Pendulum in accelerating traincar

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SUMMARY

The discussion centers on determining the oscillatory period τ of a pendulum suspended in a constantly accelerating train car. The governing differential equation derived from the forces acting on the pendulum is mgθ + ma = mlθ̈, leading to the equation θ̈ + (g/l)θ + (a/l) = 0. The small angle approximation simplifies the analysis, and participants explore methods to solve this differential equation, with Fourier transformation being suggested as a potential approach.

PREREQUISITES
  • Understanding of classical mechanics, specifically pendulum motion.
  • Familiarity with differential equations and their solutions.
  • Knowledge of small angle approximation in physics.
  • Experience with Fourier transforms and their applications in solving differential equations.
NEXT STEPS
  • Research methods for solving second-order linear differential equations.
  • Study the application of Fourier transforms in physics problems.
  • Learn about the effects of acceleration on pendulum dynamics.
  • Explore numerical methods for simulating pendulum motion in non-inertial frames.
USEFUL FOR

Physics students, educators, and anyone interested in the dynamics of pendulums in non-inertial reference frames.

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Homework Statement


A pendulum bob of mass m is suspended by massless thread of length l from the ceiling of a boxcar. The car undergoes constant acceleration a along a straight, level track. What, in the small angle approximation, is the oscillatory period tau of the pendulum?

Homework Equations


[tex]F_g=mg\sin\theta=mg\theta[/tex]
[tex]F_a=ma\cos\theta=ma[/tex]

The Attempt at a Solution


[tex]mg\theta+ma=ml\ddot{\theta}[/tex]
[tex]\frac{g}{l} \theta+\frac{a}{l}=\ddot{\theta}[/tex]

What's the quickest way to solve this differential equation?
 
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My first idea was to Fourier transform it, but I'm not sure if that would be the best approach. Any suggestions?
 

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