23.3. STOKE’S THEOREM FROM GREEN’S THEOREM 437

Theorem 23.3.4 (Stoke’s Theorem) Let U be any region in R2 for which the conclusionof Green’s theorem holds and let R ∈ C2

(U ,R3

)be a one to one function satisfying

|(Ru×Rv)(u,v)| ̸= 0 for all (u,v) ∈U and let S denote the surface

S ≡ {R(u,v) : (u,v) ∈U} ,∂S ≡ {R(u,v) : (u,v) ∈ ∂U}

where the orientation on ∂S is consistent with the counter clockwise orientation on ∂U (Uis on the left as you walk around ∂U). Then for F a C1 vector field defined near S,∫

∂SF ·dR=

∫S

curl(F ) ·ndS

where n is the normal to S defined by

n≡ Ru×Rv

|Ru×Rv|.

Proof: Letting C be an oriented part of ∂U having parametrization,

r (t)≡ (u(t) ,v(t))

for t ∈ [α,β ] and letting R(C) denote the oriented part of ∂S corresponding to C,∫R(C)

F ·dR

=∫

β

α

F (R(u(t) ,v(t))) ·(Ruu′ (t)+Rvv′ (t)

)dt

=∫

β

α

F (R(u(t) ,v(t)))Ru (u(t) ,v(t))u′ (t)dt

+∫

β

α

F (R(u(t) ,v(t)))Rv (u(t) ,v(t))v′ (t)dt

=∫

C((F ◦R) ·Ru,(F ◦R) ·Rv) ·dr.

Since this holds for each such piece of ∂U , it follows∫∂SF ·d R=

∫∂U

((F ◦R) ·Ru,(F ◦R) ·Rv) ·dr.

By the assumption that the conclusion of Green’s theorem holds for U , this equals∫U[((F ◦R) ·Rv)u− ((F ◦R) ·Ru)v]dA

=∫

U[(F ◦R)u ·Rv +(F ◦R) ·Rvu− (F ◦R) ·Ruv− (F ◦R)v ·Ru]dA

=∫

U[(F ◦R)u ·Rv− (F ◦R)v ·Ru]dA

23.3. STOKE’S THEOREM FROM GREEN’S THEOREM 437Theorem 23.3.4 (Stoke’s Theorem) Let U be any region in R? for which the conclusionof Green’s theorem holds and let R € C* (U, R3) be a one to one function satisfying|(R, x R,) (u,v)| 40 for all (u,v) € U and let S denote the surfaceS = {R(u,v): (u,v) €U},OS = {R(u,v): (u,v) € au}where the orientation on OS is consistent with the counter clockwise orientation on QU (Uis on the left as you walk around OU). Then for F aC! vector field defined near S,F-dR= ewtF) -ndSas swhere n is the normal to S defined byn= R, x R,~ |R, x R,|’Proof: Letting C be an oriented part of QU having parametrization,for t € [a, B] and letting R(C) denote the oriented part of 0S corresponding to C,F-dRR(C)BI F(R(u(t),v(t)))- (Buu! (t) +. Ryv' (1) dtB=f FRWO.»O) Rau) xu Oat°B+ [| FRU), yO) Rou vO) at[Pe R): Ry, (Fo R)-Ry)-dr.Since this holds for each such piece of OU, it followsi F-dR=[| ((FoR)-R,,(FoR)-R,)-dr.as aUBy the assumption that the conclusion of Green’s theorem holds for U, this equals[Pe R)- Re), — (FoR) Ry) )dA= | (FoR), -Ry+(FoR): Ry — (FoR) Ry —(FoR),-R,]dAU= | (FoR), Ry (FoR), -Ry]dA