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LEC 16 (Conservation Energy 042 )

Jun 02, 2018

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  • 8/11/2019 LEC 16 (Conservation Energy 042 )

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    King Fahd University ofPetroleum & Minerals

    Mechanical EngineeringDynamics ME 201

    B

    Dr! Meyassar "! #l$%addadecture ' 1(

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    Chapter 14

    Kinetics of a Particle ; Work & Energy

    Objectives To develop the principle of work and energy and

    apply it solve problems that involve force, velocity,and displacement.

    To study problems that involve power and

    efficiency.

    To introduce the concept of a conservative forceand apply the theorem of conservation of energy

    to solve kinetic problems.

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    Work of a Force

    F

    S

    U = F . S

    F

    U = (F cos ) . S

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    Work of a Weight

    )(21 yWU =

    nt.displacemeverticalits

    timesweightsparticle'theofmagnitude

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    Work of a Spring Force

    )2

    1

    2

    1(

    21

    2221 ksksU =

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    Work and Energy relation

    =+ 2211 TUT

    Initial .! " #ork $one % &inal .!

    )2

    1(])(

    2

    1[)

    2

    1(

    2

    2

    22

    1 mvmv NsyWksFs k =+

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    Power and Efficiency

    'ower is defined as the amount of work performed per unit time.

    (rate of downing work)

    *echanical !fficiency +

    vFr

    FrF

    ==

    ==dt

    d

    dt

    d

    dt

    dUP

    W

    slbfthpsJsmNW

    746

    !!"1

    =

    ===

    inputenerg#outputenerg#

    inputpoweroutputpower)(%fficienc# == 1

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    14. Conser!ati!e Forces and Potential Energy

    1onservative &orce+independent of the path

    !ample weight 2 spring force

    The work done by the frictional and applied force

    /3 depends on the path /3 non/conservative/3 the work is dissipated 4heat5

    'otential !nergy+(capacity for doing work)

    !nergy comes from the motion /3 inetic energy

    !nergy comes from the position/3 'otential energy

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    6ravitational potential !nergy:

    WyVg =

    2

    2

    1

    ksV +=

    !lastic potential energy:

    do!ny

    upy

    +

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    2

    2

    1ksWsVVV g +=+=

    'otential &unction+particle subjective to both gravitational and elastic force

    )(2

    1

    )(

    )2

    1()

    2

    1(

    *+or,

    2

    1

    2

    212

    2

    22

    2

    112121

    2121

    ksksssW

    ksWsksWsVVU

    VVU

    =

    ++==

    =

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    Conser!ation of "echanical Energy

    +=+ 2211 VTVT

    2.21211 -)()( TUVVT non"ons =++

    2211 VTVT +=+2

    2

    1mvT=

    2

    2

    1skyWV +=

    &or a system of 'articles

    =+ 2211 TUT

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    1

    2

    '

    [ ] Whghg

    WWv

    g

    WVT# =

    =+=+=

    22

    22

    1"

    2

    1

    !ample

    WhWhVT# =+=+= "111

    WhWhghg

    W#

    ghh

    gv$y%yavv

    hWv

    g

    WVT#

    C

    =+=

    ==+=

    +=+=

    2

    1

    2

    1

    222

    22

    1

    2

    "

    2

    "

    2

    2

    2222

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    NmgT

    mgT

    maF nn

    14!.14""1!cos

    2"

    !.1&"""1!cos

    2

    2

    =+=

    =

    =

    1!

    "

    6"

    &"""

    2

    21

    1

    =

    =

    ==

    =

    =

    T

    vv

    &stat

    kgm

    o

    o

    !ample -/7

    2211 VTVT +=+

    smv

    g

    gv

    gvg

    !.1

    &.1&246!."4"

    )6"cos1!(cos2"&"""4"""

    1

    1!cos2"&"""&"""2

    1

    6"cos2"&""""

    2

    2

    2

    2

    2

    =

    ==

    =

    =

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    8eview

    !ample -/9

    !ample -/-:

    !ample -/--

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