A subscription to JoVE is required to view this content.
The movement of a rigid object can be understood through the equations that explain both translational and rotational motion about the center of mass of the object, point G. This center of mass is the point where the equation of motion for translational motion comes into play, as per Newton's Second Law.
The combined moments generated about the center of mass of the object are equal to the rate of change of the angular momentum of the body. An external force, when applied at a different point other than the center of mass of the object, causes the body to rotate and generates a moment.
The angular momentum of this point is articulated as a vector product, incorporating its relative position and velocity with respect to the center of mass of the object. The derivative of angular momentum with respect to time provides us with the moment generated at a point where an external force is applied. By summing the moments of all points within the rigid body, one can calculate the total moment of the system about the center of mass of the object.
From Chapter 16:
Now Playing
3-Dimensional Kinetics of a Rigid Body
238 Views
3-Dimensional Kinetics of a Rigid Body
368 Views
3-Dimensional Kinetics of a Rigid Body
273 Views
3-Dimensional Kinetics of a Rigid Body
231 Views
3-Dimensional Kinetics of a Rigid Body
169 Views
3-Dimensional Kinetics of a Rigid Body
172 Views
3-Dimensional Kinetics of a Rigid Body
160 Views
3-Dimensional Kinetics of a Rigid Body
187 Views
3-Dimensional Kinetics of a Rigid Body
188 Views
3-Dimensional Kinetics of a Rigid Body
414 Views
Copyright © 2025 MyJoVE Corporation. All rights reserved
We use cookies to enhance your experience on our website.
By continuing to use our website or clicking “Continue”, you are agreeing to accept our cookies.