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• DECEMBER 2019
Rigid Body Dynamics
Time Integration Method – Lesson 4
Rigid Body Dynamics
We discussed solving dynamics problem by implicit and explicit methods to obtain the response of
structures under dynamic loads. The outputs included deformation, stress, strain, etc. For large-scale
and long-duration dynamics problems, the computation cost to solve them are significant. In some
cases, when deformation of material is not the main concern, but the rigid motion is the response
engineers are looking for, rigid dynamics is the right path. This applies when:
• Objects are very stiff.
• Deformation of material points is not important.
• You are dealing with a large-scale, complex system.
No need to solve for things you don’t care about. Assume perfect rigid bodies!
• The structural stiffness K is removed from the equation of motion.
• Different rigid parts are linked by joints/contacts.
Rigid Body Dynamics (cont.)
Hardball Rigid Motion
Softball Distortion
Rigid Body Dynamics: Degrees of Freedom (DOFs)
Unlike dynamics for flexible bodies which looks for deformation at each material point, rigid body
dynamics looks for the rigid motion of the system. Especially, it solves for relative displacement
between different parts.
Revolute joint
5x2 = 10
constraint equation
Revolute joint
6x2 = 12 DOF 5 Constrained:
Ux, Uy, Uz, ROTx, ROTy
• One rigid body has at most 6 degrees of freedom in 3D space. 1 Free: ROTz
• The number of DOFs is largely reduced if using relative DOFs.
• Because parts are rigid, relative DOFs are sufficient to describe the mechanism.
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