The Bohr Model of the Hydrogen Atom — Question 6

Section 39-7 · Physics pages 6542–6543

Question 6 Ionization from an excited Bohr level requires less than the ground-state binding A hydrogen atom starts in mode n = 3 and absorbs a photon of energy 2.00 eV. Neglect nuclear recoil and assume ionization occurs. 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. n = 1 n = 2 n = 3 n = 4 E E = 0 continuum Schematic; labels, not drawing lengths, specify the data. (a) Find the ionization threshold from that level. (b) Find the outgoing electron kinetic energy and explain the energy reference used.
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Question 6 - Solution Ionization from an excited Bohr level requires less than the ground-state binding n = 1 n = 2 n = 3 n = 4 E E = 0 continuum (a) Method and calculation E3 = −13.6/9 eV = −1.51111 eV. Ethreshold = 0 −E3 = 1.51111 eV . (b) Interpretation and further calculation E3 + Eγ = Kout ⇒ Kout = .488889 eV . Efinal = Kout > 0 relative to separated particles at rest. Physical check Ionization reaches a continuum rather than another discrete bound level. The positive excess photon energy becomes outgoing kinetic energy in the stated recoil-free model.

Question 6

Ionization from an excited Bohr level requires less than the ground-state binding

A hydrogen atom starts in mode n=3n=3 and absorbs a photon of energy 2.00eV2.00\,\mathrm{eV}. Neglect nuclear recoil and assume ionization occurs. 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 the ionization threshold from that level.

  2. Find the outgoing electron kinetic energy and explain the energy reference used.

Question 6 - Solution

Ionization from an excited Bohr level requires less than the ground-state binding

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E3=−13.6/9eV=−1.51111eV.E_3=-13.6/9\,\mathrm{eV}=-1.51111\,\mathrm{eV}.Ethreshold=0−E3=1.51111eV.\boxed{E_{\mathrm{threshold}}=0-E_3=1.51111\,\mathrm{eV}}.

(b) Interpretation and further calculation

E3+Eγ=Kout⇒Kout=.488889eV.E_3+E_\gamma=K_{\mathrm{out}}\quad\Rightarrow\quad\boxed{K_{\mathrm{out}}=.488889\,\mathrm{eV}}.Efinal=Kout>0relative to separated particles at rest.\boxed{E_{\mathrm{final}}=K_{\mathrm{out}}>0}\quad\text{relative to separated particles at rest}.

Physical check

Ionization reaches a continuum rather than another discrete bound level. The positive excess photon energy becomes outgoing kinetic energy in the stated recoil-free model.