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Let \(v_{n}\) and \(E_{n}\) be the respective speed and energy of an electron in the horbit of radius \(r_{n}\), in a hydrogen atom, as predicted by Bohr's model. Then
(A) plot of \(E_{n} r_{n} / E_{1} r_{1}\) as a function of \(n\) is a straight line of slope 0 .
(B) plot of \(\mathrm{r}_{\mathrm{n}} \mathrm{v}_{\mathrm{n}} / \mathrm{r}_{1} \mathrm{v}_{1}\) as a function of \(\mathrm{n}\) is a straight line of slope 1 .
(C) plot of \(\ln \left(\frac{r_{n}}{r_{1}}\right)\) as a function of \(\ln (n)\) is a straight line of slope 2 .
(D) plot of \(\ln \left(\frac{r_{n} E_{1}}{E_{n} r_{1}}\right)\) as a function of \(\ln (n)\) is a straight line of slope 4 .

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Ans: (A,B,C,D)
\(v_{n} \propto \frac{1}{n}\)
\(E_{n} \propto \frac{1}{n^{2}}\)
\(r_{n} \propto n^{2}\)
\(\therefore E_{n} r_{n} \propto n^{0}\)
\(\therefore E_{n} r_{n} \propto E_{1} r_{1}\)
\(\frac{E_{n} r_{n}}{E_{1} r_{1}}=\) cons \(t\) an \(t(\therefore\) slope \(=0)\)
\(r_{n} v_{n} \propto n^{2} \times \frac{1}{n} \propto n\)
\(\therefore \frac{r_{n} v_{n}}{r_{1} v_{1}}=n\)
\((\therefore\) slope \(=1)\)
\(r_{n} \propto n^{2}\)
\(\therefore \frac{\mathrm{r}_{\mathrm{n}}}{\mathrm{r}_{1}}=\mathrm{n}^{2}\)
\(\ln \left(\frac{r_{n}}{r_{1}}\right)=2 \ln (n) \quad(\therefore\) slope \(=2)\)
\(\frac{r_{n}}{E_{n}} \propto n^{4}\)
\(\therefore \frac{r_{n}}{E_{n}} \times \frac{E_{1}}{r_{1}}=n^{4}\)
\(\ln \left(\frac{r_{n} E_{1}}{E_{n} r_{1}}\right)=4 \ln (n)\)
\((\therefore\) slope \(=4)\)
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