A New Look at Momentum — Question 4

Section 37-10 · Physics pages 6218–6219

Question 4 Parallel and transverse forces produce different acceleration responses At one instant a particle has velocity v and acceleration a. Differentiate p = γmv, using dγ/dt = γ3v · a/c2. v F∥ F⊥ Schematic; labels, not drawing lengths, specify the data. (a) Derive the force components parallel and perpendicular to the velocity. (b) At v = 0.80c, compare the acceleration magnitudes caused by equal-magnitude purely parallel and purely transverse forces.
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Question 4 - Solution Parallel and transverse forces produce different acceleration responses v F∥ F⊥ (a) Method and calculation F = γma + γ3mv · a c2 v. F∥= γ3ma∥, F⊥= γma⊥. (b) Interpretation and further calculation |F∥| = |F⊥| : |a⊥| |a∥| = γ2. |a⊥|/|a∥| = 25/9 . Physical check The invariant mass is unchanged. The different responses arise from differentiating a velocity-dependent momentum.

Question 4

Parallel and transverse forces produce different acceleration responses

At one instant a particle has velocity 𝒗\mathbf v and acceleration 𝒂\mathbf a. Differentiate 𝒑=γm𝒗\mathbf p=\gamma m\mathbf v, using dγ/dt=γ3𝒗⋅𝒂/c2d\gamma/dt=\gamma^3\mathbf v\cdot\mathbf a/c^2.

Diagram shown in the original SVG worksheet.

  1. Derive the force components parallel and perpendicular to the velocity.

  2. At v=0.80cv=0.80c, compare the acceleration magnitudes caused by equal-magnitude purely parallel and purely transverse forces.

Question 4 - Solution

Parallel and transverse forces produce different acceleration responses

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑭=γm𝒂+γ3m𝒗⋅𝒂c2𝒗.\mathbf F=\gamma m\mathbf a+\gamma^3m\frac{\mathbf v\cdot\mathbf a}{c^2}\mathbf v.F∥=γ3ma∥,F⟂=γma⟂.\boxed{F_\parallel=\gamma^3ma_\parallel},\qquad\boxed{F_\perp=\gamma ma_\perp}.

(b) Interpretation and further calculation

|F∥|=|F⟂|:|a⟂||a∥|=γ2.|F_\parallel|=|F_\perp|:\quad\frac{|a_\perp|}{|a_\parallel|}=\gamma^2.|a⟂|/|a∥|=25/9.\boxed{|a_\perp|/|a_\parallel|=25/9}.

Physical check

The invariant mass is unchanged. The different responses arise from differentiating a velocity-dependent momentum.