Building the Periodic Table — Question 10

Section 40-8 · Physics pages 6730–6731

Question 10 Orbital penetration breaks the same-shell hydrogenic energy degeneracy In a supplied screened one-electron model, Enl = −13.6 eV Z2 eff,l/n2. For two valence orbitals with n = 3, use Zeff,s = 4.20 and Zeff,p = 3.50. Assume a vacant final p spin orbital, and hold both effective charges fixed during excitation. 3s 3p ∆E Schematic; labels, not drawing lengths, specify the data. (a) Calculate the s and p energies and identify the more tightly bound orbital. (b) Find the s-to-p excitation energy and its photon wavelength using hc = 1240 eV nm.
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Question 10 - Solution Orbital penetration breaks the same-shell hydrogenic energy degeneracy 3s 3p ∆E (a) Method and calculation E3s = −13.6(4.20)2/9 = −26.656 eV . E3p = −13.6(3.50)2/9 = −18.511 eV ⇒3s more tightly bound . (b) Interpretation and further calculation ∆E = 13.6 9 [(4.20)2 −(3.50)2] = 8.1449 eV . λ = hc/∆E = 152.24 nm . Physical check Greater penetration exposes the s orbital to less screened nuclear attraction in this model. The supplied effective charges replace a self-consistent many-electron calculation; they are not universal constants for all atoms.

Question 10

Orbital penetration breaks the same-shell hydrogenic energy degeneracy

In a supplied screened one-electron model, Enl=−13.6eVZeff,l2/n2E_{nl}=-13.6\,\mathrm{eV}\,Z_{\mathrm{eff,l}}^2/n^2. For two valence orbitals with n=3n=3, use Zeff,s=4.20Z_{\mathrm{eff,s}}=4.20 and Zeff,p=3.50Z_{\mathrm{eff,p}}=3.50. Assume a vacant final p spin orbital, and hold both effective charges fixed during excitation.

Diagram shown in the original SVG worksheet.

  1. Calculate the s and p energies and identify the more tightly bound orbital.

  2. Find the s-to-p excitation energy and its photon wavelength using hc=1240eVnmhc=1240\,\mathrm{eV\,nm}.

Question 10 - Solution

Orbital penetration breaks the same-shell hydrogenic energy degeneracy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E3s=−13.6(4.20)2/9=−26.656eV.E_{3s}=-13.6(4.20)^2/9=\boxed{-26.656\,\mathrm{eV}}.E3p=−13.6(3.50)2/9=−18.511eV⇒3s more tightly bound.E_{3p}=-13.6(3.50)^2/9=\boxed{-18.511\,\mathrm{eV}}\Rightarrow\boxed{3s\text{ more tightly bound}}.

(b) Interpretation and further calculation

ΔE=13.69[(4.20)2−(3.50)2]=8.1449eV.\Delta E=\frac{13.6}{9}[(4.20)^2-(3.50)^2]=\boxed{8.1449\,\mathrm{eV}}.λ=hc/ΔE=152.24nm.\boxed{\lambda=hc/\Delta E=152.24\,\mathrm{nm}}.

Physical check

Greater penetration exposes the s orbital to less screened nuclear attraction in this model. The supplied effective charges replace a self-consistent many-electron calculation; they are not universal constants for all atoms.