To determine the induced EMF in the loop at \(t = 10 \text{ s}\), we apply Faraday's law of electromagnetic induction. This law states that the induced EMF in a closed loop equals the negative rate of change of magnetic flux through it.
The formula for induced EMF \((\varepsilon)\) is:
\(\varepsilon = -\frac{{d\Phi}}{{dt}}\)
where \(\Phi\) is the magnetic flux.
Magnetic flux \((\Phi)\) through a coil is calculated as:
\(\Phi = B \times A\)
where \(B\) is the magnetic field strength and \(A\) is the area of the coil within the magnetic field.
Consider the square loop's position. The magnetic field is 50 cm wide, and the loop's side is 15 cm.
At \(t = 0\), the front edge of the loop begins entering the magnetic field.
By \(t = 10 \text{ s}\), the loop has traveled:
\(d = \text{velocity} \times \text{time} = 2 \, \text{cm/s} \times 10 \, \text{s} = 20 \, \text{cm}\)
Since the loop has moved 20 cm and its side is 15 cm, the entire loop is outside the magnetic field because \(20 \, \text{cm}\) is less than \(15 \, \text{cm} + 50 \, \text{cm}\). The loop has not fully entered the field, and it has not yet exited.
Therefore, the magnetic flux through the loop is zero at \(t=10\) s.
Consequently, the rate of change of magnetic flux \((\frac{d\Phi}{dt})\) is zero, resulting in an induced EMF of:
\(\varepsilon = 0 \, \text{V}\)
Thus, the induced EMF in the loop is zero.

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:
A proton is moving undeflected in a region of crossed electric and magnetic fields at a constant speed of \( 2 \times 10^5 \, \text{m/s} \). When the electric field is switched off, the proton moves along a circular path of radius 2 cm. The magnitude of electric field is \( x \times 10^4 \, \text{N/C} \). The value of \( x \) is \(\_\_\_\_\_\). (Take the mass of the proton as \( 1.6 \times 10^{-27} \, \text{kg} \)).