Is the motion of a pendulum restricted by a cycloid surface cyclical?

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Discussion Overview

The discussion revolves around the nature of motion of a pendulum constrained by a cycloidal surface, specifically whether the motion can be considered cyclical. Participants explore the mathematical representation of cycloids and the implications for pendulum dynamics, including oscillatory behavior.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents the equations for a cycloid and questions whether using ##\theta = \cos(\omega t)## still results in a cycloid, suggesting that their teacher insists on oscillatory behavior for ##\theta##.
  • Another participant suggests plotting the cases to visually determine if they represent a cycloid and questions the definition of a cycloid.
  • A participant mentions that while their graph shows oscillatory behavior for ##x## and ##y##, the solution derived from the Lagrangian does not reflect oscillatory motion, raising concerns about the interpretation of the cycloidal path.
  • Further, a participant critiques the domain of the graph as insufficient to capture the cycloidal behavior and emphasizes the need to clarify the physical meaning of the angle ##\theta## in relation to the pendulum's motion.
  • Another participant proposes a parameterization of the cycloid to avoid confusion with time parameters and suggests that the angle should be defined in relation to the vertical line through the pivot, which could indeed be oscillatory.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the angle ##\theta## and its relationship to oscillatory motion. There is no consensus on whether the motion of the pendulum can be classified as cyclical under the given conditions, and the discussion remains unresolved.

Contextual Notes

Participants highlight the need for clarity regarding definitions and the mathematical representation of cycloids. There are unresolved questions about the assumptions underlying the Lagrangian formulation and the implications for the pendulum's motion.

alejandrito29
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the coordinates of cycloide are

##x= a (\theta- sin \theta)##
##y= a(cos \theta -1)##

If i use ##\theta =\omega t## this is a example of cycloid

but, if i use ##\theta=\cos (\omega t)##, ¿this is a cycloid?

My teacher says that in a cycloid pendulum ##\theta## must be oscillatory, but i think that if ##\theta=\cos \omega t## then, this is not cycloid.

Also the dynamics of the pendulum on the cycloid is oscillatory, but, the ##x= a (\theta- sin \theta)## is not oscillatory.
 

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Have you tried plotting the different cases out and seeing for yourself if it's a cycloid and of what kind?
Also - what is the definition of a cycloid? (How would you know one if you saw it?)
 
sss

Simon Bridge said:
Have you tried plotting the different cases out and seeing for yourself if it's a cycloid and of what kind?
Also - what is the definition of a cycloid? (How would you know one if you saw it?)

this is my graph, but, at the lagrangian the solution is ##\theta=\omega t## but, my teacher says that the solution must be ##\theta## oscillatory.

I Says that the length of the proyection cycloid is oscillatory ## ds/d\theta = \sqrt{(dx/d\theta)^2+(dy/d\theta)^2}## but, the x coordinate is not oscillatory.

Clearly in the graph, x, and y are oscillatory, but this is not the solution of the lagrangian

Pd: the originall problem is the huygens pendulum

http://books.google.cl/books?id=E64...nepage&q=huygens pendulum lagrangian&f=false
 

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The domain of your graph is not big enough to see the cycloidal behavior of the equations.
Did you try plotting the cyclical angle version of the formula from before?

What is the angle ##\theta## the angle of? What is the physical behavior of the angle going to be?

Perhaps you should be asking about the problem you have to solve instead of (as well as) the particular solutions you have?

The diagram in post #1 looks like you are supposed to solve for the motion of a pendulum whose path is restricted by a cycloidal surface. In which case, I'd have expected the angle to be measured between the line joining the pivot to the bob and the vertical line through the pivot. This angle would, indeed, be oscillatory, but it has nothing to do with the form of the cycloid restriction.

In order to solve the Lagrangian for that problem, you need to express the restriction in terms of y(x)

parameterizing the cylcoid by "A" (so we don't get confused with the time parameter)

##x(A)= R(A-\sin k A),\; y(A)=-R(1-\cos kA)## where R and k are constants.
 
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