Step 1: Understanding the Magnetic Field Formula The magnetic field at the center of a circular orbit due to an orbiting charge is given by: \[ B = \frac{\mu_0}{2} \frac{I}{r} \] where: - \( \mu_0 = 4\pi \times 10^{-7} \) \( H/m \) (permeability of free space), - \( I \) is the current due to the orbiting electron, - \( r \) is the radius of the orbit.
Step 2: Calculating the Current Current due to an electron in circular motion is given by: \[ I = \frac{e f}{T} \] Since \( f \) is the frequency of revolution, we can write: \[ I = e f \] Given: \[ e = 1.6 \times 10^{-19} C, \quad f = 6.6 \times 10^{15} Hz \] \[ I = (1.6 \times 10^{-19}) \times (6.6 \times 10^{15}) \] \[ I = 1.056 \times 10^{-3} A \]
Step 3: Calculating the Magnetic Field The radius of the orbit is given as: \[ r = 0.47 \text{ Å} = 0.47 \times 10^{-10} m \] Using the formula: \[ B = \frac{\mu_0}{2} \frac{I}{r} \] \[ B = \frac{(4\pi \times 10^{-7})}{2} \times \frac{1.056 \times 10^{-3}}{0.47 \times 10^{-10}} \] \[ B = 2\pi \times \frac{1.056 \times 10^{-3}}{0.47 \times 10^{-10}} \] \[ B = 6.28 \times \frac{1.056 \times 10^{-3}}{0.47 \times 10^{-10}} \] \[ B \approx 14 wb \ m^{-2} \]
Step 4: Conclusion Thus, the magnetic field at the center of the orbit is \( 14 \ wb \ m^{-2} \).
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____.
The value of shunt resistance that allows only 10% of the main current through the galvanometer of resistance \( 99 \Omega \) is:
A current of \(6A\) enters one corner \(P\) of an equilateral triangle \(PQR\) having three wires of resistance \(2 \Omega\) each and leaves by the corner \(R\) as shown in figure. Then the currents \(I_1\) and \(I_2\) are respectively