Find Integrals of Motion for Particle in Magnetic Dipole Field

AI Thread Summary
To find the first integrals of motion for a particle in a magnetic dipole field, one should compute the vector potential A in cylindrical coordinates and apply Lagrangian mechanics to derive the equations of motion. The magnetic dipole moment, represented as a vector, is a constant that should be included in the calculations without needing to change its direction arbitrarily. The scalar potential is specified as zero to clarify the problem's conditions, indicating no additional potential energy is involved. While cylindrical coordinates can simplify the analysis, it is advisable to derive as much as possible without committing to a specific coordinate system initially. Understanding the relationship between the magnetic dipole and the particle's motion is crucial for solving the problem effectively.
Mumba
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Find the fi rst integrals of motion for a particle of mass m and charge q in a magnetic field given by the vector potential (scalar potential \Phi= 0)

(i) of a constant magnetic dipole m_{d}

A=\frac{\mu_{0}}{4 pi}\frac{m_{d} \times r}{r^{3}}

Hint: Cylindrical coordinates are useful.


I think what i should do is to compute A for cylindrical coordinate system and then use Lagrangian mechanics to get a equation of motion? Is this correct? (we have the charge q given, so we can use the kinetic engergy?)

I tried to compute A but i don't really understand what to do with the magnetic dipole (as a vector)? Whats the story whith that scalar potential?

Thanks for your help,
Mumba
 
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Mumba said:
I think what i should do is to compute A for cylindrical coordinate system and then use Lagrangian mechanics to get a equation of motion? Is this correct? (we have the charge q given, so we can use the kinetic engergy?)
That would probably be my first thought as well. But I wouldn't write A in cylindrical coordinates just yet. Try to go as far as you can without expressing it in any particular coordinate system.
Mumba said:
I tried to compute A but i don't really understand what to do with the magnetic dipole (as a vector)? Whats the story whith that scalar potential?
\vec{m}_d is just a given vector. You don't really do anything with it, except carry it through the calculation. And I think they just tell you that the scalar potential is zero to clarify the conditions of the problem... I can't imagine why you would think that the scalar potential would be nonzero, unless you were specifically told so.
 
Hi Thanks for the answer.

But i can't go very far without a coordinate system, can I?
I mean, using cyl. coordinates, my degrees of freedom would be just R and \Theta.

So i can get the components of r=(Rcos\Theta, Rsin\Theta, z), where the z-axis is pointing upwards and \Theta the angle between the x-axis (pointing towards you) and R.

What can i do with m_{d}? Should be a vector so i can't really just set it on the origin?! Can i give it an arbitrary direction, say m_{d}=(m_{d},0,0)?

Thanks,
Mumba
 
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