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Question: A charged particle is moving perpendicular to a uniform magnetic field. What will be the path of the...

A charged particle is moving perpendicular to a uniform magnetic field. What will be the path of the

Answer

Circle

Explanation

Solution

  • Lorentz Force: When a charged particle with charge qq moves with velocity v\vec{v} in a uniform magnetic field B\vec{B}, it experiences a magnetic force given by the Lorentz force formula: F=q(v×B)\vec{F} = q(\vec{v} \times \vec{B})

  • Direction of Force: Since the particle is moving perpendicular to the magnetic field (vB\vec{v} \perp \vec{B}), the angle between v\vec{v} and B\vec{B} is 9090^\circ. The magnitude of the force is F=qvBsin(90)=qvBF = |q|vB \sin(90^\circ) = |q|vB. The direction of this force is always perpendicular to both v\vec{v} and B\vec{B}.

  • Work Done by Magnetic Force: Because the magnetic force F\vec{F} is always perpendicular to the velocity v\vec{v} of the particle, the work done by the magnetic force on the particle is zero (W=Fvdt=0W = \vec{F} \cdot \vec{v} dt = 0). This implies that the kinetic energy of the particle remains constant, and thus its speed (v|\vec{v}|) remains constant.

  • Centripetal Force: A force that is always perpendicular to the velocity and has a constant magnitude, causing the particle to move with constant speed, acts as a centripetal force. This force continuously changes the direction of the velocity without changing its magnitude.

  • Circular Motion: For uniform circular motion, the centripetal force required is Fc=mv2rF_c = \frac{mv^2}{r}, where mm is the mass of the particle and rr is the radius of the circular path. Equating the magnetic force to the centripetal force: qvB=mv2r|q|vB = \frac{mv^2}{r} Solving for the radius rr: r=mvqBr = \frac{mv}{|q|B} Since mm, vv (constant speed), q|q|, and BB (uniform field) are all constant, the radius rr of the path is constant.

Therefore, the charged particle will follow a circular path.