Brachistochrone: Difference between revisions
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=== Rolling Ball: Angular momentum === | === Rolling Ball: Angular momentum === | ||
The rotational energy is <math>E_\text{rot} = \frac12 I \omega^2</math> and by applying non-slipping condition | The rotational energy is <math>E_\text{rot} = \frac12 I \omega^2</math> and by applying non-slipping condition <math>v = \omega r</math> we get <math>E_\text{rot} = \frac {v^2}{2r^2} I</math> | ||
=== Friction === | === Friction === |
Revision as of 10:47, 20 February 2021
Introduction
To find the shape of the curve which the time is shortest possible. . .
Theory
Variational Calculus and Euler--Lagrange Equation
The time from to is where is the Pythagorean distance measure and is determined from the the law of conservation of energy . giving . Plugging these in, we get , where is the function subject to variational consideration.
According to the Euler--Lagrange differential equation the stationary value is to be found, if E-L equation is satisfied.
No Friction
We get . Since does not depend on , we may use the simplified E--L formula .
Thus, we have So we have and multiplying this with the denominator and rearring, we have by redefining the constant. The standard solution to this equation is given by
and is the equation of a cycloid.
Rolling Ball: Angular momentum
The rotational energy is and by applying non-slipping condition we get
Friction
Rolling Cylinder
References
https://mathworld.wolfram.com/BrachistochroneProblem.html
https://physicscourses.colorado.edu/phys3210/phys3210_sp20/lecture/lec04-lagrangian-mechanics/
http://hades.mech.northwestern.edu/images/e/e6/Legeza-MechofSolids2010.pdf
https://www.tau.ac.il/~flaxer/edu/course/computerappl/exercise/Brachistochrone%20Curve.pdf