Equation Demonstration -- Comparing a pendulum's motion to an LC circuit

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Homework Help Overview

The discussion revolves around comparing the motion of a physical pendulum and an LC circuit, both of which exhibit simple harmonic motion. The original poster seeks a demonstration of the equations governing these systems, specifically referencing the formulas associated with each example.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants suggest setting up equations of motion for both systems, with references to Newton's second law and Kirchhoff's laws. There is a mention of deriving relationships between the two formulas through their respective differential equations.

Discussion Status

Some participants have offered guidance on how to approach the problem, emphasizing the need for the original poster to demonstrate their understanding before further help can be provided. There are multiple lines of reasoning being explored, including energy considerations and the relationship between natural frequency and system parameters.

Contextual Notes

Participants note the requirement for the original poster to show their efforts in working through the problem, as per forum guidelines. There is also a reference to another unresolved thread regarding a different physics problem, indicating ongoing engagement with related topics.

Andrei0408
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Homework Statement
I need the demonstration of the attached equations.
Relevant Equations
I've attached the 2 equations.
I've just learned about simple harmonic motion and I've been given the following examples: The physical pendulum (for small oscillations sin(theta)~theta), with the formula (1st pic), and the LC circuit, with the formula (2nd pic). If possible, I need the demonstration for these 2 formulas. Thank you!
 

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For the first one, set ##\tau_z = I_z \ddot{\theta}_z##. For the second one, write out Kirchoff's law for the circuit. Unfortunately, the laws of Physics forums prevent me from helping any further until you've given it a shot!
 
Andrei0408 said:
Homework Statement:: I need the demonstration of the attached equations.
Relevant Equations:: I've attached the 2 equations.

I've just learned about simple harmonic motion and I've been given the following examples: The physical pendulum (for small oscillations sin(theta)~theta), with the formula (1st pic), and the LC circuit, with the formula (2nd pic). If possible, I need the demonstration for these 2 formulas. Thank you!
You know that you are required to show your efforts to work the problem before we can offer tutorial help. See what you can find as references for those two situations please.

Also, you never replied in your other thread about the car and the banked turn. What did you end up finding on that problem?

https://www.physicsforums.com/threa...ed-turn-in-a-road-for-a-maximum-speed.994630/
 
berkeman said:
You know that you are required to show your efforts to work the problem before we can offer tutorial help. See what you can find as references for those two situations please.

Also, you never replied in your other thread about the car and the banked turn. What did you end up finding on that problem?

https://www.physicsforums.com/threa...ed-turn-in-a-road-for-a-maximum-speed.994630/
Sorry I didn't reply faster, I had a lot of uni work. Yes I did manage to solve it, by adding half of the angle of the friction cone to the equation, then I used trigonometric functions to find out theta.
 
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(1) The general form for the natural frequency ##ω_0## (or at least the way I learned it) is: ##ω_0=\sqrt\frac{k}{m}##
(2) Look at the differential equations for Newton's second law and Kirchoff's second rule for circuits. If you can find the differences in the coefficients for each of these equations, it might help in understanding how the two formulas you provided are related to each other. Good luck!
 
Sometimes you can derive these things nicely by considering energy, for instance for the pendulum$$\begin{align*}E &= \frac{1}{2}mr^2 \dot{\theta}^2 - mgr\cos{\theta} \\ \frac{dE}{dt} &= mr^2 \ddot{\theta}\dot{\theta} + mgr \dot{\theta} \sin{\theta} \approx mr^2 \dot{\theta} \ddot{\theta} + mgr \theta \dot{\theta} \\ \\ \frac{dE}{dt} &= 0 \implies \ddot{\theta} \approx -\frac{g}{r}\theta \end{align*}$$Can you use the same approach, with ##E = \frac{1}{2}CV^2 + \frac{1}{2}Li^2##, to derive the EoM for the LC circuit?
 
etotheipi said:
##\dots~##to derive the EoM for the LC circuit?
Do LC circuits move? 🤔
 
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kuruman said:
Do LC circuits move? 🤔

Ahaha, you never know! My differential equations prof. uses "equation of motion" to refer to any solution that is a function of time, e.g. ##i(t)##.
 

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