MHT CET · Physics · Magnetic Effects of Current
In the Bohr model, an electron moves in a circular orbit around the nucleus. Considering an orbiting electron to be a circular current loop, the magnetic moment of the hydrogen atom, when the electron is in nth excited state, is ( \(\mathrm{e}=\) electronic charge, \(\mathrm{m}_{\mathrm{e}}=\) mass of the electron, \(\mathrm{h}=\) Planck's constant)
- A \(\left(\frac{\mathrm{e}}{\mathrm{m}_{\mathrm{e}}}\right) \frac{\mathrm{nh}}{2 \pi}\)
- B \(\left(\frac{\mathrm{e}}{\mathrm{m}_{\mathrm{e}}}\right) \frac{\mathrm{n}^2 \mathrm{~h}}{2 \pi}\)
- C \(\left(\frac{\mathrm{e}}{2 \mathrm{~m}_{\mathrm{e}}}\right) \frac{\mathrm{n}^2 \mathrm{~h}}{2 \pi}\)
- D \(\left(\frac{\mathrm{e}}{2 \mathrm{~m}_{\mathrm{e}}}\right) \frac{\mathrm{nh}}{2 \pi}\)
Answer & Solution
Correct Answer
(D) \(\left(\frac{\mathrm{e}}{2 \mathrm{~m}_{\mathrm{e}}}\right) \frac{\mathrm{nh}}{2 \pi}\)
Step-by-step Solution
Detailed explanation
Current due to motion of electron, \(i=\frac{e v}{2 \pi r}\) Magnetic moment,
\(
\mathrm{M}=\mathrm{iA}=\frac{\mathrm{ev}}{2 \pi \mathrm{r}} \times \pi \mathrm{r}^2=\frac{\mathrm{evr}}{2}=\frac{\mathrm{e}}{2 \mathrm{~m}}(\mathrm{mvr})=\frac{\mathrm{e}}{2 \mathrm{~m}}\left(\frac{\mathrm{nh}}{2 \pi}\right)
\)
\(
\mathrm{M}=\mathrm{iA}=\frac{\mathrm{ev}}{2 \pi \mathrm{r}} \times \pi \mathrm{r}^2=\frac{\mathrm{evr}}{2}=\frac{\mathrm{e}}{2 \mathrm{~m}}(\mathrm{mvr})=\frac{\mathrm{e}}{2 \mathrm{~m}}\left(\frac{\mathrm{nh}}{2 \pi}\right)
\)
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