With good sketch, derive the equation of motion of a compound pendulum. What is the difference between a simple pendulum and a compound pendulum? State the equation(s) for calculating natural frequency in both pendulums.

Physics

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Answer

Iθ¨+mgLθ=0I\ddot{\theta} + mgL\theta = 0

ωn=gL\omega_n = \sqrt{\frac{g}{L}}

ωn=mgLI\omega_n = \sqrt{\frac{mgL}{I}}

Step-by-step solution

4 steps

Here are the explanations and derivations for pendulums:

  1. Derivation of the Equation of Motion of a Compound Pendulum
    • Sketch: Imagine a rigid body of mass mm suspended from a pivot point O. Let G be the center of mass (CM) of the body, located at a distance LL from the pivot O. When the body is displaced by a small angle θ\theta from its equilibrium position, the gravitational force mgmg acts vertically downwards through G.

      • Draw a pivot point O.
      • Draw a rigid body hanging from O.
      • Mark the center of mass G, a distance LL below O when at equilibrium.
      • Show the body displaced by an angle θ\theta from the vertical.
      • Draw the gravitational force mgmg acting downwards through G.
      • Indicate the perpendicular distance from O to the line of action of mgmg, which is Lsin⁡θL \sin\theta.
    • Derivation:

  1. Identify the forces and torques.

    The only force creating a torque about the pivot O is gravity, mgmg, acting at the center of mass G.
    The torque τ\tau due to gravity about the pivot O is given by: τ=−(mg)(Lsin⁡θ) \tau = -(mg)(L \sin\theta) The negative sign indicates that the torque acts to restore the pendulum to its equilibrium position (opposite to the direction of increasing θ\theta).

  2. Apply Newton's second law for rotational motion.

        The rotational equivalent of Newton's second law is $\tau = I\alpha$, where $I$ is the moment of inertia of the compound pendulum about the pivot O, and $\alpha$ is the angular acceleration ($\ddot{\theta}$).
        $$
        -mgL \sin\theta = I\ddot{\theta}
        $$
    
  3. Rearrange the equation.

        $$
        I\ddot{\theta} + mgL \sin\theta = 0
        $$
    
  4. For small angles of oscillation, sin⁡θ≈θ\sin\theta \approx \theta.

        Substituting this approximation into the equation:
        $$
        I\ddot{\theta} + mgL\theta = 0
        $$
        This is the equation of motion for a compound pendulum under small oscillations.
        $$
        \boxed{I\ddot{\theta} + mgL\theta = 0}
        $$
    

    2. Difference between a Simple Pendulum and a Compound Pendulum * A simple pendulum consists of a point mass (bob) suspended by a massless, inextensible string from a fixed pivot. All its mass is concentrated at a single point. * A compound pendulum (or physical pendulum) is any rigid body that oscillates about a fixed pivot point under the influence of gravity. Its mass is distributed throughout its volume, and its moment of inertia about the pivot is a significant factor in its motion.

    1. Equations for Calculating Natural Frequency
      • Simple Pendulum: The natural angular frequency ωn\omega_n for a simple pendulum of length LL is:

        ωn=gL\boxed{\omega_n = \sqrt{\frac{g}{L}}}

        where gg is the acceleration due to gravity.

      • Compound Pendulum: The natural angular frequency ωn\omega_n for a compound pendulum is:

        ωn=mgLI\boxed{\omega_n = \sqrt{\frac{mgL}{I}}}

        where mm is the total mass of the pendulum, gg is the acceleration due to gravity, LL is the distance from the pivot to the center of mass, and II is the moment of inertia of the pendulum about the pivot point.

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