Heisenberg's Uncertainty Principle — Question 2

Section 38-7 · Physics pages 6374–6375

Question 2 Localization sets a lower bound on kinetic energy even with zero mean momentum A nonrelativistic electron has σx = .100 nm and mean momentum p0. Use ℏ2/(2me) = .0381 eV nm2. All uncertainties here are standard deviations, with σxσp ≥ℏ/2. x ⟨p⟩= 0 Schematic; labels, not drawing lengths, specify the data. (a) Derive a lower bound on its mean kinetic energy in terms of p0 and σx. (b) Evaluate the minimum possible mean kinetic energy for p0 = 0.
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Question 2 - Solution Localization sets a lower bound on kinetic energy even with zero mean momentum x ⟨p⟩= 0 (a) Method and calculation ⟨K⟩= ⟨p2⟩ 2me = p2 0 + σ2 p 2me . ⟨K⟩≥ p2 0 2me + ℏ2 8meσ2x . (b) Interpretation and further calculation p0 = 0 : Kmin = .0381 eV nm2 4(.100 nm)2 . Kmin = .9525 eV . Physical check Zero mean momentum is compatible with nonzero kinetic energy: positive and negative momenta contribute equally to the mean while their squares remain positive.

Question 2

Localization sets a lower bound on kinetic energy even with zero mean momentum

A nonrelativistic electron has σx=.100nm\sigma_x=.100\,\mathrm{nm} and mean momentum p0p_0. Use ℏ2/(2me)=.0381eVnm2\hbar^2/(2m_e)=.0381\,\mathrm{eV\,nm^2}. All uncertainties here are standard deviations, with σxσp≥ℏ/2\sigma_x\sigma_p\ge\hbar/2.

Diagram shown in the original SVG worksheet.

  1. Derive a lower bound on its mean kinetic energy in terms of p0p_0 and σx\sigma_x.

  2. Evaluate the minimum possible mean kinetic energy for p0=0p_0=0.

Question 2 - Solution

Localization sets a lower bound on kinetic energy even with zero mean momentum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨K⟩=⟨p2⟩2me=p02+σp22me.\langle K\rangle=\frac{\langle p^2\rangle}{2m_e}=\frac{p_0^2+\sigma_p^2}{2m_e}.⟨K⟩≥p022me+ℏ28meσx2.\boxed{\langle K\rangle\ge\frac{p_0^2}{2m_e}+\frac{\hbar^2}{8m_e\sigma_x^2}}.

(b) Interpretation and further calculation

p0=0:Kmin=.0381eVnm24(.100nm)2.p_0=0:\quad K_{\min}=\frac{.0381\,\mathrm{eV\,nm^2}}{4(.100\,\mathrm{nm})^2}.Kmin=.9525eV.\boxed{K_{\min}=.9525\,\mathrm{eV}}.

Physical check

Zero mean momentum is compatible with nonzero kinetic energy: positive and negative momenta contribute equally to the mean while their squares remain positive.