String Waves and Matter Waves — Question 7

Section 39-1 · Physics pages 6424–6425

Question 7 Two measured wave numbers reveal whether the evolution is dispersive Two narrow matter-wave components have wave numbers k and 2k, both positive, with ω = ℏk2/(2m). For comparison a string has ω = vk. Define a two-component envelope speed as ∆ω/∆k. k ω Schematic; labels, not drawing lengths, specify the data. (a) Find that envelope speed for the matter wave. (b) Compare it with the group velocity at the midpoint wave number and with the string envelope speed.
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Question 7 - Solution Two measured wave numbers reveal whether the evolution is dispersive k ω (a) Method and calculation ∆ω = ℏ 2m[(2k)2 −k2] = 3ℏk2 2m , ∆k = k. venv = 3ℏk/(2m) . (b) Interpretation and further calculation kc = 3k/2 : vg(kc) = dω dk kc = 3ℏk/(2m) . ωs = vk ⇒∆ωs/∆k = v . Physical check For a quadratic dispersion the secant slope equals the tangent slope at the midpoint. This equality would not hold exactly for an arbitrary dispersion law.

Question 7

Two measured wave numbers reveal whether the evolution is dispersive

Two narrow matter-wave components have wave numbers k and 2k2k, both positive, with ω=ℏk2/(2m)\omega=\hbar k^2/(2m). For comparison a string has ω=vk\omega=vk. Define a two-component envelope speed as Δω/Δk\Delta\omega/\Delta k.

Diagram shown in the original SVG worksheet.

  1. Find that envelope speed for the matter wave.

  2. Compare it with the group velocity at the midpoint wave number and with the string envelope speed.

Question 7 - Solution

Two measured wave numbers reveal whether the evolution is dispersive

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δω=ℏ2m[(2k)2−k2]=3ℏk22m,Δk=k.\Delta\omega=\frac{\hbar}{2m}[(2k)^2-k^2]=\frac{3\hbar k^2}{2m},\quad\Delta k=k.venv=3ℏk/(2m).\boxed{v_{\mathrm{env}}=3\hbar k/(2m)}.

(b) Interpretation and further calculation

kc=3k/2:vg(kc)=dωdk|kc=3ℏk/(2m).k_c=3k/2:\quad\boxed{v_g(k_c)=\left.\frac{d\omega}{dk}\right|_{k_c}=3\hbar k/(2m)}.ωs=vk⇒Δωs/Δk=v.\omega_s=vk\Rightarrow\boxed{\Delta\omega_s/\Delta k=v}.

Physical check

For a quadratic dispersion the secant slope equals the tangent slope at the midpoint. This equality would not hold exactly for an arbitrary dispersion law.