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Circular Motion, Gravitation, Rotation, Bodies in Equilibrium

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Chapter 6,9,10 Circular Motion, Gravitation, Rotation, Bodies in Equilibrium Example A turntable is a uniform disk of metal of mass 1.5 kg and radius 13 cm. – PowerPoint PPT presentation

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Title: Circular Motion, Gravitation, Rotation, Bodies in Equilibrium


1
Chapter 6,9,10
  • Circular Motion, Gravitation, Rotation, Bodies in
    Equilibrium

2
Circular Motion
  • Ball at the end of a string revolving
  • Planets around Sun
  • Moon around Earth

3
The Radian
  • The radian is a unit of angular measure
  • The radian can be defined as the arc length s
    along a circle divided by the radius r

57.3
4
More About Radians
  • Comparing degrees and radians
  • Converting from degrees to radians

5
Angular Displacement
  • Axis of rotation is the center of the disk
  • Need a fixed reference line
  • During time t, the reference line moves through
    angle ?

6
Angular Displacement, cont.
  • The angular displacement is defined as the angle
    the object rotates through during some time
    interval
  • The unit of angular displacement is the radian
  • Each point on the object undergoes the same
    angular displacement

7
Average Angular Speed
  • The average angular speed, ?, of a rotating rigid
    object is the ratio of the angular displacement
    to the time interval

8
Angular Speed, cont.
  • The instantaneous angular speed
  • Units of angular speed are radians/sec
  • rad/s
  • Speed will be positive if ? is increasing
    (counterclockwise)
  • Speed will be negative if ? is decreasing
    (clockwise)

9
Average Angular Acceleration
  • The average angular acceleration of an object
    is defined as the ratio of the change in the
    angular speed to the time it takes for the object
    to undergo the change

10
Angular Acceleration, cont
  • Units of angular acceleration are rad/s²
  • Positive angular accelerations are in the
    counterclockwise direction and negative
    accelerations are in the clockwise direction
  • When a rigid object rotates about a fixed axis,
    every portion of the object has the same angular
    speed and the same angular acceleration

11
Angular Acceleration, final
  • The sign of the acceleration does not have to be
    the same as the sign of the angular speed
  • The instantaneous angular acceleration

12
Analogies Between Linear and Rotational Motion
Linear Motion with constant acc. (x,v,a)
Rotational Motion with fixed axis and constant
a (q,?,a)

13
Examples
  • 78 rev/min?
  • A fan turns at a rate of 900 rpm
  • Tangential speed of tips of 20cm long blades?
  • Now the fan is uniformly accelerated to 1200 rpm
    in 20 s

14
Relationship Between Angular and Linear Quantities
  • Displacements
  • Speeds
  • Accelerations
  • Every point on the rotating object has the same
    angular motion
  • Every point on the rotating object does not have
    the same linear motion

15
Centripetal Acceleration
  • An object traveling in a circle, even though it
    moves with a constant speed, will have an
    acceleration
  • The centripetal acceleration is due to the change
    in the direction of the velocity

16
Centripetal Acceleration, cont.
  • Centripetal refers to center-seeking
  • The direction of the velocity changes
  • The acceleration is directed toward the center of
    the circle of motion

17
Centripetal Acceleration, final
  • The magnitude of the centripetal acceleration is
    given by
  • This direction is toward the center of the circle

18
Centripetal Acceleration and Angular Velocity
  • The angular velocity and the linear velocity are
    related (v ?R)
  • The centripetal acceleration can also be related
    to the angular velocity

19
Forces Causing Centripetal Acceleration
  • Newtons Second Law says that the centripetal
    acceleration is accompanied by a force
  • F ma ?
  • F stands for any force that keeps an object
    following a circular path
  • Tension in a string
  • Gravity
  • Force of friction

20
Examples
  • Ball at the end of revolving string
  • Fast car rounding a curve

21
More on circular Motion
  • Length of circumference 2?R
  • Period T (time for one complete circle)

22
Example
  • 200 grams mass revolving in uniform circular
    motion on an horizontal frictionless surface at 2
    revolutions/s. What is the force on the mass by
    the string (R20cm)?

23
Newtons Law of Universal Gravitation
  • Every particle in the Universe attracts every
    other particle with a force that is directly
    proportional to the product of the masses and
    inversely proportional to the square of the
    distance between them.

24
Universal Gravitation, 2
  • G is the constant of universal gravitational
  • G 6.673 x 10-11 N m² /kg²
  • This is an example of an inverse square law

25
Universal Gravitation, 3
  • The force that mass 1 exerts on mass 2 is equal
    and opposite to the force mass 2 exerts on mass 1
  • The forces form a Newtons third law
    action-reaction

26
Universal Gravitation, 4
  • The gravitational force exerted by a uniform
    sphere on a particle outside the sphere is the
    same as the force exerted if the entire mass of
    the sphere were concentrated on its center

27
Gravitation Constant
  • Determined experimentally
  • Henry Cavendish
  • 1798
  • The light beam and mirror serve to amplify the
    motion

28
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29
Applications of Universal Gravitation
  • Weighing the Earth

30
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31
Applications of Universal Gravitation
  • g will vary with altitude

32
Escape Speed
  • The escape speed is the speed needed for an
    object to soar off into space and not return
  • For the earth, vesc is about 11.2 km/s
  • Note, v is independent of the mass of the object

33
Various Escape Speeds
  • The escape speeds for various members of the
    solar system
  • Escape speed is one factor that determines a
    planets atmosphere

34
Motion of Satellites
  • Consider only circular orbit
  • Radius of orbit r
  • Gravitational force is the centripetal force.

35
Motion of Satellites
  • Period ?

Keplers 3rd Law
36
Communications Satellite
  • A geosynchronous orbit
  • Remains above the same place on the earth
  • The period of the satellite will be 24 hr
  • r h RE
  • Still independent of the mass of the satellite

37
Satellites and Weightlessness
  • weighting an object in an elevator
  • Elevator at rest mg
  • Elevator accelerates upward m(ga)
  • Elevator accelerates downward m(ga) with alt0
  • Satellite a-g!!

38
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40
Force vs. Torque
  • Forces cause accelerations
  • Torques cause angular accelerations
  • Force and torque are related

41
Torque
  • The door is free to rotate about an axis through
    O
  • There are three factors that determine the
    effectiveness of the force in opening the door
  • The magnitude of the force
  • The position of the application of the force
  • The angle at which the force is applied

42
Torque, cont
  • Torque, t, is the tendency of a force to rotate
    an object about some axis
  • t is the torque
  • F is the force
  • symbol is the Greek tau
  • l is the length of lever arm
  • SI unit is N.m
  • Work done by torque W??

43
Direction of Torque
  • If the turning tendency of the force is
    counterclockwise, the torque will be positive
  • If the turning tendency is clockwise, the torque
    will be negative

44
Multiple Torques
  • When two or more torques are acting on an object,
    the torques are added
  • If the net torque is zero, the objects rate of
    rotation doesnt change

45
Torque and Equilibrium
  • First Condition of Equilibrium
  • The net external force must be zero
  • This is a necessary, but not sufficient,
    condition to ensure that an object is in complete
    mechanical equilibrium
  • This is a statement of translational equilibrium

46
Torque and Equilibrium, cont
  • To ensure mechanical equilibrium, you need to
    ensure rotational equilibrium as well as
    translational
  • The Second Condition of Equilibrium states
  • The net external torque must be zero

47
Equilibrium Example
  • The woman, mass m, sits on the left end of the
    see-saw
  • The man, mass M, sits where the see-saw will be
    balanced
  • Apply the Second Condition of Equilibrium and
    solve for the unknown distance, x

48
Moment of Inertia
  • The angular acceleration is inversely
    proportional to the analogy of the mass in a
    rotating system
  • This mass analog is called the moment of inertia,
    I, of the object
  • SI units are kg m2

49
Newtons Second Law for a Rotating Object
  • The angular acceleration is directly proportional
    to the net torque
  • The angular acceleration is inversely
    proportional to the moment of inertia of the
    object

50
More About Moment of Inertia
  • There is a major difference between moment of
    inertia and mass the moment of inertia depends
    on the quantity of matter and its distribution in
    the rigid object.
  • The moment of inertia also depends upon the
    location of the axis of rotation

51
Moment of Inertia of a Uniform Ring
  • Image the hoop is divided into a number of small
    segments, m1
  • These segments are equidistant from the axis

52
Other Moments of Inertia
53
Example
  • Wheel of radius R20 cm and I30kgm². Force
    F40N acts along the edge of the wheel.
  • Angular acceleration?
  • Angular speed 4s after starting from rest?
  • Number of revolutions for the 4s?
  • Work done on the wheel?

54
Rotational Kinetic Energy
  • An object rotating about some axis with an
    angular speed, ?, has rotational kinetic energy
    KEr½I?2
  • Energy concepts can be useful for simplifying the
    analysis of rotational motion
  • Units (rad/s)!!

55
Total Energy of a System
  • Conservation of Mechanical Energy
  • Remember, this is for conservative forces, no
    dissipative forces such as friction can be
    present
  • Potential energies of any other conservative
    forces could be added

56
Rolling down incline
  • Energy conservation
  • Linear velocity and angular speed are related
    vR?
  • Smaller I, bigger v, faster!!

57
Work-Energy in a Rotating System
  • In the case where there are dissipative forces
    such as friction, use the generalized Work-Energy
    Theorem instead of Conservation of Energy
  • (KEtKERPE)iW(KEtKERPE)f

58
Angular Momentum
  • Similarly to the relationship between force and
    momentum in a linear system, we can show the
    relationship between torque and angular momentum
  • Angular momentum is defined as
  • L I ?
  • and

59
Angular Momentum, cont
  • If the net torque is zero, the angular momentum
    remains constant
  • Conservation of Angular Momentum states The
    angular momentum of a system is conserved when
    the net external torque acting on the systems is
    zero.
  • That is, when

60
Conservation Rules, Summary
  • In an isolated system, the following quantities
    are conserved
  • Mechanical energy
  • Linear momentum
  • Angular momentum

61
Conservation of Angular Momentum, Example
  • With hands and feet drawn closer to the body, the
    skaters angular speed increases
  • L is conserved, I decreases, w increases

62
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64
Example
  • A 500 grams uniform sphere of 7.0 cm radius spins
    at 30 rev/s on an axis through its center.
  • Moment of inertia
  • Rotational kinetic energy
  • Angular momentum

65
Example
  • Find work done to open 30? a 1m wide door with a
    steady force of 0.9N at right angle to the
    surface of the door.

66
Example
  • A turntable is a uniform disk of metal of mass
    1.5 kg and radius 13 cm. What torque is required
    to drive the turntable so that it accelerates at
    a constant rate from 0 to 33.3 rpm in 2 seconds?

67
Center of Gravity
  • The force of gravity acting on an object must be
    considered
  • In finding the torque produced by the force of
    gravity, all of the weight of the object can be
    considered to be concentrated at a single point

68
Calculating the Center of Gravity
  • The object is divided up into a large number of
    very small particles of weight (mg)
  • Each particle will have a set of coordinates
    indicating its location (x,y)

69
Calculating the Center of Gravity, cont.
  • We wish to locate the point of application of the
    single force whose magnitude is equal to the
    weight of the object, and whose effect on the
    rotation is the same as all the individual
    particles.
  • This point is called the center of gravity of the
    object

70
Coordinates of the Center of Gravity
  • The coordinates of the center of gravity can be
    found

71
Center of Gravity of a Uniform Object
  • The center of gravity of a homogenous, symmetric
    body must lie on the axis of symmetry.
  • Often, the center of gravity of such an object is
    the geometric center of the object.

72
Example
  • Find the center of mass (gravity) of these
    masses 3kg (0,1), 2kg (0,0)
  • And 1kg (2,0)

73
Example
  • Find the center of mass (gravity) of the
    dumbbell, 4 kg and 2 kg with a 4m long 3kg rod.

74
Torque, review
  • t is the torque
  • F is the force
  • symbol is the Greek tau
  • l is the length of lever arm
  • SI unit is N.m

75
Direction of Torque
  • If the turning tendency of the force is
    counterclockwise, the torque will be positive
  • If the turning tendency is clockwise, the torque
    will be negative

76
Multiple Torques
  • When two or more torques are acting on an object,
    the torques are added
  • If the net torque is zero, the objects rate of
    rotation doesnt change

77
Example
  • A 2 m by 2 m square metal plate rotates about its
    center. Calculate the torque of all five forces
    each with magnitude 50N.

78
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79
Torque and Equilibrium
  • First Condition of Equilibrium
  • The net external force must be zero
  • The Second Condition of Equilibrium states
  • The net external torque must be zero

80
Example
  • The system is in equilibrium. Calculate W and
    find the tension in the rope (T).

81
Example
  • A 160 N boy stands on a 600 N concrete beam in
    equilibrium with two end supports. If he stands
    one quarter the length from one support, what are
    the forces exerted on the beam by the two
    supports?

82
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