A bead of mass is attached to a smooth wire in the shape of the curve . One end of a spring is attached to the bead, and the other end is fixed at the origin. The spring constant and the spring's un-stretched length is zero.
There is an ambient downward gravitational acceleration of .
At a particular instant in time, the horizontal position and horizontal velocity are the following: What is the horizontal acceleration at this same instant in
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Relevant wiki: Lagrangian Mechanics
Here's a Lagrangian mechanics solution:
Spatial Coordinates:
x = x y = x 2 x ˙ = x ˙ y ˙ = 2 x x ˙
Square of velocity and kinetic energy:
v 2 = x ˙ 2 + y ˙ 2 = ( 1 + 4 x 2 ) x ˙ 2 E = 2 1 m v 2 = 2 1 m ( 1 + 4 x 2 ) x ˙ 2
Gravitational potential energy:
U g = m g y = m g x 2
Spring potential energy:
U s = 2 1 k ( x 2 + x 4 )
Lagrangian:
L = E − U g − U s = 2 1 m ( 1 + 4 x 2 ) x ˙ 2 − m g x 2 − 2 1 k ( x 2 + x 4 )
Equation of Motion:
d t d ∂ x ˙ ∂ L = ∂ x ∂ L
Inner left term:
∂ x ˙ ∂ L = m ( 1 + 4 x 2 ) x ˙
Left term:
d t d ∂ x ˙ ∂ L = m ( 1 + 4 x 2 ) x ¨ + 8 m x x ˙ 2
Right term:
∂ x ∂ L = 4 m x x ˙ 2 − 2 m g x − k x − 2 k x 3
Equating:
m ( 1 + 4 x 2 ) x ¨ + 8 m x x ˙ 2 = 4 m x x ˙ 2 − 2 m g x − k x − 2 k x 3 m ( 1 + 4 x 2 ) x ¨ = − 4 m x x ˙ 2 − 2 m g x − k x − 2 k x 3
Final expression for horizontal acceleration:
x ¨ = m ( 1 + 4 x 2 ) − 4 m x x ˙ 2 − 2 m g x − k x − 2 k x 3
Plugging in numbers:
x ¨ = ( 1 ) ( 1 + 4 ( 2 1 ) 2 ) − 4 ( 1 ) ( 2 1 ) ( 3 2 ) − 2 ( 1 ) ( 1 0 ) ( 2 1 ) − ( 5 ) ( 2 1 ) − ( 2 ) ( 5 ) ( 2 1 ) 3 = − 1 5 . 8 7 5