is the cross product of the magnetic moment vector and the magnetic field vector.
τ=m×B
The Final Calculation
Let's plug in our vectors. We need to take the cross product of NIπr2j^ with Bi^.
τ=(NIπr2j^)×(Bi^)
Remember your cross products? j^×i^ gives us −k^.
τ=NIπr2B(j^×i^)
τ=−NIπr2Bk^
This means the torque acts along the negative Z-axis, trying to flip the coil! However, the question asks for the magnitude of this torque. We just drop the direction vector and the negative sign.