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Exercises · 4.5

Q.What is the magnitude of magnetic force per unit length on a wire carrying a current of 8 A8\ \text{A} and making an angle of 30∘30^\circ with the direction of a uniform magnetic field of 0.15 T0.15\ \text{T}?

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The magnetic force per unit length on a current-carrying wire depends on the current, the magnetic field, and the sine of the angle between them. Using F/L=IBsin⁡θF/L = I B \sin\theta, the answer is 0.6 N/m0.6\ \text{N/m}.

The core idea here is that a magnetic field exerts a force on a moving charge — and since current in a wire is just a stream of moving charges, the wire itself experiences a force. But the force is not simply IBLI B L; it depends on the orientation of the wire relative to the field. Only the component of the current perpendicular to the magnetic field contributes to the force. That’s why the sine of the angle appears.

Let’s work through it step by step.

  1. Recall the formula for magnetic force on a straight current-carrying wire. When a wire of length LL carries a current II in a uniform magnetic field BB, the magnitude of the magnetic force is:

F=ILBsin⁡θF = I L B \sin\theta

where θ\theta is the angle between the direction of the current and the magnetic field vector.

This formula comes directly from the Lorentz force law: F=qvBsin⁡θF = q v B \sin\theta, summed over all moving charges in the wire.

  1. We need force per unit length, so divide both sides by LL:

FL=IBsin⁡θ\frac{F}{L} = I B \sin\theta

  1. Plug in the given values. Current I=8 AI = 8\ \text{A}, magnetic field B=0.15 TB = 0.15\ \text{T}, and angle θ=30∘\theta = 30^\circ. So:

FL=(8 A)×(0.15 T)×sin⁡30∘\frac{F}{L} = (8\ \text{A}) \times (0.15\ \text{T}) \times \sin 30^\circ

  1. Evaluate sin⁡30∘\sin 30^\circ.

    From trigonometry, sin⁡30∘=12=0.5\sin 30^\circ = \frac{1}{2} = 0.5.

  2. Calculate the product: …

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