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Question: In the given wave function, $\psi = \frac{1}{81} (\frac{2}{\pi})^{\frac{1}{2}} (\frac{1}{a_0})^{\fra...

In the given wave function, ψ=181(2π)12(1a0)32(6ra0r2a02)er3a0cosθ\psi = \frac{1}{81} (\frac{2}{\pi})^{\frac{1}{2}} (\frac{1}{a_0})^{\frac{3}{2}} (6 - \frac{r}{a_0} - \frac{r^2}{a_0^2}) e^{-\frac{r}{3a_0}} \cos \theta

Identify the correct choice(s).

A

The given orbital is 3pz3p_z.

B

The given orbital is 3dz23d_{z^2}.

C

The nodal surface is at a radical distance of 6a06a_0 from the nucleus.

D

The number of angular nodes in the given orbital are 2.

Answer

The nodal surface is at a radical distance of 6a06a_0 from the nucleus.

Explanation

Solution

Solution:

The given wave function is

ψ=181(2π)1/2(1a0)3/2(6ra0r2a02)er3a0cosθ.\psi = \frac{1}{81}\left(\frac{2}{\pi}\right)^{1/2}\left(\frac{1}{a_0}\right)^{3/2}\left(6 - \frac{r}{a_0} - \frac{r^2}{a_0^2}\right)e^{-\frac{r}{3a_0}}\cos\theta.
  1. Angular Part:
    The factor cosθ\cos\theta is the angular part. For hydrogen-like orbitals, cosθ\cos\theta corresponds to the spherical harmonic Y10(θ,ϕ)Y_1^0(\theta,\phi) which represents a pzp_z orbital (with l=1l=1). In contrast, a 3dz23d_{z^2} orbital would have an angular part proportional to (3cos2θ1)(3\cos^2\theta - 1).

  2. Radial Part and Radial Node:
    The radial part is given by

R(r)(6ra0r2a02)er3a0.R(r) \propto \left(6 - \frac{r}{a_0} - \frac{r^2}{a_0^2}\right)e^{-\frac{r}{3a_0}}.

Setting the polynomial equal to zero to find the radial node:

6ra0r2a02=0.6 - \frac{r}{a_0} - \frac{r^2}{a_0^2} = 0.

Multiply by a02a_0^2:

r2+ra06a02=0.r^2 + r\,a_0 - 6a_0^2 = 0.

Let x=ra0x = \frac{r}{a_0}; then

x2+x6=0.x^2 + x - 6 = 0.

Solving, we get:

x=1±1+242=1±52.x = \frac{-1 \pm \sqrt{1+24}}{2} = \frac{-1 \pm 5}{2}.

The positive root is:

x=2r=2a0.x = 2 \quad\Rightarrow\quad r = 2a_0.

So the radial node is at 2a02a_0 and not at 6a06a_0.

  1. Angular Nodes:
    Since cosθ\cos\theta vanishes at θ=π/2\theta = \pi/2, there is 1 angular node. (For l=1l=1 there is exactly one angular node.)