Physics 101 Chapter 8 Rotation
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Transcript of Physics 101 Chapter 8 Rotation
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2010 Pearson Education, Inc. Fig. 5-CO, p.76
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Chapter 8:
ROTATIONAL MOTION
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Circular Motion
When an object turns about an internal
axis, it is undergoing circular motion or
rotation. Circular Motion is characterized by two
kinds of speeds:
tangential(or linear) speed. rotational(or circular) speed.
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Tangential Speed
The distancetraveled by a point on the rotating objectdivided by the time taken to travel that distance is called itstangential speed (symbol v)
Points closer to the circumference have a highertangentialspeedthan points closer to the center.
Fig. 8.1
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A ladybug sits halfway between the rotational axis and the outer
edge of the turntable . When the turntable has a rotationalspeed of 20 RPM and the bug has a tangential speed of 2 cm/s,what will be the rotational and tangential speeds of her friendwho sits at the outer edge?
A. 1 cm/s B. 2 cm/s C. 4 cm/s D. 8 cm/s
Rotational and Tangential Speed
CHECK YOUR NEIGHBOR
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A ladybug sits halfway between the rotational axis and the
outer edge of the turntable . When the turntable has arotational speed of 20 RPM and the bug has a tangentialspeed of 2 cm/s, what will be the rotational and tangentialspeeds of her friend who sits at the outer edge?
A. 1 cm/sB. 2 cm/s
C. 4 cm/s
D. 8 cm/s
Rotational and Tangential Speed
CHECK YOUR ANSWER
Explanation:
Tangential speed =
Rotational speed of both bugs is the same, so
if radial distance doubles, tangential speed
also doubles.So, tangential speed is 2 cm/s 2 = 4 cm/s.
r
Can we make this
compl icated?!!!
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Rotational Inertia
An object rotating about an axis tends to
remain rotating about the same axis at the
same rotational speed unless interfered
with by some external influence.
The propertyof an object to resist changes
in its rotational state of motion is called
rotational inertia (symbol I).
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Rotational Inertia
Depends upon
massof object.
distribution of mass around axis of
rotation.
The greater the distance
between an objects mass
concentration and the axis, the
greater the rotational inertia.
Fig. 8.9
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Rotational Inertia
The greater the rotational inertia, the harder it is
to change its rotational state. A tightrope walker carries a long pole that has a high rotational
inertia, so it does not easily rotate.
Keeps the tightrope walker stable.
Fig. 8.10
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Rotational Inertia
Depends upon the axis aroundwhich it rotates
Easier to rotate pencil around an
axis passing through it.
Harder to rotate it around verticalaxis passing through center.
Hardest to rotate it around vertical
axis passing through the end.
Fig. 8.11
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Rotational Inertia
The rotational inertia depends upon the shape of theobject and its rotational axis.
Fig. 8.15
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A hoop and a disk are released from the top of an
incline at the same time. Which one will reach thebottom first?
A. Hoop
B. DiskC. Both together
D. Not enough information
Rotational Inertia
CHECK YOUR NEIGHBOR
Fig. 8.14
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Torque
The tendency of a force to cause rotation is called
torque. Torque depends upon three factors:
Magnitude of the force
The direction in which it acts
The point at which it is applied on the object
Fig. 8.16
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Torque lever arm force
Torque
The equation for Torque is
The lever arm depends upon
where the force is applied.
The direction in which it acts.
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TorqueExample
1stpicture: Lever arm is lessthanlength of handle
because of direction of force. 2nd picture: Lever arm is equalto length of handle.
3rdpicture: Lever arm is longerthan length ofhandle.
Fig. 8.20
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Torque
Clockwise Torque = Counterclockwise Torque
Fig. 8.18
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Center of Mass and Center of Gravity
Center of mass (CM)is the averageposition of all the mass that makes up the
object.
Center of gravity (CG) is the averageposition of weight distribution.
Since weight and mass are proportional,
center of gravity and center of mass usually
refer to the same point of an object.
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Fig. 8.22
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To determine the center of gravity
Of a regular object,move fingers from ends toward center of
object (Fig. 8.25)
Center of Mass and Center of Gravity
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Center of Mass and Center of Gravity
Of an irregular object suspend the object from a point and draw a vertical line
from suspension point.
repeat after suspending from another point.
The center of gravity lies where the two linesintersect.
Fig. 8.28
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The center of mass of a non-vertically or
non-horizontally thrown or fired objectfollows aparabolictrajectory.
Fig. 8.21
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Center of gravity(mass) may lie outside of an
objects mass
Fig. 8.27
Fig. 8.28
Fig. 8.31
Fig. 8.32
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Center of GravityStability
The location of the center of gravity
is important for stability.
If we draw a line straight down from the
center of gravity and it falls insidethe
base of the object, it is in stable
equi l ibr ium; it will balance.
If it falls outside the base, it is unstable.
Fig. 8.29
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An object with a wide base and low center of
gravity is more stable.
Fig. 8.36
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Centripetal Force
Any force directed towarda fixed centeris called a
centr ipetalforce. Centripetal means center-seeking or toward the
center.
Examples of the centripetal force
Ball on a string Car in a curve
Space shuttle in orbit
Amusement park rotor ride
Note: Something must provide the centripetal force for
an object to travel in a circle!
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Centripetal Force
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When a car rounds a
curve, the centripetal force
prevents it from skidding
off the road.
If the road is wet, or if thecar is going too fast, the
centripetal force is
insufficient to prevent
skidding off the road.
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Centripetal Force
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Suppose you take a sharper turn than before and
halvethe radius, by what factor will the centripetalforce need to change to prevent skidding?
A. Double
B. Four timesC. Half
D. One-quarter
Centripetal Force
CHECK YOUR NEIGHBOR
Centripetal Force
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Suppose you take a sharper turn than before and
halvethe radius, by what factor will the centripetalforce need to change to prevent skidding?
A. Double
B. Four timesC. Half
D. One-quarter
Centripetal Force
CHECK YOUR NEIGHBOR
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Lift force on the wings provides
the centripetal forceto keep the
airplane flying in a loop
Centripetal acceleration may
be several times as great as g,so pilot may experience forces
several times greater than his
weight (g forces)
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A l M
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Angular Momentum
Theinertiaof rotation of rotating objects is called
angu lar m omentum. This is analogous to inertia of motion, which was
momentum.
Linear momentum mass velocity (Chapter 6)
Linear momentum = mv
Angular momentum rotational inertia angular velocity
Angular momentum = I
=mvr
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C ti f A l M t
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Conservation of Angular Momentum
An external net torque is required to change the angular
momentum of an object.
Rotational version of Newtons first law: m1v1= m2v2 (Ch. 6)
The law of conservation of angular momentum states:
If no external net torqueacts on a rotating system, the
angular momentum of that system remains constant.
m1v1r1 = m2v2r2
Angular Momentum
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Suppose you are swirling a can around and suddenly
decide to pull the rope in halfway; by what factor wouldthe speed of the can change?
A. Double
B. Four timesC. Half
D. One-quarter
g
CHECK YOUR NEIGHBOR
Angular Momentum
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Suppose you are swirling a can around and suddenly
decide to pull the rope in halfway; by what factor wouldthe speed of the can change?
A. Double
B. Four timesC. Half
D. One-quarter
g
CHECK YOUR NEIGHBOR
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Angular Momentum
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Suppose by pulling the weights inward, the rotational
inertia of the man reduces to half its value. By whatfactor would his angular velocity change?
A. Double
B. Three timesC. Half
D. One-quarter
g
CHECK YOUR NEIGHBOR
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Fig. 8.53
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Precession