Motion of a charge in a magnetic field

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SUMMARY

The discussion focuses on the motion of a charged particle in a magnetic field, specifically analyzing a particle with charge q and mass m that starts from the origin with an initial velocity u=a i. The uniform magnetic field is defined as B=b/4 i + (sin 60)/2 j. Participants clarify that while the magnetic force has no component in the Y direction initially, the particle's motion will eventually produce a Y component due to the interaction of the magnetic field with the velocity vector as it moves in a circular path. The solution involves applying the Lorentz force law and solving the resulting differential equations to determine the velocity components over time.

PREREQUISITES
  • Understanding of Lorentz force law
  • Familiarity with vector calculus
  • Knowledge of differential equations
  • Concept of circular motion in magnetic fields
NEXT STEPS
  • Study the application of the Lorentz force law in electromagnetic theory
  • Learn how to solve differential equations related to motion in magnetic fields
  • Explore the concept of circular motion and its mathematical representation
  • Investigate the effects of varying magnetic fields on charged particles
USEFUL FOR

Physics students, electrical engineers, and anyone interested in the dynamics of charged particles in magnetic fields will benefit from this discussion.

harini_5
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A particle of charge q and mass m starts its motion from origin with u=a i.A uniform B=b/4 i + (sin 60)/2 j exists everywhere in space.Find the component of velocity in y direction when z coordinate of it becomes maximum

Sir, if I find the magnetic force,Its component is 0 in Y direction.With no force acting in Y direction ,how come its velocity changes??

then I thought that

I'm missing one step:the force is in z direction initially but when it starts going in a circular motion then the x component of the field will cross with velocity and produce a force which has a component in y direction.
please help me!

thanks in advance
 
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Treat your velocity as some unknown function of time: [itex]\vec{u}(t)=u_x(t)\hat{i}+u_y(t)\hat{j}+u_z(t)\hat{k}[/itex]. Then use the expression for the magnetic field and the Lorentz force law to find the equation of motion for the particle. Then solve that differential equation for [itex]\vec{u}(t)[/itex] and plug in the initial condition [itex]\vec{u}(0)=a\hat{i}[/itex]. Finally, find where the maximum of the z-component occurs.
 

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