Question:medium

When a proton is released from rest in a room, it starts with an initial acceleration $a_0$ towards west. When it is projected towards north with a speed $v_0$ it moves with an initial acceleration $3a_0$ towards west. The electric and magnetic fields in the room are:

Updated On: May 22, 2026
  • $ \frac{ma_0}{e} east, \frac{3ma_0}{ev_0} down$
  • $ \frac{ma_0}{e} west, \frac{2ma_0}{ev_0} up$
  • $ \frac{ma_0}{e} west, \frac{2ma_0}{ev_0} down$
  • $ \frac{ma_0}{e} east, \frac{3ma_0}{ev_0} up$
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The Correct Option is C

Solution and Explanation

To determine the electric and magnetic fields in the room, we need to analyze the motion of the proton under the given conditions.

  1. Analyzing Initial Condition:
    • When the proton is released from rest, it experiences an initial acceleration $a_0$ towards the west. This indicates the presence of an electric field $\vec{E}$ in the room.
    • The force on the proton due to the electric field is given by $F = eE$, where $e$ is the charge of the proton.
    • Using Newton's second law, $F = ma_0$, we equate it to the electric force: $eE = ma_0$.
    • Thus, the electric field is $E = \frac{ma_0}{e}$ and it is directed towards the west.
  2. Analyzing Second Condition:
    • When the proton is projected towards the north with speed $v_0$, it has an initial acceleration of $3a_0$ towards the west.
    • The additional acceleration of $2a_0$ (since the total is $3a_0$ and from the electric field is already $a_0$) must be due to the magnetic field.
    • For a charged particle in a magnetic field, the magnetic force is given by $F = evB$, where $v$ is the velocity and $B$ is the magnetic field.
    • The magnetic force causes an acceleration of $2a_0$, so: $$ ev_0B = m \cdot 2a_0 $$
    • This gives the magnetic field as: $$ B = \frac{2ma_0}{ev_0} $$.
    • Using the right-hand rule and given that the force is directed west while the velocity is north, the magnetic field must be directed downwards.
  3. Conclusion:
    • The electric field in the room is $ \frac{ma_0}{e}$ directed west.
    • The magnetic field in the room is $ \frac{2ma_0}{ev_0}$ directed down.
    • Thus, the correct answer is: $ \frac{ma_0}{e} \text{ west, } \frac{2ma_0}{ev_0} \text{ down}$.
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