\( 4:1 \)
Step 1: Work done by an electric field
The work done by an electric field on a charged particle is given by: \[ W = q V \] where: - \( W \) is the work done, - \( q \) is the charge of the particle, - \( V \) is the potential difference through which the particle is accelerated.
Step 2: Charge of proton and \( \alpha \)-particle
- The charge of a proton is \( q_p = +e \). - The charge of an \( \alpha \)-particle (which is a helium nucleus) is \( q_\alpha = +2e \).
Step 3: Work done on each particle
Since both the proton and the \( \alpha \)-particle are accelerated in the same electric field, they experience the same potential difference \( V \). The work done on each is: \[ W_p = eV \] \[ W_\alpha = 2eV \]
Step 4: Work done over a given time
The kinetic energy gained by the particles is given by: \[ KE = W \] Since both particles start from rest, their velocities will be different due to their different masses, but the total work done depends only on charge and voltage. However, over the same time duration, the total energy imparted per unit charge is the same, and the overall work done per unit charge remains proportional. Thus, over a given time, the ratio of work done on the proton and the \( \alpha \)-particle remains: \[ \frac{W_p}{W_\alpha} = \frac{eV}{eV} = 1:1 \]
Two point charges +q and −q are held at (a, 0) and (−a, 0) in x-y plane. Obtain an expression for the net electric field due to the charges at a point (0, y). Hence, find electric field at a far off point (y ≫ a).
Match the following: