Harmonic oscillations and electric dipoles

AI Thread Summary
The discussion revolves around deriving the frequency of harmonic oscillations for an electric dipole in an external electric field. The key equation involves using torque (T=Ia) and relates the dipole moment (p), electric field (E), and moment of inertia (I) to the frequency of oscillation (v). The process requires replacing angular acceleration with a second-order derivative and solving a differential equation, leading to a sinusoidal solution. The initial confusion about the calculations was resolved, prompting curiosity about the sudden understanding. The conversation highlights the challenges and breakthroughs in understanding the dynamics of electric dipoles in oscillatory motion.
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).
 
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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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