The magnetic field inside a solenoid is given by the formula:
\( B = \mu_0 \cdot n \cdot I \)
Where:
First, calculate the number of turns per unit length: \[ n = \frac{N}{l} = \frac{60}{0.15} = 400 \, \text{turns/m} \] Now substitute into the formula: \[ B = \mu_0 \cdot n \cdot I \] \[ 2.4 \times 10^{-3} = (4\pi \times 10^{-7}) \cdot 400 \cdot I \]
Rearranging the formula for \( I \): \[ I = \frac{B}{\mu_0 \cdot n} \] Substituting the values: \[ I = \frac{2.4 \times 10^{-3}}{(4\pi \times 10^{-7}) \cdot 400} \] Simplify: \[ I = \frac{2.4 \times 10^{-3}}{1.6 \times 10^{-4}} \] \[ I = 100 \, \text{A} \]
The current in the solenoid is \( \boxed{100 \, \text{A}} \).
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:


In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: