Differentiation in P3

A2 · P3 · 14 min

In P1 you could only differentiate powers of xx. P3 widens the toolkit to every function on the syllabus: exe^x, ln⁡x\ln x, the six trigonometric functions and tan⁡−1x\tan^{-1} x, combined in sums, products, quotients and composites, and extended to curves given implicitly or parametrically. This note is the map: it collects the standard derivatives, sharpens the chain rule (the one rule used in almost every P3 calculus question), and shows how gradients, tangents, normals and stationary points are examined now that the functions are harder. Differentiation appears on every P3 paper, often as a whole question and always as a step inside integration, numerical methods and differential equations questions.

What changes from P1

Nothing about the meaning of a derivative changes. dydx\dfrac{dy}{dx} is still the gradient of the curve, the rate at which yy changes as xx changes. What changes is the range of functions you can feed in and the number of rules you combine.

P1P3
xnx^n for rational nnxnx^n, exe^x, ln⁡x\ln x, sin⁡x\sin x, cos⁡x\cos x, tan⁡x\tan x, sec⁡x\sec x, cosec⁡x\operatorname{cosec} x, cot⁡x\cot x, tan⁡−1x\tan^{-1} x
Chain rule for (ax+b)n(ax+b)^n and similarChain rule for any composite, including layered ones such as ln⁡(cos⁡2x)\ln(\cos 2x)
No products or quotientsProduct rule and quotient rule
Curves y=f(x)y = f(x) onlyImplicit curves such as x2+y2=xy+7x^2 + y^2 = xy + 7 and parametric curves x=f(t)x = f(t), y=g(t)y = g(t)
Answers usually integers or fractionsAnswers usually exact: ln⁡3\ln 3, e−2e^{-2}, π4\tfrac{\pi}{4}, 3\sqrt{3}

The dedicated notes cover each new piece in depth:

The standard derivatives

Every derivative in P3 is built from this table plus the chain, product and quotient rules. Learn the left-hand block by heart; the right-hand block follows from it, and you should be able to derive any line in under a minute.

Standard derivatives
f(x)f(x)f′(x)f'(x)f(x)f(x)f′(x)f'(x)
xnx^nnxn−1nx^{n-1}tan⁡x\tan xsec⁡2x\sec^2 x
exe^xexe^xsec⁡x\sec xsec⁡xtan⁡x\sec x \tan x
ln⁡x\ln x1x\dfrac{1}{x}cosec⁡x\operatorname{cosec} x−cosec⁡xcot⁡x-\operatorname{cosec} x \cot x
sin⁡x\sin xcos⁡x\cos xcot⁡x\cot x−cosec⁡2x-\operatorname{cosec}^2 x
cos⁡x\cos x−sin⁡x-\sin xtan⁡−1x\tan^{-1} x11+x2\dfrac{1}{1 + x^2}

With a linear inside, the chain rule just multiplies by aa:

ddxeax+b=aeax+b,ddxln⁡(ax+b)=aax+b,ddxsin⁡(ax+b)=acos⁡(ax+b)\frac{d}{dx} e^{ax+b} = a e^{ax+b}, \qquad \frac{d}{dx} \ln(ax+b) = \frac{a}{ax+b}, \qquad \frac{d}{dx}\sin(ax+b) = a\cos(ax+b)

The trigonometric results hold only when xx is in radians.

The list of formulae given in the exam contains most of the right-hand column and the product and quotient rules, but not the basics. More importantly, you will not have time to look things up while chaining several rules together. Know them cold.

Radians only

ddxsin⁡x=cos⁡x\dfrac{d}{dx}\sin x = \cos x is true only when xx is measured in radians. If a question is set in degrees you must convert first. In calculus questions in P3, always set your calculator to radians and leave angles such as π6\tfrac{\pi}{6} exact.

The chain rule, properly

The chain rule is the engine of P3 differentiation. It deals with a composite function, a function of a function, such as ln⁡(3x2+2)\ln(3x^2 + 2): first you compute u=3x2+2u = 3x^2 + 2 (the inner function), then you take ln⁡u\ln u (the outer function).

Why rates multiply

Suppose uu changes 6 times as fast as xx, and yy changes 15\tfrac{1}{5} as fast as uu. Then yy changes 6×156 \times \tfrac{1}{5} times as fast as xx. Rates of change through a chain of dependencies multiply. That is all the chain rule says.

Chain rule

If yy is a function of uu and uu is a function of xx, then

dydx=dydu×dudx\frac{dy}{dx} = \frac{dy}{du} \times \frac{du}{dx}

In function notation: ddxf(g(x))=f′(g(x))×g′(x)\dfrac{d}{dx} f\big(g(x)\big) = f'\big(g(x)\big) \times g'(x).

In words: differentiate the outside, keep the inside unchanged, then multiply by the derivative of the inside.

The form in words is the one to use in practice. For ln⁡(3x2+2)\ln(3x^2 + 2): the outside is ln⁡( ⋅ )\ln(\ \cdot\ ), whose derivative is 1( ⋅ )\dfrac{1}{(\ \cdot\ )}; keep the inside, giving 13x2+2\dfrac{1}{3x^2+2}; multiply by the derivative of the inside, 6x6x. Result: 6x3x2+2\dfrac{6x}{3x^2+2}.

Layered composites

Some functions have three or more layers. Peel them from the outside in, one factor per layer.

sin⁡32x\sin^3 2x means (sin⁡2x)3(\sin 2x)^3. The layers, from outside in, are: cube, sine, 2x2x.

ddx(sin⁡2x)3=3(sin⁡2x)2⏟cube×cos⁡2x⏟sine×2⏟2x=6sin⁡22xcos⁡2x\frac{d}{dx}(\sin 2x)^3 = \underbrace{3(\sin 2x)^2}_{\text{cube}} \times \underbrace{\cos 2x}_{\text{sine}} \times \underbrace{2}_{2x} = 6\sin^2 2x\cos 2x
Differentiating a composite
  1. Write the function so its layers are visible: sin⁡32x=(sin⁡2x)3\sin^3 2x = (\sin 2x)^3, 1+ex=(1+ex)1/2\sqrt{1 + e^x} = (1 + e^x)^{1/2}, 1cos⁡x=(cos⁡x)−1\dfrac{1}{\cos x} = (\cos x)^{-1}.
  2. Differentiate the outermost layer, leaving everything inside it untouched.
  3. Multiply by the derivative of the next layer in, and so on, until you reach xx.
  4. Tidy the product: constants to the front, powers combined, a recognisable trig form if there is one.

The derivative of an inverse

A useful consequence: if you can write xx as a function of yy, then

dydx=1  dxdy  \frac{dy}{dx} = \frac{1}{\;\dfrac{dx}{dy}\;}

This is how ddxln⁡x\dfrac{d}{dx}\ln x and ddxtan⁡−1x\dfrac{d}{dx}\tan^{-1}x are found from exe^x and tan⁡x\tan x. It also appears directly in questions such as "given x=y2+ln⁡yx = y^2 + \ln y, find dydx\dfrac{dy}{dx} in terms of yy".

Reading the structure before you start

Most errors in P3 differentiation are not algebra slips; they are choosing the wrong rule. Before you write anything, ask what the last operation would be if you evaluated the expression for a particular xx.

Last operationExampleRule
Adding or subtractinge2x−3ln⁡xe^{2x} - 3\ln xDifferentiate term by term
Multiplying two functions of xxx2e−xx^2 e^{-x}Product rule
Dividing two functions of xxln⁡xx+1\dfrac{\ln x}{x+1}Quotient rule
Applying a function to an expressionln⁡(cos⁡2x)\ln(\cos 2x), ex2e^{x^2}, (1+tan⁡x)4(1 + \tan x)^4Chain rule
Multiplying by a constant5sin⁡3x5\sin 3xKeep the constant, differentiate the rest

Inside each rule, the pieces may themselves need the chain rule. For x2e−xx^2 e^{-x} the last operation is a multiplication (product rule), and differentiating e−xe^{-x} inside it needs the chain rule.

Simplify first

Some functions become much easier after a rewrite. Do it before differentiating, not after.

  • Logarithm laws. ln⁡x2+1=12ln⁡(x2+1)\ln\sqrt{x^2+1} = \tfrac{1}{2}\ln(x^2 + 1), and ln⁡(2x+1)3x−1=3ln⁡(2x+1)−ln⁡(x−1)\ln\dfrac{(2x+1)^3}{x-1} = 3\ln(2x+1) - \ln(x-1). Differentiating the expanded form avoids a chain rule inside a quotient rule.
  • Indices. 3x=3x−1/2\dfrac{3}{\sqrt{x}} = 3x^{-1/2}; e3x+1ex=e2x+e−x\dfrac{e^{3x} + 1}{e^x} = e^{2x} + e^{-x}.
  • Splitting a fraction with a single-term denominator: x2+4x=x+4x−1\dfrac{x^2 + 4}{x} = x + 4x^{-1}.
  • Trigonometric identities. 2sin⁡xcos⁡x=sin⁡2x2\sin x\cos x = \sin 2x; sin⁡xcos⁡x=tan⁡x\dfrac{\sin x}{\cos x} = \tan x.

Applications: gradients, tangents, normals and stationary points

The applications are the same as in P1. What makes them P3 questions is that the functions are harder and the answers are exact.

Using the derivative
  • Gradient at x=ax = a: f′(a)f'(a).
  • Tangent at (a,f(a))(a, f(a)): y−f(a)=f′(a)(x−a)y - f(a) = f'(a)(x - a).
  • Normal at (a,f(a))(a, f(a)): gradient −1f′(a)-\dfrac{1}{f'(a)}, since perpendicular gradients multiply to −1-1.
  • Stationary point: where dydx=0\dfrac{dy}{dx} = 0.
  • Nature: d2ydx2>0\dfrac{d^2y}{dx^2} > 0 means a minimum, d2ydx2<0\dfrac{d^2y}{dx^2} < 0 a maximum. If it is 00 or awkward, check the sign of dydx\dfrac{dy}{dx} either side.
  • Increasing where dydx>0\dfrac{dy}{dx} > 0, decreasing where dydx<0\dfrac{dy}{dx} < 0.

In P3, setting dydx=0\dfrac{dy}{dx} = 0 often leads to an equation that cannot be solved exactly. Then the question says "show that the xx-coordinate of the stationary point satisfies the equation x=…x = \ldots" and continues with an iteration. See numerical methods for the second half.

Tip

Exponentials are never zero. When dydx\dfrac{dy}{dx} factorises as esomething×(…)e^{\text{something}} \times (\ldots), the stationary points come only from the bracket. Say so in one line: "since e−x>0e^{-x} > 0, dydx=0⇒2x−x2=0\dfrac{dy}{dx} = 0 \Rightarrow 2x - x^2 = 0."

Worked examples

Composites with each standard function

Differentiate with respect to xx:

(a) e1−4xe^{1 - 4x} (b) ln⁡(3x2+2)\ln(3x^2 + 2) (c) sin⁡32x\sin^3 2x (d) tan⁡−12x\tan^{-1} 2x

Solution

(a) Outer e(⋅)e^{(\cdot)}, inner 1−4x1 - 4x with derivative −4-4:

ddxe1−4x=−4e1−4x\frac{d}{dx}e^{1-4x} = -4e^{1-4x}

(b) Outer ln⁡(⋅)\ln(\cdot), inner 3x2+23x^2 + 2 with derivative 6x6x:

ddxln⁡(3x2+2)=6x3x2+2\frac{d}{dx}\ln(3x^2 + 2) = \frac{6x}{3x^2 + 2}

(c) Three layers: cube, sine, 2x2x.

ddx(sin⁡2x)3=3(sin⁡2x)2⋅cos⁡2x⋅2=6sin⁡22xcos⁡2x\frac{d}{dx}(\sin 2x)^3 = 3(\sin 2x)^2 \cdot \cos 2x \cdot 2 = 6\sin^2 2x \cos 2x

(d) Outer tan⁡−1(⋅)\tan^{-1}(\cdot) with derivative 11+(⋅)2\dfrac{1}{1 + (\cdot)^2}, inner 2x2x:

ddxtan⁡−12x=11+(2x)2×2=21+4x2\frac{d}{dx}\tan^{-1} 2x = \frac{1}{1 + (2x)^2} \times 2 = \frac{2}{1 + 4x^2}
Simplify, then differentiate

Find dydx\dfrac{dy}{dx} when (a) y=ln⁡x2+1y = \ln\sqrt{x^2 + 1} and (b) y=ln⁡(2x+1)3x−1y = \ln \dfrac{(2x + 1)^3}{x - 1}.

Solution

(a) Use ln⁡ak=kln⁡a\ln a^k = k\ln a first: y=12ln⁡(x2+1)y = \tfrac{1}{2}\ln(x^2 + 1).

dydx=12×2xx2+1=xx2+1\frac{dy}{dx} = \frac{1}{2} \times \frac{2x}{x^2 + 1} = \frac{x}{x^2 + 1}

(b) Expand with the log laws: y=3ln⁡(2x+1)−ln⁡(x−1)y = 3\ln(2x + 1) - \ln(x - 1).

dydx=3×22x+1−1x−1=62x+1−1x−1\frac{dy}{dx} = \frac{3 \times 2}{2x + 1} - \frac{1}{x - 1} = \frac{6}{2x+1} - \frac{1}{x-1}

Over a common denominator this is 6(x−1)−(2x+1)(2x+1)(x−1)=4x−7(2x+1)(x−1)\dfrac{6(x-1) - (2x+1)}{(2x+1)(x-1)} = \dfrac{4x - 7}{(2x + 1)(x - 1)}.

Exact tangent

The curve y=e2x−4xy = e^{2x} - 4x has a point PP where x=ln⁡2x = \ln 2. Find the equation of the tangent at PP, and the exact yy-coordinate of the point where it crosses the yy-axis.

Solution

At x=ln⁡2x = \ln 2: e2ln⁡2=eln⁡4=4e^{2\ln 2} = e^{\ln 4} = 4, so y=4−4ln⁡2y = 4 - 4\ln 2.

dydx=2e2x−4\dfrac{dy}{dx} = 2e^{2x} - 4, so at PP the gradient is 2(4)−4=42(4) - 4 = 4.

Tangent:

y−(4−4ln⁡2)=4(x−ln⁡2)⇒y=4x+4−8ln⁡2y - (4 - 4\ln 2) = 4(x - \ln 2) \quad\Rightarrow\quad y = 4x + 4 - 8\ln 2

At x=0x = 0 the tangent has y=4−8ln⁡2y = 4 - 8\ln 2.

Stationary point with logarithms

Find the exact coordinates of the stationary point of y=3ln⁡(2x+1)−2xy = 3\ln(2x + 1) - 2x, for x>−12x > -\tfrac{1}{2}, and determine its nature.

Solutiondydx=62x+1−2\frac{dy}{dx} = \frac{6}{2x + 1} - 2

Set equal to zero: 62x+1=2⇒2x+1=3⇒x=1\dfrac{6}{2x+1} = 2 \Rightarrow 2x + 1 = 3 \Rightarrow x = 1.

Then y=3ln⁡3−2y = 3\ln 3 - 2. The stationary point is (1, 3ln⁡3−2)(1,\ 3\ln 3 - 2).

d2ydx2=−12(2x+1)2,at x=1: −129=−43<0\frac{d^2y}{dx^2} = -\frac{12}{(2x + 1)^2}, \qquad \text{at } x = 1:\ -\frac{12}{9} = -\frac{4}{3} < 0

so it is a maximum.

Stationary points of a product

Find the coordinates of the stationary points of y=x2e−xy = x^2e^{-x} and determine their nature.

Solution

By the product rule,

dydx=2xe−x−x2e−x=e−x(2x−x2)=xe−x(2−x)\frac{dy}{dx} = 2xe^{-x} - x^2e^{-x} = e^{-x}(2x - x^2) = xe^{-x}(2 - x)

Since e−x>0e^{-x} > 0, dydx=0\dfrac{dy}{dx} = 0 gives x=0x = 0 or x=2x = 2. The points are (0,0)(0, 0) and (2,4e−2)(2, 4e^{-2}).

Differentiating again (product rule on e−x(2x−x2)e^{-x}(2x - x^2)):

d2ydx2=−e−x(2x−x2)+e−x(2−2x)=e−x(x2−4x+2)\frac{d^2y}{dx^2} = -e^{-x}(2x - x^2) + e^{-x}(2 - 2x) = e^{-x}(x^2 - 4x + 2)

At x=0x = 0: 2>02 > 0, a minimum. At x=2x = 2: e−2(4−8+2)=−2e−2<0e^{-2}(4 - 8 + 2) = -2e^{-2} < 0, a maximum.

y = x^2 e^(-x) (2, 0) -- (2, 4 e^(-2))

The curve y=x2e−xy = x^2e^{-x} touches the origin (a minimum) and has a maximum at x=2x = 2, then decays towards the xx-axis.

Exam-hard: a stationary point you cannot solve exactly

The curve y=ln⁡xx+1y = \dfrac{\ln x}{x + 1} has one stationary point.

(a) Show that its xx-coordinate satisfies x=e1+1/xx = e^{1 + 1/x}.

(b) Use the iteration xn+1=e1+1/xnx_{n+1} = e^{1 + 1/x_n} with x1=3.5x_1 = 3.5 to find the xx-coordinate correct to 2 decimal places, showing the result of each iteration to 4 decimal places.

Solution

(a) Quotient rule with u=ln⁡xu = \ln x, v=x+1v = x + 1:

dydx=(x+1)⋅1x−ln⁡x⋅1(x+1)2\frac{dy}{dx} = \frac{(x+1)\cdot\frac{1}{x} - \ln x \cdot 1}{(x + 1)^2}

At a stationary point the numerator is zero:

x+1x=ln⁡x⇒ln⁡x=1+1x⇒x=e1+1/x\frac{x + 1}{x} = \ln x \quad\Rightarrow\quad \ln x = 1 + \frac{1}{x} \quad\Rightarrow\quad x = e^{1 + 1/x}

(b) x1=3.5x_1 = 3.5, x2=3.6173x_2 = 3.6173, x3=3.5839x_3 = 3.5839, x4=3.5931x_4 = 3.5931, x5=3.5906x_5 = 3.5906, x6=3.5913x_6 = 3.5913, x7=3.5911x_7 = 3.5911.

The iterates agree to 2 d.p., so x=3.59x = 3.59 (2 d.p.).

Common mistakes
  • Forgetting the inner derivative. ddxex2=2xex2\dfrac{d}{dx}e^{x^2} = 2xe^{x^2}, not ex2e^{x^2}. ddxsin⁡4x=4cos⁡4x\dfrac{d}{dx}\sin 4x = 4\cos 4x, not cos⁡4x\cos 4x.
  • Treating ln⁡(ax)\ln(ax) like ln⁡(ax+b)\ln(ax+b) wrongly. ddxln⁡7x=77x=1x\dfrac{d}{dx}\ln 7x = \dfrac{7}{7x} = \dfrac{1}{x}. That is correct, because ln⁡7x=ln⁡7+ln⁡x\ln 7x = \ln 7 + \ln x.
  • Misreading powers of trig functions. sin⁡2x\sin^2 x means (sin⁡x)2(\sin x)^2, derivative 2sin⁡xcos⁡x2\sin x\cos x. It is not sin⁡(x2)\sin(x^2), whose derivative is 2xcos⁡(x2)2x\cos(x^2).
  • Normal gradient. The normal gradient is −1m-\dfrac{1}{m}, not −m-m and not 1m\dfrac{1}{m}.
  • Using degrees. Calculator in degree mode when substituting x=0.5x = 0.5 gives nonsense.
  • Dividing by a possible zero. When solving xe−x(2−x)=0x e^{-x}(2 - x) = 0, do not divide by xx; you lose the root x=0x = 0.
Exam tip
  • "Find the exact coordinates" or "exact value" means no decimals anywhere: leave ln⁡3\ln 3, e−2e^{-2}, 3\sqrt{3}, π\pi in the answer. A correct decimal usually loses the final mark.
  • "Show that" questions give you the answer. Every step must be visible, including setting the derivative to zero and the rearrangement. The final line should match the printed result exactly.
  • For the nature of a stationary point, state the sign of the second derivative and the conclusion: "d2ydx2=−43<0\dfrac{d^2y}{dx^2} = -\tfrac{4}{3} < 0, so maximum." The conclusion without the evidence earns nothing.
  • When differentiation is the first part of a longer question (iteration, area, equation of a tangent), a wrong derivative costs you the whole question. Check it by substituting a value of xx and comparing with a quick numerical gradient on your calculator, if time allows.
Summary
  • The meaning of a derivative is unchanged; P3 adds exe^x, ln⁡x\ln x, all six trig functions and tan⁡−1x\tan^{-1}x.
  • The chain rule: differentiate the outside, keep the inside, multiply by the derivative of the inside. Peel layered composites one layer at a time.
  • Linear insides just multiply by aa: ddxeax+b=aeax+b\dfrac{d}{dx}e^{ax+b} = ae^{ax+b}, ddxln⁡(ax+b)=aax+b\dfrac{d}{dx}\ln(ax+b) = \dfrac{a}{ax+b}.
  • Identify the last operation to choose the rule: sum, product, quotient or composite.
  • Simplify first with log laws, indices and identities.
  • dydx=1/dxdy\dfrac{dy}{dx} = 1 \Big/ \dfrac{dx}{dy}.
  • Trig derivatives need radians.
  • Tangent y−y1=m(x−x1)y - y_1 = m(x - x_1); normal gradient −1/m-1/m; stationary points where dydx=0\dfrac{dy}{dx} = 0; nature from the sign of d2ydx2\dfrac{d^2y}{dx^2}.
  • Exact answers stay exact.

Practice

Question
  1. Differentiate (a) 4e−x/24e^{-x/2} (b) ln⁡(5−2x)\ln(5 - 2x) (c) cos⁡23x\cos^2 3x (d) tan⁡−1x3\tan^{-1}\dfrac{x}{3}.
  2. Given y=ln⁡(x32x−1)y = \ln\big(x^3\sqrt{2x - 1}\big), find dydx\dfrac{dy}{dx}.
  3. Find the exact gradient of y=e2xsin⁡xy = e^{2x}\sin x at the point where x=π4x = \tfrac{\pi}{4}.
  4. Find the equation of the normal to y=ln⁡(3x−2)y = \ln(3x - 2) at the point where x=1x = 1, and the point where it meets the yy-axis.
  5. Find the exact coordinates of the stationary point of y=xe−2xy = xe^{-2x} and determine its nature.
  6. Given x=y2+ln⁡yx = y^2 + \ln y for y>0y > 0, find dydx\dfrac{dy}{dx} in terms of yy, and its value when y=1y = 1.
  7. The curve y=e2x−6ex+4xy = e^{2x} - 6e^x + 4x has two stationary points. Find their exact coordinates and determine the nature of each.
  8. Find the exact xx-coordinates of the stationary points of y=(x+1)e−x2y = (x + 1)e^{-x^2}, and state, with a reason, which is a maximum.
  9. The curve y=exx2+1y = \dfrac{e^x}{x^2 + 1} is defined for all xx. Show that dydx≥0\dfrac{dy}{dx} \geq 0 for all xx, and find the coordinates of the point where the gradient is zero.
Answers
  1. (a) 4×(−12)e−x/2=−2e−x/24 \times \left(-\tfrac{1}{2}\right)e^{-x/2} = -2e^{-x/2}. (b) −25−2x\dfrac{-2}{5 - 2x}. (c) 2cos⁡3x×(−sin⁡3x)×3=−6sin⁡3xcos⁡3x2\cos 3x \times (-\sin 3x) \times 3 = -6\sin 3x\cos 3x, which is −3sin⁡6x-3\sin 6x. (d) 11+x2/9×13=39+x2\dfrac{1}{1 + x^2/9} \times \dfrac{1}{3} = \dfrac{3}{9 + x^2}.

  2. Simplify: y=3ln⁡x+12ln⁡(2x−1)y = 3\ln x + \tfrac{1}{2}\ln(2x - 1). Then dydx=3x+12⋅22x−1=3x+12x−1\dfrac{dy}{dx} = \dfrac{3}{x} + \dfrac{1}{2} \cdot \dfrac{2}{2x - 1} = \dfrac{3}{x} + \dfrac{1}{2x - 1}.

  3. dydx=2e2xsin⁡x+e2xcos⁡x=e2x(2sin⁡x+cos⁡x)\dfrac{dy}{dx} = 2e^{2x}\sin x + e^{2x}\cos x = e^{2x}(2\sin x + \cos x). At x=π4x = \tfrac{\pi}{4}: eπ/2(22+12)=32eπ/2=322eπ/2e^{\pi/2}\left(\tfrac{2}{\sqrt{2}} + \tfrac{1}{\sqrt{2}}\right) = \dfrac{3}{\sqrt{2}}e^{\pi/2} = \dfrac{3\sqrt{2}}{2}e^{\pi/2}.

  4. At x=1x = 1, y=ln⁡1=0y = \ln 1 = 0. dydx=33x−2=3\dfrac{dy}{dx} = \dfrac{3}{3x - 2} = 3 at x=1x = 1, so the normal gradient is −13-\tfrac{1}{3}. Normal: y=−13(x−1)y = -\tfrac{1}{3}(x - 1), i.e. x+3y=1x + 3y = 1. It meets the yy-axis at (0,13)\left(0, \tfrac{1}{3}\right).

  5. dydx=e−2x−2xe−2x=e−2x(1−2x)=0⇒x=12\dfrac{dy}{dx} = e^{-2x} - 2xe^{-2x} = e^{-2x}(1 - 2x) = 0 \Rightarrow x = \tfrac{1}{2}, y=12e−1y = \tfrac{1}{2}e^{-1}. d2ydx2=e−2x(4x−4)\dfrac{d^2y}{dx^2} = e^{-2x}(4x - 4), which at x=12x = \tfrac{1}{2} is −2e−1<0-2e^{-1} < 0: a maximum at (12,12e)\left(\tfrac{1}{2}, \tfrac{1}{2e}\right).

  6. dxdy=2y+1y=2y2+1y\dfrac{dx}{dy} = 2y + \dfrac{1}{y} = \dfrac{2y^2 + 1}{y}, so dydx=y2y2+1\dfrac{dy}{dx} = \dfrac{y}{2y^2 + 1}. At y=1y = 1: 13\tfrac{1}{3}.

  7. dydx=2e2x−6ex+4=2(ex−1)(ex−2)\dfrac{dy}{dx} = 2e^{2x} - 6e^x + 4 = 2(e^x - 1)(e^x - 2). Zero when ex=1e^x = 1 or ex=2e^x = 2: x=0x = 0 or x=ln⁡2x = \ln 2. Points (0,−5)(0, -5) and (ln⁡2, 4ln⁡2−8)(\ln 2,\ 4\ln 2 - 8). d2ydx2=4e2x−6ex\dfrac{d^2y}{dx^2} = 4e^{2x} - 6e^x: at x=0x = 0 it is −2<0-2 < 0 (maximum); at x=ln⁡2x = \ln 2 it is 16−12=4>016 - 12 = 4 > 0 (minimum).

  8. dydx=e−x2−2x(x+1)e−x2=e−x2(1−2x−2x2)\dfrac{dy}{dx} = e^{-x^2} - 2x(x + 1)e^{-x^2} = e^{-x^2}(1 - 2x - 2x^2). Since e−x2>0e^{-x^2} > 0, solve 2x2+2x−1=02x^2 + 2x - 1 = 0: x=−1±32x = \dfrac{-1 \pm \sqrt{3}}{2}. The quadratic 1−2x−2x21 - 2x - 2x^2 is positive between its roots and negative outside, so dydx\dfrac{dy}{dx} goes −,+,−-, +, -. Hence x=−1−32x = \dfrac{-1 - \sqrt{3}}{2} is a minimum and x=−1+32x = \dfrac{-1 + \sqrt{3}}{2} is a maximum (gradient changes from positive to negative).

  9. Quotient rule: dydx=(x2+1)ex−ex⋅2x(x2+1)2=ex(x−1)2(x2+1)2\dfrac{dy}{dx} = \dfrac{(x^2 + 1)e^x - e^x \cdot 2x}{(x^2 + 1)^2} = \dfrac{e^x(x - 1)^2}{(x^2 + 1)^2}. Every factor is non-negative, so dydx≥0\dfrac{dy}{dx} \geq 0 for all xx. It is zero only at x=1x = 1, giving the point (1,e2)\left(1, \tfrac{e}{2}\right). (This is a stationary point of inflexion: the gradient is positive on both sides.)

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