For hydrogen atoms, the wave function for the state \(n=3\) \(\ell=0, m_{\ell}=0\) is $$\psi_{300}=\frac{1}{81 \sqrt{3 \pi}}\left(\frac{1}{a_{0}}\right)^{3 / 2}\left(27-18 \sigma+2 \sigma^{2}\right) e^{-\sigma \beta}$$ where \(\sigma=r / a_{0}\) and \(a_{0}\) is the Bohr radius $\left(5.29 \times 10^{-11} \mathrm{m}\right) .$ Calculate the position of the nodes for this wave function.

Short Answer

Expert verified
The nodes for the wave function \(\psi_{300}\) are the positions in terms of r where the probability density of finding an electron is zero. To find these positions, we set the wave function equal to zero and solve for r. We find the node positions to be: \[r_1 = \left(\frac{18 + \sqrt{216}}{4}(5.29 \times 10^{-11}\mathrm{m})\right)\] \[r_2 = \left(\frac{18 - \sqrt{216}}{4}(5.29 \times 10^{-11}\mathrm{m})\right)\]

Step by step solution

01

Identify the wave function for the given quantum numbers

We are given the wave function for the hydrogen atom in the state with quantum numbers n=3, l=0, and m_l=0: \[\psi_{300}=\frac{1}{81 \sqrt{3 \pi}}\left(\frac{1}{a_{0}}\right)^{3 / 2}\left(27-18 \sigma+2 \sigma^{2}\right) e^{-\sigma \beta}\] where \(\sigma = r/a_0\) and \(a_0\) is the Bohr radius (\(5.29 \times 10^{-11}\) m).
02

Set the wave function equal to zero

To find the nodes, we want to find the values of r for which the wave function is equal to zero: \[\frac{1}{81 \sqrt{3 \pi}}\left(\frac{1}{a_{0}}\right)^{3 / 2}\left(27-18 \sigma+2 \sigma^{2}\right) e^{-\sigma \beta} = 0\]
03

Identify the factors affecting the result

The exponential term \(e^{-\sigma \beta}\) is always positive and can never be equal to zero. The same goes for the constants in the expression. Therefore, the key term to focus on is the polynomial one: \[27-18 \sigma+2 \sigma^{2} = 0\] Replace \(\sigma\) with \(r/a_{0}\) to find the nodes in terms of r: \[27-18\left(\frac{r}{a_{0}}\right) + 2 \left(\frac{r}{a_{0}}\right)^2 = 0\]
04

Solve the quadratic equation for r

Solve the quadratic equation to find the roots (i.e., node positions) in terms of r: \[2\left(\frac{r}{a_{0}}\right)^2 - 18\left(\frac{r}{a_{0}}\right) + 27 = 0\] Let \(x = \frac{r}{a_{0}}\), so the equation becomes: \[2x^2 - 18x + 27 = 0\] Use the quadratic formula to solve for x: \[x = \frac{-b \pm \sqrt{b^2 - 4ac}}{2a}\] where a = 2, b = -18, and c = 27. \[x = \frac{18 \pm \sqrt{(-18)^2 - 4(2)(27)}}{2(2)}\] Simplify and solve for x: \[x = \frac{18 \pm \sqrt{216}}{4}\] This gives us two values for \(x\): \[x_1 = \frac{18 + \sqrt{216}}{4}\] \[x_2 = \frac{18 - \sqrt{216}}{4}\]
05

Convert the x values back to r-values

Recall that \(x = \frac{r}{a_{0}}\). Multiply both sides by \(a_{0}\) to obtain the node positions, \(r_1\) and \(r_2\): \[r_1 = x_1a_0 = \left(\frac{18 + \sqrt{216}}{4}\right)(5.29 \times 10^{-11}\mathrm{m})\] \[r_2 = x_2a_0 = \left(\frac{18 - \sqrt{216}}{4}\right)(5.29 \times 10^{-11}\mathrm{m})\] Now you have found the position of the nodes for this wave function.

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