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Question #43381

Difficulty: 8/10 | 🟢 Free

The Question

An infinitely long straight wire carries a steady current II in the positive zz-direction. The wire is kept parallel to the zz-axis and is undergoing constant acceleration aa along the positive xx-axis. At time t=0t=0, the wire passes through the origin (x=0,y=0x=0, y=0) with an instantaneous velocity v0i^v_0 \hat{i}. At this exact instant (t=0t=0), a point charge +q+q of mass mm is located at (d,0,0)(d, 0, 0) and is moving with velocity v⃗p=ui^+uj^\vec{v}_p = u \hat{i} + u \hat{j}. Assuming v0≪cv_0 \ll c such that the quasi-static approximation is valid (ignoring radiation effects), what is the instantaneous electromagnetic force vector on the particle at t=0t=0?

Options

  • A.

    μ0qIu2πdk^\frac{\mu_0 q I u}{2\pi d} \hat{k}

  • B.

    μ0qI(u−v0)2πdk^\frac{\mu_0 q I (u - v_0)}{2\pi d} \hat{k}

  • C.

    μ0qI(u+v0)2πdk^\frac{\mu_0 q I (u + v_0)}{2\pi d} \hat{k}

  • D.

    −μ0qIv02πdk^-\frac{\mu_0 q I v_0}{2\pi d} \hat{k}

Check Your Answer

Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Lorentz Force Vector Direction|Magnetic Flux Scalar Sign|Derived Units via Fundamental Constants

Why This Question Is Tricky

Common Mistakes

This question tests the student's understanding of the Lorentz force in the context of a non-inertial, moving current source.

The primary trap is calculating only the magnetic force F⃗m=q(v⃗×B⃗)\vec{F}_m = q(\vec{v} \times \vec{B}) using the instantaneous Biot-Savart field, which leads directly to Option A.

Students often fail to recognize that a moving magnetic field source generates an induced electric field (via Faraday's Law, ∇×E⃗=−∂B⃗/∂t\nabla \times \vec{E} = -\partial \vec{B}/\partial t) in the lab frame.

By applying the low-velocity field transformation E⃗=−v⃗source×B⃗\vec{E} = -\vec{v}_{source} \times \vec{B}, the problem reveals that the total electromagnetic force depends on the relative velocity between the charge and the source.

This is a profound relativistic concept that manifests even at non-relativistic speeds, forcing students to look beyond simple static formulas.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterMoving Charges and Magnetism - Class 12
ConceptLorentz Force Vector Direction
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree