Increase in energy in an electric field

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Discussion Overview

The discussion revolves around the behavior of an electron moving between two oppositely charged plates and the implications for energy conservation and kinetic energy increase. Participants explore theoretical aspects of electric fields, potential energy, and the dynamics of charged particles in a non-connected system.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions how an electron can gain kinetic energy when it escapes the region between charged plates that are not connected to a power source.
  • Another participant suggests that the plates would experience a reaction force, implying that the system as a whole can still account for energy changes.
  • Concerns are raised about the application of Gauss' law and how it relates to the electric field experienced by the electron.
  • Some participants argue that the electron's motion is analogous to projectile motion, maintaining that its horizontal component remains constant while it gains vertical motion due to the electric field.
  • There is a discussion about the conservation of energy, with some participants asserting that the electron's initial and final kinetic energies should be equal, while others propose that potential energy changes must be considered.
  • One participant suggests that the increase in kinetic energy could be explained by the work done against a net field acting on the electron.
  • References to textbooks are made, with some participants expressing confusion over differing interpretations of energy dynamics in this context.

Areas of Agreement / Disagreement

Participants express differing views on the conservation of energy in this scenario, with no consensus reached. Some argue that energy is conserved while others suggest that potential energy changes must be accounted for, leading to ongoing debate.

Contextual Notes

Participants note the limitations of applying Gauss' law in this context and the assumptions made regarding the symmetry of the electron's trajectory. The discussion also highlights the complexities involved in analyzing energy changes in non-ideal systems.

Who May Find This Useful

This discussion may be of interest to students and educators in physics, particularly those exploring concepts of electric fields, energy conservation, and the dynamics of charged particles in theoretical frameworks.

Mr.4
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I was explaining the construction of Thomson's apparatus for determination of specific charge for an exam today and suddenly something popped up:

Consider 2 oppositely charged plates held using insulated handles (They're not connected to a battery). If an electron moving with a velocity v passes perpendicular to this field then it will experience a force eE causing it to accelerate towards the positive plate. Suppose v is such that the electron escapes the volume between the plates before it can reach the positive plate. Thus the electron leaving the area between the plates would have a greater kinetic energy because the magnitude of v vector would have increased. How can one account for this energy? The plates could not have lost any energy since they are not connected to a cell or allowed to move. And the net field outside the plate system would be zero from Gauss law. Then where did this extra energy come from?!
 
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It's easy to see how to balance the momentum: the plates will be electrostatically pushed in the opposite direction, so claiming they aren't "allowed to move" just means the entire support is pushed as well. As for energy, which other of your statements may be faulty?

Gauss' law is only useful given a higher degree of symmetry, since the net field doesn't tell you what the field at every point is like. When the electron travels through the finite plate system, it first approaches from a little bit closer to the negative side (so, is a little repulsed from approaching at all) and leaves from a little bit closer to the positive plate (vainly attracting it to not leave at all).

So sure, the electron gains a second component to its motion. But since the first component of its motion is decreased in your scenario, you have not demonstrated that the electron escapes with any extra energy.
 
What happened to accounting for potential energies?
 
@cesiumfrog what if the electron is approaching symmetrically from infinity. There would be a point midway between the plates where potential is zero.

And are you sure that a considerably large apparatus would move?!

And no the first component is not decreased. The motion in the electric field is parabolic and analogous to projectile motion under gravity so that horizontal component always remains constant. But unlike projectile motion the electron doesn't come back to 'ground' level in projectile motion. I hope I'm clear.
 
Mr.4 said:
@cesiumfrog what if the electron is approaching symmetrically from infinity. There would be a point midway between the plates where potential is zero.
Yes, but even if it approaches along that mid-surface, it will not leave along the same surface; the point is that the force as it departs will not be canceled by the force as it approaches.

Mr.4 said:
And are you sure that a considerably large apparatus would move?!
Momentum is conserved, but for a large apparatus (compared to an electron) this produces neglegible velocity (and, in the limit, removes no energy). It is actually not relevant to your main question.

Mr.4 said:
And no the first component is not decreased. The motion in the electric field is parabolic and analogous to projectile motion under gravity so that horizontal component always remains constant. But unlike projectile motion the electron doesn't come back to 'ground' level in projectile motion. I hope I'm clear.
You are only considering the motion while the electron is between the two plates (and you are approximating those plates as infinite). You should also consider the motion when the electron is not between the plates (and notice that there will still be an electric field, which also isn't completely perpendicular to the plates).

I thought it would be redundant to quote the laws of thermodynamics, since I assumed you had realized that energy must be conserved (and therefore, the reasoning that suggested otherwise to you is flawed). Was I mistaken?
 
Of course I'm aware of the conservation of energy (and hence the question!). But do the math. I've referred multiple textbooks and they all suggest that when the magnitude of the leaving velocity will be greater anyhow. But back to my original question: Where does this energy come from?

From some of your statements I'm concluding that there must have been a net field acting on the electron against which we had to work to bring it to the initial path. This work would account for the increase in kinetic energy after moving through the field. Is that true?!
 
Mr.4 said:
But do the math. I've referred multiple textbooks and they all suggest that when the magnitude of the leaving velocity will be greater anyhow. But back to my original question: Where does this energy come from?

From some of your statements I'm concluding that there must have been a net field acting on the electron against which we had to work to bring it to the initial path. This work would account for the increase in kinetic energy after moving through the field. Is that true?!

No, I was not considering whether work must be done to put the electron on its initial path; I'm arguing that the electron's initial kinetic energy (far before the plates) will be exactly equal to the electron's final kinetic energy (far after the plates). Hence, as no energy is gained, there is also no place for it to have come from. Since this seems to contradict what your textbooks suggest, would you mind giving the references?
 
cesiumfrog said:
No, I was not considering whether work must be done to put the electron on its initial path; I'm arguing that the electron's initial kinetic energy (far before the plates) will be exactly equal to the electron's final kinetic energy (far after the plates).
Not unless the trajectory is symmetric with respect to the mid-plane normal to the plates and the plane of motion. The electron's total energy is conserved, not its kinetic energy. After entering the region between the plates, the electron exits in a manner that puts it closer to the positive plate (than the negative one). It loses PE as a result.

PS: Just noticed the qualifier "far", in which limit, the above statement is, indeed true.
 
Gokul43201 said:
PS: Just noticed the qualifier "far"
yup, but now I realize what the textbook might have been saying. Sounds like Mr4 just needs to find a picture of the electric field outside of a (finite) parallel plate capacitor.
 
  • #10
cesiumfrog said:
yup, but now I realize what the textbook might have been saying. Sounds like Mr4 just needs to find a picture of the electric field outside of a (finite) parallel plate capacitor.

Duh, that's what i was saying in my previous posts. I'm referring some Indian textbooks namely HC verma and Nootan ISC physics (+2).

I agree with Gokul's statement but then what does the far have to do with anything if the K.E, P.E distribution is modified.
 
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