A point mass m slides without friction from O = (0,0) to P = (a, b) on a curve C under the action of constant gravity (see Figure) with vanishing initial velocity. The time it takes for m to reach P is given by P 1 -ds, Jo T = where ds = V(dr)² + (dy)² and v is the speed. The goal is P=(a,b) y to find the curve C that minimises T. (a) Write T as T = Sº F[y(x), y'(x)]dx and determine the function F. (b) Making use of F – y = const (see Problem 1), derive the relation y' y ƏF dy' V# - 1, where d is a constant. (c) Use the parametric representation y(@) = d sin² = $(1 – cos ø) and determine r(6). %3D The extremal curve is a cycloid.

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A point mass m slides without friction from O = (0,0) to
P = (a, b) on a curve C under the action of constant gravity
(see Figure) with vanishing initial velocity. The time it takes
for m to reach P is given by
P
1
-ds,
Jo
T =
where ds =
V(dr)² + (dy)² and v is the speed. The goal is
P=(a,b)
y
to find the curve C that minimises T.
(a) Write T as T =
Sº F[y(x), y'(x)]dx and determine the function F.
(b) Making use of F – y = const (see Problem 1), derive the relation y'
y ƏF
dy'
V# - 1, where d is
a constant.
(c) Use the parametric representation y(@) = d sin² = $(1 – cos ø) and determine r(6).
%3D
The extremal curve is a cycloid.
Transcribed Image Text:A point mass m slides without friction from O = (0,0) to P = (a, b) on a curve C under the action of constant gravity (see Figure) with vanishing initial velocity. The time it takes for m to reach P is given by P 1 -ds, Jo T = where ds = V(dr)² + (dy)² and v is the speed. The goal is P=(a,b) y to find the curve C that minimises T. (a) Write T as T = Sº F[y(x), y'(x)]dx and determine the function F. (b) Making use of F – y = const (see Problem 1), derive the relation y' y ƏF dy' V# - 1, where d is a constant. (c) Use the parametric representation y(@) = d sin² = $(1 – cos ø) and determine r(6). %3D The extremal curve is a cycloid.
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