The Implicit and Inverse Function Theorems Notes to Supplement Chapter 13

The Implicit and Inverse Function Theorems Notes to Supplement Chapter 13

The Implicit and Inverse Function Theorems Notes to supplement Chapter 13. Remark: These notes are still in draft form. Examples will be added to Section 5. If you see any errors, please let me know. 1. Notation Let X and Y be two normed linear spaces, and let f : X ! Y be a function de¯ned in some neighborhood of the origin of X. We say that f(x) = o(jjxjjn) if jjf(x)jjY lim n = 0: x!0 jjxjjX Analogously, we say that f(x) = O(jjxjjn) if there exists some number C, and some neighborhood G of the origin in X such that n jjf(x)jjY · C jjxjjX ; 8x 2 G: 2. Differentiation on Banach Space Recall that a function f : R ! R is \di®erentiable" at a point x0 if there exists a number a such that (1) f(x) = f(x0) + a (x ¡ x0) + o(jx ¡ x0j): We usually write a = f 0(x). The right hand side of (1) is a linear approximation of f, valid near x0. This de¯nition can straight-forwardly be generalized to functions between two Banach spaces. De¯nition 1. Let X and Y be Banach spaces, let f be a map from X to Y , and let x0 be a point in X. We say that f is di®erentiable at x0 if there exists a map A 2 B(X; Y ) such that f(x) = f(x0) + A (x ¡ x0) + o(jjx ¡ x0jj): 0 The number A is called the \Fr¶echet Derivative" of f at x0. We write A = f (x) = df = D f = fx. Note that the de¯nition makes sense even if f is de¯ned only in a neighborhood of x0 (it does not need to be de¯ned on all of x). It follows directly from the de¯nition that if f is di®erentiable at x0, then it is also continuous as x0. The function f 0(x) is not a map from X to Y , it is a map from X to B(X; Y ). n m Example 1: Let f be a function from R to R . Let fi denote the component functions of f so that f = (f1; f2; : : : ; fm). If the partial derivatives @fi fi;j = @xj n all exist at some x0 2 R , then f is di®erentiable at x0 and 2 3 f1;1(x0) f1;2(x0) ¢ ¢ ¢ f1;n(x0) 6 f (x ) f (x ) ¢ ¢ ¢ f (x ) 7 0 6 2;1 0 2;2 0 2;n 0 7 f (x0) = 6 . 7 : 4 . 5 fm;1(x0) fm;2(x0) ¢ ¢ ¢ fm;n(x0) Example: Let (X; ¹) be a measure space and consider the function f : L3(X; ¹) ! L1(X; ¹): ' 7! '3: In order to see if f is di®erentiable, we need to see if there exists an A 2 B(L3;L1) such that jjf(' + Ã) ¡ f(') ¡ AÃjj (2) lim 1 = 0: jjÃjj3!0 jjÃjj3 We have f(' + Ã) = '3 + 3'2 à + 3'Ã2 + Ã3: Therefore, if f is di®erentiable, we must have Aà = 3'2 Ã. That A is a bounded map is clear since (applying HÄolder'sinequality with p = 3, q = 2=3) Z µZ ¶1=3 µZ ¶2=3 2 3 3 2 jjAÃjj1 = 3 j'j jÃj · 3 jÃj j'j = 3 jjÃjj3 jj'jj3 A similar calculation shows that 2 3 jjf(' + Ã) ¡ f(') ¡ AÃjj1 = jj3 'à + à jj1 2 3 2 3 · 3 jj'à jj1 + jjà jj1 · 3 jj'jj3 jjÃjj3 + jjÃjj3: It follows that (2) holds. Thus f is di®erentiable, and f 0('): à 7! 3 '2 Ã. Example: Set I = [0; 1] and consider the function Z 1 f : C(I) ! R : ' 7! sin('(x)) dx: 0 The function f is di®erentiable at ' if there exists an A 2 B(C(I);R) = C(I)¤ such that jf(' + Ã) ¡ AÃj (3) lim = 0: jjÃjju!0 jjÃjju We ¯nd that Z Z f(' + Ã) = sin(' + Ã) = (sin ' cos à + cos ' sin Ã): 2 When jjÃjju is small, Ã(x) is small for every x, and so cos à = 1 + O(à ), and sin à = à + O(Ã2). An informal calculation then yields Z Z f('+Ã) = ((sin ')(1+O(Ã2))+(cos ')(Ã+O(Ã2))) = f(')+ ((cos ')Ã)+O(Ã2): If f is di®erentiable, we must have Z 1 A : à 7! cos('(x)) Ã(x) dx: 0 It remains to prove that (3) holds. We have Z 1¡ ¢ f(' + Ã) ¡ f(') ¡ Aà = sin(' + Ã) ¡ sin(') ¡ cos(') à dx 0 Z 1 = (sin(')(cos(Ã) ¡ 1) + cos(')(sin(Ã) ¡ Ã)) dx: 0 Using that j1 ¡ cos tj · t2 and j sin t ¡ tj · t2 for all t 2 R, we obtain Z 1 2 2 jf(' + Ã) ¡ f(') ¡ AÃj · (j sin '(x)j + j cos '(x)j) jÃ(x)j dx · 2 jjÃjju: 0 Therefore (3) holds, and f is di®erentiable. Example: Read Example 13.7 in the textbook. Theorem 1 (Chain rule). Let X, Y , and Z denote Banach spaces. Suppose that the functions f : X ! Y , and g : Y ! Z are di®erentiable. Then g ± f : X ! Z is di®erentiable, and (g ± f)0(x) = g0(f(x)) f 0(x): Note that all properties of the functions in Theorem 1 are local, so it would have been su±cient to assume only that f is di®erentiable in some neighborhood of x, and g is di®erentiable in some neighborhood of f(x). The notion of di®erentiation de¯ned in Def. 1 is the direct generalization of the \Jacobian matrix" of multivariate analysis. We can also de¯ne a generalization of the concept of a directional derivative: De¯nition 2. Let X and Y be Banach spaces and let f denote a function from X to Y . Letting x and u denote elements of X, we de¯ne the directional derivative of f at x, in the direction u, by f(x + t u) ¡ f(x) (Duf)(x) = lim : t!0 t Note that (Duf)(x) is simply an element of Y . Remark 1. In the environment of Banach spaces, the directional derivative is fre- quently called a \G^ateauxderivative". Sometimes, this term is used to denote the vector (Duf)(x), but the text book uses a di®erent terminology. To avoid confusion, we will avoid the term \G^ateauxderivative". Example: Let f be as in Example 1, and let u 2 Rm. Then 2 3 u ¢ rf1(x) 6 7 6 u ¢ rf2(x) 7 (Duf)(x) = 6 . 7 : 4 . 5 u ¢ rfn(x) Note that if X and Y are Banach spaces, and f is a di®erentiable function from X to Y , then f(x + t u) = f(x) + f 0(x)(t u) + o(jjt ujj): Consequently, 0 (Duf)(x) = f (x) u: In other words, every (Fr¶echet) di®erentiable functions has directional derivatives in all directions. The converse is not true. In fact, it is not even true in R2 as the following example shows: 2 2 2 2 Example: Set X = R and Y = R. De¯ne ­ = f(x1; x2) 2 R : x1 < x2 < 2 x1g 2 and set f = ­. Then (Du f)(0) exists for all u 2 R , but f is not even continuous at 0. 3. Partial derivatives Let X, Y , and Z be Banach spaces and let F be a map from X £ Y to Z. Then F is di®erentiable at (^x; y^) 2 X £ Y if and only if there exist maps A 2 B(X; Z) and B 2 B(Y; Z) such that F (x; y) = F (^x; y^) + A (x ¡ x^) + B (y ¡ y^) + o(jjx ¡ x^jjX + jjy ¡ y^jjY ): We call the maps A and B the partial derivatives of F with respect to x and y, A = Fx(^x; y^);B = Fy(^x; y^): Note that A is simply the derivative of the map x 7! F (x; y^), and similarly B is the derivative of the map y 7! F (^x; y). 4. Minimization of functionals (View this section as a large example.) The directional derivative can be used to derive necessary conditions for a sta- 1 tionary point of a function. As an example, set I = [0; 1], X = C0 (I), and let us consider the functional Z 1 (4) I : X ! R : u 7! L(x; u(x); u0(x)) dx; 0 where L = L(x; u; v) is a function that is continuously di®erentiable in each of its arguments. Suppose that u 2 X is a point where I is minimized. Then for any ' 2 X, d 0 = I(u + "') = [D I](u): d" ' In other words, if u is a minimizer, then the directional derivative [D'I](u) must be zero for all ' 2 X. For the particular functional I, we ¯nd that ¯ Z 1 d ¯ £ 0 0 0¤ I(u + "')¯ = Lu(x; u; u ) ' + Lv(x; u; u ) ' dx: d" "=0 0 Performing a partial integration (using that '(0) = '(1) = 0), we obtain Z 1 · ¸ 0 d 0 (5) 0 = Lu(x; u; u ) ¡ Lv(x; u; u ) '(x) dx: 0 dx 1 For (5) to hold for every ' 2 C0 ([0; 1]) we must have d (6) L (x; u(x); u(x)0) ¡ L (x; u(x); u0(x)) = 0; x 2 [0; 1]: u dx v That the (potentially non-linear) ODE (6) holds is a necessary condition that a minimizer u must satisfy. This equation is called the \Euler-Lagrange" equation.

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