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  • 8/13/2019 MATEMATIKA 4 Theorema.pptx

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    Greens

    Theorem

    Gauss

    Theorem

    Stokes

    Theorem

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    1. Greens Theorem

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    (No, he was not French)

    George Green

    Jul

    y 14, 1793 - May 31, 1841

    British mathematician and physicist

    First person to try to explain a mathematical theory ofelectricity and magnetism

    Almost entirely self-taught!

    Published An Essay on the Application of MathematicalAnalysis to the Theories of Electricity and Magnetismin

    1828. Entered Cambridge University as an undergraduate in

    1833 at age 40.

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    The Theory

    Consider a simple closed curve C,and let Dbe the regionenclosed by the curve.

    Notes:

    The simple, closed curve has no holesin the region D

    A direction has been put on the curve with the convention that the curve C

    has a positive orientationif the region Dis on the leftas we traverse the path.

    dAy

    f

    x

    ggdyfdx

    C D

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    Example

    Section 13.2, problem 2A particle moves once counterclockwise about the circle of radius 6

    about

    the origin, under the influence of the force:

    Calculate the work done.

    jxyixxyeF x )())cosh(( 2/3

    )sin(6),cos(6)( tttC

    )2,0(: tI

    6

    F

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    I

    dttCtCFW )(')(

    dtttttttte t )cos(6),sin(6)cos(6)(sin6)),cos(6cosh()cos(6)sin(62

    0

    23

    )cos(6

    )sin(6),cos(6)( tttC

    jxyixxyeF x )())cosh(( 2/3

    Remember:

    dttttttet t

    2

    0

    23

    )cos(6 36)(sin)cos(36))cos(6cosh()cos()sin(36)sin(6

    72

    Direct computation:

    C

    sdFWork

    dttCsd )('

    I dttCtCFWork )(')(

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    Greens Theoremand beyond

    Greens Theorem is a crucial component in

    the development of many famous works:

    James Maxwells EquationsGauss Divergence Theorem

    Stokes Integral Theorem

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    13.7 Gauss Divergence

    Theorem

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    (Also not French)

    Gauss in the House

    German mathematician, lived1777-1855

    Born in Braunschweig, Duchy ofBraunschweig-Lneburg inNorthwestern Germany

    Published DisquisitionesArithmeticaewhen he was 21 (andwhat have youdone today?)

    As a workaholic, was onceinterrupted while working and toldhis wife was dying. He repliedtell her to wait a moment untilIm finished.

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    Gauss Divergence Theorem

    The integral of a continuously differentiable

    vector field across a boundary (flux) is equal

    to the integral of the divergence of that vectorfield within the region enclosed by the

    boundary.

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    Applications The Aerodynamic Continuity Equation

    The surface integral of mass flux around a control volumewithout sources or sinks is equal to the rate of mass storage.

    If the flow at a particular point is incompressible, then the netvelocity flux around the control volume must be zero.

    As net velocity flux at a point requires taking the limit of anintegral, one instead merely calculates the divergence.

    If the divergence at that point is zero, then it is incompressible. Ifit is positive, the fluid is expanding, and vice versa

    Gausss Theorem can be applied to any vector field which obeys an

    inverse-square law (except at the origin), such as gravity,electrostatic attraction, and even examples in quantum physics suchas probability density.

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    The unit normal of the sphere is defined as

    It will be much easier to compute this integral in sphericalcoordinates, making:

    The 3-D surface integral for radius = 1 (plus Jacobian) isequal to:

    Unit Normal Integration

    ),,( zyxn

    ))cos()sin()cos(,)sin()sin(),cos()sin()cos()sin(( 3322223 V

    ))cos(),sin()cos(),sin()(sin( n

    0)cos()sin()cos()sin()sin()cos()sin()cos()sin( 324342

    2

    00

    dd

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    Now, Gauss Divergence Theorem shall be used, and the sameresult should be obtained

    The divergence of the vector V:

    The integration results in:

    This verifies Gauss Theorem

    Keep in mind however that this is only possible with continuouslydifferentiable functions, not all functions

    Gauss Divergence Integration

    )sin()sin(2)]cos()sin()sin()cos()sin()cos(2[22

    2

    xzyyzV

    0)(sin)sin(2)]cos()(sin)sin()cos()(sin)cos(2[

    )sin()(

    23224

    1

    0

    2

    00

    2

    1

    0

    2

    00

    ddd

    dddV

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    13.8 The Integral

    Theorem of Stokes

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    Sir George Gabriel Stokes

    (Aug. 13, 1819Feb. 1, 1903)

    Irish mathematician and physicist who attended

    Pembroke College (Cambridge University).

    (Again, also not French)

    After graduating as Senior Wrangler (first in class inmathematics) and as a Smiths Prizemen (award for

    excellence in research), he was awarded a fellowship

    and did much of his lifes work at Cambridge.

    Stokes was the oldest of the trio of natural

    philosophers who contributed to the fame of theCambridge University school of Mathematical Physics

    in the middle of the 19thcentury. The others were:

    James Clark Maxwell - Maxwells Equations,

    electricity, magnetism and inductance.

    Lord Kelvin - Thermodynamics, absolutetemperature scale.

    Stokes is remembered for his numerous contributions

    to science and mathematics which included research

    in the areas of hydrodynamics, viscosity, elasticity,

    wave theory of light and optics.

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    Stokes TheoremInteresting Fact :This theorem is also known as the KelvinStokes Theorem because it was actually

    discovered by Lord Kelvin. Kelvin then presented his discovery in a letter to Stokes. Stokes, who was

    teaching at Cambridge at the time, made the theory a proof on the Smiths Prize exam and the namestuck. Additionally, this theorem was used in the derivation of 2 of Maxwells Equations!

    Given:A three dimensional surfacein a vector field F. Its

    boundary is denoted by orientation n.

    Stokes Theorem:

    So what does it mean?

    As Greenes Theorem provides the transformation from a line integral to a surface integral, Stokes

    theorem provides the transformation from a line integral to a surface integral in three-dimensionalspace.

    Simply said, the surface integral of the curl of a vector field over a three dimensional surface is equal

    to the line integral of the vector field over the boundary of the surface.

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    An application from Aerodynamics

    The circulation, of a flow is defined as the line integral of the velocity over a closed curve, C:

    C

    V

    ndA

    C sdV

    Given:A three dimensional surface in Velocity Field V with boundary C.

    Now, by Stokes Theorem, we can say that the circulation around the closed contour C is equal to the

    surface integral of the curl of the velocity field over the surface. Mathematically, this is written as:

    dAnVsdV

    AC

    )(

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    Example from Aerodynamics

    Given:An incompressible, steady from where the velocity field is:

    jxy

    y

    ixyyxV )3()( 2

    322

    vdyudxsdVC

    Find: For the plane shown, show that the circulation around the boundary is equal to the

    surface integral of the curl of the velocity field over the surface (verify Stokes Theorem).

    Solution:

    x

    y

    y=x

    (1,1)

    1

    23

    1

    0

    0

    0

    23

    22)

    3()( dyxyy

    dxxyyx1.)

    y = 0, x = x

    = 0

    2.)

    y = y, x = 1

    1

    1

    1

    0

    23

    22 )3

    ()( dyxyy

    dxxyyx = -1/4

    0

    1

    0

    1

    23

    22 )3

    ()( dyxyy

    dxxyyx3.)

    y = x

    = 1/6

    12

    1

    TOTAL

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    Now, evaluating the curl of the velocity vector over the surface.

    Example from Aerodynamics (continued)

    03

    23

    22 xyy

    xyyx

    zyx

    kji

    V

    dAnVA

    )(

    kxyxy )2( 22

    1

    0 0

    22 )2()(

    x

    A

    dydxkkxyxydAnV

    1

    0

    3

    3

    1dxx

    12

    1

    12

    1)( dAnVsdV

    AC

    Thus, Stokes Theorem is verified:

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    Summary

    Greens Theorem discovered in 1825 Gauss Theorem discovered in 1813

    Stokes Theorem discovered in 1850

    Gauss

    (Germany)

    Stokes

    (Ireland)Green

    (England)

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    http://www.jhelvy.com/elephant/home.htm