Rotational Motion
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Transcript Rotational Motion
Rotational Motion
Rigid Body
Real objects have mass at
points other than the center
of mass.
ri
Each point in an object can
be measured from an origin
at the center of mass.
If the positions are fixed
compared to the center of
mass it is a rigid body.
Translation and Rotation
The motion of a rigid body
includes the motion of its
center of mass.
This is translational motion
vCM
A rigid body can also move
while its center of mass is
fixed.
This is rotational motion.
Angular Acceleration
ar
at
at v
v
r
r
t
t
The angular acceleration is
In uniform circular motion
there is a constant radial
acceleration.
• ar = v2 / r = r2
If the angular velocity
changes there is
acceleration tangent to the
circle as well as radially.
The Effect of Torque
A tangential force on a mass creates an acceleration.
• Tangential force: Ft = m at
• Tangential acceleration: at = r
The force is associated with a torque.
• Torque: t = r Ft
r
Ft
m
Rotational Law of Acceleration
The force law can be combined with rotational
motion.
• Torque: t = r Ft = r m at = m r2
If torque replaces force, and angular acceleration
replaces acceleration, this looks like the law of
acceleration.
t (mr 2 ) I
Rotation and Translation
A rolling wheel is moving
forward with kinetic energy.
A rolling wheel is rotating
with kinetic energy.
The velocity is measured at
the center of mass.
The axis of rotation is at the
center of mass.
• Krot = ½ I 2
• KCM = ½ m v2
v
Rolling Energy
The energy of a rolling wheel
is due to both the translation
and rotation.
The velocity is linked to the
angular velocity.
The effective energy is the
same as a wheel rotating
about a point on its edge.
• Parallel axis theorem
K K CM K rot
K 12 mv 2 12 I 2
K 12 (mR 2 I ) 2
Energy Conserved
A change in kinetic energy is
due to work done on the
wheel.
• Work is from a force
• Force acts as a torque
v
R
Rolling down an incline the
force is from gravity.
F = mg
q
• Pivot at the point of contact
The potential energy is
converted to kinetic energy.
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