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Lecture Rigid Body Dynamics
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Rigid Bodies Rigid bodies have both a position and orientation
Rigid bodies assume no object deformation Rigid body motion is represented by 2 parameters - center of mass - orientation (rotation matrix)
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Rigid Bodies Objects are defined in body space and transformed
by the position and orientation into world space
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Linear Velocity The change of the center of mass over time
For a pure translation ( constant), all points move with velocity
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Angular Velocity The change in orientation over time
Encodes both the axis and speed of the rotation direction encodes the axis magnitude encodes the speed (rad/s) But, how are and related?
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Angular Velocity For a given vector
The columns of represent the transformed axes
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Angular Velocity We can represent the cross product with a matrix
Therefore
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Velocity of a Point Since a point can be represented at any time by
Total velocity can then be expressed as Which can be rewritten as
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Force We can apply forces to the object at any point
Total force on an object is simply No information about where the forces are applied
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Torque Torque describes the “rotational force”
Total torque on an object is simply Tells us about the force distribution over the object
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Linear Momentum Linear momentum of a particle is
Linear momentum of a rigid body is then density integration over the body
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Linear Momentum Linear momentum can be simplified as follows
Assuming constant mass gives
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Angular Momentum Angular momentum of a rigid body
inertia tensor Taking the time derivative Angular momentum is conserved for no torque
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THANK YOU
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