A New Look at Energy — Question 3

Section 37-11 · Physics pages 6236–6237

Question 3 The first correction to classical kinetic energy is quartic in speed For a massive particle, K = (γ −1)mc2, with γ = (1 −β2)−1/2 and β = v/c. β K/(mc2) Schematic; labels, not drawing lengths, specify the data. (a) Expand K through order β4. (b) At v = 0.60c, compare the exact, classical and quartic-approximation energies, all in units of mc2.
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Question 3 - Solution The first correction to classical kinetic energy is quartic in speed β K/(mc2) (a) Method and calculation γ = 1 + 1 2β2 + 3 8β4 + O(β6). K = 1 2mv2 + 3 8mv4/c2 + O(mv6/c4) . (b) Interpretation and further calculation Kexact/mc2 = .2500 , Kcl/mc2 = .1800 , K4/mc2 = .2286 . Kexact −Kcl Kexact = .28 , Kexact −K4 Kexact = .0856 . Physical check The quartic term improves the approximation, but beta 0.60 is large enough that higher terms are still visible.

Question 3

The first correction to classical kinetic energy is quartic in speed

For a massive particle, K=(γ−1)mc2K=(\gamma-1)mc^2, with γ=(1−β2)−1/2\gamma=(1-\beta^2)^{-1/2} and β=v/c\beta=v/c.

Diagram shown in the original SVG worksheet.

  1. Expand K through order β4\beta^4.

  2. At v=0.60cv=0.60c, compare the exact, classical and quartic-approximation energies, all in units of mc2mc^2.

Question 3 - Solution

The first correction to classical kinetic energy is quartic in speed

Diagram shown in the original SVG worksheet.

(a) Method and calculation

γ=1+12β2+38β4+O(β6).\gamma=1+\tfrac12\beta^2+\tfrac38\beta^4+O(\beta^6).K=12mv2+38mv4/c2+O(mv6/c4).\boxed{K=\tfrac12mv^2+\tfrac38mv^4/c^2+O(mv^6/c^4)}.

(b) Interpretation and further calculation

Kexact/mc2=.2500,Kcl/mc2=.1800,K4/mc2=.2286.\boxed{K_{\mathrm{exact}}/mc^2=.2500},\quad\boxed{K_{\mathrm{cl}}/mc^2=.1800},\quad\boxed{K_4/mc^2=.2286}.Kexact−KclKexact=.28,Kexact−K4Kexact=.0856.\frac{K_{\mathrm{exact}}-K_{\mathrm{cl}}}{K_{\mathrm{exact}}}=\boxed{.28},\qquad\frac{K_{\mathrm{exact}}-K_4}{K_{\mathrm{exact}}}=\boxed{.0856}.

Physical check

The quartic term improves the approximation, but beta 0.60 is large enough that higher terms are still visible.