Energy Balance
Force |
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Moment |
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Gravity |
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Friction |
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Spring |
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Rigid Body Work - Energy Terms |
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The Principle of Work and Energy equates the total work performed on a body to the change in kinetic energy,
Σ Work = Δ Kinetic Energy
Another way to express this concept is
where
T1 = kinetic energy (translational and rotational)
at position 1
T2 = kinetic energy (translational and rotational)
at position 2
ΣU1-2 =
total change in energy (i.e. work)
between positions 1 and 2
Work on a rigid body is the same as work on a particle, with the addition of rotational energy. Recall from Particle Energy Methods section, there are various ways to model energy for a particle. These are listed in the table at the left. |
Rotational and Translational
Kinetic Energy |
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For a particle that has no rotation, the
kinetic energy is simply,
T = 1/2 m v2
This equation can be applied to every particle that makes up a rigid
body,
However, if the particle is a rigid body with dimensions, then the velocity needs to be written as
where G is the center of gravity. The second terms models the rotation of the object. Substituting vi into the kinetic equation and noting that a magnitude of vi/G = ri/G ω gives
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T = 1/2 m vG2 + 1/2
IG ω2
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If the rigid body has a fixed point, then the equation becomes
T = 1/2 Io ω2
where Io is moment of inertia about the fixed point. |