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 \( 1.6 \times 10^{-27} \, \text{kg} \)).
To determine the magnitude of the electric field \( E \) for an undeviated proton in crossed electric (\( E \)) and magnetic (\( B \)) fields, the electric force must equal the magnetic force: \( qE = qvB \). Here, \( q \) is the proton's charge (\( 1.6 \times 10^{-19} \, \text{C} \)) and \( v \) is its velocity (\( 2 \times 10^5 \, \text{m/s} \)). This simplifies to \( E = vB \).
When the electric field is removed and the proton moves circularly due to the magnetic force alone, the magnetic force provides the centripetal force: \( \frac{mv^2}{r} = qvB \). Here, \( m \) is the proton's mass (\( 1.6 \times 10^{-27} \, \text{kg} \)) and \( r \) is the circular path's radius (\( 0.02 \, \text{m} \)). Rearranging yields \( B = \frac{mv}{qr} \).
Substituting values: \( B = \frac{1.6 \times 10^{-27} \times 2 \times 10^5}{1.6 \times 10^{-19} \times 0.02} = \frac{3.2 \times 10^{-22}}{3.2 \times 10^{-21}} = 0.1 \, \text{T} \).
Substituting \( B \) into \( E = vB \): \( E = 2 \times 10^5 \times 0.1 = 2 \times 10^4 \, \text{N/C} \).
The electric field magnitude is \( x \times 10^4 \, \text{N/C} \), with \( x = 2 \). This value falls within the specified range of 1 to 10.

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: