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Electric and magnetic field are directed as `E_(0) hat(i)` and `B_(0) hat(k)`, a particle of mass m and charge + q is released from position (0,2,0) from rest. The velocity of that particle at (x,5,0) is `(5 hat(i) + 12 hat(j))` the value of x will be

A

`(169 m)/(2qE_(0))`

B

`(25 m)/(2qE_(0))`

C

`(25 m)/(12 qE_(0))`

D

`(144 m)/(12qE_(0))`

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The correct Answer is:
To solve the problem, we will apply the work-energy theorem, which states that the work done by the forces acting on a particle is equal to the change in its kinetic energy. ### Step-by-Step Solution: 1. **Identify the Given Information:** - Electric field \( \vec{E} = E_0 \hat{i} \) - Magnetic field \( \vec{B} = B_0 \hat{k} \) - Initial position of the particle: \( (0, 2, 0) \) - Initial velocity: \( \vec{v}_0 = 0 \) (released from rest) - Final position of the particle: \( (x, 5, 0) \) - Final velocity: \( \vec{v} = 5 \hat{i} + 12 \hat{j} \) 2. **Calculate the Final Kinetic Energy:** - The magnitude of the final velocity \( v \) is given by: \[ v = \sqrt{(5^2 + 12^2)} = \sqrt{25 + 144} = \sqrt{169} = 13 \, \text{m/s} \] - The final kinetic energy \( KE_f \) is: \[ KE_f = \frac{1}{2} m v^2 = \frac{1}{2} m (13^2) = \frac{1}{2} m (169) = \frac{169m}{2} \] - The initial kinetic energy \( KE_i \) is: \[ KE_i = 0 \quad (\text{since the particle is at rest}) \] 3. **Apply the Work-Energy Theorem:** - The work done by the electric field \( W_E \) and the magnetic field \( W_B \) is given by: \[ W_E + W_B = KE_f - KE_i \] - Since the work done by the magnetic field is zero (as it does no work on the charged particle), we have: \[ W_E = KE_f \] 4. **Calculate the Work Done by the Electric Field:** - The electric force \( \vec{F_E} \) acting on the particle is: \[ \vec{F_E} = q \vec{E} = q E_0 \hat{i} \] - The displacement in the x-direction is \( x - 0 = x \). - Therefore, the work done by the electric field is: \[ W_E = \vec{F_E} \cdot \vec{d} = (q E_0 \hat{i}) \cdot (x \hat{i}) = q E_0 x \] 5. **Set Up the Equation:** - From the work-energy theorem, we have: \[ q E_0 x = \frac{169m}{2} \] 6. **Solve for \( x \):** - Rearranging the equation gives: \[ x = \frac{169m}{2q E_0} \] ### Final Answer: The value of \( x \) is: \[ x = \frac{169m}{2q E_0} \]
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