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Differentiation

Board Coverage

BoardPaperNotes
AQAPaper 1, 2First principles, rules, applications in P1; chain/product in P2
EdexcelP1, P2Similar split
OCR (A)Paper 1, 2Includes connected rates in P2
CIE (9709)P1, P2, P3Basic differentiation in P1; product/quotient/chain in P2/P3
info

The formula booklet lists derivatives of standard functions. You must know how to apply the product, quotient, and chain rules, and how to find stationary points.


1. The Derivative from First Principles

1.1 Definition

Definition. The derivative of ff at xx is

f(x)=limh0f(x+h)f(x)hf'(x) = \lim_{h\to 0}\frac{f(x+h)-f(x)}{h}

provided this limit exists. If it does, we say ff is differentiable at xx.

Geometric interpretation. The quantity f(x+h)f(x)h\dfrac{f(x+h)-f(x)}{h} is the gradient of the secant line through the points (x,f(x))(x, f(x)) and (x+h,f(x+h))(x+h, f(x+h)). As h0h \to 0, this secant approaches the tangent, so f(x)f'(x) is the gradient of the tangent at xx.

info

info there. Continuity is necessary but not sufficient — f(x)=xf(x) = |x| is continuous at x=0x=0 but not differentiable.


2. Derivative of xnx^n from First Principles

Theorem. For nNn \in \mathbb{N}, ddxxn=nxn1\dfrac{d}{dx}x^n = nx^{n-1}.

Proof. By the limit definition:

f(x)=limh0(x+h)nxnhf'(x) = \lim_{h\to 0}\frac{(x+h)^n - x^n}{h}

Expanding (x+h)n(x+h)^n using the binomial theorem:

(x+h)n=xn+(n1)xn1h+(n2)xn2h2++hn(x+h)^n = x^n + \binom{n}{1}x^{n-1}h + \binom{n}{2}x^{n-2}h^2 + \cdots + h^n

Subtracting xnx^n and dividing by hh:

(x+h)nxnh=(n1)xn1+(n2)xn2h++hn1\frac{(x+h)^n - x^n}{h} = \binom{n}{1}x^{n-1} + \binom{n}{2}x^{n-2}h + \cdots + h^{n-1}

Taking h0h \to 0, every term containing hh vanishes:

f(x)=(n1)xn1=nxn1f'(x) = \binom{n}{1}x^{n-1} = nx^{n-1} \quad \blacksquare

This proof extends to negative and fractional powers using the limit definition with the generalised binomial theorem or logarithmic differentiation.

Intuition. The power rule says: "bring the power down and reduce it by one." This works because the leading-order term in (x+h)nxn(x+h)^n - x^n is nxn1hnx^{n-1}h, and dividing by hh leaves nxn1nx^{n-1}.


3. The Product Rule

Theorem. If u=f(x)u = f(x) and v=g(x)v = g(x) are differentiable, then

ddx(uv)=udvdx+vdudx\frac{d}{dx}(uv) = u\frac{dv}{dx} + v\frac{du}{dx}

3.1 Proof from first principles

Let F(x)=f(x)g(x)F(x) = f(x)g(x). Then:

F(x)=limh0F(x+h)F(x)h=limh0f(x+h)g(x+h)f(x)g(x)h\begin{aligned} F'(x) &= \lim_{h\to 0}\frac{F(x+h)-F(x)}{h} \\ &= \lim_{h\to 0}\frac{f(x+h)g(x+h) - f(x)g(x)}{h} \end{aligned}

We add and subtract f(x+h)g(x)f(x+h)g(x):

=limh0f(x+h)g(x+h)f(x+h)g(x)+f(x+h)g(x)f(x)g(x)h= \lim_{h\to 0}\frac{f(x+h)g(x+h) - f(x+h)g(x) + f(x+h)g(x) - f(x)g(x)}{h}

=limh0[f(x+h)g(x+h)g(x)h+g(x)f(x+h)f(x)h]= \lim_{h\to 0}\left[f(x+h)\frac{g(x+h)-g(x)}{h} + g(x)\frac{f(x+h)-f(x)}{h}\right]

Since ff is differentiable (hence continuous), limh0f(x+h)=f(x)\lim_{h\to 0}f(x+h) = f(x):

=f(x)g(x)+g(x)f(x)= f(x) \cdot g'(x) + g(x) \cdot f'(x) \quad \blacksquare

Intuition. Think of the area of a rectangle with sides uu and vv. If uu changes by δu\delta u and vv by δv\delta v, the change in area is approximately vδu+uδvv\,\delta u + u\,\delta v (the two thin strips along the edges; the corner piece δuδv\delta u\,\delta v is negligible).


4. The Quotient Rule

Theorem. If u=f(x)u = f(x) and v=g(x)v = g(x) are differentiable with v0v \neq 0, then

ddx(uv)=LBvdudxudvdxRB◆◆LBv2RB\frac{d}{dx}\left(\frac{u}{v}\right) = \frac◆LB◆v\frac{du}{dx} - u\frac{dv}{dx}◆RB◆◆LB◆v^2◆RB◆

4.1 Proof from the product rule

Write uv=uv1\dfrac{u}{v} = u \cdot v^{-1}. Applying the product rule:

ddx(uv)=dudxv1+uddx(v1)\frac{d}{dx}\left(\frac{u}{v}\right) = \frac{du}{dx} \cdot v^{-1} + u \cdot \frac{d}{dx}(v^{-1})

By the chain rule, ddx(v1)=v2dvdx\dfrac{d}{dx}(v^{-1}) = -v^{-2}\dfrac{dv}{dx}:

=1vdudxuv2dvdx=LBvdudxudvdxRB◆◆LBv2RB= \frac{1}{v}\frac{du}{dx} - \frac{u}{v^2}\frac{dv}{dx} = \frac◆LB◆v\frac{du}{dx} - u\frac{dv}{dx}◆RB◆◆LB◆v^2◆RB◆ \quad \blacksquare

warning

The quotient rule has a minus sign in the numerator: vuuvv\,u' - u\,v'. Getting this the wrong way around is one of the most common errors in A Level mathematics.


5. The Chain Rule

Theorem. If y=f(g(x))y = f(g(x)), then

dydx=dydududx\frac{dy}{dx} = \frac{dy}{du} \cdot \frac{du}{dx}

where u=g(x)u = g(x).

5.1 Proof (informal)

If xx changes by δx\delta x, then uu changes by approximately g(x)δxg'(x)\,\delta x, and yy changes by approximately f(u)g(x)δxf'(u) \cdot g'(x)\,\delta x. Dividing by δx\delta x and taking the limit:

dydx=f(g(x))g(x)\frac{dy}{dx} = f'(g(x)) \cdot g'(x)

A fully rigorous proof uses the mean value theorem to handle the case when g(x)=0g'(x) = 0.

Intuition. The chain rule handles composite functions: "differentiate the outer function, then multiply by the derivative of the inner function." Think of it as a gearing mechanism: a small turn in xx causes a turn in uu, which causes a turn in yy, and the overall effect is the product of the two gear ratios.


6. Derivatives of Standard Functions

6.1 Derivative of sinx\sin x from first principles

Theorem. ddxsinx=cosx\dfrac{d}{dx}\sin x = \cos x.

Proof. Using the limit definition and the compound angle formula sin(α+β)=sinαcosβ+cosαsinβ\sin(\alpha + \beta) = \sin\alpha\cos\beta + \cos\alpha\sin\beta:

ddxsinx=limh0LBsin(x+h)sinxRB◆◆LBhRB=limh0LBsinxcosh+cosxsinhsinxRB◆◆LBhRB=limh0[sinxLBcosh1RB◆◆LBhRB+cosxLBsinhRB◆◆LBhRB]\begin{aligned} \frac{d}{dx}\sin x &= \lim_{h\to 0}\frac◆LB◆\sin(x+h) - \sin x◆RB◆◆LB◆h◆RB◆ \\ &= \lim_{h\to 0}\frac◆LB◆\sin x\cos h + \cos x\sin h - \sin x◆RB◆◆LB◆h◆RB◆ \\ &= \lim_{h\to 0}\left[\sin x \cdot \frac◆LB◆\cos h - 1◆RB◆◆LB◆h◆RB◆ + \cos x \cdot \frac◆LB◆\sin h◆RB◆◆LB◆h◆RB◆\right] \end{aligned}

Using the standard limits limh0LBsinhRB◆◆LBhRB=1\displaystyle\lim_{h\to 0}\frac◆LB◆\sin h◆RB◆◆LB◆h◆RB◆ = 1 and limh0LBcosh1RB◆◆LBhRB=0\displaystyle\lim_{h\to 0}\frac◆LB◆\cos h - 1◆RB◆◆LB◆h◆RB◆ = 0:

=sinx0+cosx1=cosx= \sin x \cdot 0 + \cos x \cdot 1 = \cos x \quad \blacksquare

6.2 Derivative of cosx\cos x

Theorem. ddxcosx=sinx\dfrac{d}{dx}\cos x = -\sin x.

Proof. Write cosx=sin ⁣(LBπRB◆◆LB2RBx)\cos x = \sin\!\left(\dfrac◆LB◆\pi◆RB◆◆LB◆2◆RB◆ - x\right). By the chain rule:

ddxcosx=cos ⁣(LBπRB◆◆LB2RBx)(1)=sinx\frac{d}{dx}\cos x = \cos\!\left(\frac◆LB◆\pi◆RB◆◆LB◆2◆RB◆-x\right) \cdot (-1) = -\sin x \quad \blacksquare

6.3 Derivative of exe^x

As proved in the Exponentials and Logarithms chapter: ddxex=ex\dfrac{d}{dx}e^x = e^x.

6.4 Derivative of lnx\ln x

From the Fundamental Theorem of Calculus applied to lnx=1x1tdt\ln x = \displaystyle\int_1^x \frac{1}{t}\,dt:

ddxlnx=1x\frac{d}{dx}\ln x = \frac{1}{x}

6.5 Derivative of tanx\tan x

ddxtanx=ddx(LBsinxRB◆◆LBcosxRB)=LBcosxcosxsinx(sinx)RB◆◆LBcos2xRB=LBcos2x+sin2xRB◆◆LBcos2xRB=sec2x\frac{d}{dx}\tan x = \frac{d}{dx}\left(\frac◆LB◆\sin x◆RB◆◆LB◆\cos x◆RB◆\right) = \frac◆LB◆\cos x \cdot \cos x - \sin x \cdot (-\sin x)◆RB◆◆LB◆\cos^2 x◆RB◆ = \frac◆LB◆\cos^2 x + \sin^2 x◆RB◆◆LB◆\cos^2 x◆RB◆ = \sec^2 x

6.6 Summary table

f(x)f(x)f(x)f'(x)
xnx^nnxn1nx^{n-1}
exe^xexe^x
ekxe^{kx}kekxke^{kx}
lnx\ln x1/x1/x
sinx\sin xcosx\cos x
cosx\cos xsinx-\sin x
tanx\tan xsec2x\sec^2 x

7. Second Derivatives and Stationary Points

7.1 Definition

The second derivative is the derivative of the first derivative:

f(x)=d2ydx2=ddx(dydx)f''(x) = \frac{d^2y}{dx^2} = \frac{d}{dx}\left(\frac{dy}{dx}\right)

7.2 Stationary points

Definition. A point x=ax = a is a stationary point of ff if f(a)=0f'(a) = 0.

There are three types:

TypeConditionShape
Maximumf(a)=0f'(a) = 0, f(a)<0f''(a) \lt{} 0\cap
Minimumf(a)=0f'(a) = 0, f(a)>0f''(a) \gt{} 0\cup
Point of inflectionf(a)=0f'(a) = 0, f(a)=0f''(a) = 0 (may be)S-shape

7.3 Proof of the second derivative test (Taylor expansion intuition)

Near a stationary point x=ax = a, we can approximate ff using its Taylor expansion:

f(x)f(a)+f(a)(xa)+f(a)2(xa)2f(x) \approx f(a) + f'(a)(x-a) + \frac{f''(a)}{2}(x-a)^2

Since f(a)=0f'(a) = 0 at a stationary point:

f(x)f(a)f(a)2(xa)2f(x) - f(a) \approx \frac{f''(a)}{2}(x-a)^2

  • If f(a)>0f''(a) \gt{} 0: f(x)f(a)>0f(x) - f(a) \gt{} 0 for xax \neq a, so f(a)f(a) is a minimum.
  • If f(a)<0f''(a) \lt{} 0: f(x)f(a)<0f(x) - f(a) \lt{} 0 for xax \neq a, so f(a)f(a) is a maximum.
  • If f(a)=0f''(a) = 0: the test is inconclusive; use a nature table or higher derivatives.
warning

warning point could still be a maximum, minimum, or inflection. Always use a nature table (checking the sign of ff' on either side) if the second derivative test is inconclusive.

Function, Derivative, and Tangent Line

Observe how the derivative relates to the gradient of the tangent line. Move the point along the curve to see how the tangent changes slope, and note where the derivative is zero at stationary points.


8. Connected Rates of Change

When two quantities are related by an equation, their rates of change are related by the chain rule.

Method:

  1. Write down the relationship between the variables.
  2. Differentiate both sides with respect to tt (time).
  3. Substitute known values and solve for the unknown rate.

Example. The radius rr of a circle increases at 2cm/s2\,\mathrm{cm/s}. Find the rate of change of the area when r=5r = 5.

A=πr2A = \pi r^2. Differentiating with respect to tt:

dAdt=2πrdrdt\frac{dA}{dt} = 2\pi r \frac{dr}{dt}

At r=5r = 5, drdt=2\dfrac{dr}{dt} = 2:

dAdt=2π(5)(2)=20πcm2/s\frac{dA}{dt} = 2\pi(5)(2) = 20\pi \,\mathrm{cm}^2\mathrm{/s}


9. Increasing and Decreasing Functions

Definition.

  • ff is increasing on an interval if f(x)0f'(x) \geq 0 for all xx in that interval.
  • ff is strictly increasing if f(x)>0f'(x) \gt{} 0 for all xx.
  • ff is decreasing if f(x)0f'(x) \leq 0 for all xx.
  • ff is strictly decreasing if f(x)<0f'(x) \lt{} 0 for all xx.

Example. Show that f(x)=x33x+2f(x) = x^3 - 3x + 2 is increasing for x>1x \gt{} 1.

f(x)=3x23=3(x21)=3(x1)(x+1)f'(x) = 3x^2 - 3 = 3(x^2 - 1) = 3(x-1)(x+1).

For x>1x \gt{} 1: (x1)>0(x-1) \gt{} 0 and (x+1)>0(x+1) \gt{} 0, so f(x)>0f'(x) \gt{} 0. Hence ff is strictly increasing for x>1x \gt{} 1.

tip

tip inequality. When asked to "show that a function is increasing", verify that f(x)>0f'(x) \gt{} 0 (or 0\geq 0) on the given interval.


10. Points of Inflection

A point of inflection is where the curve changes concavity (from concave up to concave down, or vice versa). This occurs where f(x)=0f''(x) = 0 and the sign of f(x)f''(x) changes.

warning

warning point of inflection at x=0x = 0, but f(0)=0f'(0) = 0 in this case. Consider f(x)=x3+xf(x) = x^3 + x: f(x)=6x=0f''(x) = 6x = 0 at x=0x = 0, giving a point of inflection, but f(0)=10f'(0) = 1 \neq 0.


11. Differentiation of Parametric Equations

If x=x(t)x = x(t) and y=y(t)y = y(t), then

dydx=dy/dtdx/dt\frac{dy}{dx} = \frac{dy/dt}{dx/dt}

Example. x=2costx = 2\cos t, y=2sinty = 2\sin t. Find dydx\dfrac{dy}{dx} at t=π/4t = \pi/4.

dxdt=2sint,dydt=2cost\frac{dx}{dt} = -2\sin t, \quad \frac{dy}{dt} = 2\cos t

dydx=LB2costRB◆◆LB2sintRB=cott\frac{dy}{dx} = \frac◆LB◆2\cos t◆RB◆◆LB◆-2\sin t◆RB◆ = -\cot t

At t=π/4t = \pi/4: dydx=cot(π/4)=1\dfrac{dy}{dx} = -\cot(\pi/4) = -1.


12. Implicit Differentiation

When yy is defined implicitly by an equation F(x,y)=0F(x,y) = 0, differentiate both sides with respect to xx, treating yy as a function of xx.

Example. Find dydx\dfrac{dy}{dx} where x2+y2=25x^2 + y^2 = 25.

Differentiating: 2x+2ydydx=02x + 2y\dfrac{dy}{dx} = 0, so dydx=xy\dfrac{dy}{dx} = -\dfrac{x}{y}.


Problem Set

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Problem 1 Differentiate f(x)=xf(x) = \sqrt{x} from first principles.

Details

Solution 1 f(x)=limh0LBx+hxRB◆◆LBhRBLBx+h+xRB◆◆LBx+h+xRB=limh0LB(x+h)xRB◆◆LBh(x+h+x)RB=limh0LB1RB◆◆LBx+h+xRB=LB1RB◆◆LB2xRBf'(x) = \lim_{h\to 0}\frac◆LB◆\sqrt{x+h}-\sqrt{x}◆RB◆◆LB◆h◆RB◆ \cdot \frac◆LB◆\sqrt{x+h}+\sqrt{x}◆RB◆◆LB◆\sqrt{x+h}+\sqrt{x}◆RB◆ = \lim_{h\to 0}\frac◆LB◆(x+h)-x◆RB◆◆LB◆h(\sqrt{x+h}+\sqrt{x})◆RB◆ = \lim_{h\to 0}\frac◆LB◆1◆RB◆◆LB◆\sqrt{x+h}+\sqrt{x}◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆2\sqrt{x}◆RB◆

If you get this wrong, revise: The Derivative from First Principles — Section 1.

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Problem 2 Find the stationary points of f(x)=x36x2+9x+1f(x) = x^3 - 6x^2 + 9x + 1 and determine their nature.

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Solution 2 f(x)=3x212x+9=3(x24x+3)=3(x1)(x3)f'(x) = 3x^2 - 12x + 9 = 3(x^2 - 4x + 3) = 3(x-1)(x-3).

Stationary points at x=1x = 1 and x=3x = 3.

f(x)=6x12f''(x) = 6x - 12. At x=1x = 1: f(1)=6<0f''(1) = -6 \lt{} 0, so local maximum. f(1)=16+9+1=5f(1) = 1 - 6 + 9 + 1 = 5. At x=3x = 3: f(3)=6>0f''(3) = 6 \gt{} 0, so local minimum. f(3)=2754+27+1=1f(3) = 27 - 54 + 27 + 1 = 1.

If you get this wrong, revise: Second Derivatives and Stationary Points — Section 7.

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Problem 3 Differentiate y=LBx2exRB◆◆LBsinxRBy = \dfrac◆LB◆x^2 e^x◆RB◆◆LB◆\sin x◆RB◆.

Details

Solution 3 Let u=x2exu = x^2 e^x and v=sinxv = \sin x.

u=2xex+x2ex=ex(x2+2x)u' = 2xe^x + x^2 e^x = e^x(x^2 + 2x) (product rule). v=cosxv' = \cos x.

dydx=LBex(x2+2x)sinxx2excosxRB◆◆LBsin2xRB=LBxex[(x+2)sinxxcosx]RB◆◆LBsin2xRB\frac{dy}{dx} = \frac◆LB◆e^x(x^2+2x)\sin x - x^2 e^x \cos x◆RB◆◆LB◆\sin^2 x◆RB◆ = \frac◆LB◆xe^x[(x+2)\sin x - x\cos x]◆RB◆◆LB◆\sin^2 x◆RB◆

If you get this wrong, revise: The Quotient Rule — Section 4 and The Product Rule — Section 3.

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Problem 4 Find dydx\dfrac{dy}{dx} where x3+y3=3xyx^3 + y^3 = 3xy.

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Solution 4 Differentiating implicitly: 3x2+3y2dydx=3y+3xdydx3x^2 + 3y^2\dfrac{dy}{dx} = 3y + 3x\dfrac{dy}{dx}.

3y2dydx3xdydx=3y3x23y^2\frac{dy}{dx} - 3x\frac{dy}{dx} = 3y - 3x^2 dydx(y2x)=yx2\frac{dy}{dx}(y^2 - x) = y - x^2 dydx=yx2y2x\frac{dy}{dx} = \frac{y - x^2}{y^2 - x}

If you get this wrong, revise: Implicit Differentiation — Section 12.

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Problem 5 A spherical balloon is being inflated at a rate of 100cm3/s100\,\mathrm{cm}^3\mathrm{/s}. Find the rate of increase of the radius when the radius is 5cm5\,\mathrm{cm}.

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Solution 5 V=43πr3V = \dfrac{4}{3}\pi r^3. Differentiating with respect to tt:

dVdt=4πr2drdt\frac{dV}{dt} = 4\pi r^2 \frac{dr}{dt}

At r=5r = 5 with dVdt=100\dfrac{dV}{dt} = 100:

100=4π(25)drdt    drdt=LB100RB◆◆LB100πRB=LB1RB◆◆LBπRB0.318cm/s100 = 4\pi(25)\frac{dr}{dt} \implies \frac{dr}{dt} = \frac◆LB◆100◆RB◆◆LB◆100\pi◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆\pi◆RB◆ \approx 0.318 \,\mathrm{cm/s}

If you get this wrong, revise: Connected Rates of Change — Section 8.

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Problem 6 Show that f(x)=ex+exf(x) = e^x + e^{-x} is strictly increasing for x>0x \gt{} 0.

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Solution 6 f(x)=exexf'(x) = e^x - e^{-x}.

For x>0x \gt{} 0: ex>1>exe^x \gt{} 1 \gt{} e^{-x}, so exex>0e^x - e^{-x} \gt{} 0. Hence f(x)>0f'(x) \gt{} 0 for all x>0x \gt{} 0, so ff is strictly increasing on (0,)(0, \infty).

If you get this wrong, revise: Increasing and Decreasing Functions — Section 9.

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Problem 7 Find the equation of the tangent to y=lnxy = \ln x at the point where x=ex = e.

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Solution 7 At x=ex = e: y=lne=1y = \ln e = 1. The point is (e,1)(e, 1).

dydx=1x\dfrac{dy}{dx} = \dfrac{1}{x}, so at x=ex = e: gradient m=1em = \dfrac{1}{e}.

y1=1e(xe)    y=xey - 1 = \frac{1}{e}(x - e) \implies y = \frac{x}{e}

If you get this wrong, revise: Derivatives of Standard Functions — Section 6.

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Problem 8 Given x=t2+1x = t^2 + 1 and y=t33ty = t^3 - 3t, find the coordinates of the stationary points and determine their nature.

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Solution 8 dydx=dy/dtdx/dt=3t232t=3(t21)2t\dfrac{dy}{dx} = \dfrac{dy/dt}{dx/dt} = \dfrac{3t^2 - 3}{2t} = \dfrac{3(t^2-1)}{2t}.

Stationary when dy/dx=0dy/dx = 0: t2=1    t=±1t^2 = 1 \implies t = \pm 1.

t=1t = 1: x=2x = 2, y=2y = -2. Point (2,2)(2, -2). t=1t = -1: x=2x = 2, y=2y = 2. Point (2,2)(2, 2).

For nature, check d2ydx2\dfrac{d^2y}{dx^2} or the sign of dydx\dfrac{dy}{dx}:

Near t=1t = 1: for t=0.5t = 0.5, dydx=3(0.251)1=94<0\dfrac{dy}{dx} = \dfrac{3(0.25-1)}{1} = -\dfrac{9}{4} \lt{} 0; for t=2t = 2, dydx=3(41)4>0\dfrac{dy}{dx} = \dfrac{3(4-1)}{4} \gt{} 0. So t=1t=1 is a minimum.

Near t=1t = -1: for t=2t = -2, dydx<0\dfrac{dy}{dx} \lt{} 0; for t=0.5t = -0.5, dydx>0\dfrac{dy}{dx} \gt{} 0. So t=1t=-1 is a minimum.

If you get this wrong, revise: Differentiation of Parametric Equations — Section 11.

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Problem 9 Prove that ddxsecx=secxtanx\dfrac{d}{dx}\sec x = \sec x \tan x.

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Solution 9 secx=LB1RB◆◆LBcosxRB=(cosx)1\sec x = \dfrac◆LB◆1◆RB◆◆LB◆\cos x◆RB◆ = (\cos x)^{-1}.

ddxsecx=(cosx)2(sinx)=LBsinxRB◆◆LBcos2xRB=LB1RB◆◆LBcosxRBLBsinxRB◆◆LBcosxRB=secxtanx\frac{d}{dx}\sec x = -(\cos x)^{-2} \cdot (-\sin x) = \frac◆LB◆\sin x◆RB◆◆LB◆\cos^2 x◆RB◆ = \frac◆LB◆1◆RB◆◆LB◆\cos x◆RB◆ \cdot \frac◆LB◆\sin x◆RB◆◆LB◆\cos x◆RB◆ = \sec x \tan x \quad \blacksquare

If you get this wrong, revise: The Chain Rule — Section 5.

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Problem 10 Find the minimum value of f(x)=x+4xf(x) = x + \dfrac{4}{x} for x>0x \gt{} 0.

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Solution 10 f(x)=14x2=x24x2=0    x2=4    x=2f'(x) = 1 - \dfrac{4}{x^2} = \dfrac{x^2 - 4}{x^2} = 0 \implies x^2 = 4 \implies x = 2 (since x>0x \gt{} 0).

f(x)=8x3f''(x) = \dfrac{8}{x^3}. At x=2x = 2: f(2)=1>0f''(2) = 1 \gt{} 0, so minimum.

f(2)=2+42=4f(2) = 2 + \dfrac{4}{2} = 4.

If you get this wrong, revise: Second Derivatives and Stationary Points — Section 7.

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Problem 11 Differentiate y=sin3(2x2+1)y = \sin^3(2x^2 + 1).

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Solution 11 Let u=sin(2x2+1)u = \sin(2x^2+1), so y=u3y = u^3.

dydu=3u2\dfrac{dy}{du} = 3u^2, dudx=cos(2x2+1)4x\dfrac{du}{dx} = \cos(2x^2+1) \cdot 4x.

dydx=3sin2(2x2+1)cos(2x2+1)4x=12xsin2(2x2+1)cos(2x2+1)\frac{dy}{dx} = 3\sin^2(2x^2+1) \cdot \cos(2x^2+1) \cdot 4x = 12x\sin^2(2x^2+1)\cos(2x^2+1)

If you get this wrong, revise: The Chain Rule — Section 5.

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Problem 12 Find the points of inflection of f(x)=x44x3+6x24x+1f(x) = x^4 - 4x^3 + 6x^2 - 4x + 1.

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Solution 12 f(x)=4x312x2+12x4f'(x) = 4x^3 - 12x^2 + 12x - 4. f(x)=12x224x+12=12(x22x+1)=12(x1)2f''(x) = 12x^2 - 24x + 12 = 12(x^2 - 2x + 1) = 12(x-1)^2.

f(x)=0f''(x) = 0 when x=1x = 1. But f(x)=12(x1)20f''(x) = 12(x-1)^2 \geq 0 for all xx — the second derivative does not change sign at x=1x = 1. So there is no point of inflection.

(Note: f(x)=(x1)4f(x) = (x-1)^4, which is concave up everywhere.)

If you get this wrong, revise: Points of Inflection — Section 10.

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Problem 13 A curve has equation y=2x+1x3y = \dfrac{2x+1}{x-3}. Find the equations of the asymptotes and the coordinates of any stationary points.

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Solution 13 Vertical asymptote: x=3x = 3 (where denominator is zero).

As x±x \to \pm\infty: y2y \to 2. Horizontal asymptote: y=2y = 2.

y=2(x3)(2x+1)(x3)2=7(x3)2y' = \dfrac{2(x-3) - (2x+1)}{(x-3)^2} = \dfrac{-7}{(x-3)^2}.

Since y<0y' \lt{} 0 for all x3x \neq 3, there are no stationary points. The function is strictly decreasing on each branch.

If you get this wrong, revise: The Quotient Rule — Section 4 and Stationary Points — Section 7.2.

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Problem 14 Water flows into a cone of height hh and base radius rr at a rate of 5cm3/s5\,\mathrm{cm}^3\mathrm{/s}. The cone has semi-vertical angle 3030^\circ. Find dh/dtdh/dt when h=10cmh = 10\,\mathrm{cm}.

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Solution 14 With semi-vertical angle 3030^\circ: r=htan30°=h/3r = h\tan 30° = h/\sqrt{3}.

V=13πr2h=13πh23h=LBπh3RB◆◆LB9RBV = \dfrac{1}{3}\pi r^2 h = \dfrac{1}{3}\pi \dfrac{h^2}{3} h = \dfrac◆LB◆\pi h^3◆RB◆◆LB◆9◆RB◆.

dVdt=LBπh2RB◆◆LB3RBdhdt\frac{dV}{dt} = \frac◆LB◆\pi h^2◆RB◆◆LB◆3◆RB◆ \cdot \frac{dh}{dt}

At h=10h = 10 with dV/dt=5dV/dt = 5:

5=LB100πRB◆◆LB3RBdhdt    dhdt=LB15RB◆◆LB100πRB=LB3RB◆◆LB20πRB0.0478cm/s5 = \frac◆LB◆100\pi◆RB◆◆LB◆3◆RB◆ \cdot \frac{dh}{dt} \implies \frac{dh}{dt} = \frac◆LB◆15◆RB◆◆LB◆100\pi◆RB◆ = \frac◆LB◆3◆RB◆◆LB◆20\pi◆RB◆ \approx 0.0478 \,\mathrm{cm/s}

If you get this wrong, revise: Connected Rates of Change — Section 8.

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