Schrödinger's Equation and the Hydrogen Atom — Question 8

Section 39-8 · Physics pages 6566–6567

Question 8 The 2p radial distribution has one positive maximum and a different mean radius Treat hydrogen with a fixed nucleus, a nonrelativistic Coulomb potential and no spin, fine structure or external field. Write the Bohr length as a. The normalized radial function is R21(r) = [1/(2 √ 6 a3/2)](r/a)e−r/(2a). Its radial probability density is Pr = r2|R21|2, because the angular factor integrates to one. Use ∫∞ 0 rne−r/adr = n!an+1. r Pr 4a Schematic; labels, not drawing lengths, specify the data. (a) Find Pr and its most probable radius. (b) Check radial normalization and calculate the mean radius.
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Question 8 - Solution The 2p radial distribution has one positive maximum and a different mean radius r Pr 4a (a) Method and calculation Pr(r) = r4 24a5 e−r/a . d dr ln Pr = 4 r −1 a = 0 ⇒rmode = 4a . (b) Interpretation and further calculation ∫∞ 0 Prdr = 4!a5 24a5 = 1 . ⟨r⟩= 5!a6 24a5 = 5a . Physical check The 2p radial mode equals the n=2 Bohr radius, but the distribution has a finite width and a different mean. This agreement does not justify a definite orbit.

Question 8

The 2p radial distribution has one positive maximum and a different mean radius

Treat hydrogen with a fixed nucleus, a nonrelativistic Coulomb potential and no spin, fine structure or external field. Write the Bohr length as a. The normalized radial function is R21(r)=[1/(26a3/2)](r/a)e−r/(2a)R_{21}(r)=[1/(2\sqrt6\,a^{3/2})](r/a)e^{-r/(2a)}. Its radial probability density is Pr=r2|R21|2P_r=r^2|R_{21}|^2, because the angular factor integrates to one. Use ∫0∞rne−r/adr=n!an+1\int_0^\infty r^ne^{-r/a}dr=n!a^{n+1}.

Diagram shown in the original SVG worksheet.

  1. Find PrP_r and its most probable radius.

  2. Check radial normalization and calculate the mean radius.

Question 8 - Solution

The 2p radial distribution has one positive maximum and a different mean radius

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Pr(r)=r424a5e−r/a.\boxed{P_r(r)=\frac{r^4}{24a^5}e^{-r/a}}.ddrln⁡Pr=4r−1a=0⇒rmode=4a.\frac d{dr}\ln P_r=\frac4r-\frac1a=0\Rightarrow\boxed{r_{\mathrm{mode}}=4a}.

(b) Interpretation and further calculation

∫0∞Prdr=4!a524a5=1.\int_0^\infty P_rdr=\frac{4!a^5}{24a^5}=\boxed{1}.⟨r⟩=5!a624a5=5a.\boxed{\langle r\rangle=\frac{5!a^6}{24a^5}=5a}.

Physical check

The 2p radial mode equals the n=2 Bohr radius, but the distribution has a finite width and a different mean. This agreement does not justify a definite orbit.