first year em ppt.pdf

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W2 T

Transcript of first year em ppt.pdf

  • W2

    T

  • Question 1Question-1

    W1

    W2Yaxis

    W1

    XaxisX axis

  • SolutionSolutionFree body diagrams of W1 and W2 arFreebodydiagramsofW1andW2ar

    T T

    W1Freebodydiagramforblock1

    re as following:reasfollowing:

    W2b d d f bl kFreebodydiagramforblock2

  • Equilibrium equationsEquilibrium equationss for block 1s for block 1

  • Equilibrium equationsEquilibrium equationss for block 2s for block 2

  • Question 2Question 2

  • Solutions:Solutions:-eebodydiagramsofW1andW2areasfollowing:

    Freebodydiagramforblock1y g

    Freebodydiagramforblock2

  • Equilibrium equationsEquilibrium equationss for block 1s for block 1

  • Equilibrium equationsEquilibrium equationss for block 2s for block 2

  • Question 3Question 3

    T bl k f i ht W1 100TwoblocksareofweightW1=100andsupportsonitstopanotherblweightW2isattachedbyaninclineg yFindthemagnitudeofthehorizontblocktocauseslippingtoimpend.contact surface is 0 3contactsurfaceis0.3

    3

    4

    3

    00N t h i t l f00NrestsonahorizontalsurfaceockofweightW2=250N.TheedstringABtotheverticalwall.gtalforcePappliedtothelowerThecoefficientoffrictionforall

    P

  • SolutionSolutionFreebodydiagramsofW1andW2ar

    T

    Freebodydiagramforblock2

    reasfollowing:

    P

    Freebodydiagramforblock1

  • Equilibrium equationsEquilibrium equationss for block 2s for block 2

    T

  • Equilibrium equationsEquilibrium equationss for block 1s for block 1

    P

    Free body diagram for block 1Freebodydiagramforblock1

  • Question 10Question-10

    Wh t i th l f P i th tWhatisthevalueofPinthesystemimpend?Assumetheepulleyissmbetweentheothercontactsurface

    h t th ti tmshowntocausethemotiontomoothandcoefficientoffrictionesis0.2

    P

    500N

    P

  • IntroductionIntroduction Basic terms:Basicterms:

    Motion :Abodyissaidtobeinmotionifitischangingitspo

    DistanceandDisplacement :Distanceisthetotallengthofpathcoveredbythecalar quantitycalarquantity.Displacementisthelineardistancebetweenthepthasmagnitudeanddirectionthusitisvectorqua

    peedandVelocity:peedisdefinedastherateofchangeofdistanceV l it i d fi d th t f h f di lVelocityisdefinedastherateofchangeofdisplace

    to Dynamicsto Dynamics

    ositionwithrespecttoareferencepoint.

    bodytoreachfrompointAtopointB.Itisa

    ointAandpointB.antity.

    withtime.Speedisscalarquantity.t ith ti V l it i t titementwithtime.Velocityisvectorquantity.

  • Types of motionTypes of motionTranslation: Amotionissaidtobetranslationifa

    ll l i i i l i i iaralleltoitsoriginalpositionatanytime.

    Rectilinearmotion: Duringtranslationifthepathalled rectilinear motionalledrectilinearmotion

    Curvilinearmotion: Duringtranslationifthepathalledcurvilinearmotion.

    Rotation: Amotionissaidtobeinrotationalmotioncentriccircles.

    Motioncanbeacombinationoftranslationandroorexamplemotionofawheelofacarisbothrota

    astraightdrawnonthemovingbodyremains

    tracedbyanypointinthebodyisstraight,itis

    htracedbyanypointinthebodyiscurve,itis

    ionifalltheparticleoftherigidbodymovein

    otation.ationalandtranslational

  • Motion of body with uniforMotion of body with uniforrm(constant) accelerationrm(constant) acceleration

  • Question bank (10 mQuestion bank (10 mark)ark)

  • D Alemberts principlD Alembert s principlee

  • Work Energy methodWork Energy methoddd

  • Work Energy EquatioWork- Energy Equatioon for translationon for translation