THEORY OF MACHINE
DIPLOMA IN MECHANICAL ENGINEERING
3rd SEMESTER
Dr. Durjyodhan Sethi
PROFESSOR
GANDHI INSTITUTE FOR EDUCATION AND TECHNOLOGY, BANIATANGI, BHUBANESWAR
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KINEMATICS OF MECHINERY
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KINEMATICS OF MECHINERY
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Unit – I-Basics of Mechanism
1.Terminologies
Machine
Mechanism
Kinematic Pair
Links
Kinematic Chain
2.DOF
Kutzhback Equation
Grubler Equation
3.Grashoff Law
4.Mechanism
Four Bar
Single-Slider Crank
Double-Slider
5.Inversion of Mechanism
6.Mechanical Advantage
7.Transmission Angle
8.Design of Mechanism
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MECHANISM
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Mechanism – Part of a machine, which transmit motion and power from input point to output point
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Example for Mechanism
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Example for Mechanism
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PLANAR MECHANISMS
When all the links of a mechanism have plane motion, it is called as a planar mechanism. All the links in a planar mechanism move in planes parallel to the reference plane.
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MACHINE
A machine is a mechanism or collection of mechanisms, which transmit force from the source of power to the resistance to be overcome.
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Though all machines are mechanisms, all mechanisms are not machines
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KINEMATICS
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RELEVANCE OF KINEMATIC STUDY
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MOTION STUDY
Study of position, displacement, velocity and acceleration of different elements of mechanism
Given input Desired output
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Motion requirement
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DESIGN REQUIREMENTS
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Design: determination of shape and size
Requires knowledge of load acting
(i) static load
(ii) dynamic/inertia load
DYNAMIC/INERTIA LOAD
Inertia load require acceleration
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LINK OR ELEMENT
Any body (normally rigid) which has motion relative to another
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Examples of rigid links
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PAIRING ELEMENTS
Pairing elements: the geometrical forms by which two members of a mechanism are joined together, so that the relative motion between these two is consistent. Such a pair of links is called Kinematic Pair.
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PAIRING ELEMENTS
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PAIRING ELEMENTS
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KINEMATIC PAIRS
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TYPES OF KINEMATIC PAIRS
Based on nature of contact between elements
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Flat(or)PlanarPair
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(ii) Higher pair: The contact between the pairing elements takes place at a point or along a line.
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Based on relative motion between pairing elements
(a) Siding pair [DOF = 1]
(b) Turning pair (revolute pair)
[DOF = 1]
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Based on relative motion between pairing elements
(c) Cylindrical pair [DOF = 2]
(d) Rolling pair
[DOF = 1]
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Based on relative motion between pairing elements
(e) Spherical pair [DOF = 3]
(f) Helical pair or screw pair [DOF = 1]
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Based on the nature of mechanical constraint
(a) Closed pair
(b) Unclosed or force closed pair
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CONSTRAINED MOTION
one element has got only one definite motion relative to the other
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(a) Completely constrained motion
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(b) Successfully constrained motion
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(c) Incompletely constrained motion
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KINEMATIC CHAIN
Group of links either joined together or arranged in a manner that permits them to move relative to one another.
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Kinematic Chain
Relation between Links, Pairs and Joints
L=2P-4
J=(3/2) L – 2
L => No of Links
P => No of Pairs
J => No of Joints
L.H.S > R.H.S => Locked chain
L.H.S = R.H.S => Constrained Kinematic Chain
L.H.S < R.H.S => Unconstrained Kinematic Chain
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LOCKED CHAIN (Or) STRUCTURE
Links connected in such a way that no relative motion is possible.
L=3, J=3, P=3 L.H.S>R.H.S
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Kinematic Chain Mechanism
Slider crank and four bar mechanisms
L=4, J=4, P=4
L.H.S=R.H.S
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Working of slider crank mechanism
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Unconstrained kinematic chain��L=5,P=5,J=5 �� L.H.S < R.H.S
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DEGREES OF FREEDOM (DOF):
It is the number of independent coordinates required to describe the position of a body.
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Degrees of freedom/mobility of a mechanism
It is the number of inputs (number of independent coordinates) required to describe the configuration or position of all the links of the mechanism, with respect to the fixed link at any given instant.
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GRUBLER’S CRITERION
Number of degrees of freedom of a mechanism is given by
F = 3(n-1)-2l-h. Where,
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Examples - DOF
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Examples - DOF
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Examples - DOF
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Examples - DOF
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Examples - DOF
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Examples - DOF
(a) F = 3(n-1)-2l-h Here, n = 4, l = 5 and h = 0. F = 3(4-1)-2(5) = -1 I.e., it is a structure | (b) F = 3(n-1)-2l-h Here, n = 3, l = 2 and h = 1. F = 3(3-1)-2(2)-1 = 1 | (c) F = 3(n-1)-2l-h Here, n = 3, l = 2 and h = 1. F = 3(3-1)-2(2)-1 = 1 |
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Determining DOF and Pairs
P=N+L-1
M=N-(2L+1)
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Determining DOF and Pairs
P=N+L-1
M=N-(2L+1)
Nb = 4,Nt=2, N0=0
N=6, L=2
Sol:
P=6+2-1=7
M=6-(2x2 +1)=1
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Determining DOF and Pairs
P=N+L-1
M=N-(2L+1)
Nb = 5,Nt=1, N0=0
N=6, L=2
Sol:
P=6+2-1=7
M=6-(2x2 +1)=1
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Determining DOF and Pairs
P=N+L-1
M=N-(2L+1)
Nb = 9,Nt=0, N0 =2
N=11, L=5
Sol:
P=11+5-1=15
M=11-(2x5 +1)=0
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Grashoff Law
s+l < p+q
(e.x) (1+2) < (3+4)
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INVERSIONS OF MECHANISM
A mechanism is one in which one of the links of a kinematic chain is fixed. Different mechanisms can be obtained by fixing different links of the same kinematic chain. These are called as inversions of the mechanism.
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INVERSIONS OF MECHANISM
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1. FOUR BAR CHAIN
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INVERSIONS OF FOUR BAR CHAIN
Fix link 1& 3. Crank-rocker
or Crank-Lever
mechanism
Fix link 2. Drag link
or Double Crank
mechanism
Fix link 4. Double rocker
mechanism
Pantograph
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APPLICATION�link-1 fixed-� CRANK-ROCKER MECHANISM OSCILLATORY MOTION
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CRANK-ROCKER MECHANISM
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Link 2 Fixed- DRAG LINK MECHANISM
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Locomotive Wheel - DOUBLE CRANK MECHANISM
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��2.SLIDER CRANK CHAIN�Link1=Ground�Link2=Crank�Link3=ConnectingRod �Link4=Slider� �
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lnversions of slider crank chain
Link 2 fixed Link 3 fixed Link 4 fixed
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Application�Inversion II – Link 2 Crank fixed �Whitworth quick return motion mechanism
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Quick return motion mechanisms
Drag link mechanism
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Rotary engine– II inversion of slider crank mechanism. (crank fixed)
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Application�Inversion III -Link 3 Connecting rod fixed �Crank and slotted lever quick return mechanism
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Crank and slotted lever quick return motion mechanism
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Crank and slotted lever quick return motion mechanism
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Application of Crank and slotted lever quick return motion mechanism
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Oscillating cylinder engine–III inversion of slider crank mechanism (connecting rod fixed)
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Application�Inversion IV – Link 4 Slider fixed �Pendulum pump or bull engine
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3. DOUBLE SLIDER CRANK CHAIN
It is a kinematic chain consisting of two turning pairs and two sliding pairs.
Link 1 Frame
Link 2 Slider -I
Link 3 Coupler
Link 4 Slider - II
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Inversion I – Frame Fixed�Double slider crank mechanism
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Elliptical trammel
AC = p and BC = q, then,
x = q.cosθ and y = p.sinθ.
Rearranging,
Inversion II – Slider - I Fixed �SCOTCH –YOKE MECHANISM
Turning pairs –1&2, 2&3; Sliding pairs – 3&4, 4&1
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Inversion III – Coupler Fixed �OLDHAM COUPLING
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Other Mechanisms�1.Straight line motion mechanisms
Condition for perfect steering
Locus of pt.C will be a straight line, ┴ to AE if,
is constant.
Proof:
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1.a) Peaucellier mechanism
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1.b) Robert’s mechanism
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1.c) Pantograph
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2.Indexing Mechanism�
Geneva wheel mechanism
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3.Ratchets and Escapements
Ratchet and pawl mechanism
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Application of Ratchet Pawl mechanism
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4. Toggle mechanism
Considering the equilibrium condition of slider 6,
For small angles of α, F is much smaller than P.
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5.Hooke’s joint
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Hooke’s joint
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6.Steering gear mechanism
Condition for perfect steering
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Ackermann steering gear mechanism
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Mechanical �Advantage
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Transmission �Angle
θ = a1=Crank Angle
γ = a2 =Angle between crank and Coupler
μ = a3 =Transmission angle
Cosine Law
a2 + d2 -2ad cos θ =
b2 + c2 -2 bc cos μ
Where a=AD, b=CD,
c=BC, d=AB
Determine μ.
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Design of �Mechanism
Link Lengths, Stroke Length, Crank Angle specified.
Link Lengths, Stroke Length, Crank Angle, Time Ratio specified.
Link Lengths and Rocker angle Specified.
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ALL THE BEST
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