Calculating Electric Field from a Dipole: Is This Equation Accurate?

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SUMMARY

The discussion centers on the accurate calculation of the electric field (\(\vec E\)) at a point \(P\) from a dipole. The correct formula for the electric field is derived as \(E = 2kQx/r^3\), where \(k\) is Coulomb's constant, \(Q\) is the charge, \(x\) is the horizontal distance, and \(r\) is the distance from the dipole. Participants emphasized the importance of vector addition and correctly identifying the components of the electric field, clarifying that the x-components cancel while the y-components do not in this context.

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novelriver
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Is this the correct equation to find the electric field at point p from a dipole?
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Hello Novel, :welcome:

You don't want to delete the template; it's very useful for you as well as for us. See the guidelines.

Answer to your question: No. ##\ \vec E\ ## is a vector. What does your E describe, you think ?
 
BvU said:
Hello Novel, :welcome:

You don't want to delete the template; it's very useful for you as well as for us. See the guidelines.

Answer to your question: No. ##\ \vec E\ ## is a vector. What does your E describe, you think ?

Thanks for your reply. I'll make sure to not delete the template next time. I think my E describes the magnitude of the electric field. After calculating the magnitude, I can decide if it's positive or negative. So in this case, E is negative, because E is going down, away from positive and toward negative. Is this right?
 
I'll give you some leeway because you are new here (let's hope I don't get chastized for that).
Also because I think you have a fair idea what you are doing, but you stumble because you are going too fast.

Again, ##\vec E## is a vector. I've drawn the two contributions from the +Q and the -Q in the figure.
There are no other contributions, so the field at P is the sum of these two. The vector sum, that is. Your job to do this vector addition. Andf yes, x/r appears in there (not x/R but x/r; I don't see or know of R in your post. Work accurately :smile:). And yes, it's downwards. Easy exercise, but a good vehicle to learn to work systematically.
upload_2016-9-9_12-12-42.png
 
BvU said:
I'll give you some leeway because you are new here (let's hope I don't get chastized for that).
Also because I think you have a fair idea what you are doing, but you stumble because you are going too fast.

Again, ##\vec E## is a vector. I've drawn the two contributions from the +Q and the -Q in the figure.
There are no other contributions, so the field at P is the sum of these two. The vector sum, that is. Your job to do this vector addition. Andf yes, x/r appears in there (not x/R but x/r; I don't see or know of R in your post. Work accurately :smile:). And yes, it's downwards. Easy exercise, but a good vehicle to learn to work systematically.View attachment 105666

I think I understand.

E = kQ/r2 * cos(theta) because the y-components cancel out and we just want to get the x-component. I'll call the horizontal distance d (in a real problem it would be given or I could find it with trig), so cos(theta) = d/r. Therefore E = kQ/r2 * d/r = kQd/r3.
 
novelriver said:
I think I understand.

E = kQ/r2 * cos(theta) because the y-components cancel out and we just want to get the x-component. I'll call the horizontal distance d (in a real problem it would be given or I could find it with trig), so cos(theta) = d/r. Therefore E = kQ/r2 * d/r = kQd/r3.

I just realized my mistake. It's the x-components that cancel, not the y. So E = kQ/r2 * sin(theta) = kQ/r2 * x/r = kQx/r3 and then multiply by 2 because there are two charges acting on P in the same direction. So E = 2kQx/r3.
 
Looks good to me. x and y are a bit confusing here because of the x's in the figure.
 
BvU said:
Looks good to me. x and y are a bit confusing here because of the x's in the figure.

Right, I realized that I should have chose a different variable name than x. Thank you for your help! I appreciate it!
 

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