Electromagnetism - particle moving in magnetic field

[latentcorpse]

A amssive charged particle moves under the influence of a time varying magnetic field \mathbf{B}=B(r,t)\mathbf{\hat{z}}, where r is the distance from the z axis. Show that the particle can move in a circular orbit in a plane perpendicular to the field, accelerating and decelerating under the influence of the electric field induced by the temporal variation of the magnetic field, provided that the average value of the magnetic field inside the orbit is twice the magetic field at the orbit.

[i.e. if a is the radius of the orbit and \Phi(t) the flux through it, \frac{\Phi(t)}{\pi a^2}=2B(a,t)

I can't really get started on this one. any ideas?

 

[quantumdude]

Well if you're going to calculate the path of the electron then Newton's second law would be a good place to start, right? So what's the force on a charged particle that is subjected to both electric and magnetic fields?

 

[latentcorpse]

ok. yep, Lorentz force is \mathbf{F}=q(\mathbf{E}+|mathbf{v \wedge B}). We know B is in the z direction so the magnetic part of the force can't be in the z direction. I'm not sure about tackling the electric part, or how to express any of this argument mathematically though?

 

[Phrak]

2. Go back to Maxwell to get E.

 

[latentcorpse]

do you mean \int_C \mathfb{E \cdot dl}==-\frac{d \Phi}{dt} as i have an expression for \Phi?

 

[gabbagabbahey]

do you mean \int_C \mathfb{E \cdot dl}==-\frac{d \Phi}{dt} as i have an expression for \Phi?

That would be the one...

 

[quantumdude]

However I would have went with the differential form of that equation.

 

[latentcorpse]

ok. so we get

\nabla \wedge \mathbf{E}=-\frac{2}{\pi a^2} \frac{d \Phi(t)}{dt}

how do i solve this for E?

 

[gabbagabbahey]

What is curl(E) in cylindrical coords?

 

[latentcorpse]

ok i have that expression, how does that help me?
also surely in the equation i wrote in post 8, the rhs should have a direction? would it be the \mathbf{\hat{z}} direction? does that mean i just compare the z components of lhs and rhs to get the z component of E?

 

[gabbagabbahey]

ok i have that expression, how does that help me?

Compare components and integrate.

also surely in the equation i wrote in post 8, the rhs should have a direction? would it be the \mathbf{\hat{z}} direction? does that mean i just compare the z components of lhs and rhs to get the z component of E?

Yes, but I don't see any reason to use the flux instead of the magnetic field...

 

[Phrak]

Aren't you lucky! Three mentor types, helping out.

ok. so we get

\nabla \wedge \mathbf{E}=-\frac{2}{\pi a^2} \frac{d \Phi(t)}{dt}

how do i solve this for E?

You might be getting off track. You want the integral form you posted in #5. C, is the closed loop encompasing the magnetic flux, \Phi. The length of the loop is 2 \pi a of course.

(By the way, why do you represent the cross product with a wedge operator? I haven't seen that before. Doesn't that give you a 2-form?)

 

[latentcorpse]

ok,
1, as to the wedge product. my lecturer uses it, so i do. But yes, I'm also confused about that because I'm taking a course ind ifferential geometry and seeing as \vec{E} is a 1-form and we can consider \vec{\nabla} a 1-form, there wedge product should be a 2-form.

I have a couple of questions about this point:
(i) can we consider \vec{\nabla} as a vector and hence a 1-form?
(ii) is it true that a 2-form is different from a vector? if so, i will ask my lecturer why he's using this notation on Monday?

2, so |\vec{E}|2 \pi a=-2 \pi a^2 \frac{\partial{\vec{B}(\vec{r},t)}}{\partial{t}}

(i) \vec{dl} is an infinitesimal vector round the loop, correct? i.e. its in the \mathbf{\hat{\phi}} direction. How do we know \vec{E} is also in this direction? Surely if the electric field is induced by the magnetic field the only requirement is that it be in the plane perpendicular to B i.e. surely it could just as easily be in the \mathbf{\hat{r}} direction, in which case the dot product in the integral form of Maxwell equation would be 0 and hence game over?
(ii)I still can't see how to proceed without knowing what B is?

 

[gabbagabbahey]

2, so |\vec{E}|2 \pi a=-2 \pi a^2 \frac{\partial{\vec{B}(\vec{r},t)}}{\partial{t}}

This assumes that \vec{E} is uniform over the loop and points in the \mathbf{\hat{\phi}} direction (otherwise you can't pull it out of the integral). If you can't think of any justification for this assumption, then don't make it Try solving the PDE instead

 

[latentcorpse]

can you advise me on that question about the wedge product and differential forms at all?

also what PDE?

 

[gabbagabbahey]

I'm not sure about the wedge product, it's not notation that I'm familiar with.

As for the PDE, that is your curl(E) equation.

 

[Phrak]

Don't get too distracted by this business, but yes, \nabla can be, and is used as a one-form.

\nabla \wedge V = 2 \partial_{[i} V_{j]} = \partial_i V_j - \partial_j V_i = T_{ij}
U_k = (1/2) \epsilon_{ijk} T_{ij}

 

[latentcorpse]

ok. can i just ask where the factor of 2 comes from in \nabla \wedge V=2 \partial_i V_j

also, using this definition we get

\partial_i E_j - \partial_j E_j = - \frac{2}{\pi a^2} \frac{d \Phi}{dt}

how do i solve that? do i need to pick a coordinate system?

 

[Phrak]

If you're still interested in wedge products n stuf later, ask again.

But gabbagabbahey is right! you need the differential form. Phi just gets in the way. What was I thinking?

The only non zero electric field is in the tangential direction. What is E expressed in terms of B?

 

[gabbagabbahey]

\partial_i E_j - \partial_j E_j = - \frac{2}{\pi a^2} \frac{d \Phi}{dt}

how do i solve that? do i need to pick a coordinate system?

Try cylindrical coordinates instead. Compare the components of curl(E) with the components of dB/dt.

 

[gabbagabbahey]

The only non zero electric field is in the tangential direction.

If that were the case, the particle would not move in an orbit. The magnetic field would exert a force in the radial direction out to infinity. An radial component that cancels the magnetic force is necessary.

EDIT Actually there will be a non-zero radial acceleration, so E may or may not have a radial component. However, it will certainly not completely cancel the magnetic force.

 

[Phrak]

If that were the case, the particle would not move in an orbit. The magnetic field would push in the axial direction out to infinity. An axial component that cancels the magnetic force is necessary.

??

In cylindrical coordinates

Z -- axial
R -- radial
Theta -- tangential, or what would you call the theta direction?

 

[gabbagabbahey]

??

In cylindrical coordinates

Z -- axial
R -- radial
Theta -- tangential, or what would you call the theta direction?

Sorry, I meant radial not axial.

 

[Phrak]

Sorry, I meant radial not axial.

No problem. We know the radial component of the electric field must be zero without some centrally located charge. Gauss's Law.

\nabla \cdot E = 0

I'm assuming this all must work out somehow, without actually having solved this problem yet, gabbagabbahey, for no other reason than that betatrons have been built--and somehow have worked, so I hear.

 

[gabbagabbahey]

No problem. We know the radial component of the electric field must be zero without some centrally located charge. Gauss's Law.

\nabla \cdot E = 0

Hmmm, just because \vec{\nabla} \cdot \vec{E} = 0 doesn't necessarily mean that the radial component of E is zero does it?...What if E_r \propto \frac{1}{r}

I'm assuming this all must work out somehow, without actually having solved this problem yet, gabbagabbahey, for no other reason than that betatrons have been built--and somehow have worked, so I hear.

Indeed, I think I even have an old action figure of Betatron somewhere...or was that Galvatron?

 

[Phrak]

Hmmm, just because \vec{\nabla} \cdot \vec{E} = 0 doesn't necessarily mean that the radial component of E is zero does it?...What if E_r \propto \frac{1}{r}

Are you sure your not mixing up r and theta? E_theta is proportional to 1/r where the contained magnetic flux is the same independent of r.

So, you've driven me to look up the integral form, to make sure, which is

\oint_{S} E \cdot dA = Q / \epsilon

Any flux passing through the cylindrical surface sums to zero when Q is zero. By symmetry the flux is everwhere equal in magnitude, and therefore zero.

I have an unfair disadvantage having gone through something similar in regards to solenoids on this forum. I know I have a text on this matter that would settle the problem, but that would be no fun at all.

 

[latentcorpse]

\left(\frac{1}{r} \frac{\partial{E_z}}{\partial{\theta}} - \frac{\partial{E_{\theta}}}{\partial{z}}\right)\mathbf{\hat{r}} + \left(\frac{\partial{E_r}}{\partial{z}} - \frac{\partial{E_z}}{\partial{r}}\right) \mathbf{\hat{\theta}} + \frac{1}{r} \left[ \frac{\partial}{\partial{r}}\left(rE_{\theta}\right) - \frac{\partial{E_{r}}}{\partial{\theta}}\right] \mathbf{\hat{z}} = -\frac{\partial{B}}{\partial{t}}

who can we compare components though? we don't have an expression for B?

 

[gabbagabbahey]

Are you sure your not mixing up r and theta? E_theta is proportional to 1/r where the contained magnetic flux is the same independent of r.[/itex]

I'm sure. As an example, suppose we had \vec{E}=\frac{k\cos\theta}{r}\hat{r}+f(r)\hat{\theta}, would the divergence of that be non-zero?

So, you've driven me to look up the integral form, to make sure, which is

\oint_{S} E \cdot dA = Q / \epsilon

Any flux passing through the cylindrical surface sums to zero when Q is zero. By symmetry the flux is everwhere equal in magnitude, and therefore zero.

By what symmetry exactly? Just because the flux is zero (and it is), doesn't mean the fields can't have a non-zero radial component. Calculate for my above example if you don't believe me.

To be clear, I'm not saying that there has to be a non-zero radial field, I'm saying that there could be. Gauss' Law alone does not exclude this possibility.

 

[gabbagabbahey]

\left(\frac{1}{r} \frac{\partial{E_z}}{\partial{\theta}} - \frac{\partial{E_{\theta}}}{\partial{z}}\right)\mathbf{\hat{r}} + \left(\frac{\partial{E_r}}{\partial{z}} - \frac{\partial{E_z}}{\partial{r}}\right) \mathbf{\hat{\theta}} + \frac{1}{r} \left[ \frac{\partial}{\partial{r}}\left(rE_{\theta}\right) - \frac{\partial{E_{r}}}{\partial{\theta}}\right] \mathbf{\hat{z}} = -\frac{\partial{B}}{\partial{t}}

who can we compare components though? we don't have an expression for B?

Your told B points in the z-direction. \vec{B}=B(r,t)\hat{z}

 

[latentcorpse]

so, if we take, say the \phi component to start with, we get

\partial{E_r} \partial{r} = \partial{E_z} \partial{z}

we don't know what E_r,E_z are though so we can't carry out any integration can we?