Schrödinger's Equation — Question 1

Section 38-6 · Physics pages 6352–6353

Question 1 Substitution into the wave equation fixes the time evolution of a plane wave A particle of mass m moves in constant potential V0. Consider Ψ = Aei(kx−ωt). Use iℏ∂tΨ = −(ℏ2/2m)∂2 xΨ + V Ψ. x j Schematic; labels, not drawing lengths, specify the data. (a) Substitute the wave into the equation and determine ω. (b) Find its probability density and current, and check the continuity equation. The probability current is j = (ℏ/m) Im(Ψ∗∂xΨ).
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Question 1 - Solution Substitution into the wave equation fixes the time evolution of a plane wave x j (a) Method and calculation ∂tΨ = −iωΨ, ∂2 xΨ = −k2Ψ. ℏω = ℏ2k2/(2m) + V0 . (b) Interpretation and further calculation ρ = |A|2, j = (ℏk/m)|A|2 . ∂tρ + ∂xj = 0 + 0 = 0 . Physical check A plane wave is an idealized flux state rather than a square-normalizable state on the full real line. A localized packet can be assembled from such components.

Question 1

Substitution into the wave equation fixes the time evolution of a plane wave

A particle of mass m moves in constant potential V0V_0. Consider Ψ=Aei(kx−ωt)\Psi=Ae^{i(kx-\omega t)}. Use iℏ∂tΨ=−(ℏ2/2m)∂x2Ψ+VΨi\hbar\partial_t\Psi=-(\hbar^2/2m)\partial_x^2\Psi+V\Psi.

Diagram shown in the original SVG worksheet.

  1. Substitute the wave into the equation and determine ω\omega.

  2. Find its probability density and current, and check the continuity equation. The probability current is j=(ℏ/m)Im⁡(Ψ*∂xΨ)j=(\hbar/m)\operatorname{Im}(\Psi^*\partial_x\Psi).

Question 1 - Solution

Substitution into the wave equation fixes the time evolution of a plane wave

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∂tΨ=−iωΨ,∂x2Ψ=−k2Ψ.\partial_t\Psi=-i\omega\Psi,\quad\partial_x^2\Psi=-k^2\Psi.ℏω=ℏ2k2/(2m)+V0.\boxed{\hbar\omega=\hbar^2k^2/(2m)+V_0}.

(b) Interpretation and further calculation

ρ=|A|2,j=(ℏk/m)|A|2.\boxed{\rho=|A|^2,\qquad j=(\hbar k/m)|A|^2}.∂tρ+∂xj=0+0=0.\boxed{\partial_t\rho+\partial_xj=0+0=0}.

Physical check

A plane wave is an idealized flux state rather than a square-normalizable state on the full real line. A localized packet can be assembled from such components.