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File: Surface Integral Pdf 171737 | Lecture35
1 lecture 35 surface area surface integrals in the previous lecture we dened the surface area a s of the parametric surface s dened by r u v on t ...

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                                                                                                                    1
                                          Lecture 35 : Surface Area; Surface Integrals
                In the previous lecture we defined the surface area a(S) of the parametric surface S, defined by
                r(u,v) on T, by the double integral     RR
                                                a(S) =     k r ×r kdudv.                                           (1)
                                                              u    v
                                                         T
                    Wewill now drive a formula for the area of a surface defined by the graph of a function.
                Area of a surface defined by a graph: Suppose a surface S is given by z = f(x,y), (x,y) ∈ T,
                that is, S is the graph of the function f(x,y). (For example, S is the unit hemisphere defined by
                    p       2    2                                             2   2
                z =    1−x −y where(x,y)liesinthecircular region T : x +y ≤ 1.) Then S can be considered
                as a parametric surface defined by:
                                              r(x,y) = xi+yj +f(x,y)k,       (x,y) ∈ T.
                In this case the surface area becomes
                                                            RR q      2     2
                                                    a(S) =       1+f +f dxdy.                                      (2)
                                                                      x    y
                                                            T q
                because k r ×r k = k −f i−f j +k k =             1+f2+f2.
                            u    v          x     y                   x    y
                                                                                                   2    2     2      2
                Example 1: Let us find the area of the surface of the portion of the sphere x + y + z = 4a
                                               2    2
                that lies inside the cylinder x + y = 2ax. Note that the sphere can be considered as a union of
                                    p 2       2    2
                two graphs: z = ±      4a −x −y . We will use the formula given in (2) to evaluate the surface
                                         p 2       2    2
                area. Let z = f(x,y) =     4a −x −y . Then
                                  √ −x                √ −y                q       2    2    q 4a2
                            fx =              , fy =                and      1+f +f =           2   2  2.
                                      2  2   2            2  2   2                x    y      4a −x −y
                                    4a −x −y            4a −x −y
                Let T be the projection of the surface z = f(x,y) on the xy-plane (see Figure 1). Then, because
                of the symmetry, the surface area is
                                                q                          π 2acosθ
                                                                           2
                                              RR      4a2                  R   R    2ardrdθ
                                     ( ) = 2                 dxdy      ×           √       .
                                    a S            4a2−x2−y2      =2 2                2   2
                                              T                            0   0     4a −r
                Remark: Since
                              2         2      2    2           2      2         2             2     2           2
                   k r ×r k = kr k kr k sin θ = kr k kr k (1−cos θ) = kr k kr k −(r ·r ) ,
                      u    v         u      v                u      v                       u      v       u   v
                the formula given in (1) can be written as RR √
                                                     a(S) =      EG−F2dudv                                         (3)
                                                             T
                where E = r ·r ,G = r ·r and F = r ·r .
                             u   u       v   v            u   v
                                                                                                                        2
                 Example 2: Let us compute the area of the torus
                                       x=(a+bcosφ)cosθ, y =(a+bcosφ)sinθ, z =bsinφ
                 where 0 ≤ θ ≤ 2π, 0 ≤ φ ≤ 2π, and a and b are constants such that 0 < b < a. Since the surface is
                 given in the parametric form with the parameters θ and φ, we can either use the formula given in
                 (1) or (3) and find the surface area. We do not have to know how the surface looks like. However
                 the surface is given in Figure 2 for understanding. Note that
                 r =−(a+bcosφ)sinθi+(a+bcosφ)cosθj+0k, rv =−bsinφcosθi−bsinφsinθj+bcosφk.
                  θ
                                                              2                2            √          2
                 This implies that E = r ·r = (a+bcosφ) , F = 0, G = b and hence              EG−F =b(a+bcosϕ).
                                          u  u
                 Therefore, by (3), the surface area is
                                     a(S) = RR b(a+bcosϕ)dθdφ = R2πR2πb(a+bcosϕ)dθdφ = 4π2ab.
                                                                        0   0
                                              T
                 Note that this problem can also be solved using the Pappus theorem : a(S) = 2πρL = 2π ·a·2πb.
                 Surface Integrals: We will define the concept of integrals, called surface integrals, to the scalar
                 functions defined on parametric surfaces. Surface integrals are used to define center of mass and
                 moment of inertia of surfaces, and the surface integrals occur in several applications. We will not
                 get in to the applications of the surface integrals in this course. We will define the surface integrals
                 and see how to evaluate them.
                    Let S be a parametric surface defined by r(u,v),(u,v) ∈ T. Suppose r and r are continuous.
                                                                                               u       v
                 Let g : S → R be bounded. The surface integral of g over S, denoted by RR gdσ, is defined by
                                                                                               S
                                    RR         RR                                RR           √          2
                                       g dσ =     g(r(u,v)) k r ×r k dudv =         g(r(u,v)) EG−F dudv               (4)
                                                                u    v
                                     S          T                                 T
                 provided the RHS double integral exists. If S is defined by z = f(x,y), then
                                           RR         RR               q       2     2
                                              g dσ =     g[x,y,f(x,y)]    1+f +f dxdy.                                (5)
                                                                               x     y
                                            S          T
                 where T is the projection of the surface S over the xy-plane.
                                                                          2   2    2 1/2                 RR         dσ
                 Example3: LetSbethehemisphericalsurfacez = (a −x −y )                  . Let us evaluate     2   2      2 1/2.
                                                                                                          S [x +y +(z+a) ]
                 Wefirst parameterize the surface S as follows:
                             S := r(θ,φ) = (asinφcosθ, asinφsinθ, acosφ), 0 ≤ θ ≤ 2π, 0 ≤ φ ≤ π.
                                                √          2     2            2    2        2 1/2          φ
                 Simplecalculation shows that     EG−F =a sinφand[x +y +(z+a) ]                   =2acos 2. Therefore,
                 by equation (4), the surface integral is
                                               RR        dσ        =R2πRπ/2 a2sinφ dφdθ.
                                                    2  2      2 1/2    0   0         φ
                                                S [x +y +(z+a) ]                2acos 2
                 Example4: LetusevaluatethesurfaceintegralRR g dσ whereg(x,y,z) = x+y+z andthesurface
                                                                      S
                 Sisdescribedbyz = 2x+3y, x ≥ 0, y ≥ 0andx+y ≤ 2. Weusetheformulagivenin(5)toevaluate
                 the surface integral. Note that the projection T of the surface is {(x,y) : x ≥ 0, y ≥ 0, x+y ≤ 2}.
                 The surface integral is
                             RR         RR            q       2     2         R2R2−y                     √
                                g dσ =     (x+y+z) 1+fx+fy dxdy= 0 0 (x+y+2x+3y) 14dxdy.
                              S          T
                 Remark: Under certain general conditions (we deal with surfaces satisfying such conditions) the
                 value of the surface integral is independent of the representation.
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