1 Introduction to theory of machines

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    Theory of Machines & Mechanisms

    MCT 2212

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    Introduction

    Rigid BodyMechanics

    Statics

    Body at rest

    Body withconstantvelocity

    DynamicsBody with

    acceleratedmotion

    under the

    action offorces andmoments

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    Theory of Machines andMechanisms

    Mechanisms/

    Linkages

    Parts/ Link

    Jointsdeals with the determinationof the forces and motions of

    links in machines

    Susystems ofmachines to facilitate

    analysis

    Introduction

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    Links! rigid memer ha"ing nodes# i$e$ attachment %oints inary link! 2 nodes

    Ternary link! ' nodes

    (uaternary link! ) nodes

    Links & joints

    Joint! connection etween two links *at their nodes+ which allows

    motionClassified y ty%e of contact# numer of ,-.# ty%e of %hysical

    closure# or numer of links oined$

    kinematic pair! Joints are also known as kinematic %air

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    Joint Classification

    Type of contact!

    line/%oint i$e$ higher %air#

    area/surface i$e$ lower %air

    Number of DOF!

    full oint01,-.#

    half oint02,-.

    Form closed *closed y geometry+ orForce closed *needs an eternal force to

    kee% it closed+

    Joint order = number of links-1

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    Full Joint! %ermits one relati"e motion etween adacent links$ ll of these

    kinematic %airs are referred to as one degree of freedom*,-.+ %airs$

    Turning pairs allow relati"e turning motion etween two

    links$# e$g$ earings# %i"ots# or %in oints$

    olling pairs allow relati"e rolling motion etween two links#

    e$g$ %air of friction wheels .or a rolling %air# it is assumed that

    there is no sli%%age etween the links$

    !liding pairsallow relati"e sliding motion etween two links#

    e$g Piston3Cylinder$

    "alf Joint! allows two relati"e motions simultaneously

    etween the adacent links and referred to as two degree of

    freedom %airs$

    !liding pairs

    Turning pairs

    "alf Joint

    #inematic $airs

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    Types of joints

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    "ig%er $airs

    & Loer $airs

    Loer pairs' kinematic

    %air or oint with

    surface/area contact$

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    "ig%er $airs & Loer $airs

    "ig%er pairs' kinematic %air or oint with %oint contact or line contact$

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    Mechanism

    (obility or DOF of a mec%anism! The moility of a mechanism is defined as

    the numer of inde%endent %arameters re4uired to s%ecify the %osition of all

    links of the mechanism$ 5t also s%ecify the numer of in%ut/actuators needed to

    o%erate the mechanism$

    kinematic c%ain ' kinematic chain is an assemly of links formed y

    %lacing kinematic %airs at each of the nodes without s%ecifying the ground

    link$

    6inematic chains may e either open type or close type$

    (ec%anism! 5t is an assemlage of links and oints with at least one link grounded and

    interconnected in a way to %ro"ide controlled out%ut motions in res%onse to su%%lied

    in%ut motions$

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    Link classification!

    7round! fied wrt$ reference frame

    Crank! %i"oted to ground# makes com%lete re"olutions

    8ocker! %i"oted to ground# has oscillatory motion

    Cou%ler! link has com%le motion# not attached to ground

    (ac%ine! mechanism designed to do work$

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    A simple machine may also be considered as a singlemechanism.

    .igure 1$'*+ shows a free ody diagram of

    the system used to analy9e the manual force

    re4uired to generate sufficient gri%%ing force$

    .igure 1$'*a+ The tongs

    can e considered either

    as a machine or as amechanism$

    igure! "nline 4#$ylinder %ngineigure! "$ %ngine Demonstration

    (ac%ine & (ec%anism

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    igure! A &aper' $ard &unching Machineigure! (uic) return mechanism

    (ac%ine & (ec%anism

    igure! Slider cran) mechanism

    igure! Scotch *o)e mechanism

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    Mechanisms are widely used in a%%lications where %recise relati"e

    mo"ement and transmission of force are re4uired$ Motions may e

    continuous or intermittent# linear and/or angular$

    (ec%anisms

    :orm;gear 7ear3gear 7ear3rack

    )*amples of continuous motion output

    )*amples of intermittent motion output

    Cam

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    >"ery mechanism has one stationary ase link$ ll other links may mo"e

    relati"e to the fied ase link$ .rom the same kinematic chain# an in"ersion os

    a mechanism is otained y making the originally fied link into a mo"ing

    link and selecting an originally mo"ing link to e the fied link $

    (ec%anism In+ersion

    .igure 1$'? Slider crank mechanism and its three in"ersions

    *a+ slider crank mechanism *link 1 fied+#

    *+ in"ersion @1

    *link 2 fied+#

    *c+ in"ersion @2

    *link ' fied+#

    *d+ in"ersion @'

    *link ) fied+$

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    Planar motion is restricted to a %lane$ .or a %lanar mechanism# the motions of

    all of its links must take %lace either in the same %lane or in %lanes that are

    %arallel to one another$ The slider crank mechanism and four3ar mechanism

    are eam%les of %lanar mechanisms$

    $lanar (ec%anism

    Figure 1.5 Slider cran) mechanismFigure 1.7 Slider cran) mechanism with o+set

    Figure 1.8 our#bar mechanism

    The 7ruelerAs e4uation for the moility#

    m, of a %lanar mechanism is gi"en as

    n0 numer of links in the mechanism

    J10umer of one degree of freedom %airs

    J20umer of two degree of freedom %airs

    212+1*' JJnm =

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    If, m< 0 i.e. ve, Preloaded Structure, may require force to

    assemle ! Indeterminate "rolem .If, m# 0 , Structure.

    If, m$0 i.e. %ve, &ec'anism.

    (obility

    e ve re oa e tructure may requ re orce to

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    ,-Figure 1.36 %amples of mobility.

    e. ve , re oa e tructure, may requ re orce to

    tructure.

    . %ve, &ec'anism.

    (obility

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    ,/

    Figure 1.36 (Continued)

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    n=5; J1=6; J2=0;m=0

    n=5; J1=6; J2=0;m=0 but, m=1.

    .ull Joint#

    Pure rolling#

    no sliding

    In case of pure rolling,

    n=3; J1=3; J2=0;m=0

    In case of rolling sli!ing,

    n=3; J1=2; J2=1;

    m=1

    Balf Joint#

    rolling &

    sliding

    ,

    --

    -

    ./

    0

    - - -

    . /

    0

    ,

    .

    ,

    - -

    (obility $arado*es

    The 7rueler criterion %ays no attention to

    link si9es or sha%es# it can gi"e misleading

    results in the face of uni4ue geometric

    configurations$

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    Idle Degrees of Freedom

    n 5dle degree of freedom is one that a%%ears *and is+ %resent ut its "alue has

    no effect on the in%ut < out%ut relationshi%s of interest

    To identify 5dle degrees of freedom# first identify the in%ut and out%ut links

    Then we must determine if a single link or cominations of links can mo"e

    without affecting the in%ut/out%ut link %ositions

    Like a connecting link rotating *aout its ais+ in a steering mechanism

    without changing the relationshi% etween the steering wheel and the front

    tires in a "ehicle

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    ,0'1',4 M% 2320 &age 33

    ote! &in#in#slot $am $ontact arehalf 6ointsBere#

    The Structure has fi"e ,-. with two 5dle ,-.As$

    They are the roller and the cam rocker $

    mActual7 M8heoretical # m"dle

    75#3 7 2

    Idle Degrees of Freedom

    C

    21'2+112*'

    2+1*'

    2

    1'

    12

    21

    2

    1

    =

    =

    =

    =

    =

    =

    JJnm

    J

    J

    n

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    .igure 1$2? *a+ a %rosthetic hand .igure 1$2?*+ .ingers wra%

    around an oect as shown in

    5n a s%atial mechanism# links mo"e in three dimensions$ .or

    eam%le# in a %rosthetic hand# the thum mo"es in a %lane that is

    not %arallel to the %lanes of motion of the other four fingers$

    where the suscri%t refers to the numer of freedoms of the oint$

    spatial mec%anism

    The 6ut9ach moility e4uation for s%atial linkages!

    C)'21 2')C+1*D JJJJJn" =

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    )*ample of !patial Linkage

    ) LinksE 2 s%herical Joints# 1cylindrical oint and 1 re"olute oint$

    ,-. of a S%herical Joint is '

    ,-. of a Cylindrical Joint is 2

    ,-. of a 8e"olute Joint is 1

    '

    2'1)1C+1)*D

    2')C+1*DC)'21

    =

    =

    = JJJJJn"

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    Four12ar (ec%anism13ras%of4s Criterion

    .our3ar mechanisms may e studied y distinguishing the link lengths as

    follows!

    s! the length of the shortest link

    l! the length of the longest link

    ", q! the lengths of the other two links

    To assemle the kinematic chain it is necessary that#

    The ty%e of a four3ar mechanism may e determined using 7rashofFs

    Criterion#

    *i+ *ii+ *iii+

    8hen9 only case :i; o+ers all three types of a four#barmechanisms.

    l#ps ++

    #pls ++ #pls +=+

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    Class_I Class_II Class_III

    *i+ 5f s is the in%ut link# then

    the mechanism is a crank

    rocker$

    *ii+ 5f s is the ase link# then

    the mechanism is a drag link$

    *iii+ 5f otherwise# then the

    mechanism is a rocker3rocker$

    8ocker;8ocker Change Point

    Four12ar (ec%anism13ras%of4s Criterion

    #pls ++ #pls +=+

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    ure 1.43 8ypes of four#bar mechanisms :a; cran) roc)er9 :b; drag lin)9 :c; roc)er#roc)er.

    For !5L6$57

    Crank1rockerif either link adacent to shortest is grounded

    Double crank if shortest link is groundedDouble rocker if link o%%osite to shortest is grounded

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    For !5L8$57

    ll in"ersions will e doule rockers

    Go link can fully rotate

    .igure! .our ar doule rockersFor !5L9$57 :!pecial case 3ras%of;

    ll in"ersions will e doule cranks or crank rockers

    Linkage can form %arallelogram or anti%arallelogram

    -ften used to kee% cou%ler %arallel *drafting machine+

    3-

    Parallelogram form nti %arallelogram form ,eltoid form

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    .igure 1$)H .our3ar mechanisms!crank rocker

    Let the lengths of the three mo"ing links are r20 2$I cmE r'0)$I

    cmE r)0$I cm, adusting the length of the ase link we can get the

    following in"ersion of four ar mechanism$

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