Differential Equation with Vector Product

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SUMMARY

The discussion centers on proving that the speed \( v \equiv \left| \frac{d\vec{r}}{dt} \right| \) of a charged particle in an arbitrary magnetic field remains constant, as described by the differential equation \( m\frac{d^2\vec{r}}{dt^2} = \frac{e}{c}\frac{d\vec{r}}{dt} \times \vec{H} \). Participants emphasize that the acceleration affects only the direction of the velocity vector, not its magnitude. Key insights include using the dot product to demonstrate that the change in speed is zero, leveraging the property that the vector \( \vec{v} \times \vec{H} \) is always perpendicular to \( \vec{v} \).

PREREQUISITES
  • Understanding of vector calculus and differential equations.
  • Familiarity with the concepts of magnetic fields and charged particle dynamics.
  • Knowledge of vector products and their properties in physics.
  • Basic grasp of classical mechanics, particularly circular motion.
NEXT STEPS
  • Study the properties of vector products in differential equations.
  • Learn about the implications of the Lorentz force on charged particles in magnetic fields.
  • Explore the concept of conservation of angular momentum in magnetic fields.
  • Investigate the mathematical techniques for handling cross products in calculus.
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Students and professionals in physics, particularly those focusing on electromagnetism and classical mechanics, as well as anyone interested in the dynamics of charged particles in magnetic fields.

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If a particle with charge e and mass m is in an arbitrary magnetic field has motion described by:

m\frac{d^2\vec{r}}{dt^2}=\frac{e}{c}\frac{d\vec{r}}{dt}\times\vec{H}

prove that the speed v\equiv\left\vert\frac{d\vec{r}}{dt}\right\vert is constant.

I don't understand how to do this when the field isn't necessarily constant.
Any suggestions would be greatly appreciated. Thanks!
 
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Vector Product Differential Equation

If a particle with charge e and mass m is in an arbitrary magnetic field has motion described by:

m\frac{d^2\vec{r}}{dt^2}=\frac{e}{c}\frac{d\vec{r} }{dt}\times\vec{H}

prove that the speed v\equiv\left\vert\frac{d\vec{r}}{dt}\right\vert is constant.

I don't understand how to do this when the field isn't necessarily constant.
Any suggestions would be greatly appreciated. Thanks!

i posted this elsewhere here but after browsing the site i thought this was a more appropriate place to put it...
 


Does it specify a variable or constant field?

The fact that the speed is constant means that any acceleration is involved in changing the direction rather than tangential velocity.
 


Astronuc said:
Does it specify a variable or constant field?

The fact that the speed is constant means that any acceleration is involved in changing the direction rather than tangential velocity.

it just says arbitrary, so I'm assuming it means it could be variable or constant (it's definitely not reliably constant because the next question is "assuming the field is a constant")

i tried using circular motion with it for the constant speed, but i didn't understand how to apply it using vector products in differential equations.
 


I would start by finding

\frac {d}{dt} \left| \frac{d \vec r}{dt} \right|

Then you should be able to show, from your available equations, that the above expression is zero.

Note that in general, the vector v x H is always perpendicular to v. This should be enough to prove what you want.
 
what happens if you take the dot product with dr/dt?
to the right side? (should get 0).
to the left side? (do you recognize a complete derivative?)
 
qbert said:
what happens if you take the dot product with dr/dt?
to the right side? (should get 0).
to the left side? (do you recognize a complete derivative?)
I don't see how that helps, don't you get 0 on the left hand side as well since a vector and its derivative are perpendicular?
 
A vector and its derivative are NOT necessarily perpendicular. That is true only if the vector has constant length- which is what you are trying to prove.
 
  • #10
i tried to find \frac{d}{dt}\left\vert\frac{d\vec{r}}{dt}\right\vert but i don't know how to handle a diff eq with a vector product in it - i understand in theory how proving all the above mentioned things would work, my main question was how to handle a cross product in a differential equation... i looked in all my textbooks and on all sorts of websites and nothing helped.
 
  • #11
For the question in the original post, qbert (post #6) has given, in my opinion, the best hints.
 
  • #12
ah yes, i got it.
i was so caught up in the diff eq part of it i forgot about simple vecor analysis. i always make things more complicated than they are :/
thank you so much everyone for your help, particularly qbert, your hint really helped :)
 
Last edited:
  • #13
Here you can find the answer of your question
http://www.iop.org/EJ/abstract/0953-4075/42/5/055504/
this Is Stimulated Raman adiabatic passage analogues in classical physics
or here in the arxiv
http://arxiv.org/abs/0812.0361
 
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