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Generalized Stokes' Theorem Chapter 4 Generalized Stokes’ Theorem “It is very difficult for us, placed as we have been from earliest childhood in a condition of training, to say what would have been our feelings had such training never taken place.” Sir George Stokes, 1st Baronet 4.1. Manifolds with Boundary We have seen in the Chapter 3 that Green’s, Stokes’ and Divergence Theorem in Multivariable Calculus can be unified together using the language of differential forms. In this chapter, we will generalize Stokes’ Theorem to higher dimensional and abstract manifolds. These classic theorems and their generalizations concern about an integral over a manifold with an integral over its boundary. In this section, we will first rigorously define the notion of a boundary for abstract manifolds. Heuristically, an interior point of a manifold locally looks like a ball in Euclidean space, whereas a boundary point locally looks like an upper-half space. n 4.1.1. Smooth Functions on Upper-Half Spaces. From now on, we denote R+ := n n f(u1, ... , un) 2 R : un ≥ 0g which is the upper-half space of R . Under the subspace n n n topology, we say a subset V ⊂ R+ is open in R+ if there exists a set Ve ⊂ R open in n n n R such that V = Ve \ R+. It is intuitively clear that if V ⊂ R+ is disjoint from the n n n subspace fun = 0g of R , then V is open in R+ if and only if V is open in R . n n Now consider a set V ⊂ R+ which is open in R+ and that V \ fun = 0g 6= Æ. We need to first develop a notion of differentiability for functions such an V as their domain. m Given a vector-valued function G : V ! R , then near a point u 2 V \ fun = 0g, we can only approach u from one side only, namely from directions with positive un-coordinates. The usual definition of differentiability does not apply at such a point, so we define: 99 100 4. Generalized Stokes’ Theorem k n n n Definition 4.1 (Functions of Class C on R+). Let V ⊂ R+ be open in R+ and that m k V \ fun = 0g 6= Æ. Consider a vector-valued function G : V ! R . We say G is C k (resp. smooth) at u 2 V \ fun = 0g if there exists a C (resp. smooth) local extension m n Ge : B#(u) ! R such that Ge(y) = G(y) for any y 2 B#(u) \ V. Here B#(u) ⊂ R refers to an open ball in Rn. k If G is C (resp. smooth) at every u 2 V (including those points with un > 0), then we say G is Ck (resp. smooth) on V. Figure 4.1. G is Ck at u if there exists a local extension Ge near u. 2 2 2 Example 4.2. Let V = f(x, y) : y ≥ 0 and x + y < 1g, which is an open set in R+ 2 2 2 since V = f(x, y) : x + y < 1g \ R+. Then f (x, y) : V ! R defined by f (x, y) = | {z } open in R2 p p 1 − x2 − y2 is a smooth function on V since 1 − x2 − y2 is smoothly on the whole ball x2 + y2 < 1. p However, the function g : V ! R defined by g(x, y) = y is not smooth at every ¶g + point on the y-axis because ¶y ! ¥ as y ! 0 . Any extension ge of g will agree with g ¶ge + on the upper-half plane, and hence will also be true that ¶y ! ¥ as y ! 0 , which is sufficient to argue that such ge is not smooth. 2 2 Exercise 4.1. Consider f : R+ ! R defined by f (x, y) = jxj. Is f smooth on R+? 2 2 If not, at which point(s) in R+ is f not smooth? Do the same for g : R+ ! R defined by g(x, y) = jyj. 4.1.2. Boundary of Manifolds. After understanding the definition of a smooth function when defined on subsets of the upper-half space, we are ready to introduce the notion of manifolds with boundary: 4.1. Manifolds with Boundary 101 Definition 4.3 (Manifolds with Boundary). We say M is a smooth manifold with boundary if there exist two families of local parametrizations Fa : Ua ! M where Ua is n n open in R , and Gb : Vb ! M where Vb is open in R+ such that every Fa and Gb is a homeomorphism between its domain and image, and that the transition functions of all types: −1 −1 −1 −1 Fa ◦ Fa0 Fa ◦ Gb Gb ◦ Gb0 Gb ◦ Fa are smooth on the overlapping domain for any a, a0, b and b0. Moreover, we denote and define the boundary of M by: [ ¶M := fGb(u1,..., un−1, 0) : (u1,..., un−1, 0) 2 Vbg. b Remark 4.4. In this course, we will call these Fa’s to be local parametrizations of interior type, and these Gb’s to be local parametrizations of boundary type. Figure 4.2. A manifold with boundary Example 4.5. Consider the solid ball B2 := fx 2 R2 : jxj ≤ 1g. It can be locally parametrized using polar coordinates by: G : (0, 2p) × [0, 1) ! B2 G(q, r) := (1 − r)(cos q, sin q) Note that the domain of G can be regarded as a subset 2 V := f(q, r) : q 2 (0, 2p) and 0 ≤ r < 1g ⊂ R+. Here we used 1 − r instead of r so that the boundary of B2 has zero r-coordinate, and the interior of B2 has positive r-coordinate. Note that the image of G does not cover the whole solid ball B2. Precisely, the image of G is B2nfnon-negative x-axisg. In order to complete the proof that B2 is a manifold with boundary, we cover B2 by two more local parametrizations: Ge : (−p, p) × [0, 1) ! B2 Ge(q, r) := (1 − r)(cos q, sin q) and also the inclusion map i : fu 2 R2 : juj < 1g ! B2. We need to show that the transition maps are smooth. There are six possible transition maps: − − − − − − Ge 1 ◦ G, G 1 ◦ Ge, i 1 ◦ G, i 1 ◦ Ge, G 1 ◦ i, and Ge 1 ◦ i. 102 4. Generalized Stokes’ Theorem The first one is given by (we leave it as an exercise for computing these transition maps): − Ge 1 ◦ G : ((0, p) [ (p, 2p)) × [0, 1) ! ((−p, 0) [ (0, p)) × [0, 1) ( − (q, r) if q 2 (0, p) Ge 1 ◦ G(q, r) = (q − 2p, r) if q 2 (p, 2p) which can be smoothly extended to the domain ((0, p) [ (p, 2p)) × (−1, 1). Therefore, Ge−1 ◦ G is smooth. The second transition map G−1 ◦ Ge can be computed and verified to be smooth in a similar way. For i−1 ◦ G, by examining the overlap part of i and G on B2, we see that the domain of the transition map is an open set (0, 2p) × (0, 1) in R2. On this domain, i−1 ◦ G is essentially G, which is clearly smooth. Similar for i−1 ◦ Ge. To show G−1 ◦ i is smooth, we use the Inverse Function Theorem. The domain of i−1 ◦ G is (0, 2p) × (0, 1). By writing (x, y) = i−1 ◦ G(q, r) = (1 − r)(cos q, sin q), we check that on the domain of i−1 ◦ G, we have: ¶(x, y) det = 1 − r 6= 0. ¶(q, r) Therefore, the inverse G−1 ◦ i is smooth. Similar for Ge−1 ◦ i. Combining all of the above verifications, we conclude that B2 is a 2-dimensional manifold with boundary. The boundary ¶B2 is given by points with zero r-coordinates, namely the unit circle fjxj = 1g. Exercise 4.2. Compute all transition maps − − − − − − Ge 1 ◦ G, G 1 ◦ Ge, i 1 ◦ G, i 1 ◦ Ge, G 1 ◦ i, and Ge 1 ◦ i in Example 4.5. Indicate clearly their domains, and verify that they are smooth on their domains. Exercise 4.3. Let f : Rn ! R be a smooth scalar function. The region in Rn+1 above the graph of f is given by: n+1 G f := f(u1,..., un+1) 2 R : un+1 ≥ f (u1,..., un)g. Show that G f is an n-dimensional manifold with boundary, and the boundary ¶G f is the graph of f in Rn+1. Exercise 4.4. Show that ¶M (assumed non-empty) of any n-dimensional manifold M is an (n − 1)-dimensional manifold without boundary. From the above example and exercise, we see that verifying a set is a manifold with boundary may be cumbersome. The following proposition provides us with a very efficient way to do so. Proposition 4.6. Let f : Mm ! R be a smooth function from a smooth manifold M. Suppose c 2 R such that the set S := f −1([c, ¥)) is non-empty and that f is a submersion at any p 2 f −1(c), then the set S is an m-dimensional manifold with boundary. The boundary ¶S is given by f −1(c). Proof. We need to construct local parametrizations for the set S. Given any point p 2 S, then by the definition of S, we have f (p) > c or f (p) = c. 4.1. Manifolds with Boundary 103 For the former case f (p) > c, we are going to show that near p there is a local parametrization of S of interior type.
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