FOrmula AMME2500

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  • 7/29/2019 FOrmula AMME2500

    1/3

    AMME2500 Formula Sheet 2012 P age 1 of 3

    SOME USEFUL FORMULAE

    1. Two Dimensional KinematicsNon-rotation reference attached to B for 2 points A and B in a rigid body

    Equation of velocity: B/ABA vvv +=

    Equation of acceleration: B/ABA aaa += or

    ( ) ( ) ( ) ( ) ( ) ( )tB/AnB/AtBnBtAnA aaaaaa +++=+

    where: ( )ra = n)( and ra = t)( are the normal and tangential accelerations.Rotation reference attached to B for 2 points A and B in a rigid body

    Equation of velocity:relBA vrvv ++=

    Equation of acceleration: ( ) relrelBA avrraa ++++= 2 where relv and rela are relative velocity and relative acceleration respectively

    2. Two Dimensional Kinetics

    Equation of motion (G centre of mass): xx amF = yy amF = IMG = Work Energy principle: eg VVTU ++=21

    Work done by external force = rF dU and by external couple dMU = ,22

    2

    1

    2

    1IvmT += kinetic energy, hmgVg = gravitational P.E.,

    2

    2

    1kxVe = elastic P.E.

    Impulse-Momentum principle:

    Linear: 22122

    1

    vvG-GF mmdtt

    t==

    =

    =

    122

    1

    12

    2

    1

    :

    :

    yy

    t

    ty

    xx

    t

    tx

    vmvmdtFy

    vmvmdtFx

    Angular: 12GG 122

    1

    IIHHdtMt

    t G==

    3. Steady Mass Flow and Variable MassSteady Mass Flow:

    Resultant force: ( )12 vvGF == 'm& Resultant moment about O: ( )1122 vdvdHM == 'mOO &

    where 'm is mass flow rate, v1 entering velocity and v2 leaving velocity.

    Variable Mass: uvF mm && = where m is mass of system at time t, v is velocity of system, u is velocity of the rejected mass,

    F the external force acting on the system.

    4. Eulers First Law

    FR =Gm &&

    where RG is the position vector of mass center and F is the external force acting on the body

    5. Eulers Second Law

    H =& where H is angular momentum and = i ii FrM is the external moment acting on the body

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    AMME2500 Formula Sheet 2012 Page 2 of 3

    6. Angular Momentum

    ==

    z

    y

    x

    zzyxxz

    yxyyxy

    xzxyxx

    III

    III

    III

    IH

    where

    ( ) ( ) ++== B

    n

    i

    iiixx dmzyzymI22

    1

    22 == B

    n

    i

    iiixy xydmyxmI1

    ( ) ( ) ++== B

    n

    i

    iiiyy dmzxzxmI22

    1

    22 == B

    n

    i

    iiixz xzdmzxmI

    1

    ( ) ( ) ++== B

    n

    i

    iiizz dmyxyxmI22

    1

    22 == B

    n

    i

    iiiyz yzdmzymI1

    7. Parallel Axis Theorem

    xxXxXX ImdI +=2

    where Xxd is the distance between the these two axes (XXandxx)

    8. Parallel Plane Theorem

    xyGGXY IYmXI +=

    whereXG, YG, ZG are the coordinate of the center of mass.

    9. Kinetic Energy of A Rigid Body

    GGGmT HVV += 2

    1

    2

    1T

    where VG is the velocity of the center of mass, is the angular velocity of the body, HG isangular momentum of the body about the center of mass.

    10. Lagranges Equations

    ( )NCk

    kkk

    Qq

    V

    q

    T

    q

    T

    dt

    d=

    +

    & r,,k L1=

    where Tis the kinetic energy, Vthe potential energy, qk the generalized coordinates and( )NCkQ the non-conservative generalized forces.

    11. Integration

    ( ) 11

    Cbtalnbbta

    dt+=

    ( ) ( ) ( ) 2111

    1 Ctatlnata

    dtatln += where C1 and C2 are constant of integration

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    AMME2500 Formula Sheet 2012 Page 3 of 3

    12. Mass Moment of Inertia

    Geometry Mass moment of inertia

    xy

    R

    SphereG

    2

    5

    2mRIII zzyyxx ===

    0=== zxyzxy III

    x

    y

    z

    x

    y

    z

    h

    R

    Cylinder G

    ( )22312

    1hRmII yyxx +==

    2

    2

    1mRIzz =

    0=== zxyzxy III

    xy

    z

    xy

    z

    RDisk G

    24

    1mRII yyxx == , 22

    1mRIzz =

    0=== zxyzxy III

    x

    y

    x

    yl G

    l/2

    l/2

    Slender

    bar

    2

    12

    1mlII yyxx ==

    2

    3

    1mlII 'y'y'x'x ==

    0==== zzzxyzxy IIII

    x

    y

    z

    R

    h

    h/4

    Cone

    G

    ( )22480

    3hRmII yyxx +==

    2

    10

    3mRIzz =

    0=== zxyzxy III

    x

    y

    z

    ab

    cBlock G

    ( )22121 cbmIxx += , ( )22121 camIyy +=

    ( )2212

    1bamIzz +=

    0=== zxyzxy III

    ab

    cPlate

    x

    y

    z

    G

    2

    12

    1mbIxx = ,

    2

    12

    1maIyy =

    ( )2212

    1bamIzz +=

    0=== zxyzxy III