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