Solving Rotation Condition for Equation of Motion

In summary, the Rotation Condition in the Equation of Motion is the requirement that the net torque acting on a rotating object must be equal to the product of its moment of inertia and its angular acceleration. This condition can be solved using the equation σ = Iα, and has units of Newton-meters (N*m) for torque, kilograms per square meter (kg/m^2) for moment of inertia, and radians per second squared (rad/s^2) for angular acceleration. The Rotation Condition ensures that the angular velocity of a rotating object remains constant, and can be applied to all types of rotating objects.
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If I know the equation of motion of the following form

[tex]\ddot{\theta} + k^2\sin\theta = 0[/tex]

(for pendulum for example). What's the condition (minimum angular velocity) to keep it rotate instead of just oscillation?
 
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Writing [tex]\omega = \dot \theta[/tex], that equation becomes (using the chain rule)

[tex]\omega \frac{d\omega}{d\theta} + k^2 \sin \theta = 0[/tex]

and solving that differential equation gives

[tex]\frac12 \omega^2 = k^2 \cos \theta + C.[/tex]

Once you have that, what condition on C do you need for [tex]\theta = \pi[/tex] to be possible? (Note that each side of this equation corresponds nicely to energy.)
 
  • #3


To solve for the rotation condition in this equation of motion, we need to consider the forces acting on the pendulum. The first term, \ddot{\theta}, represents the angular acceleration and is caused by the restoring force of gravity pulling the pendulum back towards its equilibrium position. The second term, k^2\sin\theta, represents the centripetal force, which is responsible for keeping the pendulum in circular motion.

In order for the pendulum to rotate instead of just oscillating, the centripetal force must be greater than the restoring force. This can be achieved by increasing the angular velocity, which is represented by \dot{\theta}. Therefore, the minimum angular velocity required for the pendulum to rotate is when the centripetal force is equal to the restoring force, or when \dot{\theta} = \sqrt{\frac{g}{l}}, where g is the acceleration due to gravity and l is the length of the pendulum.

It is important to note that this is the minimum angular velocity required for the pendulum to rotate, but higher angular velocities will still allow for rotation. Additionally, other factors such as air resistance and friction may also play a role in determining the minimum angular velocity for rotation. Further analysis and experimentation may be needed to fully understand and accurately determine this condition.
 

1. What is the "Rotation Condition" in the Equation of Motion?

The Rotation Condition in the Equation of Motion refers to the requirement that the net torque acting on a rotating object must be equal to the product of its moment of inertia and its angular acceleration. This condition is necessary for the object to maintain a constant angular velocity.

2. How is the Rotation Condition solved?

The Rotation Condition can be solved using the equation: σ = Iα, where σ is the net torque, I is the moment of inertia, and α is the angular acceleration. This equation can be rearranged to solve for any of the three variables.

3. What are the units of the Rotation Condition?

The units of the Rotation Condition are typically expressed as Newton-meters (N*m) for torque, kilograms per square meter (kg/m^2) for moment of inertia, and radians per second squared (rad/s^2) for angular acceleration.

4. How does the Rotation Condition affect the motion of a rotating object?

The Rotation Condition ensures that the angular velocity of a rotating object remains constant, as any changes in torque or moment of inertia will be reflected in the object's angular acceleration. If the Rotation Condition is not satisfied, the object's angular velocity will change, resulting in a change in its rotational motion.

5. Can the Rotation Condition be applied to all types of rotating objects?

Yes, the Rotation Condition is a fundamental principle of rotational motion and can be applied to all types of rotating objects, regardless of their shape, size, or composition. It is a key concept in the study of mechanics and is used in many fields of science and engineering.

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