A spatially uniform time dependent magnetic field is changing with tim...
Understanding the Scenario
In this scenario, a unit positive charge is moving in a circular path of radius \( R = 2 \, \text{m} \) perpendicular to a time-dependent magnetic field that changes at a rate of \( 1 \, \text{T/s} \).
Magnetic Field and Charge Interaction
- A changing magnetic field induces an electric field according to Faraday's law of electromagnetic induction.
- The induced electric field \( E \) can be determined using the equation:
\[
E = -\frac{d\Phi_B}{dt}
\]
- Here, \( \Phi_B \) is the magnetic flux given by \( \Phi_B = B \cdot A \), where \( A \) is the area enclosed by the circular path.
Calculating the Induced Electric Field
- The area \( A \) of the circle is calculated as:
\[
A = \pi R^2 = \pi (2)^2 = 4\pi \, \text{m}^2
\]
- Since the magnetic field changes at \( 1 \, \text{T/s} \), the induced electric field becomes:
\[
E = 1 \, \text{T/s} \cdot A = 1 \cdot 4\pi = 4\pi \, \text{V/m}
\]
Work Done on the Charge
- The work done \( W \) on a charge \( q \) moving in an electric field \( E \) over a distance \( d \) is given by:
\[
W = qEd
\]
- For one complete revolution, \( d \) is equal to the circumference of the circle:
\[
d = 2\pi R = 2\pi \cdot 2 = 4\pi \, \text{m}
\]
- Substituting \( q = 1 \, \text{C} \), \( E = 4\pi \, \text{V/m} \), and \( d = 4\pi \, \text{m} \):
\[
W = 1 \cdot 4\pi \cdot 4\pi = 16\pi^2 \, \text{J}
\]
Conclusion
- The magnitude of the work done on the unit positive charge for one complete revolution is \( 16\pi^2 \, \text{J} \).