042-Fundamentals-of-Physics-II-Electromagnetism-Optics-and-Quantum-Mechanics-R.-Shankar-Edisi-1-2016 · Problem 15.10.2

Electromagnetism and Relativity

Physics — Shankar · lorentz-force-four-vector-verification

Problem

Verify using Eqn. 15.203 that for μ=x,y,z\mu = x, y, z one recovers the Lorentz force, and for μ=0\mu = 0 one recovers the power delivered to the charge qq.
Intuitive explanation

The four-force in relativity unifies the spatial Lorentz force and energy transfer into a single four-vector. Equation 15.203 expresses this four-force in terms of the electromagnetic field tensor and four-velocity—when you extract its spatial components (μ=x,y,z\mu = x, y, z), you'll see the familiar F=q(E+v×B)\mathbf{F} = q(\mathbf{E} + \mathbf{v} \times \mathbf{B}), and when you look at the time component (μ=0\mu = 0), the power P=qE⋅vP = q\mathbf{E} \cdot \mathbf{v} emerges naturally. This problem asks you to verify that relativity's unified framework correctly reproduces both classical results.

Intuitive explanation

The four-force in relativity unifies the spatial Lorentz force and energy transfer into a single four-vector. Equation 15.203 expresses this four-force in terms of the electromagnetic field tensor and four-velocity—when you extract its spatial components (μ=x,y,z\mu = x, y, z), you'll see the familiar F=q(E+v×B)\mathbf{F} = q(\mathbf{E} + \mathbf{v} \times \mathbf{B}), and when you look at the time component (μ=0\mu = 0), the power P=qE⋅vP = q\mathbf{E} \cdot \mathbf{v} emerges naturally. This problem asks you to verify that relativity's unified framework correctly reproduces both classical results.

Related theory

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