Cycloid Lagrangian Homework - 2 Degrees of Freedom & Equations

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Homework Help Overview

The problem involves a point-like particle of mass m moving under gravity along a cycloid defined by parametric equations. The particle is released from a specific point and the discussion centers on identifying constraints, determining degrees of freedom, and expressing the Lagrangian in different forms.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the types of constraints applicable to the system and the degrees of freedom necessary to describe the motion. There is uncertainty regarding whether the radius R should be considered a degree of freedom. Some participants attempt to derive the Lagrangian and question the application of trigonometric identities to simplify their expressions.

Discussion Status

The discussion is ongoing with participants exploring various interpretations of constraints and degrees of freedom. Some have provided insights into the use of trigonometric identities, while others express confusion about variable substitutions and the implications of their choices.

Contextual Notes

Participants mention specific terminology related to constraints, such as "holonomic" and "nonholonomic," indicating a deeper exploration of the theoretical framework. There is also a reference to the complexity introduced by considering R as a degree of freedom.

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Homework Statement


A point like particle of mass m moves under gravity along a cycloid given in parametric form by
$$x=R(\phi+\sin\phi),$$
$$y=R(1-cos\phi),$$
where R is the radius of the circle generating the cycloid and ##\phi## is the parameter (angle). The particle is released at the point (##x=\pi R, y=2R##) from rest.

1) What types of constraint apply to this system and how many degrees of freedom are needed to describe the motion?

2) Show that the lagrangian of the system is
$$L=2mR^2\dot{\phi}\cos^2\frac{\phi}{2}-2mgR\sin^2\frac{\phi}{2}$$

3) Introduce a new generalised coordinate ##s=4Rsin\frac{\phi}{2}## and express the Lagrangian in terms of s.

Homework Equations

The Attempt at a Solution


1) I am not sure what the constraints are. It's just that the particle is forced to move in a cycloid. Could someone help me here?
The degrees of freedom is 2 since x and y are dependent on R and ##\phi##. So R and ##\phi## are the variables required.

2) The lagrangian is L=T-V.
Am I correct in thinking ##T=\frac{1}{2}m(\dot x^2+\dot y^2)##? I have tried taking the time derivative of the right hand side of the given equations of x and y. I got $$\dot x=R(\dot \phi+\dot \phi \cos\phi),$$
$$\dot y=R(\dot \phi \sin\phi).$$
Substituting into T, $$T=R^2m\dot \phi ^2 (1+cos\phi).$$
Similarly, $$V=mgy=mgR(1-\cos\phi)$$
Then $$L=R^2m\dot \phi ^2 (1+cos\phi)-mgR(1-\cos\phi)$$
I'm looking through the double angle formulas and can't really determine how to get to the given lagrangian.

3) What to do?

Thanks in advance
 
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1) Is R a degree of freedom? If it is, where are the derivatives of R in 2?

2) Just apply the double angle formula and the trigonometric one.

3) It is a variable substitution. What is your problem with it?
 
1) Is R a degree of freedom? If it is, where are the derivatives of R in 2?
Sorry, I realized I initially had R as a degree of freedom but after taking the derivative, it became too complex I figured R is not a degree of freedom. This makes sense because it's just the radius of a circle. So one degree of freedom, ##\psi##

2) Just apply the double angle formula and the trigonometric one.
Okay

3) It is a variable substitution. What is your problem with it?
I don't know where to substitute? Should I solve for R, so ##R=\frac{s}{4\sin\frac{\phi}{2}}## and plug it in the x and y equation?
 
spacetimedude said:

Homework Statement


1) What types of constraint apply to this system

The Attempt at a Solution


1) I am not sure what the constraints are. It's just that the particle is forced to move in a cycloid. Could someone help me here?
I'm not sure exactly what the question is asking here. But standard texts often categorize constraints using scary words. For example, have you run into the terms "holonomic", "nonholonomic", "scleronomous", and "rheonomous"?

(I studied Lagrangian mechanics in 1970 and this is the first chance that I've ever had to use any of those words. Thanks for the opportunity. :oldsmile: )
 

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