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MM203 Mechanics of Machines: Part 1

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What do dv and ds represent? Rectilinear motion. 11. Example ... Integration of F = ma w.r.t. time gives equations of impulse and momentum. ... – PowerPoint PPT presentation

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Title: MM203 Mechanics of Machines: Part 1


1
MM203Mechanics of Machines Part 1
2
Module
  • Lectures
  • Tutorials
  • Labs
  • Why study dynamics?
  • Problem solving

3
Vectors
4
Unit vectors - components
5
Direction cosines
  • l, m, and n direction cosines between v and x-,
    y-, and z-axes
  • Calculate 3 direction cosines for

6
Dot (or scalar) product
  • Component of Q in P direction

7
Angle between vectors
8
Dot product
  • Commutative and distributive

9
Particle kinematics
  • What is kinematics?
  • What is a particle?
  • Rectilinear motion - review
  • Plane curvilinear motion - review
  • Relative motion
  • Space curvilinear motion

10
Rectilinear motion
  • Combining gives
  • What do dv and ds represent?

11
Example
  • The acceleration of a particle is a 4t - 30
    (where a is in m/s2 and t is in seconds).
    Determine the velocity and displacement in terms
    of time. (Problem 2/5, MK)

12
Vector calculus
  • Vectors can vary both in length and in direction

13
Plane curvilinear motion
  • Choice of coordinate system (axes)
  • Depends on problem how information is given
    and/or what simplifies solution
  • Practice

14
Plane curvilinear motion
  • Rectangular coordinates
  • Position vector - r
  • e.g. projectile motion
  • ENSURE CONSISTENCY IN DIRECTIONS

15
Plane curvilinear motion
  • Normal and tangential coordinates
  • Instantaneous radius of curvature r
  • What is direction of v?

Note that dr/dt can be ignored in this case see
MK.
16
Plane curvilinear motion
17
Example
  • A test car starts from rest on a horizontal
    circular track of 80 m radius and increases its
    speed at a uniform rate to reach 100 km/h in 10
    seconds. Determine the magnitude of the
    acceleration of the car 8 seconds after the
    start. (Answer a 6.77 m/s2). (Problem 2/97,
    MK)

18
Example
  • To simulate a condition of weightlessness in
    its cabin, an aircraft travelling at 800 km/h
    moves an a sustained curve as shown. At what rate
    in degrees per second should the pilot drop his
    longitudinal line of sight to effect the desired
    condition? Use g 9.79 m/s2. (Answer db/dt
    2.52 deg/s). (Problem 2/111, MK)

19
Example
  • A ball is thrown horizontally at 15 m/s from the
    top of a cliff as shown and lands at point C. The
    ball has a horizontal acceleration in the
    negative x-direction due to wind. Determine the
    radius of curvature of the path at B where its
    trajectory makes an angle of 45 with the
    horizontal. Neglect air resistance in the
    vertical direction. (Answer r 41.8 m).
    (Problem 2/125, MK)

20
Plane curvilinear motion
  • Polar coordinates

21
Plane curvilinear motion
22
Example
  • An aircraft flies over an observer with a
    constant speed in a straight line as shown.
    Determine the signs (i.e. ve, -ve, or 0) for
  • for positions
  • A, B, and C.
  • (Problem 2/134, MK)

23
Example
  • At the bottom of a loop at point P as shown, an
    aircraft has a horizontal velocity of 600 km/h
    and no horizontal acceleration. The radius of
    curvature of the loop is 1200 m. For the radar
    tracking station shown, determine the recorded
    values of d2r/dt2 and d2q/dt2 for this instant.
    (Answer d2r/dt2 12.5 m/s2, d2q/dt2 0.0365
    rad/s2). (Problem 2/141, MK)

24
Relative motion
  • Absolute (fixed axes)
  • Relative (translating axes)
  • Used when measurements are taken from a moving
    observation point, or where use of moving axes
    simplifies solution of problem.
  • Motion of moving coordinate system may be
    specified w.r.t. fixed system.

25
Relative motion
  • Set of translating axes (x-y) attached to
    particle B (arbitrarily). The position of A
    relative to the frame x-y (i.e. relative to B) is

26
Relative motion
  • Absolute positions of points A and B (w.r.t.
    fixed axes X-Y) are related by

27
Relative motion
  • Differentiating w.r.t. time gives
  • Coordinate systems may be rectangular, tangential
    and normal, polar, etc.

28
Inertial systems
  • A translating reference system with no
    acceleration is known as an inertial system. If
    aB 0 then
  • Replacing a fixed reference system with an
    inertial system does not affect calculations (or
    measurements) of accelerations (or forces).

29
Example
  • A yacht moving in the direction shown is tacking
    windward against a north wind. The log registers
    a hull speed of 6.5 knots. A telltale (a string
    tied to the rigging) indicates that the direction
    of the apparent wind is 35 from the centerline
    of the boat. What is the true wind velocity?
    (Answer vw 14.40 knots). (Problem 2/191, MK)

30
Example
  • To increase his speed, the water skier A cuts
    across the wake of the boat B which has a
    velocity of 60 km/h as shown. At the instant when
    q 30, the actual path of the skier makes an
    angle b 50 with the tow rope. For this
    position, determine the velocity vA of the skier
    and the value of dq/dt. (Answer vA 80.8 km/h,
    dq/dt 0.887 rad/s). (Problem 2/193, MK)

31
Example
  • Car A is travelling at a constant speed of 60
    km/h as it rounds a circular curve of 300 m
    radius. At the instant shown it is at q 45.
    Car B is passing the centre of the circle at the
    same instant. Car A is located relative to B
    using polar coordinates with the pole moving with
    B. For this instant, determine vA/B and the
    values fo dq/dt and dr/dt as measured by an
    observer in car B. (Answer vA/B 36.0 m/s,
    dq/dt 0.1079 rad/s, dr/dt -15.71 m/s).
    (Problem 2/201, MK)

32
Space curvilinear motion
  • Rectangular coordinates (x, y, z)
  • Cylindrical coordinates (r, q, z)
  • Spherical coordinates (R, q, f)
  • Coordinate transformations not covered
  • Tangential and normal system not used due to
    complexity involved.

33
Space curvilinear motion
  • Rectangular coordinates (x, y, z) similar to 2D

34
Space curvilinear motion
  • Cylindrical coordinates (r, q, z)

35
Space curvilinear motion
  • Spherical coordinates (R, q, f)

36
Example
  • A section of a roller-coaster is a horizontal
    cylindrical helix. The velocity of the cars as
    they pass point A is 15 m/s. The effective radius
    of the cylindrical helix is 5 m and the helix
    angle is 40. The tangential acceleration at A is
    gcosg. Compute the magnitude of the acceleration
    of the passengers as they pass A. (Answer a
    27.5 m/s2). (Problem 2/171, MK)

37
Example
  • The robot shown rotates about a fixed vertical
    axis while its arm extends and elevates. At a
    given instant, f 30, df/dt 10 deg/s
    constant, l 0.5 m, dl/dt 0.2 m/s, d2l/dt2
    -0.3 m/s2, and W 20 deg/s constant. Determine
    the magnitudes of the velocity and acceleration
    of the gripped part P. (Answer v 0.480 m/s, a
    0.474 m/s2). (Problem 2/177, MK)

38
Particle kinetics
  • Newtons laws
  • Applied and reactive forces must be considered
    free body diagrams
  • Forces required to produce motion
  • Motion due to forces

39
Particle kinetics
  • Constrained and unconstrained motion
  • Degrees of freedom
  • Rectilinear motion covered
  • Curvilinear motion

40
Rectilinear motion - example
  • The 10 Mg truck hauls a 20 Mg trailer. If the
    unit starts from rest on a level road with a
    tractive force of 20 kN between the driving
    wheels and the road, compute the tension T in the
    horizontal drawbar and the acceleration a of the
    rig. (Answer T 13.33 kN, a 0.667 m/s2).
    (Problem 3/5, MK)

41
Example
  • The motorized drum turns at a constant speed
    causing the vertical cable to have a constant
    downwards velocity v. Determine the tension in
    the cable in terms of y. Neglect the diameter and
    mass of the small pulleys. (Problem 3/48, MK)
  • Answer

42
Curvilinear motion
  • Rectangular coordinates
  • Normal and tangential coordinates
  • Polar coordinates

43
Example
  • A pilot flies an airplane at a constant speed of
    600 km/h in a vertical circle of radius 1000 m.
    Calculate the force exerted by the seat on the 90
    kg pilot at point A and at point A. (Answer RA
    3380 N, RB 1617 N). (Problem 3/63, MK)

44
Example
  • The 30 Mg aircraft is climbing at an angle of 15
    under a jet thrust T of 180 kN. At the instant
    shown, its speed is 300 km/h and is increasing at
    a rate of 1.96 m/s2. Also q is decreasing as the
    aircraft begins to level off. If the radius of
    curvature at this instant is 20 km, compute the
    lift L and the drag D. (Lift and drag are the
    aerodynamic forces normal to and opposite to the
    flight direction, respectively). (Answer D
    45.0 kN, L 274 kN). (Problem 3/69, MK)

45
Example
  • A child's slide has a quarter circle shape as
    shown. Assuming that friction is negligible,
    determine the velocity of the child at the end of
    the slide (q 90) in terms of the radius of
    curvature r and the initial angle q0.
  • Answer

46
Slide
  • Does it matter what profile slide has?
  • What if friction added?

47
Example
  • A flat circular discs rotates about a vertical
    axis through the centre point at a slowly
    increasing angular velocity w. With w 0, the
    position of the two 0.5 kg sliders is x 25 mm.
    Each spring has a stiffness of 400 N/m. Determine
    the value of x for w 240 rev/min and the normal
    force exerted by the side of the slot on the
    block. Neglect any friction and the mass of the
    springs. (Answer x 118.8 mm, N 25.3 N).
    (Problem 3/83, MK)

48
Work and energy
  • Work/energy analysis dont need to calculate
    accelerations
  • Work done by force F
  • Integration of F ma w.r.t. displacement gives
    equations for work and energy

49
Work and energy
  • Active forces and reactive forces (constraint
    forces that do no work)
  • Total work done by force
  • where Ft tangential force component

50
Work and energy
  • If displacement is in same direction as force
    then work is ve (otherwise ve)
  • Ignore reactive forces
  • Kinetic energy
  • Gravitational potential energy

51
Example
  • A small vehicle enters the top of a circular path
    with a horizontal velocity v0 and gathers speed
    as it moves down the path. Determine the angle b
    (in terms of v0) at which it leaves the path and
    becomes a projectile. Neglect friction and treat
    the vehicle as a particle. (Problem 3/87, MK)
  • Answer

52
Example
  • The small slider of mass m is released from point
    A and slides without friction to point D. From
    point D onwards the coefficient of kinetic
    friction between the slider and the slide is mk.
    Determine the distance s travelled by the slider
    up the incline beyond D. (Problem 3/125, MK)
  • Answer

53
Example
  • A rope of length pr/2 and mass per unit length r
    is released with q 0 in a smooth vertical
    channel and falls through a hole in the
    supporting surface. Determine the velocity v of
    the chain as the last part of it leaves the slot.
    (Problem 3/173, MK)
  • Answer

54
Linear impulse and momentum
  • Integration of F ma w.r.t. time gives equations
    of impulse and momentum.
  • Useful where time over which force acts is very
    short (e.g. impact) or where force acts over
    specified length of time.

55
Linear impulse and momentum
  • If mass m is constant then sum of forces time
    rate of change of linear momentum
  • Linear momentum of particle
  • Units kgm/s or Ns
  • Scalar form

56
Linear impulse and momentum
  • Integrate over time
  • Product of force and time is called linear
    impulse
  • Scalar form

57
Linear impulse and momentum
  • Note that all forces must be included (i.e. both
    active and reactive)

58
Linear impulse and momentum
  • If there are no unbalanced forces acting on a
    system then the total linear momentum of the
    system will remain constant (principle of
    conservation of linear momentum)

59
Impact
  • How to determine velocities after impact?
  • Forces normal to contact surface. Fd is force
    during deformation period while Fr is force
    during recovery period.
  • The ratio of the restoration impulse to the
    deformation impulse is called the coefficient of
    restitution

60
Impact
  • For particle 1, (v0)n being the intermediate
    normal velocity component (of both particles) and
    (v1)'n being normal velocity component after
    collision
  • Similarly for particle 2

61
Impact
  • Combining gives
  • e 0 for plastic impact, e 1 for elastic
    impact
  • Note that tangential velocities are not affected
    by impact

62
Example
  • A 75 g projectile traveling at 600 m/ strikes and
    becomes embedded in the 50 kg block which is
    initially stationary. Compute the energy lost
    during the impact. Express your answer as an
    absolute value and as a percentage of the
    original energy of the system. (Problem 3/180,
    MK)

63
Example
  • The pool ball shown must be hit so as to travel
    into the side pocket as shown. Specify the
    location x of the cushion impact if e 0.8.
    (Answer x 0.268d) (Problem 3/251, MK)

64
Example
  • The vertical motion of the 3 kg load is
    controlled by the forces P applied to the end
    rollers of the framework shown. If the upward
    velocity of the cylinder is increased from 2 m/s
    to 4 m/s in 2 seconds, calculate the average
    force Rav under each of the two rollers during
    the 2 s interval. Neglect the small mass of the
    frame. (Answer Rav 16.22 N) (Problem 3/199,
    MK)

65
Example
  • A 1000 kg spacecraft is traveling in deep space
    with a speed vs 2000 m/s when struck at its
    mass centre by a 10 kg meteor with velocity vm of
    magnitude 5000 m/s. The meteor becomes embedded
    in the satellite. Determine the final velocity of
    the spacecraft. (Answer v 36.9i 1951j
    14.76k m/s) (Problem 3/201, MK)

66
Cross (or vector) product
  • Magnitude of cross-product
  • Direction of cross-product governed by right-hand
    rule

67
Right-hand rule
  • Middle finger in direction of R if thumb in
    direction of P and index finger in direction of
    Q.
  • Use right-handed reference frame for x,y, and z.

68
Cross (or vector) product
  • Distributive

69
Cross (or vector) product
  • Derivative

70
Angular impulse and momentum
  • The angular momentum of a particle about any
    point is the moment of the linear momentum about
    that point.
  • Units are kgm/sm or Nms

71
Angular impulse and momentum
  • Planar motion
  • There are 3 components of the angular momentum of
    P about arbitrary point O i.e. about x-,y-, and
    z-axes.

72
Angular impulse and momentum
  • Since P is coplanar with x- and y-axes, it has no
    moment about these axes. It only has a moment
    about the z-axis.

73
Angular impulse and momentum
  • Is angular momentum of P about O positive or
    negative? governed by right-hand rule

74
Right-hand rule
  • Curl fingers in. Rotation indicated by fingers is
    in direction of thumb. Is this positive or
    negative in this case?

75
Angular impulse and momentum
  • Direction of component about z-axis is in
    z-direction

76
Angular impulse and momentum
77
Angular impulse and momentum
  • Note

78
Angular impulse and momentum
  • The resultant moment of all forces about O is
  • From Newtons 2nd law
  • Differentiate w.r.t. time
  • Now
  • so

79
Angular impulse and momentum
  • The moment of all forces on the particle about a
    fixed point O equals the time rate of change of
    the angular momentum about that point.
  • If moment about O is zero then angular momentum
    is constant (principle of conservation of angular
    momentum).
  • If moment about any axis is zero then component
    of angular momentum about that axis is constant.

80
Angular impulse and momentum
  • Particle following circular path at constant
    angular velocity. Is angular momentum about O
    varying with time?
  • Is angular momentum about O' varying with time?
  • Is component about z-axis varying with time?

81
Angular impulse and momentum
  • i.e. change in angular momentum is equal to total
    angular impulse

82
Angular impulse and momentum
  • Example ice skater

83
Example
  • Calculate HO, the angular momentum of the
    particle shown about O (a) using the vector
    definition and (b) using a geometrical approach.
    The centre of the particle lies in the x-y plane.
    (Answer HO 128.7k Nms) (Problem 3/221, MK)

84
Example
  • A particle of mass m moves with negligible
    friction across a horizontal surface and is
    connected by a light spring fastened at point O.
    The velocity at A is as shown. Determine the
    velocity at B. (Problem 3/226, MK)

85
Example
  • Each of 4 spheres of mass m is treated as a
    particle. Spheres A and B are mounted on a light
    rod and are rotating initially with an angular
    velocity w0 about a vertical axis through O. The
    other two spheres are similarly (but
    independently) mounted and have no initial
    velocity. When assembly AB reaches the position
    indicated it latches with CD and the two move
    with a common angular velocity w. Neglect
    friction. Determine w and n the percentage loss
    of kinetic energy. (Answer w w0/5, n 80).
    (Problem 3/227, MK)

86
Example
  • The particle of mass m is launched from point O
    with a horizontal velocity u at time t 0.
    Determine its angular momentum about O as a
    function of t. (Answer H0 -½mgut2k). (Problem
    3/233, MK)

87
Relative motion
  • Fixed reference frame X-Y
  • Moving reference frame x-y

88
Relative motion
  • Special case inertial system or Newtonian
    frame of reference with zero acceleration
  • Note that work-energy and impulse momentum
    equations are equally valid in inertial system
    but relative momentum/relative energy etc. will,
    in general, be different to those measured
    relative to fixed frame of reference.

89
Example
  • The ball A of mass 10 kg is attached to the light
    rod of length l 0.8 m. The rod is attached to a
    carriage of mass 250 kg which moves on rails with
    an acceleration aO as shown. The rod is free to
    rotate horizontally about O. If dq/dt 3 rad/s
    when q 90, find the kinetic energy T of the
    system if the carriage has a velocity of 0.8 m/s.
    Treat the ball as a particle. (Answer T 112
    J). (Problem 3/311, MK)

90
Example
  • The small slider A moves with negligible friction
    down the tapered block, which moves to the right
    with constant speed v v0. Use the principle of
    work-energy to determine the magnitude vA of the
    absolute velocity of the slider as it passes
    point C if it is released at point B with no
    velocity relative to the block. (Problem 3/316,
    MK)
  • Answer
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