To solve this problem, we need to determine the mass of a charged particle that passes undeflected through regions of both electric and magnetic fields acting perpendicular to each other. Given that the kinetic energy of the particle is \( K \), we must use the relationship between the velocity of the particle, the electric field \( \vec{E} \), and the magnetic field \( \vec{B} \). We know:
\(qE = qvB\)
Where \( q \) is the charge of the particle, \( v \) is the velocity of the particle. This implies:
\(v = \frac{E}{B}\)
\(K = \frac{1}{2}mv^2\)
Substitute the expression for velocity:
\(K = \frac{1}{2}m\left(\frac{E}{B}\right)^2\)
Simplify to find the mass \( m \):
\(2K = m\frac{E^2}{B^2}\)
\(m = \frac{2KB^2}{E^2}\)
Thus, the correct option is:
This verifies the chosen option as outlined in the question.
Consider two arrangements of wires. Find the ratio of magnetic field at the centre of the semi–circular part.