The magnetic moment \( \mu \) of a current loop is defined as: \[ \mu = I A \] where \( I \) is the current and \( A \) is the area of the loop. The magnetic field \( B \) produced by a current \( I \) at the centre of a circular loop of radius \( r \) is given by: \[ B = \frac{\mu_0 I}{2r} \] From this, we can solve for \( I \): \[ I = \frac{2r B}{\mu_0} \] Now, substitute this value of \( I \) into the equation for the magnetic moment: \[ \mu = \left( \frac{2r B}{\mu_0} \right) A \] Since the area \( A \) of the loop is related to the radius by \( A = \pi r^2 \), substitute \( r = \sqrt{\frac{A}{\pi}} \) into the equation: \[ \mu = \frac{2B A}{\mu_0} \sqrt{\frac{A}{\pi}} \] Thus, the magnetic moment of the loop is: \[ \mu = \frac{2BA}{\mu_0} \sqrt{\frac{A}{\pi}} \]
Consider the following statements:
A. The junction area of a solar cell is made very narrow compared to a photodiode.
B. Solar cells are not connected with any external bias.
C. LED is made of lightly doped p-n junction.
D. Increase of forward current results in a continuous increase in LED light intensity.
E. LEDs have to be connected in forward bias for emission of light.