MHT CET · Physics · Magnetic Effects of Current
An electron moves in a circular orbit with uniform speed ' \(v^{\prime}\). It produces a
magnetic field 'B' at the centre of the circle. The radius of the circle is
\(\left[\mu_{0}=\right.\) permeability of free space, \(\mathrm{e}=\) electronic charge \(]\)
- A \(\left(\frac{\mu_{0} \mathrm{ev}}{\mathrm{B}}\right)^{1 / 2}\)
- B \(\frac{\mu_{0} \mathrm{eB}}{4 \pi \mathrm{v}}\)
- C \(\left(\frac{\mu_{0} \mathrm{ev}}{4 \pi \mathrm{B}}\right)^{1 / 2}\)
- D \(\frac{\mu_{0} \mathrm{ev}}{4 \pi \mathrm{B}}\)
Answer & Solution
Correct Answer
(C) \(\left(\frac{\mu_{0} \mathrm{ev}}{4 \pi \mathrm{B}}\right)^{1 / 2}\)
Step-by-step Solution
Detailed explanation
The magnetic field at the center of a circular orbit of a moving electron is given by
\(\begin{array}{l}
B=\frac{\mu_{0}}{4 \pi} \times \frac{e}{r^{3}}(v \times r) \\
B=\frac{\mu_{0}}{4 \pi} \times \frac{e v \sin \theta}{r^{2}}
\end{array}\)
As, in a circular path, the angle between radius vector and velocity vector is \(90^{\circ}\).
\(\begin{array}{l}
\mathrm{B}=\frac{\mu_{0}}{4 \pi} \times \frac{\mathrm{ev}}{\mathrm{r}^{2}} \\
\therefore \mathrm{r}=\left(\frac{\mu_{0} \mathrm{ev}}{4 \pi \mathrm{B}}\right)^{1 / 2}
\end{array}\)
\(\begin{array}{l}
B=\frac{\mu_{0}}{4 \pi} \times \frac{e}{r^{3}}(v \times r) \\
B=\frac{\mu_{0}}{4 \pi} \times \frac{e v \sin \theta}{r^{2}}
\end{array}\)
As, in a circular path, the angle between radius vector and velocity vector is \(90^{\circ}\).
\(\begin{array}{l}
\mathrm{B}=\frac{\mu_{0}}{4 \pi} \times \frac{\mathrm{ev}}{\mathrm{r}^{2}} \\
\therefore \mathrm{r}=\left(\frac{\mu_{0} \mathrm{ev}}{4 \pi \mathrm{B}}\right)^{1 / 2}
\end{array}\)
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