What is the Differential Equation for a Non-Linear Torsional Spring Pendulum?

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SUMMARY

The differential equation governing the dynamics of a non-linear torsional spring pendulum is derived from the forces acting on the pendulum. The spring force, defined as F = Kθ³, counteracts the gravitational force, which is expressed as T - mg sin(θ). The resulting equation of motion is in the form of θ'' = -f(θ), where f(θ) encompasses both the gravitational and spring forces. This formulation allows for the analysis of the pendulum's oscillatory behavior under the influence of these restoring forces.

PREREQUISITES
  • Understanding of classical mechanics, specifically pendulum motion.
  • Familiarity with differential equations and their applications in physics.
  • Knowledge of torsional spring dynamics and non-linear force functions.
  • Basic grasp of angular motion and acceleration concepts.
NEXT STEPS
  • Study the derivation of the differential equation for non-linear oscillators.
  • Explore the effects of damping on pendulum motion and its mathematical representation.
  • Investigate numerical methods for solving non-linear differential equations.
  • Learn about the stability analysis of pendulum systems with non-linear restoring forces.
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Students and professionals in physics, mechanical engineering, and applied mathematics who are interested in the dynamics of oscillatory systems, particularly those involving non-linear forces.

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Homework Statement



Consider a pendulum oscillation problem, where pendulum oscillates around the vertical in the downward configuration.
Assume that there is no friction at the pivot point around which the pendulum rotates, and assume that there exists a torsional spring that counter acts the pendulum motion. Let the spring force Fs be a non-linear function of the displacement of the pendulum θ from the vertical configuration, that is,
F=K[tex]\theta^{3}[/tex]
Considering the presence of gravitational forces, ignoring external torques on the pendulum

To find a the differential equation governing the pendulum dynamics.

Kind regards

Homework Equations




The Attempt at a Solution


J\ddot{\theta}=T-m*g*sin([tex]\theta[/tex])
I am tying to find T as a function of F
 
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hancock.yang@ said:

Homework Statement



Consider a pendulum oscillation problem, where pendulum oscillates around the vertical in the downward configuration.
Assume that there is no friction at the pivot point around which the pendulum rotates, and assume that there exists a torsional spring that counter acts the pendulum motion. Let the spring force Fs be a non-linear function of the displacement of the pendulum θ from the vertical configuration, that is,
F=K[tex]\theta^{3}[/tex]
Considering the presence of gravitational forces, ignoring external torques on the pendulum

To find a the differential equation governing the pendulum dynamics.
...

The Attempt at a Solution


J\ddot{\theta}=T-m*g*sin([tex]\theta[/tex])
I am tying to find T as a function of F
There are two restoring forces here: gravity and the spring force. Write out the expression for the restoring force of gravity as a function of angle [itex]\theta[/itex]. Write out the expression for the restoring force of the spring as a function of [itex]\theta[/itex]. Since the two forces are always the same direction, add them together to find the total force.

How is the total force on the pendulum bob related to its acceleration? How is this acceleration related to the angular acceleration (the rate of change of angular speed)?

Answer those questions and you will be able to set up the differential equation of motion.(hint: it is in the form:

[tex]\ddot{\theta} = -f(\theta)[/tex]

AM
 
Andrew Mason said:
There are two restoring forces here: gravity and the spring force. Write out the expression for the restoring force of gravity as a function of angle [itex]\theta[/itex]. Write out the expression for the restoring force of the spring as a function of [itex]\theta[/itex]. Since the two forces are always the same direction, add them together to find the total force.

How is the total force on the pendulum bob related to its acceleration? How is this acceleration related to the angular acceleration (the rate of change of angular speed)?

Answer those questions and you will be able to set up the differential equation of motion.(hint: it is in the form:

[tex]\ddot{\theta} = -f(\theta)[/tex]

AM
Thank you for your help.
I have already worked it out .
 

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