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DOM Manual ACT-Cycle-1 n

Mar 01, 2018

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    MECHANICAL DYNAMICS LAB

    1

    Name :

    Register No :

    Sem./Year :

    Class :

    Course Teacher Head Of Department

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    2

    MECHANICAL DYNAMICS LAB

    !ST O" #$%#R!NTS

    #'p.No.

    Title of #'periment Staff Sig.

    ( Determination of natural fre)uenc* of longitudinal+i,ration of the spring mass s*stem.

    -a Determine the characteristics of att go+ernor using

    uni+ersal go+ernor setup.-, Determine the characteristics of porter go+ernor usinguni+ersal go+ernor setup.

    / Torsional +i,ration of to rotor s*stem.

    0 Determination of hirling speed of shafts.

    1 Determination of moment of inertia of inertia of fl*heeland connecting rod.

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    3

    MECHANICAL DYNAMICS LAB

    Determination of natural fre)uenc* of longitudinal +i,ration of thespring mass s*stem

    #'p.No :( Date :

    2im :To determine time period and natural fre)uenc* of longitudinal +i,ration of thespring

    mass s*stem

    2pparatus Re)uired :(3 Helicalspring-3 %latform3 4eights03 &easuring scale13 Stop atch

    Descriptionof the setup:!t consists of an to open coil helical spring of hich one end is fi'ed to the scre rod

    and a platform to the other end. This platform is used to add eights and a loc5 nut is alsopro+ided to clamp the eights added.

    %rocedure:(3 "i' one end of the helical spring to the upper scre rod.-3 2ttach the other end to the platform and add some eight.3 Note don the deflection.03 Stretch the spring through some distance and release.13 O,ser+e the time ta5en for n 6 -7 oscillations.83 Repeat the steps from - to 1 for other 5non eights.

    "ormulae:

    (. Stiffness of the spring9 e'p 6 oad / deflection 6 4 / $ 9 N/m

    -. #'perimental time period of +i,ration9 T e'p 6tm / n 9 sec4here9 tm6 mean time ta5en for n oscillations

    n 6 num,er of oscillations 6 -7

    . #'perimental fre)uenc* of +i,ration9 " e'p 6( / T e'p 9 H;

    0. Theoritical fre)uenc* of +i,ration9 T theo 6 ?e'pm/ 4@ 9 H;

    Or6

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    S.Nooad added9

    4Deflection9

    $ < m 3

    Stiffness9 e'p 6 4

    / $

    < N / m 3

    Time ta5en for n 6 -7oscillations

    < sec 3

    %eriodof

    +i,ration

    < sec 3

    "re)uenc* of

    +i,ration

    < H; 3g N t( t- t t0 t1 tm T e'p " e'p

    (

    -

    6 Theoretical stiffness64/ 9 N/m6theoretical deflection 9m

    804 n/c4here9 R6inner radius of spring9 m

    O,ser+ation:

    < 3initial length of the spring6 9m

    < 3 length of the spring after load added6 9m

    Deflection:

    $6< 3 9 m

    Ta,ulation:

    e'pm

    &odel calculation: Reading No. :

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    Result:Thus the natural fre)uenc* of longitudinal +i,ration of spring mass s*stem is founde'perimentall* and compared ith theoretical fre)uenc*.

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    MECHANICAL DYNAMICS LAB

    6

    Determinethe characteristics of att go+ernor using uni+ersalgo+ernor setup

    #'p. No. : -a Date :

    2im : To stud* the characteristics of att go+ernor and to dra the +arious characteristicscur+es.2pparatus Re)uired:

    (. ni+ersal go+ernor-. Tachometer. Spanner

    Descriptionof the setup:The dri+e unit consists of a DC electric motor connected through ,elt and pulle*

    arrangement. &otor and test setup are mounted on a &.S. fa,ricated frame. The go+ernor spindleis dri+en ,* motor through E ,elt and is supported in a ,all ,earing.

    The optional go+ernor mechanisms can ,e mounted on spindle. Speed is controlled ,* theelectronic control unit. 2 tachometer is used to determine the speed. 2 graduated scale is fi'ed tothe slee+e and guided in +ertical direction. Slee+e displacement is to ,e noted on the scalepro+ided.

    The center slee+e of the att go+ernors incorporates no eight. DC motor ith dri+e:F H% motor and +oltage regulator control for speed +ariation. Separate lin5ages for go+ernorarrangements

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    2ngular+elocit* 9 6- N/87 9rad/sec

    O,ser+ation:

    is the initial length of the go+ernor 6 9m

    is the length of the lin5 6 L9m

    &ass of the eight ,all 6 95g

    Ta,ulation:

    Sl.No.

    Mo+ernor

    Speed

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    Result:Thus the characteristics of att go+ernor is studied and graphs are plotted.

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    MECHANICAL DYNAMICS LAB

    9

    Determinethe characteristics ofporter go+ernor using uni+ersalgo+ernor setup

    #'p. No.:-, Date :

    2im : To stud* the characteristics of porter go+ernor and to dra the +ariouscharacteristics cur+es.

    2pparatus Re)uired:(. ni+ersal go+ernor-. Tachometer. Central load0. Spanner

    Descriptionof the setup:

    The dri+e unit consists of a DC electric motor connected through ,elt and pulle*arrangement. &otor and test setup are mounted on a &.S. fa,ricated frame. The go+ernor spindleis dri+en ,* motor through E ,elt and is supported in a ,all ,earing.

    The optional go+ernor mechanisms can ,e mounted on spindle. Speed is controlled ,* theelectronic control unit. 2 tachometer is used to determine the speed. 2 graduated scale is fi'ed tothe slee+e and guided in +ertical direction. Slee+e displacement is to ,e noted on the scalepro+ided.

    The centre slee+e of the %orter and %roell go+ernors incorporates a eight slee+e tohich eights ma* ,e added. DC motor ith dri+e: F H% motor and DC dri+e controlfor speed +ariation. Separate lin5ages for go+ernor arrangements

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    1

    MECHANICAL DYNAMICS LAB

    Ta,ulation:

    Sl.No.

    Mo+ernorSpeed

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    1

    MECHANICAL DYNAMICS LAB

    Torsional +i,ration of to rotor s*stem#'p.No : Date :

    2im :To determine the time period and fre)uenc* of torsional +i,ration of the to rotor s*stem

    e'perimentall* and compare it ith the theoretical +alues.

    2pparatus Re)uired :i. #'perimental Shaft9 Spanner

    ii. Chuc5 5e*iii. &easuring tapei+. Stop atch+. 4eights and

    +i. Crossarms

    Descriptionof the setup:

    To discs ha+ing different mass moment of inertia are clamped one at each endof shaft ,* means of collet. &ass moment of inertia of an* disc can ,e changed ,* attaching thecross le+er ith eights. Goth discs are free to oscillate in the ,all ,earings. This pro+idesnegligi,le damping during e'periment.

    %rocedure:i3 "i' the discs 2 and G to the shaft and fit the shaft in ,earing.ii3 Deflect the discs 2 and G in opposite directions ,* hand and release.iii3 Note don the time re)uired for n 6 oscillations.i+3 "it the cross arm to the disc 2 and attach e)ual masses to the ends of cross arm and again

    note don time.

    +3 Repeat the a,o+e procedure ith different e)ual masses attached to the ends of cross arm."ormulae:

    ( .#'perimental %eriod of Ei,ration Te'p6 /n sec.

    here96mass time ta5en for n oscillations

    n6num,er of oscillations

    -. Theoretical %eriod of Ei,ration Ttheo 6 - = >!2 ' /M Q

    here9mass moment of inertia 6 &2

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    S.No. &ass

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    &odel calculation: Reading No. :

    Result:Thus the undamped fre)uenc* of torsional +i,ration ofto rotor s*stem is founde'perimentall* and compared ith theoretical fre)uenc*.

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    MECHANICAL DYNAMICS LAB

    1

    Determination of hirling speed of shafts

    #'p.No :0 Date :

    2im:

    To determine the hirling speed for +arious diameter shafts e'perimentall* and compareit ith the theoretical +alues.

    2pparatus Re)uired:(3Shaft nos. -3Digital tachometer3Chuc5 5e* 032C +oltage regulator

    Descriptionof the setup:The apparatus is used to stud* the hirling phenomenon of shafts. This consists of a

    frame in hich the dri+ing motor and fi'ing ,loc5s are fi'ed. 2 special design is pro+ided toclear out the effects of ,earings of motor spindle from those of testing shafts.

    %rocedure:(3 The shaft is to ,e mounted ith the end condition as simpl* supported.-3 The speed of rotation of the shaft is graduall* increased.3 4hen the shaft +i,rates +iolent in fundamental mode < (st mode 39 the speed is noted don.03 The a,o+e procedure is repeated for the remaining shafts.

    "ormulae:(. mass9 m 6 ' + 9 5g

    p 6 Densit* of material 6 B7779 5g/m

    +6 Eolume 6 =/0 ' d- ' l 9 m

    -.Theoretical fre)uenc* of trans+erse +i,ration

    "6 C

    4here# 6 Youngs modulus!6 second moment of area of shaft46 eight per unit length of shaftg 6acceleration due to gra+it*C6 constant dependent upon the end conditions.6.18

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    Sl.No

    Diameter ofthe shaft d

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    &odelcalculation : ReadingNo:

    Result:Thus the hirling speeds of different si;ed shafts found e'perimentall* and comparedith theoretical +alues.

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    MECHANICAL DYNAMICS LAB

    1

    Determination of moment of inertia of inertia of fl*heel andconnecting rod

    #'p.No :1 Date :

    2im:

    To find the mass moment of inertia of the Connecting rod ,* using oscillation method.

    2pparatus Re)uired:

    Gigger Connecting Rod Smaller Connecting Rod Stop atch

    %rocedure: &easure the center distance of the connecting rod and also measure the inner

    diameter of ,oth ends. &easure the eight of the connecting rod 2ttach the smaller ends of the connecting rod to shaft Mi+e the oscillation to connecting rod &easure the time ta5en for oscillation to calculate the time period. Remo+e the connecting rod from the shaft and again attach the ,igger rod to shaft 2gain measure the time ta5en for oscillation and calculate the time period

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    1

    MECHANICAL DYNAMICS LAB

    O,ser+ation:&ass of connecting rod

    arger6 5gSmaller6 g

    Center distance ,eteen holesGigger end6 mSmaller end6 m

    Ta,ulation:

    S.No.T*pes of

    connectingrod

    %ositionNo of

    Oscillation

    Time ta5en forn61oscillation

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    1

    MECHANICAL DYNAMICS LAB

    Result: Thus the mass moment of inertia of the gi+en to connecting rod as found ,*oscillation method.