The energy isn't conserved here Is there any thing wrong?

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The discussion centers on the behavior of a charged particle moving through an electric field created by a capacitor and its interaction with a metal box. It highlights that while the particle gains kinetic energy when moving through the electric field, the energy conservation principle must consider the entire system, including the effects of electrostatic shielding when the particle is inside the metal box. Participants clarify that the electric field between the capacitor plates and the box can indeed exist, and its strength is influenced by the configuration of the setup. The conversation also touches on the concept of "ramping," where energy input is necessary to maintain acceleration, and the limitations of electrostatic shielding when there are openings in the box. Overall, the discussion emphasizes the complexities of electric fields and energy conservation in these systems.
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The red dot represents a positively charged particle, the blue box represents a metal box, and the two dark green lines represent a capacitor, which has been charged. Each plate of the capacitor has a slit which will let the particle get through without touching the plates. And the capacitor doesn’t contact with the metal box either.

When the particle moves from A to B, it will be accelerated by the electric field. And its kinetic energy will increase.

When the particle is in the metal box, the electric field has no effects on the particle because of electrostatic shielding. So it consumes no energy to move the particle from B to A via C, D, and E.

Then, the particle will move from A to B through the electric field again, and its kinetic energy will increase again.

But in the whole process, it doesn’t need to produce work to keep the electric field, or to keep something else. So the energy except the kinetic energy of the particle doesn’t change. So the sum of energy increases.

Is there anything wrong?

(I am a foreigner, and my English is not very well,I hope you can understand what I write.)
 
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I can't see your picture, but I'll try to explain.

When then electron is accelerated, the equipment excerts a torque on the earth, changing it's angular momentum. Energy is conserved, you were just not concidering a complete system.
 
cometzir said:
When the particle is in the metal box, the electric field has no effects on the particle because of electrostatic shielding. So it consumes no energy to move the particle from B to A via C, D, and E.

Then, the particle will move from A to B through the electric field again, and its kinetic energy will increase again.

Yeah, that's called ramping. Done all the time. However, the energy required to induce ramping is greater than the energy of the output.
 
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espen180 said:
When then electron is accelerated, the equipment excerts a torque on the earth, changing it's angular momentum. Energy is conserved, you were just not concidering a complete system.

So, it is different from the cyclotron, for the electric field passes through a diameter of the circle rather than a radius. So the equipment excerts two opposite torque on the Earth per cycle, and doesn't chang its angular momentum. So the equipment can be regarded as a complete system, but the changing electric field will consume energy. Is it right?

But the electric field of the cyclotron is produced by the two metal box rather than another capacitor. Are there any differences between the electric field of the two equipment?
 
pallidin said:
Yeah, that's called ramping. Done all the time. However, the energy required to induce ramping is greater than the energy of the output.

Could you please tell me something about the "ramping"? I don't know much about it.
Do you mean that the particle needs more energy to leave the electric field?
 
Here is the picture
 

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The picture was helpful. If you add up the electric potential around the loop, the net electrical potential is unfortunately zero, for those looking for free energy.
 
There is a very sudden change in potential from outside the plates to between the plates. This sudden change in potential undoes the gain in kinetic energy that you get from accelerating between the plate. It is like rolling down a hill into slightly inclined wall of the same height.
 
cometzir said:
When the particle is in the metal box, the electric field has no effects on the particle because of electrostatic shielding. So it consumes no energy to move the particle from B to A via C, D, and E.
Hi cometzir. You understand that a metal box shields from electric fields becasue it is an equipotential surface (which is just another way of saying that all points in the metal are at the same voltage).

Now by definition the two plates on the charged capacitor must be at different potentials (from each other) therefore there must be an electric field between at least one of the capacitor plates and the box, and this is what creates the retarding electric field that DaleSpam refers to.

Hope that helps. :)
 
  • #10
So, there is another opposite electric field.But where is it? Is it in the metal box, or in the plate inside? If it is in the metal box, the electric field strength inside the box will not be zero. Is it possible?
 
  • #11
cometzir said:
So, there is another opposite electric field.But where is it? Is it in the metal box, or in the plate inside? If it is in the metal box, the electric field strength inside the box will not be zero. Is it possible?

The opposing electric field is between the capacitor plates and the metal box. This is very straight forward.
 
  • #12
uart said:
The opposing electric field is between the capacitor plates and the metal box. This is very straight forward.

If the capacitor is out of the box, the opposing electric field can be like the red line in graph 1, but if the capacitor is on the border of the box like graph 2, or even in the box like graph 3, can you draw the opposing eletric field line?
 

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  • #13
Figure 1. Yes that's how it is, neither of the other options shown can work the way you want them to.

Figure 2. If the plates are in contact with the box then all you have is a short circuit and hence no E field. Reason : Box is a conductor, plates of capacitor are conductors, and they're touching. Doh, that should have been pretty obvious to you!

Remember that if you place any insulation layer at all between the box and the plates then you just end up with the first case (figure 1) above.

3. If the capacitor is inside the box (as per 3rd picture) then it will shield the E field from exiting the box and there will definitely still be a field inside the box.
 
  • #14
Also, one thing that you should keep in mind is that the approximation of the E-field in a capacitor as being entirely between the plates and uniform is just that, an approximation. In particular, it fails near the edges and on the outside the capacitor field looks similar to a dipole.
 
  • #15
Thank you for your detailed answers.
I know it is impossible to let the equipment in the 1st and 3rd picture work. But in the 2nd pictrue, the pates can be smaller and aren't in contact with the box,as the following picture shows,if so ,where is the apposing E field?

For approximation, I know the E field isn't perfectly like the straight line.But between the two plates, I don't think there can be a apposing E field.
But I don't know whether the Electrostatic shielding is a approximation, in other words, whether there can be E field in the box if the plate isn't in the box.
 

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  • #16
cometzir said:
in the 2nd pictrue, the pates can be smaller and aren't in contact with the box,as the following picture shows,if so ,where is the apposing E field?
If the plates are not in contact with the box then the opposing E-field is between the plates and the box. If the plates are in contact with the box then the capacitor discharges and there is no E-field. You cannot have both a gap in order to have an E-field and no gap in order to avoid the opposing E-field.
 
  • #17
It is true there can be an E field between the plate and the box, but in the second situation ,if the plate is not in contact with the box, the opposing E field will be perpendicular to the E field between the plate, even though the e field line isn't straight, it won't be "opposing".
 
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  • #18
I have no idea what you are saying here, but it does not really matter. In the Coulomb gauge for electrostatics we have:

\nabla^2V=-\frac{\rho}{\epsilon_0}

Which means that it does not matter how you arrange the charges \rho, you will always get a field that can be represented as the gradient of a scalar potential V. That automatically guarantees that the field is conservative. The fields simply don't behave the way you think.
 
  • #19
cometzir said:
It is true there can be an E field between the plate and the box, but in the second situation ,if the plate is not in contact with the box, the opposing E field will be perpendicular to the E field between the plate, even though the e field line isn't straight, it won't be "opposing".

No the field won't just take the shortest (perpendicular) route to the box, it will be more like the situation in my attachment. (Which is extremely crude and not possible to show accurately in two dimensions but I hope it helps give you some sort of idea of a more realistic field pattern. Also I only "fixed up" the right hand portion.)
 

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  • #20
So the intensity of electric field in the box isn't zero even if the plate isn't in the box, and the electrostatic screen is just a approximation. Is it right?
 
  • #21
cometzir said:
So the intensity of electric field in the box isn't zero even if the plate isn't in the box, and the electrostatic screen is just a approximation. Is it right?

No, not in your example. Yes a fully enclosed perfect conductor will fully shield electric field from the interior but you've got a great big hole cut into the box and an E field source sitting right at the opening!

Consider this analogy. A fully closed opaque box will keep all light out of the box right. Now if you cut two big holes in the box and place lights right smack in the middle of those holes will it still be totally dark on the box interior. Of course not!
 
  • #22
uart said:
No, not in your example. Yes a fully enclosed perfect conductor will fully shield electric field from the interior but you've got a great big hole cut into the box and an E field source sitting right at the opening!

Consider this analogy. A fully closed opaque box will keep all light out of the box right. Now if you cut two big holes in the box and place lights right smack in the middle of those holes will it still be totally dark on the box interior. Of course not!

But a Metal Masks can also shield the E field, and there are many holes.
The metal box of the cyclotron also has holes, but it can also shield the E field.
 
  • #23
cometzir said:
But a Metal Masks can also shield the E field, and there are many holes.
The metal box of the cyclotron also has holes, but it can also shield the E field.
If you've got holes then you've only got partial shielding. A shield with holes (like a mesh) can still be very effective if the charges are not placed too close, but I guarantee that if you place a source right smack in the middle of one of these holes then E field will definitely penetrate the interior.

Similarly for shielding against EM waves (eg RFI). The shield can have holes and still be very effective, but if the wavelength of the RFI is short compared with the dimensions of the holes then the shield becomes ineffective. An example of this that most people can readily experience is driving through a small "steel truss" type bridge while listening to the radio. FM stations (which typically have a wavelength of around 3m) will usually still be received but if you try an AM station (much longer wavelength) then you'll usually have a great difficulty getting a signal.
 
  • #24
Thank you.
Another thing, think about the Linear Accelerator, it has many pair of plates. Are there any opposing E fields between the plates as the picture shows?
And why is there no E field in the metal box of the cyclotron?
 

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  • #25
cometzir said:
Thank you.
Another thing, think about the Linear Accelerator, it has many pair of plates. Are there any opposing E fields between the plates as the picture shows?
And why is there no E field in the metal box of the cyclotron?

Re the linac, yes there is opposing E field as shown in your diagram, and this is exactly why it wouldn't work properly if it was supplied with DC voltage. A linear accelerator uses very high frequency AC voltage to supply the plates so that the E field continually changes direction as the particles travel along the various regions of the tube. In other words, what would have been an opposing E field has actually reversed (due to the ac supply) by the time the accelerated particles arrive there.

Re the cyclotron. Are you referring to the "D" electrodes and the fact that there is a strong E field in the gap between the two "D" halves but no electric field within the D's themselves? Again that's only an approximation, some of the E field definitely will fringe into those slotted D's.
 
  • #26
Thank you, I think I have understand it.
 
  • #27
But how could the Linear Accelerator control the change of the E field? Does it take the same time for the particle travel from one plate to another?
 
  • #28
cometzir said:
But how could the Linear Accelerator control the change of the E field? Does it take the same time for the particle travel from one plate to another?

That's why they have electrodes of increasing length along the tube as the speed increases. If the particles reach near c speeds then increasing energy doesn't change the speed very much and the electrodes may then be of similar length.
 
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