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Subdecks (2)
Phys (Ch-3)
Phys
3 cards
Phys (CH 2)
Phys
10 cards
Cards (35)
Rotational motion
Object rotates about an axis
Examples: rotation of earth, motion of
fan blades
, motion of
Ferris wheel
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Rigid body
A body that does not
deform
or change shape, distance between any two particles remains
constant
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Rotational motion under constant angular acceleration
1. Angular
velocity
changing at a
constant
rate
2. Angular acceleration is
constant
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Angular
displacement
Measured in
radians
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Angular velocity
Magnitude of
angular velocity
of
object
at any time t
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Angular acceleration
Rate of change of
angular velocity
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Linear distance (s) and angular displacement (θ)
s = rθ, where r is
radius
of circle
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Instantaneous angular velocity
Same for all particles in
rotational
object
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Linear
velocity (v) and
angular
velocity (ω)
v = rω
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Tangential acceleration
Acceleration tangent to
circular path
, measure of how
fast tangential velocity
changes
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Tangential
acceleration
(aT) and angular
acceleration
(α)
aT = rα
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Kinematic
equations for rotational motion are
analogous
to linear motion
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Angular velocity
vector is
perpendicular
to plane of rotation and along axis of rotation
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Right-hand rule for
direction
of
angular velocity
Wrap right hand around axis
, fingers point in direction of rotation, thumb points in direction of
angular velocity
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Direction of angular acceleration
Same as
angular
velocity when increasing, opposite when
decreasing
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Centripetal acceleration
Acceleration directed along radius towards centre of
circular
path, caused by change in direction of
velocity
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Calculating centripetal acceleration
ac = v²/r, where v is
linear
velocity and r is
radius
of circle
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Unlike
tangential
acceleration,
centripetal
acceleration is present in both
uniform
and
nonuniform circular
motion.
äc
Acceleration
vector in
radial
direction
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a
Acceleration
vector in
tangential
direction
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The two
acceleration
vectors äc and a, are
perpendicular
to each other
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The resultant
acceleration
points at an
angle
between a and a.
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