String Waves and Matter Waves — Question 1

Section 39-1 · Physics pages 6412–6413

Question 1 The same spatial boundary condition produces different frequency ladders A string of wave speed v and a nonrelativistic particle of mass m occupy 0 < x < L with zero displacement or wave function at both ends. Their dispersions are ωs = vk and ωm = ℏk2/(2m). x 0 L Schematic; labels, not drawing lengths, specify the data. (a) Derive the allowed wave numbers and wavelengths. (b) Compare the ratios of second-mode to first-mode angular frequencies.
Show solutionHide solution
Question 1 - Solution The same spatial boundary condition produces different frequency ladders x 0 L (a) Method and calculation ψ = A sin kx + B cos kx, ψ(0) = 0 ⇒B = 0. sin kL = 0 ⇒kn = nπ/L, λn = 2L/n , n ≥1. (b) Interpretation and further calculation ωs,n = vnπ/L ⇒ωs,2/ωs,1 = 2 . ωm,n = ℏn2π2/(2mL2) ⇒ωm,2/ωm,1 = 4 . Physical check Boundary conditions select spatial modes. The dynamical dispersion relation determines how those modes evolve in time.

Question 1

The same spatial boundary condition produces different frequency ladders

A string of wave speed v and a nonrelativistic particle of mass m occupy 0<x<L0<x<L with zero displacement or wave function at both ends. Their dispersions are ωs=vk\omega_s=vk and ωm=ℏk2/(2m)\omega_m=\hbar k^2/(2m).

Diagram shown in the original SVG worksheet.

  1. Derive the allowed wave numbers and wavelengths.

  2. Compare the ratios of second-mode to first-mode angular frequencies.

Question 1 - Solution

The same spatial boundary condition produces different frequency ladders

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ψ=Asin⁡kx+Bcos⁡kx,ψ(0)=0⇒B=0.\psi=A\sin kx+B\cos kx,\quad\psi(0)=0\Rightarrow B=0.sin⁡kL=0⇒kn=nπ/L,λn=2L/n,n≥1.\sin kL=0\Rightarrow\boxed{k_n=n\pi/L,\quad\lambda_n=2L/n},\ n\ge1.

(b) Interpretation and further calculation

ωs,n=vnπ/L⇒ωs,2/ωs,1=2.\omega_{s,n}=vn\pi/L\Rightarrow\boxed{\omega_{s,2}/\omega_{s,1}=2}.ωm,n=ℏn2π2/(2mL2)⇒ωm,2/ωm,1=4.\omega_{m,n}=\hbar n^2\pi^2/(2mL^2)\Rightarrow\boxed{\omega_{m,2}/\omega_{m,1}=4}.

Physical check

Boundary conditions select spatial modes. The dynamical dispersion relation determines how those modes evolve in time.