The quantum-mechanical treatment of the hydrogen atom gives this expression
for the wave function, \(\psi,\) of the \(1 s\) orbital: $$
\Psi=\frac{1}{\sqrt{\pi}}\left(\frac{1}{a_{0}}\right)^{3 / 2} e^{-r l a_{0}}
$$
where \(r\) is the distance from the nucleus and \(a_{0}\) is \(52.92 \mathrm{pm}\).
The probability of finding the electron in a tiny volume at distance \(r\) from
the nucleus is proportional to \(\psi^{2}\). The total probability of finding
the electron at all points at distance \(r\) from the nucleus is proportional to
\(4 \pi r^{2} \psi^{2}\). Calculate the values (to three significant figures) of
\(\psi, \psi^{2},\) and \(4 \pi r^{2} \psi^{2}\) to fill in the following table
and sketch a plot of each set of values versus \(r .\) Compare the latter two
plots with those in Figure \(7.17 \mathrm{~A}\).