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Mathematics YMA01 · Chapter 12

Further differentiation

Derivatives of exponentials, logarithms and trigonometric functions, the product and quotient rules, and curves defined parametrically or implicitly. It also adds the inverse tangent.

Written for the 2018 specification syllabus · 4 min read

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Differentiation

Standard derivatives

yydydx\dfrac{\mathrm{d}y}{\mathrm{d}x}
ex\mathrm{e}^xex\mathrm{e}^x
ln⁡x\ln x1x\dfrac{1}{x}
sin⁡x\sin xcos⁡x\cos x
cos⁡x\cos x−sin⁡x-\sin x
tan⁡x\tan xsec⁡2x\sec^2 x
tan⁡−1x\tan^{-1} x11+x2\dfrac{1}{1 + x^2}

Composites

The chain rule gives these general results:

yydydx\dfrac{\mathrm{d}y}{\mathrm{d}x}
ef(x)\mathrm{e}^{\mathrm{f}(x)}f′(x)ef(x)\mathrm{f}'(x)\mathrm{e}^{\mathrm{f}(x)}
ln⁡f(x)\ln \mathrm{f}(x)f′(x)f(x)\dfrac{\mathrm{f}'(x)}{\mathrm{f}(x)}
sin⁡f(x)\sin \mathrm{f}(x)f′(x)cos⁡f(x)\mathrm{f}'(x)\cos \mathrm{f}(x)
cos⁡f(x)\cos \mathrm{f}(x)−f′(x)sin⁡f(x)-\mathrm{f}'(x)\sin \mathrm{f}(x)
tan⁡f(x)\tan \mathrm{f}(x)f′(x)sec⁡2f(x)\mathrm{f}'(x)\sec^2 \mathrm{f}(x)

6x e3x26x3x2+12sec⁡22x2sin⁡xcos⁡x=sin⁡2x6x\,\mathrm{e}^{3x^2} \qquad \frac{6x}{3x^2 + 1} \qquad 2\sec^2 2x \qquad 2\sin x\cos x = \sin 2x

sin⁡2x\sin^2 x means (sin⁡x)2(\sin x)^2, so use the power rule first and multiply by the derivative of sin⁡x\sin x.

The product and quotient rules

dydx=x2⋅2e2x+e2x⋅2x=2xe2x(x+1)\frac{\mathrm{d}y}{\mathrm{d}x} = x^2 \cdot 2\mathrm{e}^{2x} + \mathrm{e}^{2x}\cdot 2x = 2x\mathrm{e}^{2x}(x + 1)

dydx=x⋅1x−ln⁡x⋅1x2=1−ln⁡xx2\frac{\mathrm{d}y}{\mathrm{d}x} = \frac{x\cdot\frac{1}{x} - \ln x \cdot 1}{x^2} = \frac{1 - \ln x}{x^2}

The quotient rule also gives these results, which are worth recognising:

ddx(sec⁡x)=sec⁡xtan⁡xddx(cosec⁡x)=−cosec⁡xcot⁡xddx(cot⁡x)=−cosec⁡2x\frac{\mathrm{d}}{\mathrm{d}x}(\sec x) = \sec x\tan x \qquad \frac{\mathrm{d}}{\mathrm{d}x}(\operatorname{cosec} x) = -\operatorname{cosec} x\cot x \qquad \frac{\mathrm{d}}{\mathrm{d}x}(\cot x) = -\operatorname{cosec}^2 x

Stationary points with these functions

Set the derivative to zero and solve. A positive factor like e−x\mathrm{e}^{-x} can never be zero, so divide it out safely.

dydx=e−x−xe−x=(1−x)e−x\dfrac{\mathrm{d}y}{\mathrm{d}x} = \mathrm{e}^{-x} - x\mathrm{e}^{-x} = (1 - x)\mathrm{e}^{-x}. Since e−x>0\mathrm{e}^{-x} > 0, the only solution is x=1x = 1, at the point (1,e−1)\left(1, \mathrm{e}^{-1}\right).

The gradient goes from positive to negative through x=1x = 1, so this is a maximum.

Parametric curves

A curve can be described by writing xx and yy in terms of a third variable, the parameter tt.

dydx=6t22t=3t\dfrac{\mathrm{d}y}{\mathrm{d}x} = \dfrac{6t^2}{2t} = 3t, which is 3 at t=1t = 1. The point is (2,2)(2, 2), so the tangent is y−2=3(x−2)y - 2 = 3(x - 2), or y=3x−4y = 3x - 4.

Implicit differentiation

When yy is mixed in with xx, differentiate every term with respect to xx. Any term in yy picks up a factor of dydx\dfrac{\mathrm{d}y}{\mathrm{d}x}, and a product of xx and yy needs the product rule.

TermDerivative with respect to xx
y2y^22ydydx2y\dfrac{\mathrm{d}y}{\mathrm{d}x}
xyxyxdydx+yx\dfrac{\mathrm{d}y}{\mathrm{d}x} + y
sin⁡y\sin ycos⁡ydydx\cos y\dfrac{\mathrm{d}y}{\mathrm{d}x}

2x+xdydx+y+2ydydx=0⇒dydx=−2x+yx+2y2x + x\frac{\mathrm{d}y}{\mathrm{d}x} + y + 2y\frac{\mathrm{d}y}{\mathrm{d}x} = 0 \quad\Rightarrow\quad \frac{\mathrm{d}y}{\mathrm{d}x} = -\frac{2x + y}{x + 2y}

At (1,2)(1, 2) the gradient is −45-\dfrac{4}{5}.

The inverse tangent

ddx(tan⁡−1x)=11+x2ddx(tan⁡−12x)=21+4x2\frac{\mathrm{d}}{\mathrm{d}x}\left(\tan^{-1} x\right) = \frac{1}{1 + x^2} \qquad \frac{\mathrm{d}}{\mathrm{d}x}\left(\tan^{-1} 2x\right) = \frac{2}{1 + 4x^2}

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