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KINEMATICS OF MECHANISMS

Mechanism 1

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Page 1: Mechanism 1

KINEMATICS OF MECHANISMS

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MECHANISM

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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KINEMATICS

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RELEVANCE OF KINEMATIC STUDY

• Motion requirements

• Design requirements

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MOTION STUDYStudy 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 Design: determination of shape and size1. Requires knowledge of material

2. Requires knowledge of stress

Requires knowledge of load acting

(i) static load

(ii) dynamic/inertia load

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DYNAMIC/INERTIA LOAD

Inertia load require acceleration

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LINK OR ELEMENTAny body (normally rigid) which has motion relative to another

• Binary link• Ternary link• Quaternary link

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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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DEGREES OF FREEDOM (DOF): It is the number of independent coordinates required to

describe the position of a body.

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TYPES OF KINEMATIC PAIRS Based on nature of contact between elements (i) Lower pair : The joint by which two members are

connected has surface contact.

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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]

Eg. Ball and socket joint

(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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LOCKED CHAIN OR STRUCTURE Links connected in such a way that no relative motion is possible.

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MECHANISM

A mechanism is a constrained kinematic chain. Motion of any one link in the kinematic chain will give a definite and predictable motion relative to each of the others. Usually one of the links of the kinematic chain is fixed in a mechanism

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MECHANISMSlider crank and four bar mechanisms

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Working of slider crank mechanism

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Unconstrained kinematic chain

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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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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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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,• F = Degrees of freedom• n = Number of links in the mechanism.• l = Number of lower pairs, which is obtained by counting the

number of joints. If more than two links are joined together at any point, then, one additional lower pair is to be considered for every additional link.

• h = Number of higher pairs

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Examples - DOF

• F = 3(n-1)-2l-h

• Here, n = 4, l = 4 & h = 0.

• F = 3(4-1)-2(4) = 1

• I.e., one input to any one link will result in definite motion of all the links.

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Examples - DOF• F = 3(n-1)-2l-h

• Here, n = 5, l = 5 and h = 0.

• F = 3(5-1)-2(5) = 2

• I.e., two inputs to any two links are required to yield definite motions in all the links.

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Examples - DOF

• F = 3(n-1)-2l-h

• Here, n = 6, l = 7 and h = 0.

• F = 3(6-1)-2(7) = 1

• I.e., one input to any one link will result in definite motion of all the links.

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Examples - DOF

• F = 3(n-1)-2l-h

• Here, n = 6, l = 7 (at the intersection of 2, 3 and 4, two lower pairs are to be considered) and h = 0.

• F = 3(6-1)-2(7) = 1

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Examples - DOF

• F = 3(n-1)-2l-h

• Here, n = 11, l = 15 (two lower pairs at the intersection of 3, 4, 6; 2, 4, 5; 5, 7, 8; 8, 10, 11) and h = 0.

• F = 3(11-1)-2(15) = 0

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Examples - DOF

(a)F = 3(n-1)-2l-hHere, n = 4, l = 5 and h = 0.F = 3(4-1)-2(5) = -1I.e., it is a structure

(b)F = 3(n-1)-2l-hHere, n = 3, l = 2 and h = 1.F = 3(3-1)-2(2)-1 = 1

(c)F = 3(n-1)-2l-hHere, n = 3, l = 2 and h = 1.F = 3(3-1)-2(2)-1 = 1

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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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FOUR BAR CHAIN • (link 1) frame

• (link 2) crank

• (link 3) coupler

• (link 4) rocker

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INVERSIONS OF FOUR BAR CHAIN

1. Crank-rocker mechanism

2. Drag link mechanism

3. Double rocker mechanism

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CRANK-ROCKER MECHANISM

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CRANK-ROCKER MECHANISM

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DRAG LINK MECHANISM

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DOUBLE CRANK MECHANISM

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SLIDER CRANK CHAIN

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lnversions of slider crank chain

(a) crank fixed (b) connecting rod fixed (c) slider fixed

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Rotary engine– I inversion of slider crank mechanism. (crank fixed)

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Whitworth quick return motion mechanism

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Oscillating cylinder engine–II inversion of slider crank mechanism (connecting rod fixed)

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Crank and slotted lever quick return motion mechanism

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Pendulum pump or bull engine–III inversion of slider crank mechanism (slider fixed)

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DOUBLE SLIDER CRANK CHAIN

It is a kinematic chain consisting of two turning pairs and two sliding pairs.

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SCOTCH –YOKE MECHANISM Turning pairs –1&2, 2&3; Sliding pairs – 3&4, 4&1

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Inversions of double slider crank mechanism

1sincos 22

22

p

y

q

x

1sincos 22

22

p

y

q

x

Elliptical trammelAC = p and BC = q, then, x = q.cosθ and y = p.sinθ.Rearranging,

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OLDHAM COUPLING

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Quick return motion mechanismsDrag link mechanism

12

21

ˆ

ˆ

BAB

BAB

urnstrokeTimeforret

wardstrokeTimeforfor

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Whitworth quick return motion mechanism

2

1

2

2

ˆ

ˆ

BoB

BoB

urnstrokeTimeforret

wardstrokeTimeforfor

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Crank and slotted lever quick return motion mechanism

2

1

2

2

ˆ

ˆ

BoB

BoB

urnstrokeTimeforret

wardstrokeTimeforfor

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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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Straight line motion mechanismsCondition for perfect steering Locus of pt.C will be a straight

line, ┴ to AE if,

is constant.

Proof:

ACAB

..,

.

constACifABconstAE

constbutADAD

ACABAE

AE

AB

AC

AD

ABDAEC

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Peaucellier mechanism

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Robert’s mechanism

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Intermittent motion mechanismsGeneva wheel mechanism

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Intermittent motion mechanismsRatchet and pawl mechanism

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Application of Ratchet Pawl mechanism

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Other mechanismsToggle mechanism

Considering the equilibrium condition of slider 6,

For small angles of α, F is much smaller than P.

tan2

2tan

PFP

F

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Pantograph

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Hooke’s joint

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Hooke’s joint

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Hooke’s joint

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Steering gear mechanismCondition for perfect steering

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Ackermann steering gear mechanism

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Ackermann steering gear mechanism

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