Force on a dipole in a non uniform electric field

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SUMMARY

The discussion centers on the calculation of force on an electric dipole in a non-uniform electric field, specifically referencing the equation F = p * (∂E/∂x, ∂E/∂y, ∂E/∂z). Participants clarify that the partial derivative should be taken with respect to spatial coordinates rather than the direction of the dipole moment vector (p). The conversation highlights the importance of understanding the configuration of the dipole and the electric field, as well as the necessity of showing work for accurate assistance. Ultimately, the original poster acknowledges a misinterpretation of the problem statement.

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  • Understanding of electric dipoles and their behavior in electric fields
  • Familiarity with vector calculus, specifically partial derivatives
  • Knowledge of Newton's laws of motion as they apply to forces
  • Ability to interpret and analyze diagrams related to electric fields
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Shreya
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Homework Statement
Prove that the direction of the force on the dipole is as indicated in the diagram
Relevant Equations
F = partial derivative of p* E
I have figured out how the force is towards left in the first case. I think it is due to the larger force on - charge.
Please help me out with the second and third case.

IMG_20210725_055311.jpg
 
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Something looks off (i.e., "wrong") with the problem statement. I'm hoping your instructor didn't give you a bad problem, but it's not unheard of. Then again maybe I'm missing something myself.

From what I can tell, middle and bottom parts look wrong, although maybe the middle part is a trick question.

You haven't shown any work so we're not allowed to help help you until you do. Allow me to correct your statement,

Shreya said:
Relevant Equations:: F=p*(partial derivative of E with respect to direction of p )

That's not quite right. The partial derivative is not necessarily in respect to the direction of \vec p, but rather with respect to the spatial coordinates. \vec F, \vec p, and \vec E are all vectors, and they should be all subject to the chosen coordinate system.

It's true that
\vec F = \left( \vec p \cdot \vec \nabla \right) \vec E

and in Cartesian coordinates this becomes,
\vec F = \left( p_x \frac{\partial}{\partial x} + p_y \frac{\partial}{\partial y} + p_z \frac{\partial}{\partial z} \right) \vec E

but that's still not enough to reconcile the middle and bottom parts, unless maybe I'm missing something.

  • Is the dipole in question just an electric dipole (as opposed to a magnetic dipole), and nothing is presently moving?
  • Are all three parts intended to be taken separately (i.e., not all charges are all present simultaneously)?
  • Is there anything else in this problem that wasn't stated in the problem statement, such as other constraints or other charges or fields around?
  • Can you use my equation in Cartesian coordinates (above) to show that there is something wrong with the middle and bottom figures?
[Edit: Nevermind. I was misinterpreting the problem statement. The diagrams are fine.]
 
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collinsmark said:
You haven't shown any work so we're not allowed to help help you until you do.
For the first case, the attractive force on the negative charge is greater than the repulsion on the positive.
So net force is towards left.
 
Shreya said:
For the first case, the attractive force on the negative charge is greater than the repulsion on the positive.
So net force is towards left.
Right. I'll agree with that.

But I don't think the middle figure (diagram) and the bottom figure (diagram) are correct. [Edit: Nevermind.]
 
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collinsmark said:
Is the dipole in question just an electric dipole
Yes, that's what I have understood.
collinsmark said:
Are all three parts intended to be taken separately (i.e., not all charges are all present simultaneously)?
The question is to find the net force on the dipole due to the positive charge q (on the left).
They are not separate systems
collinsmark said:
Can you use my equation in Cartesian coordinates (above) to show that there is something wrong with the middle and bottom figures?
I don't know where to start.
 
collinsmark said:
I'm hoping your instructor didn't give you a bad problem
I think the drawings are correct. There are three ways to see this
  1. Work out the formula explicitly
  2. Consider the dipole as two point charges
  3. Consider the force on the point charge from the dipole field (equal and opposite Newton pair) if you can picture the dipole field
For the OP: do all three!
 
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collinsmark said:
Right. I'll agree with that.

But I don't think the middle figure and the bottom figure are correct.
For the second case, can you please check if my reasoning is right?
IMG_20210725_090207.jpg
 
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Shreya said:
For the second case, can you please check if my reasoning is right?
View attachment 286528
I have not consider the perpendicular forces, since they cause a torque and not a field.
 
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collinsmark said:
But I don't think the middle figure (diagram) and the bottom figure (diagram) are correct.
It's from the book titled "Basic Laws of Electromagnetism" by IE Irodov
 
  • #10
hutchphd said:
I think the drawings are correct. There are three ways to see this
  1. Work out the formula explicitly
  2. Consider the dipole as two point charges
  3. Consider the force on the point charge from the dipole field (equal and opposite Newton pair) if you can picture the dipole field
For the OP: do all three!
Yes, you are correct. I was misinterpreting the problem statement, after all. Sorry about that.

Shreya said:
For the second case, can you please check if my reasoning is right?
View attachment 286528

That's right right idea. :smile:
 
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  • #11
collinsmark said:
The partial derivative is not necessarily in respect to the direction of p→, but rather with respect to the spatial coordinates
So, the partial derivative must be taken with x, y and z?
I am not very comfortable with partial derivative , so I confused myself
 
  • #12
Will this work in the 3rd case?

IMG_20210725_091340.jpg
 
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  • #13
Shreya said:
So, the partial derivative must be taken with x, y and z?
I am not very comfortable with partial derivative , so I confused myself
You ultimately get to choose the coordinate system. So if you choose the coordinate system such that it always lines up (for example the x-axis) with the direction of \vec p then you initial statement was correct.

Being able to use other coordinate systems is more flexible though.

For example in the future, you might have a system with two dipoles in different directions. So for at least one of the dipoles its direction won't line up so nicely.
 
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  • #14
collinsmark said:
You ultimately get to choose the coordinate system. So if you choose the coordinate system such that it always lines up (for example the x-axis) with the direction of p→ then you initial statement was correct.
Thanks a lot, collinsmark!
 
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  • #15
Thank you Collinsmark and Hutchphd for helping me through this problem! 🙂🙏
 
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