Shape of equipotential surface in 3d

In summary, the shape of an equipotential surface in three-dimensional space is determined by the distribution of electric or gravitational fields. These surfaces represent locations where the potential energy is constant, meaning that no work is required to move a charge or mass along the surface. In electrostatics, equipotential surfaces are typically perpendicular to electric field lines and can take various forms, such as planes, spheres, or more complex shapes depending on the source of the field. In gravitational fields, similar principles apply, with equipotential surfaces represented by levels of constant gravitational potential energy.
  • #1
Lochikilebor
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New user has been reminded to please always show their work on schoolwork problems.
Homework Statement
Give answer
Relevant Equations
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We have 2 infinite cylinders, need to find out which shape will equipotential surface be in 3D.
9afZLc_w37E.jpg
 
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  • #2
Hi @Lochikilebor. Welcome to Physics Forums.

The way it works here is that we help/direct/advise you so that you can work out the answer for yourself. (Take a look at some of the other threads.) We don't do the problem for you!

Read the forum rules here: https://www.physicsforums.com/threads/homework-help-guidelines-for-students-and-helpers.686781/

So to start, you need to give your own thoughts, e.g. what you've tried, any relevant working, why you're stuck.

By the way, the question is not clear. Do you need to produce a drawing of the equipotentials? Or a description? Or equations? You haven't posted the full original question exactl;y as set, so we can't tell.

[Edited -typo's.]
 
  • #3
No, i only need to answer the question - which form will be the equipotential surface in 3d. I tried to imagine this some ways - like cone or spherical elongated circles, but its wrong, so teacher give me the 2d drawing:
img_245.jpg

Based on this drawing, i just need to give an answer, what shape will the equipotential surface in 3d of two infinite parallel cylinders be? According to the teacher's suggestion, the answer should be too simple, I just can't get to it.
 
  • #4
Lochikilebor said:
No, i only need to answer the question - which form will be the equipotential surface in 3d. I tried to imagine this some ways - like cone or spherical elongated circles, but its wrong, so teacher give me the 2d drawingBased on this drawing, i just need to give an answer, what shape will the equipotential surface in 3d of two infinite parallel cylinders be? According to the teacher's suggestion, the answer should be too simple, I just can't get to it.
Try a couple of easier questions first:
1) What shape are the equipotential surfaces around a uniformly charged sphere?
2) What shape are the equipotential surfaces around a single uniformly charged infinite cylinder?
 
  • #5
Around a uniformly charged sphere it must be sphere shapes surface, so the same single uniformly charged infinite cylinder must have cylinder shape surface...?
 
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  • #6
Lochikilebor said:
Around a uniformly charged sphere it must be sphere shapes surface, so the same single uniformly charged infinite cylinder must have cylinder shape surface...?
Yes. That’s right.

On a (2D) drawing for a charged sphere, we would show equipotential lines which would be circles. In real (3D) life, we actually have spherical equipotential surfaces, (because we have spherical symmetry).

On a (2D) drawing for a charged infinite cylinder, we would show equipotential lines which would also be circles. But in real (3D) life, we now have cylindrical equipotential surfaces (because we have cylindrical symmetry).

Note that for the cylinder, we could pick any 2D equipotential circle and imagine 'sliding' it in the direction parallel to the cylinder's axis. Some 3D imagination is needed. The moving circle then ‘sweeps out’ a cylindrical equipotential surface as it travels along.

(Imagine a hoop laying flat on a table. You move the hoop vertically upwards, keeping its plane parallel to the table. The hoop 'sweeps' along a cylindrical surface.)

If all that makes sense, you can go back to your Post #3 diagram. Imagine sliding the diagram along in the direction parallel to the cylinders' axes. Each dotted line (equipotential line) 'sweeps out' an equipotential surface.

The problem is then how to describe the shape of this surface in suitable words.
 

FAQ: Shape of equipotential surface in 3d

What is an equipotential surface?

An equipotential surface is a three-dimensional surface on which the potential energy is constant at every point. In the context of gravitational or electric fields, this means that no work is done when moving a charge or mass along the surface, as the potential difference is zero.

How does the shape of equipotential surfaces change with different fields?

The shape of equipotential surfaces varies depending on the nature of the field. For example, in a uniform electric field, the equipotential surfaces are parallel planes, while in a point charge field, they are concentric spheres. In gravitational fields, they can also take the form of concentric spheres around a mass.

What is the relationship between equipotential surfaces and electric field lines?

Equipotential surfaces are always perpendicular to electric field lines. This means that at any point on an equipotential surface, the electric field vector will intersect the surface at a right angle, indicating that no work is done when moving along the surface.

Can equipotential surfaces intersect each other?

No, equipotential surfaces cannot intersect each other. If they did, it would imply that a single point in space has two different potential values, which is not possible. Each equipotential surface corresponds to a unique potential value.

How can equipotential surfaces be visualized in three dimensions?

Equipotential surfaces can be visualized using contour plots or 3D modeling software. In a 3D representation, surfaces can be rendered as smooth shapes, such as spheres or planes, depending on the field. Visualization tools often use color gradients to represent different potential values, enhancing the understanding of the spatial distribution of potential.

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