LEC 11 (Rectangular 051)

download LEC 11 (Rectangular 051)

of 18

Transcript of LEC 11 (Rectangular 051)

  • 8/11/2019 LEC 11 (Rectangular 051)

    1/18

  • 8/11/2019 LEC 11 (Rectangular 051)

    2/18

  • 8/11/2019 LEC 11 (Rectangular 051)

    3/18

  • 8/11/2019 LEC 11 (Rectangular 051)

    4/18

    13.2 The Equation of Motion

    Free-Body diagram(Force Diagram)

    Kinetic diagram

    (acceleration Diagram)

    aF m

  • 8/11/2019 LEC 11 (Rectangular 051)

    5/18

    13.3 Equation of Motion for a System of

    Particles

    iiii m

    m

    afF

    aF

    G

    iii

    m

    m

    aF

    aF

    Internal forces cancel each other

  • 8/11/2019 LEC 11 (Rectangular 051)

    6/18

    13.4 Equations of Motion: Rectangular

    Coordinates When the net force is

    projected to separate

    coordinate axes theNewtons second law

    still holds

    )kji(kji

    aF

    zyxzyx aaamFFF

    m

    zz

    yy

    xx

    maF

    maF

    maF

  • 8/11/2019 LEC 11 (Rectangular 051)

    7/18

    Free Body Diagram Method

    Draw each object separately

    Draw all the forces acting on that object

    Get xand ycomponents of all the forces tocalculate the net force

    Apply Newtons second law to get

    acceleration

    Use the acceleration in any motion analysis

    and establish a Kinetic Diagram

    ma

  • 8/11/2019 LEC 11 (Rectangular 051)

    8/18

    Normal & Frictional Force

    F

    Ff

    FN

    Action-Reaction forces

    - mg = FN

    mg

  • 8/11/2019 LEC 11 (Rectangular 051)

    9/18

    Static Friction ( s )

    Static frictionparallel force on the

    surface when there is no relative motion

    between the 2 objects

    Static friction force can vary from zero to

    Maximum

    The coefficient of static friction

    is material dependent.

    Static

    Ff= msFN

    Dynamic

    Ff= mkFN

    Applied external force

    Frict

    ion

  • 8/11/2019 LEC 11 (Rectangular 051)

    10/18

    Kinetic Friction ( k )

    Kinetic frictionparallel force on thesurface when there is relative motion

    between the 2 objects

    Kinetic friction force is always the same

    The coefficient of Kinetic friction

    is material dependent.

    NkFF f

    StaticFf= msFN

    DynamicFf= mkFN

    Applied external force

    Frictio

    n

  • 8/11/2019 LEC 11 (Rectangular 051)

    11/18

    Spring Force

    Spring force

    k : spring stiffness (N/m)

    s : stretched or

    compressed length

    ksFs

    olls

    ol l

    s

  • 8/11/2019 LEC 11 (Rectangular 051)

    12/18

    m = 2 kg

    y = 1m

    smooth

    a = ?

    maFmg s sin

    2219sin

    9053cosx5.0x3coscos

    m/s.m

    ksga

    N.ksFN sc

    ma

    Example 13-4

    0cos sc FN

    1353750

    1tan

    507507501

    1

    22

    ..

    m...S

  • 8/11/2019 LEC 11 (Rectangular 051)

    13/18

    x

    ymg

    N Nkm

    Problem

    NN

    N

    369

    020cos81.940

    ;0 yF

    xx maF mamgNk m sin

    0cos mgN

    2

    /66.5

    4020sin81.940)369(25.0

    sma

    a

    x

    x

    a = ?

  • 8/11/2019 LEC 11 (Rectangular 051)

    14/18

    Example 13-5

    m A= 3 kg

    m B= 5 kg

    From rest

    vB= ? In 2 second

    yy maF AaT 32981

    Block A

    yy maF BaT 52.196

    Block B

    lss BA 2 02 BA 02 BA aa

    taBo

    Same

    Sameshould be

  • 8/11/2019 LEC 11 (Rectangular 051)

    15/18

  • 8/11/2019 LEC 11 (Rectangular 051)

    16/18

    mg Ama

    )/(62.42 smsaV AA

    )2(12525.1226

    12581.9*125

    A

    AA

    aT

    aTmaFy

    NTsmasma

    aa

    aaaa

    A

    A

    A

    c

    cc

    c

    c

    1004)/(777.1)/(888.0

    500200

    250200622200981)12525.1226(25.849

    )1()2(

    22

  • 8/11/2019 LEC 11 (Rectangular 051)

    17/18

    Review

    Example 13.1

    Example 13.2

    Example 13.3

    Example 13.4

  • 8/11/2019 LEC 11 (Rectangular 051)

    18/18