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  • 7/30/2019 Chap 13 Econ

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    VECTOR CALCULUS

    13

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    13.8

    Stokes Theorem

    In this section, we will learn about:

    The Stokes Theorem and

    using it to evaluate integrals.

    VECTOR CALCULUS

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    STOKES VS. GREENS THEOREM

    Stokes Theorem can be regarded as

    a higher-dimensional version of Greens

    Theorem.

    Greens Theorem relates a double integral over

    a plane region Dto a line integral around its planeboundary curve.

    Stokes Theorem relates a surface integral over

    a surface Sto a line integral around the boundarycurve ofS(a space curve).

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    INTRODUCTION

    The figure shows an oriented surface with

    unit normal vectorn.

    The orientation ofSinduces the positiveorientation of the

    boundary curve C.

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    INTRODUCTION

    This means that:

    If you walk in the positive direction around Cwith your head pointing in the direction ofn,

    the surface will always be on your left.

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    STOKES THEOREM

    Let:

    Sbe an oriented piecewise-smooth surfacebounded by a simple, closed, piecewise-smooth

    boundary curve Cwith positive orientation.

    F be a vector field whose components havecontinuous partial derivatives on an open region

    in that contains S.

    Then,

    3

    curlC

    S

    d d F r F S

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    STOKES THEOREM

    The theorem is named after the Irish

    mathematical physicist Sir George Stokes

    (18191903).

    What we call Stokes Theorem was actually

    discovered by the Scottish physicist Sir William

    Thomson (18241907, known as Lord Kelvin).

    Stokes learned of it in a letter from Thomson in 1850.

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    STOKES THEOREM

    Thus, Stokes Theorem says:

    The line integral around the boundary curve ofSof the tangential component ofF is equal to the surfaceintegral of the normal component of the curl ofF.

    and

    curl curl

    C C

    S S

    d ds

    d d

    F r F T

    F S F n S

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    STOKES THEOREM

    The positively oriented boundary curve of

    the oriented surface Sis often written as S.

    So,the theorem can be expressed as:

    curlS

    S

    d d

    F S F r

    Equation 1

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    STOKES THEOREM, GREENS THEOREM, & FTC

    There is an analogy among Stokes Theorem,

    Greens Theorem, and the Fundamental

    Theorem of Calculus (FTC).

    As before, there is an integral involving derivatives

    on the left side of Equation 1 (recall that curl F isa sort of derivative ofF).

    The right side involves the values ofF only onthe boundaryofS.

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    STOKES THEOREM, GREENS THEOREM, & FTC

    In fact, consider the special case

    where the surface S:

    Is flat.

    Lies in the xy-plane with upward orientation.

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    STOKES THEOREM, GREENS THEOREM, & FTC

    Then,

    The unit normal is k.

    The surface integral becomes a double integral.

    Stokes Theorem becomes:

    curl curlC

    S S

    d d dA F r F S F k

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    STOKES THEOREM

    Stokes Theorem is too difficult for us to

    prove in its full generality.

    Still, we can give a proof when:

    Sis a graph.

    F, S, and Care well behaved.

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    STOKES TH.SPECIAL CASE

    We assume that the equation ofS

    is:

    z= g(x, y), (x, y) D

    where:

    ghas continuous second-order partial derivatives.

    Dis a simple plane region whose boundary curveC1 corresponds to C.

    Proof

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    If the orientation ofSis upward, the positive

    orientation ofCcorresponds to the positive

    orientation ofC1.

    ProofSTOKES TH.SPECIAL CASE

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    STOKES TH.SPECIAL CASE

    We are also given that:

    F = Pi + Qj + Rk

    where the partial derivatives of

    P, Q, and Rare continuous.

    Proof

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    STOKES TH.SPECIAL CASE

    Sis a graph of a function.

    Thus, we can apply Formula 10 in

    Section 12.7 with F replaced by curl F.

    Proof

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    STOKES TH.SPECIAL CASE

    Suppose

    x =x(t) y =y(t) atb

    is a parametric representation ofC1.

    Then, a parametric representation ofCis:

    x =x(t) y =y(t) z =g(x(t), y(t)) a

    t

    b

    Proof

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    STOKES TH.SPECIAL CASE

    Four terms in that double integral cancel.

    The remaining six can be arranged to

    coincide with the right side of Equation 2.

    Hence,

    curlCS

    d d F r F S

    Proof

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    STOKES THEOREM

    We first compute:

    2 2

    curl 1 2yx y z

    y x z

    i j k

    F k

    Example 1

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    STOKES THEOREM

    There are many surfaces with

    boundary C.

    The most convenientchoice, though, isthe elliptical region Sin the plane y+ z= 2that is bounded by C.

    If we orient Supward,Chas the inducedpositive orientation.

    Example 1

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    STOKES THEOREM

    The projection DofSon the xy-plane

    is the disk x2 + y2 1.

    So, using Equation 10in Section 12.7 with

    z =g(x, y) = 2y,we have the following

    result.

    Example 1

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    STOKES THEOREM

    2 1

    0 0

    12 32

    00

    21 2

    2 30

    1

    2

    curl 1 2

    1 2 sin

    2 sin2 3

    sin

    2 0

    CS D

    d d y dA

    r r dr d

    r rd

    d

    F r F S

    Example 1

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    STOKES THEOREM

    Use Stokes Theorem to compute

    where:

    F(x, y, z) = xzi + yzj + xyk

    Sis the part of

    the spherex2 + y2 + z2 = 4that lies inside

    the cylinder

    x2 + y2 =1and above

    the xy-plane.

    curlS

    d F SExample 2

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    STOKES THEOREM

    A vector equation ofCis:

    r(t) = cos ti + sin tj + k 0 t 2

    Therefore, r(t) =sin ti + cos tj

    Also, we have:

    3

    Example 2

    3 cos 3 sin cos sint t t t t F r i j k

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    STOKES THEOREM

    Thus, by Stokes Theorem,

    2

    0

    2

    0

    2

    0

    curl

    ( ( )) '( )

    3 cos sin 3 sin cos

    3 0 0

    CS

    d d

    t t dt

    t t t t dt

    dt

    F S F r

    F r r

    Example 2

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    STOKES THEOREM

    In general, ifS1 and S2 are oriented surfaces

    with the same oriented boundary curve C

    and both satisfy the hypotheses of Stokes

    Theorem, then

    This fact is useful when it is difficult to integrate

    over one surface but easy to integrate over the other.

    1 2

    curl curlC

    S S

    d d d F S F r F S

    Equation 3

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    CIRCULATION

    Thus, is a measure of the tendency

    of the fluid to move around C.

    It iscalled the circulation ofv around C.

    C

    d v r

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    CURL VECTOR

    Now, let:

    P0(x0, y0, z0) be a point in the fluid.

    Sabe a small disk with radius aand centerP0.

    Then, (curl F)(P) (curl F)(P0) for all pointsPon Sabecause curl F is continuous.

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    CURL VECTOR

    Thus, by Stokes Theorem, we get

    the following approximation to the circulation

    around the boundary circle Ca:

    0 0

    2

    0 0

    curl curl

    curl

    curl

    a

    a a

    a

    CS S

    S

    d d dS

    P P dS

    P P a

    v r v S v n

    v n

    v n

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    CURL VECTOR

    The approximation becomes better as a 0.

    Thus, we have:

    0 0 201

    curl limaCa

    P P da

    v n v r

    Equation 4

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    CURL & CIRCULATION

    Equation 4 gives the relationship

    between the curl and the circulation.

    It shows that curl v n is a measure of

    the rotating effect of the fluid about the axis n.

    The curling effect is greatest about the axis

    parallel to curl v.

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    CURL & CIRCULATION

    Imagine a tiny paddle wheel placed in

    the fluid at a point P.

    The paddle wheel

    rotates fastest

    when its axis is

    parallel to curl v.

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    CLOSED CURVES

    Finally, we mention that Stokes Theorem

    can be used to prove Theorem 4 in

    Section 12.5:

    If curl F = 0 on all of , then F is conservative.3

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    CLOSED CURVES

    From Theorems 3 and 4 in Section 12.3,

    we know that F is conservative if

    for every closed path C.

    Given C, suppose we can find an orientablesurface Swhose boundary is C.

    This can be done, but the proof requiresadvanced techniques.

    0C

    d F r

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    CLOSED CURVES

    Then, Stokes Theorem gives:

    A curve that is not simple can be broken into

    a number of simple curves. The integrals around these curves are all 0.

    curl 0 0C

    S S

    d d d F r F S S

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    CLOSED CURVES

    Adding these integrals,

    we obtain:

    for any closed curve C.

    0C

    d F r