- #1
PhysicsGente
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Homework Statement
Consider a pendulum of mass m and length b in the gravitational field whose point of attachment moves horizontally [tex]x_0=A(t)[/tex] where [tex]A(t)[/tex] is a function of time.
a) Find the Lagrangian equation of motion.
b) Give the equation of motion in the case of small oscillations. What happens in that case when [tex]A(t)=cos\left(\sqrt{\frac {a} {b}}t\right)[/tex]
Homework Equations
[tex] {\cal L} = T - U [/tex]
The Attempt at a Solution
a) The position of the pendulum would be given by:
[tex] x = A(t) + bsin\left(\theta\right) [/tex] [tex] \dot{x} = \dot{A}(t) + b\dot{\theta}cos\left(\theta\right) [/tex]
[tex] y = bcos\left(\theta\right) [/tex] [tex] \dot{y} = -b\dot{\theta}sin\left(\theta\right) [/tex]
The kinetic energy [tex]T[/tex] would be equal to:
[tex] T = \frac {m} {2} \left({\dot{A}(t)}^2 + 2\dot{A}(t) b \dot{\theta} cos\left(\theta\right) + b^2\dot{\theta}^2\right) [/tex]
and taking the zero potential to be at [tex] x = 0 [/tex] I get that the potential is equal to :
[tex] U = -mgy = -mgbcos\left(\theta\right) [/tex]
And the Lagrangian would be:
[tex] {\cal L} = T - U = \frac {m} {2} \left({\dot{A}(t)}^2 + 2\dot{A}(t) b \dot{\theta} cos\left(\theta\right) + b^2\dot{\theta}^2\right) + mgbcos\left(\theta\right) [/tex]
I would like to know if I have represented the position of the pendulum the right way because I get a non-linear differential equation for part b and I doubt that's right. Thanks!