- #1
jonjacson
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Homework Statement
To find the period of oscillation of the pendulum and the equation of motion.
Homework Equations
Conservation of energy.
Potential energy in a constant field = mgh.
Kinetic energy in polar coordinates with r constant = (1/2) m r2 (dΘ2/dt2)
The Attempt at a Solution
I won't use the Newton laws because that means a second order differential equation. Instead I use the conservation of energy so I start from a first order equation.
1.- I set the origin of coordinates at the anchor point of the pendulum.
2.- I will use polar coordinates, the angle starts counting from the vertical counterclockwise.
3.- The energy is conserved so at the point 1 (at the bottom when the pendulum is faster) we have:
L is the length of the pendulum
KE =(1/2) mL2 dΘ2/dt2
Potential energy = -mgL ; I set the potential energy as zero at the origin of coordinates, the anchor point of the pendulum.
At the point 2 when the speed is zero I have:
KE = 0
PE = -mg (lcosΘ)
Now I equate the sum of the KE and PE at both points:
(1/2)mL2 dΘ2/dt2 -mgL = 0 -mg (LcosΘ)
(1/2) dΘ2/dt2 = g(1 - cos Θ ) /L
If Θ is small cos Θ can be aproximated by 1 - Θ2/2, so:
(1/2) dΘ2/dt2 = g ( 1- (1-Θ2/2))/L
Finally:
dΘ/dt = √(g/L) Θ2
dΘ/√(g/L) Θ2 = dt
Since Θ can get outside de square the integral is :
Log Θ = √L/g t + constant
And the basic expression is an exponential:
So Θ= exp t
And this is not the expected periodic movement and that does not make any sense. Does anybody know where is the mistake?
THanks