The Bohr Model of the Hydrogen Atom — Question 2

Section 39-7 · Physics pages 6534–6535

Question 2 Equal binding energies in different hydrogenic ions need not imply equal radii Compare hydrogen in its ground state with a one-electron helium ion in mode n = 2. Use the nonrelativistic Bohr model with an infinitely heavy nucleus unless stated otherwise: En = −13.6Z2/n2 eV, rn = a0n2/Z, a0 = .0529 nm, and hc = 1240 eV nm. Here Z is the nuclear charge number. +Ze v r Schematic; labels, not drawing lengths, specify the data. (a) Find both energies and radii. (b) Compare their speeds and orbital periods using vn ∝Z/n.
Show solutionHide solution
Question 2 - Solution Equal binding energies in different hydrogenic ions need not imply equal radii +Ze v r (a) Method and calculation EH,1 = −13.6 eV , EHe+,2 = −13.6(4/4) = −13.6 eV . rH,1 = a0 = .0529 nm , rHe+,2 = 2a0 = .1058 nm . (b) Interpretation and further calculation vHe+,2/vH,1 = (2/2)/(1/1) = 1 . T = 2πr/v ⇒THe+,2/TH,1 = 2 . Physical check Equal energy fixes equal speed in this infinite-nuclear-mass comparison, but the stronger central charge permits that speed at a larger radius with higher angular momentum.

Question 2

Equal binding energies in different hydrogenic ions need not imply equal radii

Compare hydrogen in its ground state with a one-electron helium ion in mode n=2n=2. Use the nonrelativistic Bohr model with an infinitely heavy nucleus unless stated otherwise: En=−13.6Z2/n2eVE_n=-13.6Z^2/n^2\,\mathrm{eV}, rn=a0n2/Zr_n=a_0n^2/Z, a0=.0529nma_0=.0529\,\mathrm{nm}, and hc=1240eVnmhc=1240\,\mathrm{eV\,nm}. Here Z is the nuclear charge number.

Diagram shown in the original SVG worksheet.

  1. Find both energies and radii.

  2. Compare their speeds and orbital periods using vn∝Z/nv_n\propto Z/n.

Question 2 - Solution

Equal binding energies in different hydrogenic ions need not imply equal radii

Diagram shown in the original SVG worksheet.

(a) Method and calculation

EH,1=−13.6eV,EHe+,2=−13.6(4/4)=−13.6eV.\boxed{E_{\mathrm{H,1}}=-13.6\,\mathrm{eV}},\qquad\boxed{E_{\mathrm{He^+,2}}=-13.6(4/4)=-13.6\,\mathrm{eV}}.rH,1=a0=.0529nm,rHe+,2=2a0=.1058nm.\boxed{r_{\mathrm{H,1}}=a_0=.0529\,\mathrm{nm}},\quad\boxed{r_{\mathrm{He^+,2}}=2a_0=.1058\,\mathrm{nm}}.

(b) Interpretation and further calculation

vHe+,2/vH,1=(2/2)/(1/1)=1.\boxed{v_{\mathrm{He^+,2}}/v_{\mathrm{H,1}}=(2/2)/(1/1)=1}.T=2πr/v⇒THe+,2/TH,1=2.T=2\pi r/v\Rightarrow\boxed{T_{\mathrm{He^+,2}}/T_{\mathrm{H,1}}=2}.

Physical check

Equal energy fixes equal speed in this infinite-nuclear-mass comparison, but the stronger central charge permits that speed at a larger radius with higher angular momentum.