What is the Electric Field at the Center of a Square with Four Charges?

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The discussion centers on calculating the electric field at the center of a square formed by four charges, with two negative and two positive charges. The electric field is derived to be [q(2)^(0.5)]/(8.pi.epsilon.(0.5)a^2) directed upwards. An electron placed at the center would accelerate opposite to the electric field direction, which is consistent with the conventional flow of electric field lines from positive to negative charges. Participants also discuss the integration of electric field to find potential across capacitor plates, confirming that the direction of integration does not affect the magnitude of the voltage difference. The consensus is that one can integrate in either direction and simply take the absolute value if a negative result occurs.
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Homework Statement



Hello, 4 charges of equal magnitude are placed on the corners of a square of length a. The two charges at the top of the square are negative, while the two charges at the bottom of the square are positive.

what is the magnitude of electric field at the centre of the square. Ok I've done this part i have [q(2)^(0.5)]/(8.pi.eplion.(0.5)a^2) in a verical (upwards direction).

what direction would an electron accelerate if placed in the centre of the square? I am not too sure on this, does an electron acelerate in a direction opposite to the resultant elecric field, since electric field goes from positive to negative.


thanks
 
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Welcome to PF!

Hi kman12! Welcome to PF! :smile:
kman12 said:
what direction would an electron accelerate if placed in the centre of the square? I am not too sure on this, does an electron acelerate in a direction opposite to the resultant elecric field, since electric field goes from positive to negative.

Yes … electric notation was fixed before electrons were discovered, so electrons always go the "wrong way"! :rolleyes:
 
cheers,
another quick question, if i want to find the potential across the plates of a capacitor, does it matter in which direction i integrate v= -∫E.ds=-∫ Edscosθ. In other words can i start from the positive end of the capactor and integrate to the negative end. so E and ds are parralal so θ=0 and then flip limits to get positive value for V. OR could i integrate from negative end towards positive end and θ=180 then i don't need to flip limits, i will already have positive v.

Obviously the potential across a capacitor is v=Ed, but I am not sure how to arrive at this
 
kman12 said:
if i want to find the potential across the plates of a capacitor, does it matter in which direction i integrate v= -∫E.ds=-∫ Edscosθ. In other words can i start from the positive end of the capactor and integrate to the negative end. so E and ds are parralal so θ=0 and then flip limits to get positive value for V. OR could i integrate from negative end towards positive end and θ=180 then i don't need to flip limits, i will already have positive v.

Obviously the potential across a capacitor is v=Ed, but I am not sure how to arrive at this

Hi kman12! :smile:

just got up :zzz: …

Not really following you :confused:

if the charge is Q on one side and -Q on the other, then you get there by forcing either Q positive charge one way, or Q negative charge the other way.

For details of the calculation, see the PF Library on https://www.physicsforums.com/library.php?do=view_item&itemid=112" :smile:
 
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kman12 said:
cheers,
another quick question, if i want to find the potential across the plates of a capacitor, does it matter in which direction i integrate v= -∫E.ds=-∫ Edscosθ. In other words can i start from the positive end of the capactor and integrate to the negative end. so E and ds are parralal so θ=0 and then flip limits to get positive value for V. OR could i integrate from negative end towards positive end and θ=180 then i don't need to flip limits, i will already have positive v.

Obviously the potential across a capacitor is v=Ed, but I am not sure how to arrive at this
If you're just trying to get the magnitude of the voltage difference (which is usually the case), no it doesn't matter which way you integrate. Magnitudes are always positive, so if your integration gives you a negative answer you just drop the sign (take the absolute value).

When I took introductory electromagnetism as a freshman in college, the professor would use this shortcut all the time - basically the idea was that if you know which sign your answer is supposed to have, there's no need to spend a lot of time figuring out the right way to set up the calculation (e.g. the right direction to integrate). You just pick one way, do the math, and if you get the wrong sign, you flip it. We named it the Verlinde theorem in his honor ("1 = -1 when necessary" :biggrin:)
 
o ok thanks guys. I think my lecturer does the same thing by dropping the sign. But sometimes he doesn't even state that the e field and length element ds, are in oppisite directions, ie 180 degrees. It makes sense now cheers.
 
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