Harmonic oscillations and electric dipoles

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Homework Help Overview

The discussion revolves around the dynamics of an electric dipole in an external electric field, specifically focusing on the conditions under which it undergoes simple harmonic oscillations. The problem involves understanding the relationship between torque, dipole moment, moment of inertia, and angular acceleration.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of torque in relation to the dipole's orientation and its motion over time. There are hints about using derivatives to express angular acceleration and solving differential equations to find a sinusoidal solution. Some participants express confusion about the differentiation process without known values.

Discussion Status

The conversation has seen some participants making progress in understanding the problem, while others continue to seek clarification on the mathematical steps involved. There is a mix of exploration and attempts to clarify concepts, but no consensus has been reached on the complete solution.

Contextual Notes

Some participants are grappling with the mathematical aspects of the problem, particularly in relation to derivatives and the implications of the dipole's orientation in the context of the external electric field.

PinkFlamingo
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Hi there, I was hoping that someone would be kind enough to help me out with this question. I don't even know where to start

Use T=Ia (where T=torque) to show that if an electric dipole with dipole moment of magnitude p and moment of inertia I is oriented with its dipole moment making a small angle theta with the direction of an external electric field of magnitude E, the dipole will execute simple harmonic oscillations about the field direction with a frequency v given by:

v= [1/(2pi)] [(pE)/I]^1/2
 
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The dipole moment and electric field will give you the torque, which is the L.H.S. of the equation τ = I α. (Big hint: it will involve orientation as a function of time, θ(t))

For the R.H.S., you need to replace angular acceleration α with a second order derivative. (Big hint: it will involve orientation as a function of time, θ(t))

Then, solve the diff. eq. The solution should be sinusoidal (with a frequency, ν).
 
Last edited:
I'm sorry... I'm still lost. I have no idea how to do any of that. How do you take the derivative if you don't know the value?
 
ok I figured it out! Thanks for your help!

:biggrin:
 
PinkFlamingo said:
ok I figured it out!
Very cool. However, I am curious:


How did you go from:
I have no idea how to do any of that.
to:
ok I figured it out!
?
 
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Likes   Reactions: gracy

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