PhysicsGente
- 87
- 3
Homework Statement
Consider a pendulum of mass m and length b in the gravitational field whose point of attachment moves horizontally x_0=A(t) where A(t) 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 A(t)=cos\left(\sqrt{\frac {a} {b}}t\right)
Homework Equations
{\cal L} = T - U
The Attempt at a Solution
a) The position of the pendulum would be given by:
x = A(t) + bsin\left(\theta\right) \dot{x} = \dot{A}(t) + b\dot{\theta}cos\left(\theta\right)
y = bcos\left(\theta\right) \dot{y} = -b\dot{\theta}sin\left(\theta\right)
The kinetic energy T would be equal to:
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)
and taking the zero potential to be at x = 0 I get that the potential is equal to :
U = -mgy = -mgbcos\left(\theta\right)
And the Lagrangian would be:
{\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)
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!