Brachistochrone
Introduction
To find the shape of the curve which the time is shortest possible. . .
Theory
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 Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle y\left( 1 + y'^{2}\right) = \frac1{2gC^2} = k^2 } by redefining the constant. The standard solution to this equation is given by
and is the equation of a cycloid.
Friction
Rolling Ball
References
https://mathworld.wolfram.com/BrachistochroneProblem.html
https://physicscourses.colorado.edu/phys3210/phys3210_sp20/lecture/lec04-lagrangian-mechanics/