Electric field lines next to conductor

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Discussion Overview

The discussion revolves around the behavior of electric field lines near a conductor placed next to a surface-charged rectangle. Participants explore the implications of surface charge on the electric field, the effects of the conductor, and the accuracy of simulation results.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant suggests that the electric field lines terminate on the conductor, leading to charge accumulation on its surfaces.
  • Another participant asserts that the electric field must be perpendicular to the surface of the conductor, with the parallel component vanishing at the surface.
  • A different viewpoint questions the simulation's accuracy, stating that the conductor should show a separation of charge due to the influence of the surface charge on the adjacent rectangle.
  • Concerns are raised about the representation of electric field lines in the simulation, with one participant noting that the field should not enter the conductor.
  • Discussion about the simulation software used (COMSOL) and its ability to accurately depict charge distribution and field intensity.
  • Some participants emphasize the importance of showing field intensity along with direction to avoid misinterpretation of the field behavior.
  • One participant proposes a simplified view of the electric field distribution based on textbook physics, suggesting that the field is nearly homogeneous between the plates and behaves similarly to a single charged object far away.

Areas of Agreement / Disagreement

Participants express differing views on the accuracy of the simulation and the behavior of electric field lines near the conductor. There is no consensus on the correct representation of the electric field or the implications of the surface charge and conductor interaction.

Contextual Notes

Limitations include the lack of clarity on the simulation's depiction of charge distribution and field intensity, as well as the potential for misinterpretation of the electric field behavior without intensity data.

mzh
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Dear Physics Forums readers
Let a two dimensional rectangle R1 carry a surface charge \sigma and be placed next to another rectangle R2 of the same shape made from metal (i.e. a conductor). What does the electric field look like close to the second rectangle?

My intuition would tell me, the field lines terminate on the close side of R2, causing accumulation of negative charge on the side close to R1 and positive charge on the far side which in turn emits a field. The net field could be seen as reaching through R2.

I tried to verify this using a finite element simulator and obtained the following image for the field (R1 left, R2 right):
field-metal.png


Now it seems to me as if the field goes around the metal. Is that correct? Or can the field only terminate *on* opposite charges?
 
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Or can the field only terminate *on* opposite charges?
It has to - a surface charge corresponds to electric field lines perpendicular to the surface.
In addition, the parallel component of the field has to vanish at the surface (the potential is constant).
 
It seems to me that the simulation is incorrect. The positive charge of the object on the left should induce a separation of charge in the object (conductor) on the right, so that its left surface acquires a negative charge and its right surface acquires a positive charge. The net charge of the conductor would of course remain zero. The electric field close to those surfaces would not be parallel to those surfaces.
 
It doesn't look right to me (But I've always had a blind spot when it comes to field lines)

The electric charges inside the conductor rearrange themselves slightly in such a way as to neutralise the field at the surface. The field is prevented from entering the conductor.

I would have expected the lines to terminate on the surface charge and start again from the other side as you did.

There's no intensity variation shown in the diagram, only directions - that may be the problem.
 
mzh - what kind of simulation software was it? Field patterns look awfully like fluid flow to me - with LHS rectangle acting as a source, and RHS rectangle simply as an obstacle. Fluid flow then has to be pretty slow to avoid vortices around RHS rectangle. And btw it would have been better to have labelled the rectangles in pic, specified sign of charge, and that charge distribution was either fixed or formed an equipotential on the source rect. But a nice idea to provide a pic that can be viewed without needing to log in first.
 
Thanks guys for the feedback.
@mfb: Ok. And can it also terminate on induced charges?
@{jtbell,AJ Bentley}: that's exactly what i was expecting. In the simulator, R2 is assigned a "metal" property. But I don't know if it can plot the actual charge distribution. Yeah, did not show the intensity of the field, but its of secondary importance to me currently.
@Q-reeus: I used COMSOL (AC/DC module). I don't think its going into PRL, so i left out the labels ;) Sign of charge should be clear from field direction on R1, no?
 
mzh said:
@Q-reeus: I used COMSOL (AC/DC module). I don't think its going into PRL, so i left out the labels ;) Sign of charge should be clear from field direction on R1, no?
Fair enough for last point, but it's always best to give a 'verbal' to such things anyway. So given this COMSOL is an AC/DC simulation, my guess is you have plotted a current flow - giving direction but not intensity, and with R2 an insulator. But that puzzles me because you say R2 was given a metal property.
 
Without intensity, E-field direction is pretty meaningless. That's why you get an apparently large 'flow' of field around the conductor. In reality that field is virtually non-existent. It's just a residual component.
 
mzh said:
@mfb: Ok. And can it also terminate on induced charges?
Right. Induced or not, a surface charge density implies a non-zero field strength (outside), which corresponds to ending field lines.
 
  • #10
AJ Bentley said:
Without intensity, E-field direction is pretty meaningless. That's why you get an apparently large 'flow' of field around the conductor. In reality that field is virtually non-existent. It's just a residual component.

Sure. I'll see what I get when considering the intensity.

To return to my main point of the thread (i'm not so much interested in how correct my simulation is done or not).

Given the above system (surface charge on R1, metallic R2). What will the field look like, say from textbook undergraduate physics?
 
  • #11
Between the plates: Nearly homogeneous (from left to right in the sketch)
To the right of the right plate: nearly homogeneous (away from the conductor)
Far away: Similar to a single charged object.
In between: Let the computer calculate it
 
  • #12
@mfb: thanks. i would think the same. something must be fishy with my simulation then.
 

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