0
$\begingroup$

Theorem 6.4.1. Let $E$ be a subset of $\mathbb{R}^n$, and let $F$ be a subset of $\mathbb{R}^m$. Let $f : E \to F$ be a function, and let $g : F \to \mathbb{R}^p$ be another function. Let $x_0$ be a point in the interior of $E$. Suppose that $f$ is differentiable at $x_0$, and that $f(x_0)$ is in the interior of $F$. Suppose also that $g$ is differentiable at $f(x_0)$. Then $g \circ f: E \to \mathbb{R}^p$ is also differentiable at $x_0$, and we have the formula $$(g \circ f)'(x_0) = g'(f(x_0)) f'(x_0).$$

Exercise 6.4.3. Prove Theorem 6.4.1. (Hint: you may wish to review the proof of the ordinary chain rule in single variable calculus. The easiest way to proceed is by using the sequence-based definition of limit)

In a single variable case, I first define $G_0(y) = \frac{g(y) - g(f(x_0))}{y-f(x_0)}$, and then extend it to $G(y) = G_0(y)$ if $y \not= f(x_0)$ and $g'(f(x_0))$ if $y = f(x_0)$. Then, we have that $$(g \circ f)'(x_0) =\lim_{n\to \infty} G(f(x_n)) \frac{f(x_n) - f(x_0)}{x_n- x_0} =g'(f(x_0)) f'(x_0).$$

I am trying to prove a multi variable case in a similar way. First, note that $(g \circ f)'(x_0) = ((g \circ f)'_1(x_0), ... , (g \circ f)_p'(x_0))$ (is this true?). Then, our task is to show the chain rule for $(g \circ f)_i: E \to \mathbb{R}$. That is, I need to show that $$\lim_{n \to \infty} \frac{(g \circ f)_i(x_n) - (g \circ f)_i(x_0)}{||x_n -x_0||} = (g'(f(x_0)) f)_i'(x_0). $$ But, I am not sure how to proceed from here. Am I using the right approach? I appreciate if you give some help.

$\endgroup$

2 Answers 2

1
$\begingroup$

This is Exercise $6.4.3$ from Tao's Analysis 2.

Let $L_1 = g'(f(x_0))$ and $L_2 = f'(x_0)$. By Proposition $3.1.5$(b), it suffices to show that $\forall \varepsilon > 0, \exists N >0$ such that $||(g \circ f)(x_n) - (g \circ f)'(x_0) - L_1L_2(x_n - x_0)|| \leqslant \varepsilon||x_n - x_0||$, for all $n \geq N$, where $(x_n)$ is any sequence converging to $x_0$.

Since $g$ is differentiable at $y_0 = f(x_0)$ and $f$ at $x_0$, we have, respectively: $||g(y_n) - g(y_0) - L_1(y_n - y_0)|| \leqslant \varepsilon^*||y_n - y_0||, \forall n \geqslant N_1 - (1)$, where $(y_n)$ converges to $y_0$. And $||f(x_n) - f(x_0) - L_2(x_n - x_0)|| \leqslant \varepsilon^*||x_n - x_0||, \forall n \geqslant N_2 - (2)$, where $(x_n)$ converges to $x_0$. By Proposition $3.1.5$(b) and the fact that f is continuous at $x_0$, we can combine $(1)$ and $(2)$, and let $C = (g \circ f)(x_n) - (g \circ f)(x_0)$ to obtain that: $||C - L_1(f(x_n) - f(x_0))|| \leqslant \varepsilon^* ||f(x_n) - f(x_0)||, \forall n \geqslant N = max(N_1, N_2) - (3)$.

By the triangle inequality, LHS of $(3) \geqslant ||C - L_1L_2(x_n - x_0)|| - ||L_1(f(x_n) - f(x_0) - f'(x_0)(x_n - x_0))||$. Hence $||C - L_1L_2(x_n - x_0)|| \leqslant ||L_1(f(x_n) - f(x_0) - f'(x_0)(x_n - x_0))|| + \varepsilon^*||f(x_n) - f(x_0)||, \forall n \geqslant N$.

By Exercise $6.1.4$, this implies that $||C - L_1L_2(x_n - x_0)|| \leqslant M||f(x_n) - f(x_0) - f'(x_0)(x_n - x_0)|| + \varepsilon^*||f(x_n) - f(x_0)||$ for some $M > 0. - (4)$

Again by the differentiability of $f$ at $x_0$, if $n$ is sufficiently large, we can make $||f(x_n) - f(x_0) - f'(x_0)(x_n - x_0)|| \leqslant \frac{\varepsilon|x_n - x_0|}{2M}$, s.t the first term on the RHS of $(4)$ is less than or equal to $\frac{\varepsilon||x_n - x_0||}{2}$. Similarly $||f(x_n) - f(x_0)|| \leqslant (M' + \varepsilon')||x_n - x_0||$ for some $M', \varepsilon' > 0$. If we let $\varepsilon^* = \frac{\varepsilon}{2(M' + \varepsilon')}$, the second term on the RHS of $(4)$ is also less than or equal to $\frac{\varepsilon||x_n - x_0||}{2}$. Hence the RHS of $(4) \leqslant \varepsilon||x_n - x_0||$, and the claim follows.

$\endgroup$
0
$\begingroup$

By definition, that $g$ is differentiable at $y_0 = f(x_0)$ signifies that $$g(y_0 + k) = g(y_0) + g'(y_0) \cdot k + \psi(k) \|k\|,$$ with $\lim_{k \to 0} \psi(k) = 0.$ Similarly, $$f(x_0 + h) = f(x_0) + f'(x_0) \cdot h + \varphi(h) \|h\|,$$ with $\lim_{h \to 0} \varphi(h) = 0.$

Plug in the expansion of $f$ into $g,$ to reach $$(g \circ f)(x_0 + h) = g(y_0) + g'(y_0) f'(x_0) \cdot h + \eta(h),$$ where $$\eta(h) = g'(y_0) \cdot \varphi(h) \|h\| + \psi(k_h) \|k_h\|$$ and $$k_h = f'(x_0) \cdot h + \varphi(h) \|h\|.$$ Observe that $$\|k_h\| \leq \|h\| \big(\|f'(x_0)\| + \|\varphi(h)\| \big) \leq 2\|f'(x_0)\| \|h\|$$ for all $h$ small enough. This entails (for $h \neq 0$) $$\dfrac{\eta(h)}{\|h\|} \leq \|g'(x_0) \cdot \varphi(h)\| + 2 \|\psi(k_h)\|$$ and since $\varphi(h) \to 0$ and $\psi(k_h) \to 0$ as $h \to 0,$ we are done. Q.E.D.

Remark. This proof works on any normed space.

$\endgroup$

You must log in to answer this question.

Not the answer you're looking for? Browse other questions tagged .