Electrostatic potential and electric fields

In summary, the given problem involves four charged particles of equal magnitude, two positive and two negative, arranged in a square with side s. In Arrangement 1, the charges of the same sign are at opposite corners, resulting in an electrostatic potential of 0 at the center of the square and a magnitude of electric field also equal to 0. In Arrangement 2, the positive charges are on the left and the negative charges are on the right, resulting in the same values for both the electrostatic potential and magnitude of electric field at the center of the square. Therefore, it can be concluded that the same amount of work would be required to remove the particle at the upper right corner in both arrangements.
  • #1
secret5437
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Homework Statement



3. Four charged particles are held fixed at the corners of a square of
side s. All the charges have the same magnitude Q, but two are
positive and two are negative. In Arrangement 1, shown ,
charges of the same sign are at opposite corners. Express your
answers to parts (a) and (b) in terms of the given quantities and
fundamental constants.

(a) For Arrangement 1, determine the following.
i. The electrostatic potential at the center of the square
ii. The magnitude of the electric field at the center of the square

The bottom two charged particles are now switched to form Arrangement 2,
shown , in which the positively charged particles are on the left and the
negatively charged particles are on the right.

(b) For Arrangement 2, determine the following.

i. The electrostatic potential at the center of the square
ii. The magnitude of the electric field at the center of the square

In which of the two arrangements would more work be required to remove the particle at the upper right corner from its present position to a distance a long way away from the arrangement? Justify your answer.



Homework Equations



V = KQ/r
E = KQ/r2



The Attempt at a Solution



I'm pretty sure the answer for Arrangement 1 is 0, for parts i. and ii.
Help on Arrangement 2, please?
 
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  • #2
You haven't given any information on what arrangement 2 is.
Or on what you did for part (a). We helpers don't really like to work out all the details to check an answer - that's your job! We love to help with the understanding, though.
 
  • #3
I know that the answer to Arrangement 1 is 0, because the two positive and two negative charges cancel each other out.
 
  • #4
and arrangement 2 looks like this:

Q+......Q-




Q+......Q-






Arrangement 1 looks like this:
Q+.....Q-





Q-......Q+


(imagine those two arrangements as squares)
 
  • #5
Oh, clever of you! Yes, I think you are right, though it seems a bit surprising at first that you can just add the potentials due to each charge. I looked it up to make sure!
I guess that is the clue for the second arrangement!
 

Related to Electrostatic potential and electric fields

1. What is the difference between electrostatic potential and electric field?

Electrostatic potential is the amount of electric potential energy per unit charge at a specific point in space, while electric field is the force per unit charge experienced by a test charge placed at that point.

2. How are electrostatic potential and electric field related?

The electric field is the negative gradient of the electrostatic potential. In other words, the electric field points in the direction of decreasing electrostatic potential.

3. What is the SI unit for electrostatic potential and electric field?

The SI unit for electrostatic potential is volts (V) and for electric field is newtons per coulomb (N/C).

4. How is the strength of an electric field related to the electrostatic potential?

The strength of an electric field is directly proportional to the gradient of the electrostatic potential. This means that the greater the change in electrostatic potential over a given distance, the stronger the electric field.

5. Can electrostatic potential and electric field be negative?

Yes, both electrostatic potential and electric field can be negative. This indicates the direction of the force on a negative test charge in the opposite direction of the field or potential gradient.

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