The de-Broglie wavelength of an electron moving in the $n^{\text {th }}$ Bohr orbit of radius $r$ is
- $\frac{n r}{2 \pi}$
- $\frac{2 \pi r}{n}$
- $\frac{n r}{\pi}$
- $n \pi r$
Solution
And for the electron moving in the \(n^{\text {th }}\) orbit,
The angular momentum \(L=\frac{n h}{2 \pi}\)
\(\begin{aligned}
& \Rightarrow m v r=\frac{n h}{2 \pi} \\
& \Rightarrow m v=\frac{n h}{2 \pi r} \quad---(2)
\end{aligned}\) Taking the ratio of equation (1) and (2), $\frac{h}{\lambda}=\frac{n h}{2 \pi r}$ $\Rightarrow \lambda=\frac{2 \pi r}{n}$ :
Asked in: MHT CET 2022 (06 Aug Shift 2)