Title: MM203 Mechanics of Machines: Part 1
1MM203Mechanics of Machines Part 1
2Module
- Lectures
- Tutorials
- Labs
- Why study dynamics?
- Problem solving
3Vectors
4Unit vectors - components
5Direction cosines
- l, m, and n direction cosines between v and x-,
y-, and z-axes
- Calculate 3 direction cosines for
6Dot (or scalar) product
- Component of Q in P direction
7Angle between vectors
8Dot product
- Commutative and distributive
9Particle kinematics
- What is kinematics?
- What is a particle?
- Rectilinear motion - review
- Plane curvilinear motion - review
- Relative motion
- Space curvilinear motion
10Rectilinear motion
- Combining gives
- What do dv and ds represent?
11Example
- 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)
12Vector calculus
- Vectors can vary both in length and in direction
13Plane curvilinear motion
- Choice of coordinate system (axes)
- Depends on problem how information is given
and/or what simplifies solution - Practice
14Plane curvilinear motion
- Rectangular coordinates
- Position vector - r
- e.g. projectile motion
- ENSURE CONSISTENCY IN DIRECTIONS
15Plane 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.
16Plane curvilinear motion
17Example
- 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)
18Example
- 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)
19Example
- 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)
20Plane curvilinear motion
21Plane curvilinear motion
22Example
- 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)
23Example
- 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)
24Relative 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.
25Relative 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
26Relative motion
- Absolute positions of points A and B (w.r.t.
fixed axes X-Y) are related by
27Relative motion
- Differentiating w.r.t. time gives
- Coordinate systems may be rectangular, tangential
and normal, polar, etc.
28Inertial 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).
29Example
- 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)
30Example
- 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)
31Example
- 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)
32Space 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.
33Space curvilinear motion
- Rectangular coordinates (x, y, z) similar to 2D
34Space curvilinear motion
- Cylindrical coordinates (r, q, z)
35Space curvilinear motion
- Spherical coordinates (R, q, f)
36Example
- 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)
37Example
- 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)
38Particle kinetics
- Newtons laws
- Applied and reactive forces must be considered
free body diagrams - Forces required to produce motion
- Motion due to forces
39Particle kinetics
- Constrained and unconstrained motion
- Degrees of freedom
- Rectilinear motion covered
- Curvilinear motion
40Rectilinear 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)
41Example
- 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)
42Curvilinear motion
- Rectangular coordinates
- Normal and tangential coordinates
- Polar coordinates
43Example
- 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)
44Example
- 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)
45Example
- 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
46Slide
- Does it matter what profile slide has?
- What if friction added?
47Example
- 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)
48Work 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
49Work and energy
- Active forces and reactive forces (constraint
forces that do no work) - Total work done by force
- where Ft tangential force component
50Work and energy
- If displacement is in same direction as force
then work is ve (otherwise ve) - Ignore reactive forces
- Kinetic energy
- Gravitational potential energy
51Example
- 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
52Example
- 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
53Example
- 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
54Linear 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.
55Linear 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
56Linear impulse and momentum
- Integrate over time
- Product of force and time is called linear
impulse - Scalar form
57Linear impulse and momentum
- Note that all forces must be included (i.e. both
active and reactive)
58Linear 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)
59Impact
- 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
60Impact
- 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
61Impact
- Combining gives
- e 0 for plastic impact, e 1 for elastic
impact - Note that tangential velocities are not affected
by impact
62Example
- 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)
63Example
- 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)
64Example
- 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)
65Example
- 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)
66Cross (or vector) product
- Magnitude of cross-product
- Direction of cross-product governed by right-hand
rule
67Right-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.
68Cross (or vector) product
69Cross (or vector) product
70Angular 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
71Angular 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.
72Angular 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.
73Angular impulse and momentum
- Is angular momentum of P about O positive or
negative? governed by right-hand rule
74Right-hand rule
- Curl fingers in. Rotation indicated by fingers is
in direction of thumb. Is this positive or
negative in this case?
75Angular impulse and momentum
- Direction of component about z-axis is in
z-direction
76Angular impulse and momentum
77Angular impulse and momentum
78Angular impulse and momentum
- The resultant moment of all forces about O is
- From Newtons 2nd law
- Differentiate w.r.t. time
- Now
- so
79Angular 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.
80Angular 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?
81Angular impulse and momentum
- i.e. change in angular momentum is equal to total
angular impulse
82Angular impulse and momentum
83Example
- 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)
84Example
- 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)
85Example
- 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)
86Example
- 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)
87Relative motion
- Fixed reference frame X-Y
- Moving reference frame x-y
88Relative 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.
89Example
- 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)
90Example
- 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