Question #60875

Write down the wave functions (i) ψ210 and (ii) ψ300 for the hydrogen atom. Obtain the
expectation value of r for the ground state hydrogen atom.

Expert's answer

Answer on question #60875 – Physics / Atomic and Nuclear Physics

Write down the wave functions (i) ψ210\psi 210 and (ii) ψ300\psi 300 for the hydrogen atom. Obtain the expectation value of rr for the ground state hydrogen atom.

Solution

ψnlm(r,ϑ,φ)=12n(nl1)!(n+l)!(2na0)32exp(rna0)(2rna0)lLnl12l+1(2rna0)Ylm(ϑ,φ),\psi_{nlm}(r, \vartheta, \varphi) = \frac{1}{\sqrt{2n(n-l-1)!(n+l)!}} \left(\frac{2}{na_0}\right)^{\frac{3}{2}} \exp\left(-\frac{r}{na_0}\right) \left(\frac{2r}{na_0}\right)^l L_{n-l-1}^{2l+1} \left(\frac{2r}{na_0}\right) Y_{lm}(\vartheta, \varphi),


Where

a0a_0 is the Bohr radius,

Lnl12l+1L_{n-l-1}^{2l+1} is a generalized Laguerre polynomial of degree n1n - \ell - 1,

Ylm(ϑ,φ)Y_{lm}(\vartheta, \varphi) is a spherical harmonic function of degree \ell and order mm.

Then


ψ210(r,ϑ,φ)=124(1a0)32exp(r2a0)(ra0)L03(ra0)Y10(ϑ,φ)=1412π(1a0)32exp(r2a0)(ra0)\begin{aligned} \psi_{210}(r, \vartheta, \varphi) &= \frac{1}{\sqrt{24}} \left(\frac{1}{a_0}\right)^{\frac{3}{2}} \exp\left(-\frac{r}{2a_0}\right) \left(\frac{r}{a_0}\right) L_0^3 \left(\frac{r}{a_0}\right) Y_{10}(\vartheta, \varphi) \\ &= \frac{1}{4} \sqrt{\frac{1}{2\pi}} \left(\frac{1}{a_0}\right)^{\frac{3}{2}} \exp\left(-\frac{r}{2a_0}\right) \left(\frac{r}{a_0}\right) \end{aligned}ψ300(r,ϑ,φ)=172(23a0)32exp(r3a0)L21(2r3a0)Y00(ϑ,φ)=11232π(23a0)32exp(r3a0)(12(2r3a0)26(2r3a0)+3)cosϑ\begin{aligned} \psi_{300}(r, \vartheta, \varphi) &= \frac{1}{\sqrt{72}} \left(\frac{2}{3a_0}\right)^{\frac{3}{2}} \exp\left(-\frac{r}{3a_0}\right) L_2^1 \left(\frac{2r}{3a_0}\right) Y_{00}(\vartheta, \varphi) \\ &= \frac{1}{12} \sqrt{\frac{3}{2\pi}} \left(\frac{2}{3a_0}\right)^{\frac{3}{2}} \exp\left(-\frac{r}{3a_0}\right) \left(\frac{1}{2} \left(\frac{2r}{3a_0}\right)^2 - 6 \left(\frac{2r}{3a_0}\right) + 3\right) \cos \vartheta \end{aligned}


For ground state we have:


ψ100(r,ϑ,φ)=1πa03exp(ra0)\psi_{100}(r, \vartheta, \varphi) = \sqrt{\frac{1}{\pi a_0^3}} \exp\left(-\frac{r}{a_0}\right)


The expectation value of rr is:


Vrψ1002dV=4ππa030r3exp(2ra0)dr=4a03(a02)40x3exp(x)dx=32a0\int_V r |\psi_{100}|^2 dV = \frac{4\pi}{\pi a_0^3} \int_0^\infty r^3 \exp\left(-\frac{2r}{a_0}\right) dr = \frac{4}{a_0^3} \left(\frac{a_0}{2}\right)^4 \int_0^\infty x^3 \exp(-x) dx = \frac{3}{2} a_0


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