Schrödinger's Equation and the Hydrogen Atom — Question 10

Section 39-8 · Physics pages 6570–6571

Question 10 Direct substitution into the radial equation recovers the hydrogen ground scale Treat hydrogen with a fixed nucleus, a nonrelativistic Coulomb potential and no spin, fine structure or external field. Write the Bohr length as a. Let V (r) = −K/r, where K = kee2. For an spherically symmetric state use −ℏ2[ψ′′ + 2ψ′/r]/(2m) −Kψ/r = Eψ. Try ψ = Ne−r/a and use ⟨1/r⟩= 1/a for the normalized exponential. r ψ Schematic; labels, not drawing lengths, specify the data. (a) Determine a and E by requiring the equation to hold for every r > 0. (b) Find the mean potential and kinetic energies and verify the Coulomb virial relation.
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Question 10 - Solution Direct substitution into the radial equation recovers the hydrogen ground scale r ψ (a) Method and calculation ψ′ = −ψ/a, ψ′′ = ψ/a2 ⇒E = −ℏ2 2ma2 + 1 r ( ℏ2 ma −K ) . a = ℏ2/(mK) , E = −ℏ2/(2ma2) . (b) Interpretation and further calculation ⟨V ⟩= −K/a = −ℏ2/(ma2) = 2E . ⟨K⟩= E −⟨V ⟩= −E , 2⟨K⟩+ ⟨V ⟩= 0 . Physical check The exponential is a spatial probability amplitude, not a circular path. The equation reproduces the Bohr ground energy while providing a different physical description of the electron.

Question 10

Direct substitution into the radial equation recovers the hydrogen ground scale

Treat hydrogen with a fixed nucleus, a nonrelativistic Coulomb potential and no spin, fine structure or external field. Write the Bohr length as a. Let V(r)=−𝒦/rV(r)=-\mathcal K/r, where 𝒦=kee2\mathcal K=k_ee^2. For an spherically symmetric state use −ℏ2[ψ′′+2ψ′/r]/(2m)−𝒦ψ/r=Eψ-\hbar^2[\psi\prime\prime+2\psi\prime/r]/(2m)-\mathcal K\psi/r=E\psi. Try ψ=Ne−r/a\psi=Ne^{-r/a} and use ⟨1/r⟩=1/a\langle1/r\rangle=1/a for the normalized exponential.

Diagram shown in the original SVG worksheet.

  1. Determine a and E by requiring the equation to hold for every r>0r>0.

  2. Find the mean potential and kinetic energies and verify the Coulomb virial relation.

Question 10 - Solution

Direct substitution into the radial equation recovers the hydrogen ground scale

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ψ′=−ψ/a,ψ′′=ψ/a2⇒E=−ℏ22ma2+1r(ℏ2ma−𝒦).\psi\prime=-\psi/a,\quad\psi\prime\prime=\psi/a^2\Rightarrow E=-\frac{\hbar^2}{2ma^2}+\frac1r\left(\frac{\hbar^2}{ma}-\mathcal K\right).a=ℏ2/(m𝒦),E=−ℏ2/(2ma2).\boxed{a=\hbar^2/(m\mathcal K)},\qquad\boxed{E=-\hbar^2/(2ma^2)}.

(b) Interpretation and further calculation

⟨V⟩=−𝒦/a=−ℏ2/(ma2)=2E.\boxed{\langle V\rangle=-\mathcal K/a=-\hbar^2/(ma^2)=2E}.⟨K⟩=E−⟨V⟩=−E,2⟨K⟩+⟨V⟩=0.\boxed{\langle K\rangle=E-\langle V\rangle=-E},\qquad\boxed{2\langle K\rangle+\langle V\rangle=0}.

Physical check

The exponential is a spatial probability amplitude, not a circular path. The equation reproduces the Bohr ground energy while providing a different physical description of the electron.