Undergrad Parallel Plate Fields: Questions & Answers

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The discussion centers on the conventions for sketching electric and magnetic field lines, particularly in relation to capacitors. Participants clarify that while arrows can be placed at different points on the lines, the important aspect is that field lines must touch the plates to accurately represent the electric field. The concept of fringe fields is introduced, noting that they are typically negligible unless the plate separation is comparable to the plate size. Additionally, it is emphasized that electric field lines originate from positive charges and terminate at negative charges, while magnetic field lines form closed loops. Overall, the conversation highlights the flexibility in representation while adhering to fundamental principles of field lines.
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Sorry for the wonky mouse sketching. Teacher said that arrows must touch the plate at the other end. Is there actually such a thing or is this just preference? I thought convention was for arrow to be in the middle of the line.
 
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As far as I am aware there is no such convention for field lines. Field lines are just curves tangent to the vector field, and don't even necessarily require arrows (although they're pretty helpful to insert).

But if you are instead sketching a vector field, i.e. drawing an arrow at every point in space, then you need to make clear whether the arrow represents the field at the point of the tip, tail or middle of the arrow. This is important, since the electric field at each point in space is a bound vector.
 
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Yeah, looks like it's done both ways.

https://buphy.bu.edu/~duffy/PY106/cap1.GIF

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https://lh3.googleusercontent.com/proxy/ot9IExHXVFIK7Fo9lRFv_gPHTkJH0XJP5j8XpDOEuPsyC3W-J3dWesF4mPw-No-pfHh109Hy9XSAIwkx4FyfaxFyyFO6ZQYWIOT6qxDg79NCnoNBjcOKGbL1X5A5tIvKDA

1597756081745.png


I usually put the arrowhead at the end for the E-field in a capacitor, but in the middle for the magnetic field around a magnetic dipole, for example.
 
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berkeman said:
Yeah, looks like it's done both ways.

https://buphy.bu.edu/~duffy/PY106/cap1.GIF

View attachment 267917

https://lh3.googleusercontent.com/proxy/ot9IExHXVFIK7Fo9lRFv_gPHTkJH0XJP5j8XpDOEuPsyC3W-J3dWesF4mPw-No-pfHh109Hy9XSAIwkx4FyfaxFyyFO6ZQYWIOT6qxDg79NCnoNBjcOKGbL1X5A5tIvKDA

View attachment 267918

I usually put the arrowhead at the end for the E-field in a capacitor, but in the middle for the magnetic field around a magnetic dipole, for example.
For the red diagram a) that you whipped up, it shows the field outside of the plates. Is that meant to be drawn?
 
aspodkfpo said:
For the red diagram a) that you whipped up, it shows the field outside of the plates. Is that meant to be drawn?
LOL, I "whipped it up" by doing a Google Images search. I find that to be a very helpful way to get a quick look at possible solutions and visulaizations. I think my search phrase at Google Images was something like Electric Field in a Capacitor or similar.

As far as the E-field outside of the volume of the capacitor, that is called the "fringe field", and is usually only relevant and considered if the spacing between the plates is on the same order as the size of the plates. When the plate separation << than the linear dimensions of the plates, the contribution to the capacitance from the fringe field is usually negligible. Does that make sense?
 
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What are the arrows representing? Field vectors or field lines? In the latter case, the important point is that the lines should touch the plates (so you don't have field lines appearing out of nowhere) not where the arrowhead is drawn. It seems possible that this is what your teacher means.
 
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The field lines must end on the plates, because that's where charges are sitting. Field lines start (positive charge) and end (negative charge) at the sources according to ##\vec{\nabla} \cdot \vec{E}=\rho/\epsilon_0##. That's also why magnetic field lines (with ##\vec{B}## as the magnetic field!) must never have a beginning and an end, i.e., they always form closed loops (sometimes in idealized situations like an infinite coil at infinity).
 
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