Electric field and electric potential

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SUMMARY

The discussion focuses on the relationship between electric field (E) and electric potential (V), emphasizing that while potentials are scalar quantities that add like numbers, electric fields are vector quantities that add like vectors. The participants clarify that to determine the electric field contributions at a point, one must assign appropriate signs to the charges involved. The conversation highlights the importance of understanding how to calculate the net electric potential and field from multiple charges, particularly in scenarios where charge signs differ.

PREREQUISITES
  • Understanding of electric fields and electric potentials
  • Familiarity with vector addition and scalar quantities
  • Knowledge of charge interactions and their effects on electric fields
  • Basic skills in solving physics problems involving multiple charges
NEXT STEPS
  • Study the principles of electric field and potential using Coulomb's Law
  • Learn how to apply the superposition principle for electric fields
  • Explore the concept of electric potential energy in systems of charges
  • Practice problems involving charge configurations and their resulting electric fields and potentials
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Students studying electromagnetism, physics educators, and anyone seeking to deepen their understanding of electric fields and potentials in various charge configurations.

vysero
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Homework Statement



Untitled.png
[/B]

Homework Equations



dV = -EdX[/B]

The Attempt at a Solution



Well I was trying to think about the relationship between E and V. So I believe the two V and E are co dependent. So in a situation where the distance and the potential are not changing then wouldn't V just be equal to -E? If that is correct then: D>E>A>F=C>B is the answer.[/B]
 
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The difference is that while potentials add like numbers, fields add like vectors. That's because potential is a scalar quantity while fields are vector quantities. Two fields of equal magnitude can cancel each other out simply by being pointed in opposite directions.
 
gneill said:
The difference is that while potentials add like numbers, fields add like vectors. That's because potential is a scalar quantity while fields are vector quantities. Two fields of equal magnitude can cancel each other out simply by being pointed in opposite directions.

I didn't think about that is my answer correct though?
 
vysero said:
I didn't think about that is my answer correct though?
Nope. You'll have to go through the diagram and assign some signs to the charges that work for the potential given, then add up the field contributions (as vectors).
 
gneill said:
Nope. You'll have to go through the diagram and assign some signs to the charges that work for the potential given, then add up the field contributions (as vectors).

I am a little confused like for case B if I say all are + and I know the value of the charges are say q for each then E is going to be zero for the point x right because all the vectors cancel. However, using that logic on case F confuses me. The two cases seem to be similar but the charges would have to be different than say q like in case B but the directions say all the charges are the same.

Something else that still confuses me is assigning signs to the charges. Like I know how to figure out the over-all pe of a system of particles but not of a system at a designated point.
 
Last edited:
vysero said:
I am a little confused like for case B if I say all are + and I know the value of the charges are say q for each then E is going to be zero for the point x right because all the vectors cancel. However, using that logic on case F confuses me. The two cases seem to be similar but the charges would have to be different than say q like in case B but the directions say all the charges are the same.
The charges all have the same magnitude but may have different signs. Case F can be solved with the correct application of signs to the charges. You know that the net potential at the origin is positive, so there must be an excess of positive charges in the scenario. So start with them all positive and then change one... If nothing else you could try trial and error :)
Something else that still confuses me is assigning signs to the charges. Like I know how to figure out the over-all pe of a system of particles but not of a system at a designated point.

The potential in this case is the electric potential (Volts). Any point in space has an electric potential due to the net effect of all the charges that exist. Fortunately most of them cancel out!
 
Okay so here is what I am thinking now:

A=F>B=C=D=E

is that correct?
 
I have to say that I'm not keen on just validating what could be guesswork without seeing the details of the work. But I get the feeling that you've put in the effort and understood what you're doing. So in this instance I will confirm that your answer is good :)
 
gneill said:
I have to say that I'm not keen on just validating what could be guesswork without seeing the details of the work. But I get the feeling that you've put in the effort and understood what you're doing. So in this instance I will confirm that your answer is good :)

Thank you for your help!
 

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