Potential energy of a dipole in an electric field

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Discussion Overview

The discussion revolves around the potential energy of a dipole in an electric field, specifically focusing on the equations that describe this energy based on different initial orientations of the dipole. Participants explore the implications of choosing different reference points for potential energy calculations and the significance of these choices in deriving equations.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant presents two equations for potential energy, W = pE(1 - cosθf) and W = -pE cosθf, and questions the rationale behind choosing different initial angles for calculations.
  • Another participant argues that while the two equations yield different values, the difference is a constant (pE), which is often irrelevant when considering changes in potential energy.
  • A participant clarifies that equation (2) gives the direct value of potential energy at an angle θ, while equation (3) requires calculating potential energy at two angles and taking their difference.
  • Further contributions emphasize that the choice of where to set the potential energy to zero is arbitrary and that different initial positions will lead to different expressions for potential energy, differing only by a constant.
  • Some participants express confusion about why potential energy is determined by the difference between values at two angles rather than an absolute value.

Areas of Agreement / Disagreement

Participants generally agree that the choice of initial position for calculating potential energy is arbitrary and that different expressions for potential energy can differ by a constant. However, there remains some confusion and debate regarding the implications of these choices and the reasoning behind using differences in potential energy.

Contextual Notes

The discussion highlights the dependence on the choice of reference points for potential energy calculations and the implications of these choices on the derived equations. There is an acknowledgment that different expressions for potential energy can arise from different initial conditions.

rajeshmarndi
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When the dipole makes an angle with an electric field, its potential energy is given as the work done in bringing the dipole from the position, when it is aligned with the electric field direction, to a desired position, i.e

W = pE [-cosθf -(-cosθi)] ...eq(1)

p = moment of the dipole
θi = initial position which is when the dipole is aligned with electric field i.e θi = 0
θf = final position of the dipole.

i.e eq(1) becomes,

W= pE(1-cosθf) ...eq(2)

But for convenience, θi is taken when the dipole is perpendicular to electric field, i.e θi= 90°
. This is where I didn't understand. In book, the explanation is just that , it is convenient to take θi=90°, as cos 90°=0, but why and how there is no explanation.

i.e eq(1) now becomes,

W = -pE cosθf ...eq(3)

eq(2) and eq(3) gives different values, so how could they both give the same potential energy of the dipole in an electric field.
 
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Well equation (3) is simpler and more convenient to use than (2). You are right that the two equations don't give the same value however it is important that the difference between the two values is only a constant pE (as long as the electric field and the dipole moment remain constant). And because we usually are interested in differences of the potential energy and not in the absolute value, that constant is eliminated anyway when we take the difference of the potential energy between two positions.
 
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Is this right?

eq(2) deduce the direct value of potential energy at θ i.e it is work done from θ=0 to θ. With Eq(3), you have to deduce the value of potential energy at θ=0 and at θ. And then there difference is the potential energy at θ.
 
It is correct, their difference is the potential energy at θ, considering as zero potential energy the potential energy at θ=0. You are free to choose where the potential energy is set to zero that's the whole point here.
 
Delta² said:
their difference is the potential energy at θ, considering as zero potential energy the potential energy at θ=0.

What am I missing?

Why are we taking difference of the potential energy to get potential energy.

To get potential energy at θ, we find the potential energy at θ=0 and at θ. And their difference is the potential energy at θ.
 
Delta² said:
And because we usually are interested in differences of the potential energy and not in the absolute value, that constant is eliminated anyway when we take the difference of the potential energy between two positions.

These two position has to be θ=0 and θ, to know potential energy at θ.

Delta² said:
You are free to choose where the potential energy is set to zero that's the whole point here.

Can you explain please, how is it, that?
 
rajeshmarndi said:
These two position has to be θ=0 and θ, to know potential energy at θ.
Can you explain please, how is it, that?

The orientation of the dipole is relevant as well as the 'position'. The reference (start) position and orientation (0° or whatever) are both relevant to the work needed to move to the test condition. Both of these are arbitrary.
 
The potential energy at a position F is the work done by the field when the dipole is moved from an initial position I to the position F. What makes you think that the choosing of initial position I is not arbitratry? You think that the position where the dipole moment is aligned with the electric field is the "only rightfull king" of initial positions?

The initial position can be any position. Ofcourse by changing the initial position we ll find a different expression for the potential energy. But any two expressions for the PE differ by a constant, like equation (2) and (3) differ by a constant.
 

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