Concept Question - Electric Potential, and Electric Fields

In summary, the conversation discusses the concepts of electric potential and electric fields. It is stated that if two points have the same electric potential, no work is required to move a test charge between them. It is also mentioned that if a charged particle moves along a path perpendicular to an electric field line, no work is required. The concept of conservative fields is introduced and it is explained that work is defined as the component of force parallel to the motion of the object times the distance. It is also clarified that in the case of electric fields, work is required to move a particle along the field, but not if moving perpendicular to it. The concept of equipotential lines is mentioned and their relation to electric fields is explained.
  • #1
DMac
32
0
I have a few questions about electric potential and electric fields.

If two points have the same electric potential, is it true that no work is required to move a test charge from one point to the other? Does that mean that no force is required as well?

Also, How much work is required to move a charged particle through an electric field if it moves along a path that is always perpendicular to an electric field line? How would the potential change along such a path?

Thanks in advance!
 
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  • #2
The electric field is a conservative field so what does this tell you?

for part b, use the classical relations for work, with F = qE:

[tex] W = q\int_{C}\vec{E}\cdot d\vec{l}[/tex]

so, what happens when [tex]d\vec{l}[/tex] and [tex]\vec{E}[/tex] are perpendicular?
 
  • #3
I mean no disrespect, but I did not understand any of that because I'm still learning basic high school physics. (So, I don't know integration, or...lol anything, really.)
 
  • #4
(All I got from the expression for Work is I know that if those two vectors are perpendicular, then the dot product is zero. But...yeah I don't understand what those two vectors are exactly. Sorry)
 
  • #5
E is the electric field vector, and dl is a small element of the path that you are taking. so when you integrate that you will get contributions of all the small work elements, dW to get your total work W. The path that you want to take is an equipotential path -- you should remember from your course that equipotential lines always lie perpendicular to the electric field, so the answer 0 is right. I hope this has cleared it up some, let me know if not
 
  • #6
My textbook never covers equipotential lines =( ...One thing I don't understand is that I always thought that it would take no work to move a particle in the same direction as the field (isn't this true for magnetic fields?) ...so...lol I'm still confused.
 
  • #7
it depends on the field. In the case of electric fields, it does take work to move a particle along a field (whether it is you doing the work or the field, depends on the circumstances). with electric fields, if you move perpendicular to the field, however, it will require no work. In fact, this will always be the case with any conservative field, because the field is constructed from a potential, the electric potential (usually denoted V or phi). Have you taken anything with vector analysis, by chance? I might be able to explain this in a more mathematical way which could make this more clear.
 
  • #8
It is true that if two points have the same potential, then no work is required to move something from one point to the other. This is analogous to gravity: picture, for example, a skater on a half pipe. If she's on one end it doesn't require any work to get to the other side (assuming no friction, air resistance, etc), she'll slide down half and that will give her enough energy to make it just to the top of the other part.

Work is defined, in general, to be the part of the force that is parallel to the motion of the object times the distance. Therefore if you're moving something perpendicular to a force, there is no component that is parallel so that the work is 0.
 
  • #9
To EngageEngage:

I know very basic vector analysis, like dot product, cross product, projections, direction cosines, etc. But that's pretty much it.
 

1. What is electric potential?

Electric potential is the amount of electrical potential energy that a charged particle has per unit of charge. It is a measure of the work required to bring a unit charge from infinity to a specific point in an electric field. It is expressed in units of volts (V).

2. How is electric potential different from electric field?

Electric potential is a scalar quantity that describes the energy per unit charge at a specific point in an electric field. Electric field, on the other hand, is a vector quantity that describes the force per unit charge at a specific point in an electric field. Electric potential is dependent on the electric field, but not vice versa.

3. How is electric potential calculated?

Electric potential is calculated by dividing the electrical potential energy by the amount of charge at a specific point. Mathematically, it is expressed as V = U/Q, where V is electric potential, U is the electrical potential energy, and Q is the charge.

4. What is the relationship between electric potential and electric potential energy?

Electric potential is a measure of the electric potential energy per unit charge. The electric potential energy is the amount of work required to move a charge from one point to another in an electric field. As the electric potential increases, the electric potential energy also increases.

5. How do electric potential and electric field affect each other?

Electric potential and electric field are closely related. The electric field is responsible for creating the electric potential, and the electric potential determines the strength and direction of the electric field. In other words, the electric field is the cause, and the electric potential is the effect.

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