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A charged particle is released from a re...

A charged particle is released from a rest in a region, having steady and uniform electric and magnetic fields . If the two fields are parallel to each other, Then the path of the particle will be :

A

ellipse

B

circle

C

helix

D

straight line

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to analyze the forces acting on a charged particle released from rest in a region with uniform electric and magnetic fields that are parallel to each other. ### Step-by-Step Solution: 1. **Understanding the Initial Conditions**: - The charged particle is initially at rest, meaning its initial velocity \( v = 0 \). - The electric field \( \vec{E} \) and magnetic field \( \vec{B} \) are parallel to each other. **Hint**: Remember that the forces acting on the charged particle depend on its initial state (rest in this case). 2. **Identifying the Forces**: - When a charged particle is placed in an electric field, it experiences an electric force given by: \[ \vec{F_E} = q \vec{E} \] - Since the particle is at rest initially, the magnetic force, which is given by: \[ \vec{F_B} = q (\vec{v} \times \vec{B}) \] will be zero because the velocity \( \vec{v} = 0 \). **Hint**: Recall that the magnetic force depends on the velocity of the charged particle. 3. **Motion Due to Electric Force**: - The electric force \( \vec{F_E} \) will cause the particle to accelerate in the direction of the electric field. - As the particle starts moving under the influence of the electric force, it gains velocity. **Hint**: The direction of the electric force is crucial as it determines the direction of motion of the particle. 4. **Analyzing the Motion**: - As the particle accelerates, its velocity becomes non-zero. However, since the magnetic field is parallel to the electric field, the angle \( \theta \) between the velocity vector and the magnetic field remains zero degrees. - The magnetic force can be expressed as: \[ \vec{F_B} = qvB \sin(\theta) \] Since \( \theta = 0 \), \( \sin(0) = 0 \), thus \( \vec{F_B} = 0 \). **Hint**: The relationship between the velocity vector and the magnetic field is key to understanding the absence of magnetic force. 5. **Conclusion on the Path of the Particle**: - Since the magnetic force is zero, the only force acting on the charged particle is the electric force. - Therefore, the charged particle will continue to move in a straight line in the direction of the electric field. **Hint**: The absence of a magnetic force means the particle does not experience any deviation from its path. ### Final Answer: The path of the charged particle will be a **straight line**.
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