Calculus I · A Toolkit for Slopes

The quotient rule (which the chain rule hands us)

Now that we have the product and chain rules, the quotient rule is almost free. Write a quotient as a product with a negative power: fg=f⋅g−1\tfrac{f}{g} = f\cdot g^{-1}. The derivative of g−1g^{-1} is, by power-rule-plus-chain, −g−2g′-g^{-2}g'. So the product rule gives f′g−1+f(−g−2g′)=f′g−fg′g2f'g^{-1} + f(-g^{-2}g') = \tfrac{f'}{g} - \tfrac{fg'}{g^2}, and combining over g2g^2:

The Quotient Rule. ddx[f(x)g(x)]=f′(x)g(x)−f(x)g′(x)(g(x))2.\displaystyle \frac{d}{dx}\left[\frac{f(x)}{g(x)}\right] = \frac{f'(x)\,g(x) - f(x)\,g'(x)}{\big(g(x)\big)^2}.

In words: bottom times derivative of top, minus top times derivative of bottom, all over the bottom squared. (The order matters — the minus sign makes it non-symmetric.) Example: ddxxx2+1=(1)(x2+1)−(x)(2x)(x2+1)2=1−x2(x2+1)2\tfrac{d}{dx}\tfrac{x}{x^2+1} = \tfrac{(1)(x^2+1) - (x)(2x)}{(x^2+1)^2} = \tfrac{1 - x^2}{(x^2+1)^2}.


The trigonometric derivatives (where Chapter 2 finally pays off)

We promised, back in Chapter 2, that the two strange limits we proved there — sin⁡hh→1\tfrac{\sin h}{h} \to 1 and cos⁡h−1h→0\tfrac{\cos h - 1}{h} \to 0 — were the tools that would unlock the derivatives of sine and cosine. Here is that promise kept, and it’s worth savoring because it’s the whole reason those limits earned a place in the book.

Figure 4.4
Figure 4.4

Differentiate sin⁡x\sin x from the definition. The key is the angle-addition formula sin⁡(x+h)=sin⁡xcos⁡h+cos⁡xsin⁡h\sin(x+h) = \sin x\cos h + \cos x\sin h:

sin⁡(x+h)−sin⁡xh=sin⁡xcos⁡h+cos⁡xsin⁡h−sin⁡xh=sin⁡x⋅cos⁡h−1h+cos⁡x⋅sin⁡hh.\frac{\sin(x+h) - \sin x}{h} = \frac{\sin x\cos h + \cos x\sin h - \sin x}{h} = \sin x\cdot\frac{\cos h - 1}{h} + \cos x\cdot\frac{\sin h}{h}.

Now let h→0h \to 0. The first fraction goes to 00 and the second goes to 11 — exactly the two Chapter 2 limits — so the whole thing becomes sin⁡x⋅0+cos⁡x⋅1\sin x \cdot 0 + \cos x \cdot 1:

ddxsin⁡x=cos⁡x\boxed{\;\frac{d}{dx}\sin x = \cos x\;}

The identical computation with cos⁡(x+h)=cos⁡xcos⁡h−sin⁡xsin⁡h\cos(x+h) = \cos x\cos h - \sin x\sin h gives

ddxcos⁡x=−sin⁡x\boxed{\;\frac{d}{dx}\cos x = -\sin x\;}

(the minus sign because cosine is falling as it leaves 00). And tan⁡x=sin⁡xcos⁡x\tan x = \tfrac{\sin x}{\cos x} now yields to the quotient rule: ddxtan⁡x=cos⁡xcos⁡x−sin⁡x(−sin⁡x)cos⁡2x=cos⁡2x+sin⁡2xcos⁡2x=1cos⁡2x=sec⁡2x\tfrac{d}{dx}\tan x = \tfrac{\cos x\cos x - \sin x(-\sin x)}{\cos^2 x} = \tfrac{\cos^2 x + \sin^2 x}{\cos^2 x} = \tfrac{1}{\cos^2 x} = \sec^2 x. These are the derivatives that Chapter 7 used to build the Taylor series of sin\sin and cos\cos (and, through them, Euler’s formula) — now derived from the ground up.


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