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Tuesday,December3 ∗ Solutions ∗ Surfaceintegralsofvectorfieldsandrelatedtheorems
1. ConsidertheregionD inR3 boundedbythexy-planeandthesurfacex2+y2+z=1.
(a) MakeasketchofD.
Solution. ThesketchofD isshownbelow.
(b) TheboundaryofD,denoted∂D,hastwoparts: thecurvedtopS1 andtheflatbottomS2.
ParameterizeS1andcalculatethefluxofF=(0,0,z)throughS1withrespecttotheupward
pointingunitnormalvectorfield. Checkyouanswerwiththeinstructor.
Solution. ToparametrizeS1,onehas
r(u, v)=〈ucosv, usinv, 1−u2〉, 0≤u≤1,0≤v≤2π.
Inordertocalculatetheflux,firstwehave
ru =〈cosv, sinv, −2u〉, rv =〈−usinv, ucosv, 0〉,
andso
ru×rv =〈2u2cosv, 2u2sinv, u〉.
Therefore,thefluxofF=(0,0,z)throughS1 withrespecttotheupwardpointingunitnor-
malvectorfieldis
ÏS1F·ndS=Z02πZ01F(u,v)·(ru×rv)dudv
=Z02πZ01(0,0,1−u2)·〈2u2cosv, 2u2sinv, u〉dudv
=Z 2πZ 1(1−u2)u dudv = π.
0 0 2
(c) Withoutdoingthefullcalculation,determinethefluxofFthroughS2 withthedownward
pointingnormals.
Solution. SinceF=0onS2,weknowthefluxofFthroughS2is
Ï F·ndS=Ï 0·ndS=0.
S2 S2
(d) DeterminethefluxofFthrough∂D withtheoutwardpointingnormals.
Solution. Byaddinguptheresultfrom(a)and(b),onegets
Ï F·ndS=Ï F·ndS+Ï F·ndS=π.
∂D S1 S2 2
(e) ApplytheDivergenceTheoremandyouranswerin(d)tofindthevolumeofD.Checkyour
answerwiththeinstructor.
Solution. BytheDivergenceTheorem,onehas
Ï∂DF·ndS=ÑDdivFdV.
SincedivF=1,onegets
Volume(D)=Ñ 1dV =Ñ divFdV =Ï F·ndS=π.
D D ∂D 2
2. ConsiderthevectorfieldF=(−y,x,z).
(a) ComputecurlF.
Solution.
i j k
curl F= ∂ ∂ ∂ =(0,0,2).
∂x ∂y ∂z
−y x z
(b) ForthesurfaceS1 above,evaluateÏS1¡curlF)·ndA.
Solution. ByapplyingtheparametrizationofS1 in1(b),onegets
Ï ¡curlF)·ndA=Z 2πZ 1(curl F)·(ru×rv)dudv
S1 0 0
=Z 2πZ 12u dudv =2π.
0 0
(c) Checkyouranswerin(b)usingStokes’Theorem.
Solution. The boundary of S1 is a unit circle centered at the origin in the xy-plane. So
wecanparametrizeitas
C: r(t)=〈cost, sint, 0〉, 0≤t≤2π.
Thus,byStokes’Theorem,onehas
Ï ¡curlF)·ndA=Z F·dr=Z 2πF(r(t))·r′(t)dt
S1 C 0
=Z 2π(−sint, cost, 0)·〈−sint, cost, 0〉dt =Z 2π1dt =2π.
0 0
3. If time remains:
(a) Checkyouranswerin1(e)bydirectlycalculatingthevolumeofD.
Solution. OnecanusethepolarcoordinatetocalculatethevolumeofD in1(e). Let
x=rcosθ, y=rsinθ, 0≤r ≤1, 0≤θ≤2π.
Then Ï Z 2πZ 1
Volume(D)= (1−x2−y2)dA= (1−r2)rdrdθ=π.
x2+y2≤1 0 0 2
(b) Repeat2(b-c)forthesurfaceS2 andalsoforthesurface∂D. Whatexactlydoes2(c)mean
for the surface ∂D?
Solution. ThenormalvectorofS2 pointingdownwardisn=−k. Thus,
Ï ¡curlF)·ndA=Ï (0,0,2)·(0,0,−1)dA=−2Ï dA=−2π.
S2 S2 S2
TochecktheaboveanswerusingStokes’Theorem,oneneedstheparametrizationofthe
boundaryofS2. NoticethatthisboundaryisthesameasthatofS1excepttheorientation.
TheboundaryofS2isparametrizedby
C′: r(t)=〈cos(2π−t), sin(2π−t), 0〉, 0≤t≤2π.
Thus,byStokes’Theorem,onehas
Ï ¡curlF)·ndA=Z ′F·dr=Z 2πF(r(t))·r′(t)dt
S2 C 0
=Z 2π(−sin(2π−t), cos(2π−t), 0)·〈sin(2π−t), −cos(2π−t), 0〉dt
0
=Z 2π−1dt=−2π.
0
Byaddingupthetwointegralsonegets
Ï∂D¡curlF)·ndA=ÏS1¡curlF)·ndA+ÏS2¡curlF)·ndA=2π+(−2π)=0.
Since ∂D is a surface without any curve boundary, then 2(c) shows that the integral of F
alongthecurveboundaryofthesurface∂D mustbe0.
(c) ForthevectorfieldF=(−y,x,z)fromthesecondproblem,computediv(curlF). Nowsup-
pose F=(F1,F2,F3) is an arbitrary vector field. Can you say anything about the function
div(curlF)?
Solution. Wealreadyknow,in2(a),thatcurl F=(0,0,2),sodiv(curlF)=0.Generally,sup-
posesupposeF=(F1,F2,F3)isanarbitraryvectorfield. Then
i j k µ∂F ∂F ∂F ∂F ∂F ∂F ¶
curlF=det ∂ ∂ ∂ = 3 − 2, 1 − 3, 2 − 1 ,
∂x ∂y ∂z ∂y ∂z ∂z ∂x ∂x ∂y
F1 F2 F3
and
div(curlF)=∂xµ∂F3 −∂F2¶+∂yµ∂F1 −∂F3¶+∂zµ∂F2 −∂F1¶
∂y ∂z ∂z ∂x ∂x ∂y
∂2F3 ∂2F2 ∂2F1 ∂2F3 ∂2F2 ∂2F1
=∂x∂y −∂x∂z +∂y∂z −∂y∂x +∂z∂x −∂z∂y =0.
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