Understanding the Potential Energy of a Dipole in an Electric Field

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SUMMARY

The discussion centers on the relationship between torque and potential energy for a dipole in a uniform electric field, as described in Gettys' Physics 2. The torque exerted on a dipole with moment p in an electric field E is given by τ = p × E. The work done to rotate the dipole from angle θ1 to θ2 is calculated using the integral ∫(θ1 to θ2) τ dθ, leading to the potential energy expression U = -p · E. A key point of confusion is clarified: the angle θ in the potential energy formula is defined from E to p, indicating that the torque τ is indeed the opposite of the torque τz.

PREREQUISITES
  • Understanding of electric dipoles and their moments
  • Familiarity with torque and its mathematical representation
  • Knowledge of potential energy concepts in conservative force fields
  • Basic calculus, particularly integration techniques
NEXT STEPS
  • Study the derivation of torque in electric fields using vector calculus
  • Explore the implications of potential energy in conservative systems
  • Learn about the behavior of dipoles in varying electric fields
  • Investigate the applications of dipole moments in molecular chemistry
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Students and professionals in physics, particularly those focusing on electromagnetism, as well as educators seeking to clarify concepts related to electric dipoles and potential energy.

DavideGenoa
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Hi, friends! I read that the torque exerced by a uniform electric field ##\mathbf{E}## on a dipole with moment ##\mathbf{p}## is ##\boldsymbol{\tau}=\mathbf{p}\times\mathbf{E}##. Then the book, Gettys' Physics 2, explain that the work made to rotate the dipole around a fixed point is

##\int_{\theta_1}^{\theta_2}\tau d\theta=\int_{\theta_1}^{\theta_2}pE\sin\theta d\theta=-pE\cos\theta_2-(-pE\cos\theta_1)=\Delta U##
and therefore potential energy can be defined as ##U=-\mathbf{p}\cdot\mathbf{E}##.

Well, there is a major obstacle to my comprehension of that: I think that ##\int_{\theta_1}^{\theta_2}\tau d\theta=\int_{\theta_1}^{\theta_2}pE\sin\theta d\theta## (where I think ##\theta## to be the oriented angle from ##\mathbf{p}## to ##\mathbf{E}##) is the work done by the electric fied while the dipole rotates from an angle ##\theta_1## with the direction of ##\mathbf{E}## to an angle ##\theta_2## with ##\mathbf{E}##, but I know the definition of the variation of potential energy ##\Delta U## as the opposite of the work done by a conservative force field: ##\Delta U=-W_{\text{conservative}}##.

Or isn't ##\int_{\theta_1}^{\theta_2}\tau d\theta## the work done by the electric field? I would think that it is, because the work done by a force ##\mathbf{F}## to move along the circumference ##\gamma## parametrized by ##\mathbf{r}:[0,2\pi]\to\mathbb{R}^3## is ## \int_{\theta_1}^{\theta_2} \mathbf{F}(\mathbf{r}(t))\cdot \mathbf{r}'(\theta)d\theta##. Here ##\mathbf{F}\cdot \mathbf{r}'=F_t R## where ##F_t## is the tangential component of the force (positive if and only if counterclockwisely oriented) and ##R## the distance of the moved object from the centre of the circle and, if I correctly understand, ##RF_t## precisely is the torque ##\tau_z## with respect to the centre of rotation of a rotating body, therefore the work done by the forces acting on the rotating body are ##W_{\text{tot}}=\int_{\theta_1}^{\theta_2} \sum\tau_z d\theta##. Or am I wrong?

I heatily thank you for any answer!​
 
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I have understood: in the formula for ##\Delta U## the angle ##\theta## is from ##\mathbf{E}## to ##\mathbf{p}##, i.e ##\tau## is the opposite of the torque ##\tau_z##.
 

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