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IB Math AA HL Calculus: Complete Guide 2026 (Limits, Derivatives, Integration)

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Quick Reference:

  • Syllabus Topics: SL 5.1–5.11 limits, derivatives, integrals · AHL 5.12–5.19 continuity, implicit differentiation, differential equations, Maclaurin series
  • Paper 1: 2 h, no calculator, show working (30%).
  • Paper 2: 2 h, GDC required, not every question (30%).
  • Paper 3: 1 h, two problem-solving questions (20%).
Topic 5 code details
  • SL 5.1 Limits; derivative as a gradient and a rate of change
  • SL 5.2 Increasing and decreasing functions
  • SL 5.3 Derivatives of integer powers
  • SL 5.4 Tangents and normals
  • SL 5.5 Anti-differentiation, definite integrals using technology, area under a curve
  • SL 5.6 Standard derivatives; chain, product and quotient rules
  • SL 5.7 Second derivative; graphs of f, f’ and f”
  • SL 5.8 Local maxima and minima, optimisation, points of inflexion
  • SL 5.9 Kinematics
  • SL 5.10 Standard integrals and the reverse chain rule
  • SL 5.11 Definite integrals and areas between curves
  • AHL 5.12 Continuity, differentiability, limits, first principles, higher derivatives
  • AHL 5.13 Limits by l’Hôpital’s rule or Maclaurin series
  • AHL 5.14 Implicit differentiation, related rates, optimisation
  • AHL 5.15 Derivatives of tan, sec, cosec, cot, exponential, log and inverse trig; partial fractions
  • AHL 5.16 Integration by substitution and by parts
  • AHL 5.17 Area with the y-axis and volumes of revolution
  • AHL 5.18 First-order differential equations
  • AHL 5.19 Maclaurin series

IB Math AA HL — Calculus

Complete Study Guide

Topics Covered

  1. Limits & Continuity
  2. Differentiation — Rules & Techniques
  3. Applications of Differentiation (optimisation, related rates, kinematics)
  4. Integration — Techniques & Standard Integrals
  5. Applications of Integration (areas, volumes of revolution)
  6. Differential Equations
  7. Maclaurin Series
  8. Practice MCQs & Exam Alerts

Topic 5 of the IB Math AA HL syllabus — Papers 1, 2 and 3

Videos on this page: Differentiation · Integration


Watch: Differentiation — Chain, Product, Quotient Rules & Applications

IB Maths Resources · Differentiation rules (chain, product, quotient), optimisation, implicit differentiation, rates of change, and equation of tangents

Watch: Integration — Techniques, Areas, Volumes & Substitutions

IB Maths Resources · Integration rules, definite integrals, areas between curves, volumes of revolution, trig substitutions, integration by parts, and u-substitutions

How to approach calculus on exams: The IB rewards structured method. Even if your final answer is wrong, showing correct working earns method marks. Always write the rule or theorem you are applying before you apply it, and show every intermediate line. A one-line answer — even if numerically correct — can score zero if no method is visible.

Prerequisites: Calculus builds on functions, algebra, and trigonometry. If you’re struggling with function notation, exponents, or trig identities, review the Functions and Geometry & Trigonometry guides first.

What is and is not in the formula booklet: Derivatives of sin⁡x\sin x, cos⁡x\cos x, exe^x, ln⁡x\ln x, and xnx^n are given. The product rule, quotient rule, and chain rule are given. Standard integrals (including ∫1x dx\int \frac{1}{x}\,dx, ∫ex dx\int e^x\,dx, ∫sin⁡x dx\int \sin x\,dx, ∫cos⁡x dx\int \cos x\,dx) are given. The integration by parts formula is given. NOT given: L’Hôpital’s rule, the formula for volumes of revolution, the Maclaurin series of exe^x, sin⁡x\sin x, cos⁡x\cos x, and ln⁡(1+x)\ln(1+x) (you must know how to derive them), and all kinematics interpretations.


Section 1: Limits and Continuity

A limit describes the value a function approaches as the input approaches some value, without necessarily reaching it. The notation lim⁡x→af(x)=L\displaystyle\lim_{x \to a} f(x) = L means “as xx gets arbitrarily close to aa (from either side), f(x)f(x) gets arbitrarily close to LL.” Limits are the rigorous foundation for both derivatives (limit of a difference quotient) and integrals (limit of a Riemann sum).

Formula booklet entries for this section: L’Hôpital’s rule is NOT in the booklet — you must state it explicitly when using it. The definition of the derivative as a limit IS given.

1.1 Evaluating Limits

Direct substitution works whenever ff is continuous at aa:

lim⁡x→af(x)=f(a)(if f is continuous at a)\lim_{x \to a} f(x) = f(a) \qquad \text{(if } f \text{ is continuous at } a\text{)}

When direct substitution gives 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} (an indeterminate form), use one of three strategies:

StrategyWhen to useMethod
FactoringRational functions, 00\frac{0}{0}Factor numerator and denominator, cancel common factor
RationalisingSquare roots, 00\frac{0}{0}Multiply by conjugate over conjugate
L’Hôpital’s rule00\frac{0}{0} or ∞∞\frac{\infty}{\infty}Differentiate top and bottom separately, then substitute

One-sided limits: lim⁡x→a−f(x)\displaystyle\lim_{x \to a^-} f(x) (approach from the left) and lim⁡x→a+f(x)\displaystyle\lim_{x \to a^+} f(x) (from the right). The two-sided limit exists if and only if both one-sided limits exist and are equal.

Infinite limits and limits at infinity:

lim⁡x→∞p(x)q(x)={leading coeff of pleading coeff of qdeg⁡p=deg⁡q0deg⁡p<deg⁡q±∞deg⁡p>deg⁡q\lim_{x \to \infty} \frac{p(x)}{q(x)} = \begin{cases} \dfrac{\text{leading coeff of } p}{\text{leading coeff of } q} & \deg p = \deg q \\[6pt] 0 & \deg p < \deg q \\[6pt] \pm\infty & \deg p > \deg q \end{cases}

Limits by factoring

Evaluate lim⁡x→3x2−9x−3\displaystyle\lim_{x \to 3} \dfrac{x^2 - 9}{x - 3}.

Step 1: Direct substitution gives 9−93−3=00\frac{9-9}{3-3} = \frac{0}{0} — indeterminate form.

Step 2: Factor the numerator: x2−9=(x−3)(x+3)x^2 - 9 = (x-3)(x+3).

Step 3: Cancel: (x−3)(x+3)x−3=x+3\dfrac{(x-3)(x+3)}{x-3} = x + 3 for x≠3x \neq 3.

Step 4: Substitute: lim⁡x→3(x+3)=6\displaystyle\lim_{x \to 3}(x+3) = 6

lim⁡x→3x2−9x−3=6\lim_{x \to 3} \frac{x^2 - 9}{x - 3} = 6

1.2 L’Hôpital’s Rule HL

Sometimes when you plug a value into a fraction, you get 00\frac{0}{0} or ∞∞\frac{\infty}{\infty} — which tells you nothing about the limit. L’Hôpital’s Rule gives you a way out: instead of the original fraction, take the derivative of the top and bottom separately, then try the limit again.

If lim⁡x→af(x)=lim⁡x→ag(x)=0\displaystyle\lim_{x \to a} f(x) = \lim_{x \to a} g(x) = 0 or both equal ±∞\pm\infty, then:

lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x)\lim_{x \to a} \frac{f(x)}{g(x)} = \lim_{x \to a} \frac{f'(x)}{g'(x)}

provided the right-hand limit exists. You may apply L’Hôpital’s rule repeatedly until the indeterminate form resolves.

L’Hôpital’s rule applies only when the limit is in the form 00\frac{0}{0} or ∞∞\frac{\infty}{\infty}. If the form is 30\frac{3}{0}, the limit is ±∞\pm\infty (or does not exist) — L’Hôpital’s rule does NOT apply. Always verify the form before using it.

L’Hôpital’s Rule

Evaluate lim⁡x→0sin⁡xx\displaystyle\lim_{x \to 0} \dfrac{\sin x}{x}.

Step 1: Direct substitution: sin⁡00=00\frac{\sin 0}{0} = \frac{0}{0} — L’Hôpital applies.

Step 2: Differentiate numerator and denominator separately:

lim⁡x→0sin⁡xx=lim⁡x→0cos⁡x1=cos⁡0=1\lim_{x \to 0} \frac{\sin x}{x} = \lim_{x \to 0} \frac{\cos x}{1} = \cos 0 = 1

This fundamental limit appears inside proofs of derivative formulas, so knowing the result lim⁡x→0sin⁡xx=1\displaystyle\lim_{x \to 0}\frac{\sin x}{x} = 1 by heart saves time.

Repeated L’Hôpital

Evaluate lim⁡x→0ex−1−xx2\displaystyle\lim_{x \to 0} \dfrac{e^x - 1 - x}{x^2}.

Step 1: e0−1−00=00\frac{e^0 - 1 - 0}{0} = \frac{0}{0} — apply L’Hôpital.

Step 2: lim⁡x→0ex−12x\displaystyle\lim_{x \to 0} \frac{e^x - 1}{2x} — still 00\frac{0}{0}, apply again.

Step 3: lim⁡x→0ex2=12\displaystyle\lim_{x \to 0} \frac{e^x}{2} = \frac{1}{2}

1.3 Continuity

Continuity captures the idea that you can draw a function’s graph without lifting your pen — no jumps, holes, or sudden breaks. It matters because many important theorems (like the Intermediate Value Theorem) only work when a function is continuous.

A function ff is continuous at x=ax = a if all three conditions hold:

  1. f(a)f(a) is defined
  2. lim⁡x→af(x)\displaystyle\lim_{x \to a} f(x) exists (both one-sided limits are equal)
  3. lim⁡x→af(x)=f(a)\displaystyle\lim_{x \to a} f(x) = f(a)

Types of discontinuity:

TypeDescriptionExample
RemovableLimit exists, but f(a)f(a) is missing or wrongf(x)=x2−1x−1f(x) = \frac{x^2-1}{x-1} at x=1x=1
JumpOne-sided limits exist but differPiecewise function with gap
InfiniteLimit is ±∞\pm\inftyf(x)=1xf(x) = \frac{1}{x} at x=0x=0

Intermediate Value Theorem (IVT): If ff is continuous on [a,b][a, b] and kk is any value strictly between f(a)f(a) and f(b)f(b), then there exists at least one c∈(a,b)c \in (a, b) with f(c)=kf(c) = k. This is used to prove roots exist.

The IVT proves existence — it tells you a root exists, not where it is. To show a root of ff exists on (a,b)(a, b), show f(a)f(a) and f(b)f(b) have opposite signs and state that ff is continuous on [a,b][a, b].

Quick Recall — Section 1

Try to answer without scrolling up:

  1. What does lim⁡x→af(x)=L\lim_{x \to a} f(x) = L mean informally?
  2. State L’Hopital’s rule.
  3. What does the Intermediate Value Theorem guarantee?
Reveal answers
  1. As xx gets arbitrarily close to aa, f(x)f(x) gets arbitrarily close to LL.
  2. If lim⁡x→af(x)/g(x)\lim_{x \to a} f(x)/g(x) gives 0/00/0 or ∞/∞\infty/\infty, then lim⁡x→af(x)/g(x)=lim⁡x→af′(x)/g′(x)\lim_{x \to a} f(x)/g(x) = \lim_{x \to a} f'(x)/g'(x) (provided the latter limit exists).
  3. If ff is continuous on [a,b][a, b] and f(a)f(a) and f(b)f(b) have opposite signs, then there exists at least one cc in (a,b)(a, b) where f(c)=0f(c) = 0.

Section 2: Differentiation

The derivative of ff at xx measures the instantaneous rate of change — equivalently, the gradient of the tangent to y=f(x)y = f(x) at that point. It is defined as a limit:

f′(x)=lim⁡h→0f(x+h)−f(x)hf'(x) = \lim_{h \to 0} \frac{f(x+h) - f(x)}{h}

This is called differentiation from first principles.

2.1 First Principles

Derivative of f(x)=x2f(x) = x^2 from first principles

Step 1: Write the difference quotient:

f(x+h)−f(x)h=(x+h)2−x2h\frac{f(x+h) - f(x)}{h} = \frac{(x+h)^2 - x^2}{h}

Step 2: Expand: =x2+2xh+h2−x2h=2xh+h2h=2x+h= \dfrac{x^2 + 2xh + h^2 - x^2}{h} = \dfrac{2xh + h^2}{h} = 2x + h

Step 3: Take the limit: f′(x)=lim⁡h→0(2x+h)=2xf'(x) = \displaystyle\lim_{h \to 0}(2x + h) = 2x

In Paper 1 questions asking for first principles, you must write the limit definition with lim⁡h→0\lim_{h \to 0}, expand fully, cancel hh from numerator and denominator, and then substitute h=0h = 0. Skipping any step loses marks. The expression f(x+h)−f(x)h\frac{f(x+h)-f(x)}{h} must appear explicitly.

2.2 Standard Derivatives

Standard Derivative Table

Function f(x)f(x)Derivative f′(x)f'(x)Notes
xnx^nnxn−1nx^{n-1}All real nn, including fractions and negatives
exe^xexe^xUnique self-derivative
ekxe^{kx}kekxke^{kx}Chain rule applied
axa^xaxln⁡aa^x \ln aa>0a > 0, a≠1a \neq 1
ln⁡x\ln x1x\dfrac{1}{x}x>0x > 0
ln⁡∣x∣\ln\lvert x\rvert1x\dfrac{1}{x}All x≠0x \neq 0
log⁡ax\log_a x1xln⁡a\dfrac{1}{x \ln a}Change of base
sin⁡x\sin xcos⁡x\cos xRadians only
cos⁡x\cos x−sin⁡x-\sin xNote the minus sign
tan⁡x\tan xsec⁡2x\sec^2 xMemorise
sec⁡x\sec xsec⁡xtan⁡x\sec x \tan xMemorise
csc⁡x\csc x−csc⁡xcot⁡x-\csc x \cot xMemorise
cot⁡x\cot x−csc⁡2x-\csc^2 xMemorise
arcsin⁡x\arcsin x11−x2\dfrac{1}{\sqrt{1-x^2}}∣x∣<1\lvert x\rvert < 1
arccos⁡x\arccos x−11−x2-\dfrac{1}{\sqrt{1-x^2}}∣x∣<1\lvert x\rvert < 1
arctan⁡x\arctan x11+x2\dfrac{1}{1+x^2}All real xx

ddx(cos⁡x)=−sin⁡x\frac{d}{dx}(\cos x) = -\sin x, NOT +sin⁡x+\sin x. This sign error is one of the most common on IB Paper 1. Write it out explicitly every time until it is automatic.

2.3 The Three Combination Rules

Most functions you encounter are combinations of simpler pieces — two things multiplied, one divided by another, or one function plugged inside another. The three rules below tell you how to differentiate each of these combinations without expanding everything out first.

Power Rule (already covered above): ddx[xn]=nxn−1\frac{d}{dx}[x^n] = nx^{n-1}

Product Rule: For y=u(x)⋅v(x)y = u(x) \cdot v(x):

dydx=u′v+uv′\frac{dy}{dx} = u'v + uv'

Quotient Rule: For y=u(x)v(x)y = \dfrac{u(x)}{v(x)}:

dydx=u′v−uv′v2\frac{dy}{dx} = \frac{u'v - uv'}{v^2}

Chain Rule: For y=f(g(x))y = f(g(x)):

dydx=f′(g(x))⋅g′(x)or equivalentlydydx=dydu⋅dudx\frac{dy}{dx} = f'(g(x)) \cdot g'(x) \qquad \text{or equivalently} \qquad \frac{dy}{dx} = \frac{dy}{du} \cdot \frac{du}{dx}

Quotient rule: the numerator is u′v−uv′u'v - uv' (top derivative first, then bottom derivative). The order is not interchangeable — uv′−u′vuv' - u'v gives the wrong sign. A memory aid: “low d-high minus high d-low, square the bottom and away you go.”

Product Rule

Differentiate y=x3e2xy = x^3 e^{2x}.

Let u=x3u = x^3, v=e2xv = e^{2x}, so u′=3x2u' = 3x^2, v′=2e2xv' = 2e^{2x}.

dydx=3x2⋅e2x+x3⋅2e2x=e2x(3x2+2x3)=x2e2x(3+2x)\frac{dy}{dx} = 3x^2 \cdot e^{2x} + x^3 \cdot 2e^{2x} = e^{2x}(3x^2 + 2x^3) = x^2 e^{2x}(3 + 2x)

Always factorise the final answer — IB mark schemes expect a simplified form.

Quotient Rule

Differentiate y=sin⁡xx2+1y = \dfrac{\sin x}{x^2 + 1}.

u=sin⁡xu = \sin x, v=x2+1v = x^2 + 1, u′=cos⁡xu' = \cos x, v′=2xv' = 2x.

dydx=cos⁡x(x2+1)−sin⁡x⋅2x(x2+1)2=(x2+1)cos⁡x−2xsin⁡x(x2+1)2\frac{dy}{dx} = \frac{\cos x (x^2+1) - \sin x \cdot 2x}{(x^2+1)^2} = \frac{(x^2+1)\cos x - 2x\sin x}{(x^2+1)^2}

Chain Rule

Differentiate y=sin⁡(x3+2x)y = \sin(x^3 + 2x).

Let u=x3+2xu = x^3 + 2x, so y=sin⁡uy = \sin u.

dydx=cos⁡u⋅dudx=cos⁡(x3+2x)⋅(3x2+2)\frac{dy}{dx} = \cos u \cdot \frac{du}{dx} = \cos(x^3+2x) \cdot (3x^2 + 2)

Nested Chain Rule

Differentiate y=esin⁡(2x)y = e^{\sin(2x)}.

Layer 1 (outermost): ddu(eu)=eu\frac{d}{du}(e^u) = e^u where u=sin⁡(2x)u = \sin(2x)

Layer 2: ddv(sin⁡v)=cos⁡v\frac{d}{dv}(\sin v) = \cos v where v=2xv = 2x

Layer 3: ddx(2x)=2\frac{d}{dx}(2x) = 2

dydx=esin⁡(2x)⋅cos⁡(2x)⋅2=2cos⁡(2x) esin⁡(2x)\frac{dy}{dx} = e^{\sin(2x)} \cdot \cos(2x) \cdot 2 = 2\cos(2x)\,e^{\sin(2x)}

2.4 Implicit Differentiation

Sometimes a curve is defined by an equation like x2+y2=25x^2 + y^2 = 25 where you can’t easily isolate yy — both variables are tangled together. Implicit differentiation lets you find the gradient anyway by differentiating both sides of the equation at once, without rearranging first.

When yy is defined implicitly by an equation in xx and yy, differentiate both sides with respect to xx, treating yy as a function of xx. Every time yy is differentiated, multiply by dydx\dfrac{dy}{dx} (chain rule).

ddx[yn]=nyn−1dydxddx[sin⁡y]=cos⁡y⋅dydx\frac{d}{dx}[y^n] = ny^{n-1}\frac{dy}{dx} \qquad \frac{d}{dx}[\sin y] = \cos y \cdot \frac{dy}{dx}

Implicit Differentiation

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

Step 1: Differentiate both sides w.r.t. xx:

2x+2ydydx=02x + 2y\frac{dy}{dx} = 0

Step 2: Solve for dydx\frac{dy}{dx}:

dydx=−xy\frac{dy}{dx} = -\frac{x}{y}

This is the gradient at any point (x,y)(x, y) on the circle. At (3,4)(3, 4): dydx=−34\frac{dy}{dx} = -\frac{3}{4}.

Implicit Differentiation — Product Term

Find dydx\dfrac{dy}{dx} for x2y+y3=5x^2 y + y^3 = 5.

Differentiate each term:

  • ddx(x2y)=2xy+x2dydx\frac{d}{dx}(x^2 y) = 2xy + x^2\frac{dy}{dx} (product rule)
  • ddx(y3)=3y2dydx\frac{d}{dx}(y^3) = 3y^2\frac{dy}{dx}
  • ddx(5)=0\frac{d}{dx}(5) = 0

Collect dydx\frac{dy}{dx} terms:

2xy+x2dydx+3y2dydx=02xy + x^2\frac{dy}{dx} + 3y^2\frac{dy}{dx} = 0

dydx(x2+3y2)=−2xy\frac{dy}{dx}(x^2 + 3y^2) = -2xy

dydx=−2xyx2+3y2\frac{dy}{dx} = \frac{-2xy}{x^2 + 3y^2}

When differentiating a product like xyxy implicitly, the product rule gives TWO terms: ddx(xy)=y+xdydx\frac{d}{dx}(xy) = y + x\frac{dy}{dx}. Students frequently write just xdydxx\frac{dy}{dx} and lose the yy term.

2.5 Derivatives of Inverse Trigonometric Functions

Inverse trig functions like arctan⁡x\arctan x and arcsin⁡x\arcsin x appear frequently in integration and in problems involving angles. Their derivatives look surprising at first, but each one can be derived using implicit differentiation — and they are worth knowing because they appear often as antiderivatives.

These arise from implicit differentiation of the definitions:

ddx[arcsin⁡x]=11−x2ddx[arctan⁡x]=11+x2\frac{d}{dx}[\arcsin x] = \frac{1}{\sqrt{1-x^2}} \qquad \frac{d}{dx}[\arctan x] = \frac{1}{1+x^2}

With chain rule:

ddx[arctan⁡(g(x))]=g′(x)1+[g(x)]2\frac{d}{dx}[\arctan(g(x))] = \frac{g'(x)}{1 + [g(x)]^2}

Inverse Trig with Chain Rule

Differentiate y=arctan⁡(e2x)y = \arctan(e^{2x}).

Outer function: arctan⁡(u)\arctan(u) where u=e2xu = e^{2x} (inner function).

Apply the derivative formula for arctan⁡\arctan:

dydx=11+(e2x)2⋅ddx[e2x]\frac{dy}{dx} = \frac{1}{1 + (e^{2x})^2} \cdot \frac{d}{dx}[e^{2x}]

Differentiate the inner function using chain rule on the exponential:

ddx[e2x]=e2x⋅2=2e2x\frac{d}{dx}[e^{2x}] = e^{2x} \cdot 2 = 2e^{2x}

Combine:

dydx=2e2x1+e4x\frac{dy}{dx} = \frac{2e^{2x}}{1 + e^{4x}}

This pattern appears frequently in Paper 2 when combining transcendental functions. A common error is forgetting to square the entire inner function in the denominator — it’s 1+(e2x)2=1+e4x1 + (e^{2x})^2 = 1 + e^{4x}, not 1+e2x1 + e^{2x}.

Quick Recall — Section 2

Try to answer without scrolling up:

  1. State the chain rule for ddx[f(g(x))]\frac{d}{dx}[f(g(x))].
  2. What is ddx[ln⁡x]\frac{d}{dx}[\ln x]?
  3. When do you use implicit differentiation?
Reveal answers
  1. f′(g(x))⋅g′(x)f'(g(x)) \cdot g'(x) — differentiate the outer function, keep the inner, multiply by the derivative of the inner.
  2. 1x\frac{1}{x}.
  3. When yy is defined implicitly as a function of xx (not isolated), or when differentiating equations like x2+y2=r2x^2 + y^2 = r^2.

Section 3: Applications of Differentiation

3.1 Tangent and Normal Lines

At the point (a,f(a))(a, f(a)) on y=f(x)y = f(x):

  • Tangent gradient: mT=f′(a)m_T = f'(a)
  • Normal gradient: mN=−1f′(a)m_N = -\dfrac{1}{f'(a)} (negative reciprocal, since tangent ⊥\perp normal)
  • Tangent equation: y−f(a)=f′(a)(x−a)y - f(a) = f'(a)(x - a)
  • Normal equation: y−f(a)=−1f′(a)(x−a)y - f(a) = -\dfrac{1}{f'(a)}(x - a)

If f′(a)=0f'(a) = 0 (horizontal tangent), the normal is a vertical line x=ax = a — it has no finite gradient. If f′(a)f'(a) is undefined (vertical tangent), the tangent is x=ax = a and the normal is horizontal with gradient 0. Never write the normal as y=10x+cy = \frac{1}{0}x + c.

Tangent and Normal

Find the equations of the tangent and normal to y=x3−2xy = x^3 - 2x at the point where x=2x = 2.

Step 1: y(2)=8−4=4y(2) = 8 - 4 = 4 so the point is (2,4)(2, 4).

Step 2: y′=3x2−2y' = 3x^2 - 2, so mT=3(4)−2=10m_T = 3(4) - 2 = 10.

Step 3: Tangent: y−4=10(x−2)⇒y=10x−16y - 4 = 10(x - 2) \Rightarrow y = 10x - 16

Step 4: Normal: mN=−110m_N = -\frac{1}{10}, so y−4=−110(x−2)⇒y=−x10+215y - 4 = -\frac{1}{10}(x-2) \Rightarrow y = -\frac{x}{10} + \frac{21}{5}

3.2 Stationary Points and Curve Sketching

A stationary point occurs where f′(x)=0f'(x) = 0. The nature of a stationary point is determined by the second derivative test or by a sign chart on f′f':

TestLocal minimumLocal maximumInconclusive
Second derivativef′′(a)>0f''(a) > 0f′′(a)<0f''(a) < 0f′′(a)=0f''(a) = 0
Sign chart on f′f'f′f' changes −→+- \to +f′f' changes +→−+ \to -f′f' doesn’t change sign

Increasing/decreasing: f′>0f' > 0 means increasing; f′<0f' < 0 means decreasing.

Concavity and inflection points:

ConditionMeaning
f′′>0f'' > 0Concave up (bowl shape)
f′′<0f'' < 0Concave down (cap shape)
f′′f'' changes sign at x=cx = cInflection point at x=cx = c

f′′(a)=0f''(a) = 0 does NOT mean x=ax = a is an inflection point. You must also verify that f′′f'' changes sign at x=ax = a. The function f(x)=x4f(x) = x^4 has f′′(0)=0f''(0) = 0 but x=0x = 0 is a minimum, not an inflection point.

Full curve-sketching checklist:

  1. Domain and any restrictions
  2. xx-intercepts (set y=0y = 0) and yy-intercept (set x=0x = 0)
  3. Vertical asymptotes (values where denominator =0= 0)
  4. Horizontal/oblique asymptotes (behaviour as x→±∞x \to \pm\infty)
  5. Stationary points: solve f′(x)=0f'(x) = 0, classify each
  6. Inflection points: solve f′′(x)=0f''(x) = 0, verify sign change in f′′f''
  7. Sketch, labelling all key features

Curve Sketching

Sketch f(x)=x2x2−4f(x) = \dfrac{x^2}{x^2 - 4}, identifying all key features.

Domain: x≠±2x \neq \pm 2

yy-intercept: f(0)=0f(0) = 0

xx-intercept: x2=0⇒x=0x^2 = 0 \Rightarrow x = 0

Vertical asymptotes: x=2x = 2 and x=−2x = -2

Horizontal asymptote: As x→±∞x \to \pm\infty, f(x)→1f(x) \to 1, so y=1y = 1

Derivative: Using the quotient rule:

f′(x)=2x(x2−4)−x2⋅2x(x2−4)2=−8x(x2−4)2f'(x) = \frac{2x(x^2-4) - x^2 \cdot 2x}{(x^2-4)^2} = \frac{-8x}{(x^2-4)^2}

Stationary point at x=0x = 0: f(0)=0f(0) = 0, f′′(0)>0f''(0) > 0 (local minimum at (0,0)(0,0))

Behaviour: f(x)>1f(x) > 1 for ∣x∣>2\lvert x\rvert > 2; f(x)≤0f(x) \leq 0 for ∣x∣<2\lvert x\rvert < 2.

3.3 Optimisation

Optimisation is how you use calculus to answer “what is the best possible outcome?” questions — the largest area you can enclose with a fixed fence, the box with maximum volume from a sheet of card, the speed that minimises fuel use. The key insight is that at a maximum or minimum, the rate of change equals zero, so you find it by solving f′(x)=0f'(x) = 0.

Optimisation problems ask for the maximum or minimum value of some quantity. The standard approach:

  1. Define the variable(s) and write the objective function (the quantity to optimise)
  2. Use any constraint to write the objective function in terms of a single variable
  3. Differentiate and solve f′(x)=0f'(x) = 0
  4. Use the second derivative or domain analysis to confirm it is a maximum/minimum
  5. Answer the question — often the maximum/minimum value is required, not just xx

Always check the domain for the optimisation problem. A critical point at x=5x = 5 is useless if the physical constraint restricts xx to [0,4][0, 4]. In that case, check the endpoints as well.

Optimisation — Closed Box

A closed rectangular box has a square base of side xx cm and height hh cm. Its surface area is 600 cm2600 \text{ cm}^2. Find the dimensions that maximise the volume.

Objective function: V=x2hV = x^2 h

Constraint: 2x2+4xh=600⇒h=600−2x24x=300−x22x2x^2 + 4xh = 600 \Rightarrow h = \dfrac{600 - 2x^2}{4x} = \dfrac{300 - x^2}{2x}

Single-variable form:

V(x)=x2⋅300−x22x=x(300−x2)2=150x−x32V(x) = x^2 \cdot \frac{300 - x^2}{2x} = \frac{x(300-x^2)}{2} = 150x - \frac{x^3}{2}

Differentiate: V′(x)=150−3x22V'(x) = 150 - \frac{3x^2}{2}

Set to zero: 150=3x22⇒x2=100⇒x=10150 = \frac{3x^2}{2} \Rightarrow x^2 = 100 \Rightarrow x = 10 (positive dimension)

Confirm maximum: V′′(x)=−3x<0V''(x) = -3x < 0 for x>0x > 0 — concave down, so this is a maximum.

Dimensions: x=10x = 10 cm, h=300−10020=10h = \frac{300-100}{20} = 10 cm. The optimal box is a cube.

Vmax⁡=1000 cm3V_{\max} = 1000 \text{ cm}^3

When two quantities are connected by a formula, changing one forces the other to change too — and you can find exactly how fast. For example, if a balloon’s radius is growing, how fast is its volume growing? Related rates use the chain rule to link these speeds together.

In related-rates problems, two or more quantities change with time. The chain rule links their rates of change.

Strategy:

  1. Identify what is changing, assign variables and their rates (typically as dydt\frac{dy}{dt}, dxdt\frac{dx}{dt}, etc.)
  2. Write a geometric or physical relationship between the variables
  3. Differentiate implicitly with respect to tt
  4. Substitute known values and solve

Related Rates — Expanding Circle

The radius of a circle is increasing at 3 cm s−13\text{ cm s}^{-1}. Find the rate of increase of the area when the radius is 55 cm.

Let rr = radius, A=πr2A = \pi r^2.

dAdt=2πr⋅drdt\frac{dA}{dt} = 2\pi r \cdot \frac{dr}{dt}

When r=5r = 5 and drdt=3\frac{dr}{dt} = 3:

dAdt=2π(5)(3)=30π≈94.2 cm2s−1\frac{dA}{dt} = 2\pi(5)(3) = 30\pi \approx 94.2 \text{ cm}^2\text{s}^{-1}

Related Rates — Conical Water Tank (8 marks)

A water tank has the shape of an inverted circular cone with base radius 66 m and height 88 m. Water is being pumped into the tank at a constant rate of 2 m3min−12\text{ m}^3\text{min}^{-1}.

(a) [2 marks] Express the radius rr of the water surface in terms of the depth hh of the water.

(b) [3 marks] Find an expression for the volume VV of water in the tank in terms of hh only.

(c) [3 marks] Find the rate at which the water level is rising when the depth is 44 m.


Solution:

(a) By similar triangles, the ratio of radius to height is constant throughout the cone.

For the full tank: 68=34\dfrac{6}{8} = \dfrac{3}{4}

For the water at depth hh:

rh=34\frac{r}{h} = \frac{3}{4}

Therefore:

r=3h4r = \frac{3h}{4}

(b) The volume of a cone is given by:

V=13πr2hV = \frac{1}{3}\pi r^2 h

Substituting r=3h4r = \dfrac{3h}{4}:

V=13π(3h4)2hV = \frac{1}{3}\pi \left(\frac{3h}{4}\right)^2 h

V=13π⋅9h216⋅hV = \frac{1}{3}\pi \cdot \frac{9h^2}{16} \cdot h

V=3πh316 m3V = \frac{3\pi h^3}{16} \text{ m}^3

(c) Differentiate V=3πh316V = \dfrac{3\pi h^3}{16} with respect to time tt:

dVdt=3π16⋅3h2⋅dhdt\frac{dV}{dt} = \frac{3\pi}{16} \cdot 3h^2 \cdot \frac{dh}{dt}

dVdt=9πh216⋅dhdt\frac{dV}{dt} = \frac{9\pi h^2}{16} \cdot \frac{dh}{dt}

We are given that dVdt=2 m3min−1\dfrac{dV}{dt} = 2\text{ m}^3\text{min}^{-1} and we want to find dhdt\dfrac{dh}{dt} when h=4h = 4 m.

Substitute known values:

2=9π(4)216⋅dhdt2 = \frac{9\pi (4)^2}{16} \cdot \frac{dh}{dt}

2=9π⋅1616⋅dhdt2 = \frac{9\pi \cdot 16}{16} \cdot \frac{dh}{dt}

2=9π⋅dhdt2 = 9\pi \cdot \frac{dh}{dt}

dhdt=29π≈0.0707 m min−1\frac{dh}{dt} = \frac{2}{9\pi} \approx 0.0707 \text{ m min}^{-1}

The water level is rising at approximately 0.071 m min−10.071\text{ m min}^{-1} (or 7.1 cm min−17.1\text{ cm min}^{-1}) when the depth is 44 m.

Related rates questions require units in the answer. If rr is in cm and tt is in seconds, then dAdt\frac{dA}{dt} is in cm2s−1\text{cm}^2\text{s}^{-1}. Missing units on a rates answer will lose the final mark.

3.5 Kinematics

For a particle moving in a straight line with displacement s(t)s(t):

v(t)=s′(t)=dsdta(t)=v′(t)=s′′(t)=d2sdt2v(t) = s'(t) = \frac{ds}{dt} \qquad a(t) = v'(t) = s''(t) = \frac{d^2s}{dt^2}

Key interpretations:

QuantitySignMeaning
v>0v > 0PositiveMoving in positive direction
v<0v < 0NegativeMoving in negative direction
v=0v = 0ZeroParticle is at rest (momentarily)
a>0a > 0PositiveVelocity increasing
a<0a < 0NegativeVelocity decreasing (decelerating if v>0v > 0)

Speed is ∣v∣\lvert v \rvert. A particle decelerates when vv and aa have opposite signs.

Total distance (not displacement): integrate ∣v(t)∣\lvert v(t) \rvert, or split the integral at points where v=0v = 0 and add absolute values.

Distance ≠\neq displacement. Displacement is ∫abv(t) dt\int_a^b v(t)\,dt (signed). Distance is ∫ab∣v(t)∣ dt\int_a^b \lvert v(t)\rvert\,dt (unsigned). If the particle reverses, the displacement integral underestimates the total path length. Always find where v=0v = 0 to check for reversal.

Kinematics

A particle has displacement s(t)=t3−6t2+9ts(t) = t^3 - 6t^2 + 9t metres, t≥0t \geq 0 seconds. Find: (a) when it is at rest, (b) its acceleration when t=3t = 3, (c) the total distance in 0≤t≤40 \leq t \leq 4.

Part (a): v=3t2−12t+9=3(t−1)(t−3)=0⇒t=1v = 3t^2 - 12t + 9 = 3(t-1)(t-3) = 0 \Rightarrow t = 1 or t=3t = 3

Part (b): a=v′=6t−12a = v' = 6t - 12. At t=3t = 3: a=18−12=6 m s−2a = 18 - 12 = 6 \text{ m s}^{-2}

Part (c): Position values: s(0)=0s(0) = 0, s(1)=4s(1) = 4, s(3)=0s(3) = 0, s(4)=4s(4) = 4

Distances: ∣4−0∣+∣0−4∣+∣4−0∣=4+4+4=12\lvert 4-0\rvert + \lvert 0-4\rvert + \lvert 4-0\rvert = 4 + 4 + 4 = 12 m


Quick Recall — Section 3

Try to answer without scrolling up:

  1. How do you find stationary points of f(x)f(x)?
  2. How do you determine if a stationary point is a maximum or minimum?
  3. In kinematics, what is velocity in terms of displacement s(t)s(t)?
Reveal answers
  1. Solve f′(x)=0f'(x) = 0.
  2. Use the second derivative test: if f′′(x)>0f''(x) > 0 it is a minimum; if f′′(x)<0f''(x) < 0 it is a maximum. Or use a sign diagram of f′f'.
  3. v(t)=dsdt=s′(t)v(t) = \frac{ds}{dt} = s'(t).

Section 4: Integration

Integration is the reverse of differentiation. The indefinite integral ∫f(x) dx\int f(x)\,dx gives a family of antiderivatives F(x)+CF(x) + C. The definite integral ∫abf(x) dx=F(b)−F(a)\int_a^b f(x)\,dx = F(b) - F(a) gives a specific number (the net signed area under the curve).

Fundamental Theorem of Calculus:

ddx∫axf(t) dt=f(x)and∫abf′(x) dx=f(b)−f(a)\frac{d}{dx}\int_a^x f(t)\,dt = f(x) \qquad \text{and} \qquad \int_a^b f'(x)\,dx = f(b) - f(a)

4.1 Standard Integrals

Standard Integral Table

Integrand f(x)f(x)∫f(x) dx\int f(x)\,dxCondition
xnx^nxn+1n+1+C\dfrac{x^{n+1}}{n+1} + Cn≠−1n \neq -1
1x\dfrac{1}{x}ln⁡∣x∣+C\ln\lvert x\rvert + Cx≠0x \neq 0
exe^xex+Ce^x + C
ekxe^{kx}1kekx+C\dfrac{1}{k}e^{kx} + Ck≠0k \neq 0
sin⁡x\sin x−cos⁡x+C-\cos x + C
cos⁡x\cos xsin⁡x+C\sin x + C
tan⁡x\tan xln⁡∣sec⁡x∣+C\ln\lvert\sec x\rvert + C
sec⁡2x\sec^2 xtan⁡x+C\tan x + C
11−x2\dfrac{1}{\sqrt{1-x^2}}arcsin⁡x+C\arcsin x + C∣x∣<1\lvert x\rvert < 1
11+x2\dfrac{1}{1+x^2}arctan⁡x+C\arctan x + C
1x2+a2\dfrac{1}{x^2 + a^2}1aarctan⁡ ⁣(xa)+C\dfrac{1}{a}\arctan\!\left(\dfrac{x}{a}\right) + C
1a2−x2\dfrac{1}{\sqrt{a^2 - x^2}}arcsin⁡ ⁣(xa)+C\arcsin\!\left(\dfrac{x}{a}\right) + C

∫1x dx=ln⁡∣x∣+C\int \frac{1}{x}\,dx = \ln\lvert x\rvert + C, NOT ln⁡(x)+C\ln(x) + C. The absolute value is essential when xx can be negative. On IB exams, omitting the absolute value bars inside a logarithm loses a mark.

4.2 Integration by Substitution

Substitution (reverse chain rule): choose u=g(x)u = g(x), then du=g′(x) dxdu = g'(x)\,dx.

∫f(g(x))⋅g′(x) dx=∫f(u) du\int f(g(x)) \cdot g'(x)\,dx = \int f(u)\,du

Key step: Always express dxdx in terms of dudu by computing dudx\frac{du}{dx}, then substitute. For definite integrals, either change the limits (using u=g(x)u = g(x)) or convert back to xx at the end.

Substitution — Indefinite

Find ∫2xcos⁡(x2) dx\displaystyle\int 2x\cos(x^2)\,dx.

Let u=x2u = x^2, so du=2x dxdu = 2x\,dx.

∫2xcos⁡(x2) dx=∫cos⁡u du=sin⁡u+C=sin⁡(x2)+C\int 2x\cos(x^2)\,dx = \int \cos u\,du = \sin u + C = \sin(x^2) + C

Substitution — Definite

Evaluate ∫01x(x2+1)3 dx\displaystyle\int_0^1 \frac{x}{(x^2+1)^3}\,dx.

Let u=x2+1u = x^2 + 1, du=2x dx⇒x dx=12dudu = 2x\,dx \Rightarrow x\,dx = \frac{1}{2}du.

Change limits: x=0⇒u=1x = 0 \Rightarrow u = 1; x=1⇒u=2x = 1 \Rightarrow u = 2.

∫121u3⋅12 du=12∫12u−3 du=12[u−2−2]12=−14[14−1]=−14⋅(−34)=316\int_1^2 \frac{1}{u^3} \cdot \frac{1}{2}\,du = \frac{1}{2}\int_1^2 u^{-3}\,du = \frac{1}{2}\left[\frac{u^{-2}}{-2}\right]_1^2 = -\frac{1}{4}\left[\frac{1}{4} - 1\right] = -\frac{1}{4} \cdot \left(-\frac{3}{4}\right) = \frac{3}{16}

4.3 Integration by Parts

When you have an integral that is a product of two different types of functions — like x⋅exx \cdot e^x or x⋅ln⁡xx \cdot \ln x — substitution doesn’t work. Integration by parts is the technique for these cases: it splits the integral into a simpler one by trading complexity between the two factors.

The integration-by-parts formula follows from reversing the product rule:

∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du

Choosing uu — LIATE order (highest priority to lowest):

PriorityTypeExample
1stLogarithmsln⁡x\ln x
2ndInverse trigarctan⁡x\arctan x
3rdAlgebraicxnx^n
4thTrigonometricsin⁡x\sin x, cos⁡x\cos x
5thExponentialexe^x

Make uu the term with the higher-priority type; let dvdv be the rest.

LIATE is a guide, not a law. For ∫xex dx\int x e^x\,dx, take u=xu = x (algebraic, priority 3) and dv=ex dxdv = e^x\,dx (exponential, priority 5) — then du=dxdu = dx and v=exv = e^x. If you take u=exu = e^x and dv=x dxdv = x\,dx, the integral becomes more complex, not simpler.

Integration by Parts — Standard

Find ∫xex dx\displaystyle\int x e^x\,dx.

u=xu = x, dv=ex dxdv = e^x\,dx ⇒\Rightarrow du=dxdu = dx, v=exv = e^x

∫xex dx=xex−∫ex dx=xex−ex+C=ex(x−1)+C\int x e^x\,dx = xe^x - \int e^x\,dx = xe^x - e^x + C = e^x(x - 1) + C

Integration by Parts — Twice (IBP2^2)

Find ∫x2ex dx\displaystyle\int x^2 e^x\,dx.

First IBP: u=x2u = x^2, dv=ex dx⇒du=2x dxdv = e^x\,dx \Rightarrow du = 2x\,dx, v=exv = e^x

∫x2ex dx=x2ex−2∫xex dx\int x^2 e^x\,dx = x^2 e^x - 2\int x e^x\,dx

Second IBP: From above, ∫xex dx=ex(x−1)+C\int x e^x\,dx = e^x(x-1) + C

=x2ex−2ex(x−1)+C=ex(x2−2x+2)+C= x^2 e^x - 2e^x(x-1) + C = e^x(x^2 - 2x + 2) + C

Integration by Parts — Cyclic

Find ∫excos⁡x dx\displaystyle\int e^x \cos x\,dx.

First IBP: u=exu = e^x, dv=cos⁡x dx⇒v=sin⁡xdv = \cos x\,dx \Rightarrow v = \sin x

I=exsin⁡x−∫exsin⁡x dxI = e^x\sin x - \int e^x\sin x\,dx

Second IBP: u=exu = e^x, dv=sin⁡x dx⇒v=−cos⁡xdv = \sin x\,dx \Rightarrow v = -\cos x

I=exsin⁡x−(−excos⁡x+∫excos⁡x dx)=exsin⁡x+excos⁡x−II = e^x\sin x - \left(-e^x\cos x + \int e^x\cos x\,dx\right) = e^x\sin x + e^x\cos x - I

Solve for II: 2I=ex(sin⁡x+cos⁡x)⇒I=ex(sin⁡x+cos⁡x)2+C2I = e^x(\sin x + \cos x) \Rightarrow I = \dfrac{e^x(\sin x + \cos x)}{2} + C

Practice: Integration by Parts — Fading Sequence

The worked examples above showed the full method. Now try these progressively: the first shows all steps, the second hides the final steps for you to attempt, and the third gives only the setup.

WORKED EXAMPLEFull worked example — all steps shown

Find ∫xsin⁡x dx\displaystyle\int x \sin x\,dx.

Step 1

Identify uu and dvdv: Using LIATE, u=xu = x (algebraic) and dv=sin⁡x dxdv = \sin x\,dx.

Step 2

Compute dudu and vv: du=dxdu = dx, v=∫sin⁡x dx=−cos⁡xv = \int \sin x\,dx = -\cos x

Step 3

Apply the formula: ∫xsin⁡x dx=x(−cos⁡x)−∫(−cos⁡x) dx=−xcos⁡x+∫cos⁡x dx\int x \sin x\,dx = x(-\cos x) - \int (-\cos x)\,dx = -x\cos x + \int \cos x\,dx

Step 4

Evaluate the remaining integral: =−xcos⁡x+sin⁡x+C= -x\cos x + \sin x + C

YOUR TURN (PARTIAL)Partial example — try the last steps yourself

Find ∫x2ln⁡x dx\displaystyle\int x^2 \ln x\,dx.

Steps 1—2 are shown. Try steps 3—4 before revealing.

Step 1

Identify uu and dvdv: Using LIATE, u=ln⁡xu = \ln x (log, highest priority) and dv=x2 dxdv = x^2\,dx.

Step 2

Compute dudu and vv: du=1x dxdu = \frac{1}{x}\,dx, v=x33v = \frac{x^3}{3}

Step 3 — Apply the IBP formula and simplify the remaining integral

Apply the formula:

∫x2ln⁡x dx=x33ln⁡x−∫x33⋅1x dx=x33ln⁡x−13∫x2 dx\int x^2 \ln x\,dx = \frac{x^3}{3}\ln x - \int \frac{x^3}{3} \cdot \frac{1}{x}\,dx = \frac{x^3}{3}\ln x - \frac{1}{3}\int x^2\,dx

Step 4 — Evaluate and write the final answer

Evaluate: =x33ln⁡x−13⋅x33+C=x33ln⁡x−x39+C= \dfrac{x^3}{3}\ln x - \dfrac{1}{3} \cdot \dfrac{x^3}{3} + C = \dfrac{x^3}{3}\ln x - \dfrac{x^3}{9} + C

YOUR TURN (SCAFFOLDED)Scaffolded — only the setup is given

Find ∫ln⁡x dx\displaystyle\int \ln x\,dx.

Work through the full solution, then reveal each step to check.

Step 1 — Choose u and dv (hint: write ln x as ln x times 1)

The trick: Write ∫ln⁡x dx=∫1⋅ln⁡x dx\int \ln x\,dx = \int 1 \cdot \ln x\,dx. Let u=ln⁡xu = \ln x, dv=1 dxdv = 1\,dx, so du=1x dxdu = \frac{1}{x}\,dx, v=xv = x.

Step 2 — Apply the IBP formula

Apply: ∫ln⁡x dx=xln⁡x−∫x⋅1x dx=xln⁡x−∫1 dx\int \ln x\,dx = x\ln x - \int x \cdot \frac{1}{x}\,dx = x\ln x - \int 1\,dx

Step 3 — Write the final answer

Result: =xln⁡x−x+C=x(ln⁡x−1)+C= x\ln x - x + C = x(\ln x - 1) + C

4.4 Partial Fractions HL

A fraction like 3x+1(x+1)(x−2)\frac{3x+1}{(x+1)(x-2)} is hard to integrate directly, but if you can split it into two simpler fractions each with a single linear denominator, each piece integrates to a natural log. Partial fractions is the technique that does this splitting.

Partial fractions decompose a rational function into simpler fractions before integrating. The method depends on the nature of the denominator’s factors.

Case 1 — Distinct linear factors: f(x)(x−a)(x−b)=Ax−a+Bx−b\dfrac{f(x)}{(x-a)(x-b)} = \dfrac{A}{x-a} + \dfrac{B}{x-b}

Case 2 — Repeated linear factor: f(x)(x−a)2=Ax−a+B(x−a)2\dfrac{f(x)}{(x-a)^2} = \dfrac{A}{x-a} + \dfrac{B}{(x-a)^2}

Case 3 — Irreducible quadratic factor: f(x)(x−a)(x2+bx+c)=Ax−a+Bx+Cx2+bx+c\dfrac{f(x)}{(x-a)(x^2+bx+c)} = \dfrac{A}{x-a} + \dfrac{Bx+C}{x^2+bx+c}

Important: If the degree of the numerator ≥\geq degree of the denominator, perform polynomial long division first to obtain a proper fraction.

Partial Fractions Integration

Find ∫3x+1(x+1)(x−2) dx\displaystyle\int \frac{3x+1}{(x+1)(x-2)}\,dx.

Step 1: Decompose: 3x+1(x+1)(x−2)=Ax+1+Bx−2\dfrac{3x+1}{(x+1)(x-2)} = \dfrac{A}{x+1} + \dfrac{B}{x-2}

Step 2: Multiply through: 3x+1=A(x−2)+B(x+1)3x+1 = A(x-2) + B(x+1)

Step 3: Substitute x=2x = 2: 7=3B⇒B=737 = 3B \Rightarrow B = \frac{7}{3}

Step 4: Substitute x=−1x = -1: −2=−3A⇒A=23-2 = -3A \Rightarrow A = \frac{2}{3}

Step 5: Integrate:

∫3x+1(x+1)(x−2) dx=23ln⁡∣x+1∣+73ln⁡∣x−2∣+C\int \frac{3x+1}{(x+1)(x-2)}\,dx = \frac{2}{3}\ln\lvert x+1\rvert + \frac{7}{3}\ln\lvert x-2\rvert + C

Before partial fractions, always check whether the rational function is proper (degree of numerator < degree of denominator). If it is improper, divide first. Attempting partial fractions on an improper fraction without dividing first gives a wrong decomposition.


Section 5: Applications of Integration

5.1 Area Under a Curve

The area between y=f(x)y = f(x) and the xx-axis from x=ax = a to x=bx = b is:

A=∫ab∣f(x)∣ dxA = \int_a^b \lvert f(x)\rvert\,dx

If f(x)≥0f(x) \geq 0 on [a,b][a, b], this simplifies to ∫abf(x) dx\int_a^b f(x)\,dx. If ff changes sign, split the interval at the zeros and add absolute values.

∫abf(x) dx\int_a^b f(x)\,dx gives the net signed area (regions below the axis subtract). For a total area, split at roots and sum the absolute values. IB questions usually ask explicitly for “area” (unsigned) or “value of the integral” (signed) — do not confuse them.

5.2 Area Between Two Curves

For f(x)≥g(x)f(x) \geq g(x) on [a,b][a, b]:

A=∫ab[f(x)−g(x)] dxA = \int_a^b \bigl[f(x) - g(x)\bigr]\,dx

If the curves cross within [a,b][a, b], find the crossing points (intersections), then split and add.

Area Between Two Curves

Find the area enclosed by y=x2y = x^2 and y=x+2y = x + 2.

Step 1: Find intersections: x2=x+2⇒x2−x−2=0⇒(x−2)(x+1)=0⇒x=−1,2x^2 = x+2 \Rightarrow x^2 - x - 2 = 0 \Rightarrow (x-2)(x+1) = 0 \Rightarrow x = -1, 2

Step 2: On [−1,2][-1, 2]: x+2≥x2x+2 \geq x^2 (check at x=0x = 0: 2>02 > 0). So f=x+2f = x+2, g=x2g = x^2.

Step 3:

A=∫−12(x+2−x2) dx=[x22+2x−x33]−12A = \int_{-1}^{2}(x+2-x^2)\,dx = \left[\frac{x^2}{2} + 2x - \frac{x^3}{3}\right]_{-1}^{2}

=(2+4−83)−(12−2+13)=103−(−76)=103+76=276=92= \left(2 + 4 - \frac{8}{3}\right) - \left(\frac{1}{2} - 2 + \frac{1}{3}\right) = \frac{10}{3} - \left(-\frac{7}{6}\right) = \frac{10}{3} + \frac{7}{6} = \frac{27}{6} = \frac{9}{2}

5.3 Volume of Revolution HL

If you take a curve and spin it around an axis, you carve out a 3D solid — like a vase or a bullet shape. The volume of revolution formula calculates that solid’s volume by treating it as a stack of thin circular discs, each with radius equal to the function’s value at that point.

Rotation about the xx-axis: The volume generated by rotating y=f(x)y = f(x) about the xx-axis from x=ax = a to x=bx = b:

V=π∫ab[f(x)]2 dxV = \pi\int_a^b [f(x)]^2\,dx

Rotation about the yy-axis: Express xx as a function of yy:

V=π∫cd[g(y)]2 dyV = \pi\int_c^d [g(y)]^2\,dy

Volume between two curves (shell method or washer method):

V=π∫ab([f(x)]2−[g(x)]2) dx(washer method, outer2−inner2)V = \pi\int_a^b \bigl([f(x)]^2 - [g(x)]^2\bigr)\,dx \qquad \text{(washer method, outer}^2 - \text{inner}^2\text{)}

The volume formula is V=π∫y2 dxV = \pi\int y^2\,dx — it is y2y^2, not yy. Students commonly write V=π∫y dxV = \pi \int y\,dx. The factor of π\pi comes from the cross-sectional area πr2=πy2\pi r^2 = \pi y^2. This formula is NOT in the IB formula booklet for AA HL — you must recall it.

Volume of Revolution

Find the volume generated when y=xy = \sqrt{x}, 0≤x≤40 \leq x \leq 4, is rotated 360°360° about the xx-axis.

V=π∫04(x)2 dx=π∫04x dx=π[x22]04=π⋅8=8πV = \pi\int_0^4 (\sqrt{x})^2\,dx = \pi\int_0^4 x\,dx = \pi\left[\frac{x^2}{2}\right]_0^4 = \pi \cdot 8 = 8\pi

5.4 Kinematics — Integration

Given acceleration a(t)a(t) or velocity v(t)v(t):

v(t)=∫a(t) dt+C1s(t)=∫v(t) dt+C2v(t) = \int a(t)\,dt + C_1 \qquad s(t) = \int v(t)\,dt + C_2

The constants are found from initial conditions: v(0)=v0v(0) = v_0 and s(0)=s0s(0) = s_0.

Displacement over [t1,t2][t_1, t_2]: ∫t1t2v(t) dt=s(t2)−s(t1)\displaystyle\int_{t_1}^{t_2} v(t)\,dt = s(t_2) - s(t_1)

Total distance over [t1,t2][t_1, t_2]: ∫t1t2∣v(t)∣ dt\displaystyle\int_{t_1}^{t_2} \lvert v(t)\rvert\,dt

Kinematics — Finding Position from Acceleration

A particle starts at rest at the origin. Its acceleration is a(t)=6t−4a(t) = 6t - 4. Find its position at t=3t = 3.

Step 1: v(t)=∫(6t−4) dt=3t2−4t+C1v(t) = \int(6t-4)\,dt = 3t^2 - 4t + C_1. Initial rest: v(0)=0⇒C1=0v(0) = 0 \Rightarrow C_1 = 0.

Step 2: s(t)=∫(3t2−4t) dt=t3−2t2+C2s(t) = \int(3t^2 - 4t)\,dt = t^3 - 2t^2 + C_2. Starts at origin: s(0)=0⇒C2=0s(0) = 0 \Rightarrow C_2 = 0.

Step 3: s(3)=27−18=9s(3) = 27 - 18 = 9 m


Section 6: Differential Equations

A differential equation is an equation that contains a function and its derivative at the same time — it describes how something changes rather than what it equals. They are the language of real-world modelling: population growth, radioactive decay, temperature cooling, and spread of disease are all described by differential equations.

A differential equation (DE) relates a function to its derivatives. The order is the highest derivative appearing. The general solution contains arbitrary constants; an initial condition (or boundary condition) pins down a particular solution.

6.1 Separable Differential Equations

The simplest differential equations to solve are ones where you can get all the yy terms on one side and all the xx terms on the other — then integrate both sides separately. This is called “separating variables.”

A first-order DE is separable if it can be written as dydx=f(x)g(y)\dfrac{dy}{dx} = f(x) g(y). Separate variables and integrate both sides:

∫1g(y) dy=∫f(x) dx\int \frac{1}{g(y)}\,dy = \int f(x)\,dx

Separable DE

Solve dydx=xy\dfrac{dy}{dx} = xy, given y(0)=2y(0) = 2.

Step 1: Separate: dyy=x dx\dfrac{dy}{y} = x\,dx

Step 2: Integrate: ln⁡∣y∣=x22+C\ln\lvert y\rvert = \dfrac{x^2}{2} + C

Step 3: Exponentiate: ∣y∣=eC⋅ex2/2\lvert y\rvert = e^C \cdot e^{x^2/2}, so y=Aex2/2y = A e^{x^2/2} where A=±eCA = \pm e^C

Step 4: Apply y(0)=2y(0) = 2: 2=Ae0=A2 = A e^0 = A

Particular solution: y=2ex2/2y = 2e^{x^2/2}

After separating and integrating, you get ln⁡∣y∣=…+C\ln\lvert y\rvert = \ldots + C. Exponentiating gives ∣y∣=eCe…\lvert y\rvert = e^C e^{\ldots}, and the ±\pm from the absolute value is absorbed into a new constant AA, so y=Ae…y = Ae^{\ldots} where A≠0A \neq 0. Do not lose the ±\pm or the constant — they combine to give AA which is determined by the initial condition.

6.2 Initial Value Problems

A differential equation’s general solution contains an unknown constant, giving a whole family of curves. An initial value problem pins down which specific curve you want by giving one known point on it — for example, the population at time zero, or the temperature at the start of an experiment.

An initial value problem (IVP) specifies the DE and a condition such as y(x0)=y0y(x_0) = y_0. The general solution’s constant is uniquely determined by substituting x0x_0 and y0y_0.

Initial Value Problem

Solve dydx=xy\dfrac{dy}{dx} = \dfrac{x}{y}, y(0)=3y(0) = 3.

Separate: y dy=x dxy\,dy = x\,dx

Integrate: y22=x22+C\dfrac{y^2}{2} = \dfrac{x^2}{2} + C

Apply IC: 92=0+C⇒C=92\dfrac{9}{2} = 0 + C \Rightarrow C = \dfrac{9}{2}

Particular solution: y2=x2+9y^2 = x^2 + 9, or y=x2+9y = \sqrt{x^2 + 9} (positive since y(0)=3>0y(0) = 3 > 0)

6.3 Modelling with Differential Equations

Many natural phenomena are modelled by DEs. Key models:

ModelDESolution
Exponential growthdNdt=kN\dfrac{dN}{dt} = kN, k>0k > 0N=N0ektN = N_0 e^{kt}
Exponential decaydNdt=−kN\dfrac{dN}{dt} = -kN, k>0k > 0N=N0e−ktN = N_0 e^{-kt}
Newton’s Law of CoolingdTdt=−k(T−Tenv)\dfrac{dT}{dt} = -k(T - T_{\text{env}})T=Tenv+(T0−Tenv)e−ktT = T_{\text{env}} + (T_0 - T_{\text{env}})e^{-kt}
Logistic growthdPdt=rP ⁣(1−PK)\dfrac{dP}{dt} = rP\!\left(1 - \dfrac{P}{K}\right)S-shaped curve, P→KP \to K

For Newton’s Law of Cooling, let θ=T−Tenv\theta = T - T_{\text{env}} (excess temperature). Then dθdt=−kθ\frac{d\theta}{dt} = -k\theta, which is a standard exponential decay. Always substitute the environmental temperature first before integrating.

Modelling — Radioactive Decay

A radioactive substance has half-life 8 years. Find: (a) the decay constant kk, (b) the fraction remaining after 20 years.

Part (a): At t=8t = 8, N=12N0N = \frac{1}{2}N_0:

N02=N0e−8k⇒12=e−8k⇒−8k=ln⁡12=−ln⁡2⇒k=ln⁡28\frac{N_0}{2} = N_0 e^{-8k} \Rightarrow \frac{1}{2} = e^{-8k} \Rightarrow -8k = \ln\frac{1}{2} = -\ln 2 \Rightarrow k = \frac{\ln 2}{8}

Part (b):

NN0=e−20k=e−20ln⁡2/8=e−5ln⁡2/2=2−5/2=142≈0.177\frac{N}{N_0} = e^{-20k} = e^{-20\ln 2/8} = e^{-5\ln 2/2} = 2^{-5/2} = \frac{1}{4\sqrt{2}} \approx 0.177

About 17.7% remains after 20 years.


Section 7: Maclaurin Series HL

Polynomials are easy to work with — you can add, multiply, differentiate, and integrate them by hand. A Maclaurin series takes a complicated function like exe^x or sin⁡x\sin x and rewrites it as an infinite polynomial. This makes it possible to approximate function values, evaluate limits that look like 00\frac{0}{0}, and integrate functions that have no closed-form antiderivative.

A Maclaurin series expresses a function as an infinite power series centred at x=0x = 0:

f(x)=f(0)+f′(0)x+f′′(0)2!x2+f′′′(0)3!x3+⋯=∑n=0∞f(n)(0)n!xnf(x) = f(0) + f'(0)x + \frac{f''(0)}{2!}x^2 + \frac{f'''(0)}{3!}x^3 + \cdots = \sum_{n=0}^{\infty} \frac{f^{(n)}(0)}{n!} x^n

The series converges to f(x)f(x) within a radius of convergence RR. Outside this radius the series diverges.

7.1 Deriving the Four Standard Series

The Four Essential Maclaurin Series (must be able to derive)

ex=1+x+x22!+x33!+x44!+⋯=∑n=0∞xnn!(all x)e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \cdots = \sum_{n=0}^{\infty}\frac{x^n}{n!} \qquad \text{(all } x\text{)}

sin⁡x=x−x33!+x55!−x77!+⋯=∑n=0∞(−1)nx2n+1(2n+1)!(all x)\sin x = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \frac{x^7}{7!} + \cdots = \sum_{n=0}^{\infty}\frac{(-1)^n x^{2n+1}}{(2n+1)!} \qquad \text{(all } x\text{)}

cos⁡x=1−x22!+x44!−x66!+⋯=∑n=0∞(−1)nx2n(2n)!(all x)\cos x = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \frac{x^6}{6!} + \cdots = \sum_{n=0}^{\infty}\frac{(-1)^n x^{2n}}{(2n)!} \qquad \text{(all } x\text{)}

ln⁡(1+x)=x−x22+x33−x44+⋯=∑n=1∞(−1)n+1xnn(−1<x≤1)\ln(1+x) = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \cdots = \sum_{n=1}^{\infty}\frac{(-1)^{n+1} x^n}{n} \qquad (-1 < x \leq 1)

Deriving the Maclaurin Series for exe^x

Let f(x)=exf(x) = e^x. Since ddx(ex)=ex\frac{d}{dx}(e^x) = e^x, all derivatives equal exe^x.

At x=0x = 0: f(n)(0)=e0=1f^{(n)}(0) = e^0 = 1 for all nn.

Substituting into the Maclaurin formula:

ex=1+x+x22!+x33!+⋯e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \cdots

Deriving the Maclaurin Series for sin⁡x\sin x

f(x)=sin⁡xf(x) = \sin x. Compute derivatives at x=0x = 0:

nnf(n)(x)f^{(n)}(x)f(n)(0)f^{(n)}(0)
0sin⁡x\sin x0
1cos⁡x\cos x1
2−sin⁡x-\sin x0
3−cos⁡x-\cos x−1-1
4sin⁡x\sin x0

The pattern is 0,1,0,−1,0,1,…0, 1, 0, -1, 0, 1, \ldots Only odd powers survive:

sin⁡x=x−x33!+x55!−⋯\sin x = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \cdots

Deriving the Maclaurin Series for cos⁡x\cos x

f(x)=cos⁡xf(x) = \cos x. Compute derivatives at x=0x = 0:

nnf(n)(x)f^{(n)}(x)f(n)(0)f^{(n)}(0)
0cos⁡x\cos x1
1−sin⁡x-\sin x0
2−cos⁡x-\cos x−1-1
3sin⁡x\sin x0
4cos⁡x\cos x1

The pattern is 1,0,−1,0,1,…1, 0, -1, 0, 1, \ldots Only even powers survive, alternating in sign:

cos⁡x=1−x22!+x44!−x66!+⋯\cos x = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \frac{x^6}{6!} + \cdots

Common Mistakes — Maclaurin Series

  1. Applying series outside the radius of convergence: Each series has a specific domain of validity. For example, ln⁡(1+x)\ln(1+x) only converges for −1<x≤1-1 < x \leq 1. Using it for x=2x = 2 produces nonsense.

  2. Confusing which series applies where: Students often mix up exe^x, e−xe^{-x}, and ex2e^{x^2}. Always substitute carefully and check signs.

  3. Forgetting factorials: The Maclaurin formula has f(n)(0)n!\frac{f^{(n)}(0)}{n!}, not just f(n)(0)f^{(n)}(0). Forgetting the factorial gives wildly incorrect coefficients.

  4. Truncating too early: Using only the first two terms of a series can produce large errors. Check the remainder term or compare with the exact value to verify accuracy.

7.2 Applications of Maclaurin Series

Substitution: Replace xx with a multiple or power to get new series.

e−x2=1−x2+x42!−x63!+⋯e^{-x^2} = 1 - x^2 + \frac{x^4}{2!} - \frac{x^6}{3!} + \cdots

Evaluating limits: Series give an exact expansion near x=0x = 0, resolving indeterminate forms.

Approximation: The first few terms give accurate approximations for small xx.

Multiplying series: Multiply term by term, collecting powers.

Limit Using Maclaurin Series

Evaluate lim⁡x→0ex−1−x−x22x3\displaystyle\lim_{x \to 0} \dfrac{e^x - 1 - x - \frac{x^2}{2}}{x^3}.

Substitute the series for exe^x:

ex−1−x−x22=(1+x+x22+x36+⋯ )−1−x−x22=x36+⋯e^x - 1 - x - \frac{x^2}{2} = \left(1 + x + \frac{x^2}{2} + \frac{x^3}{6} + \cdots\right) - 1 - x - \frac{x^2}{2} = \frac{x^3}{6} + \cdots

lim⁡x→0x3/6+⋯x3=16\lim_{x \to 0} \frac{x^3/6 + \cdots}{x^3} = \frac{1}{6}

Integration Using Maclaurin Series

Find ∫00.1e−x2 dx\displaystyle\int_0^{0.1} e^{-x^2}\,dx to 5 decimal places.

Using e−x2=1−x2+x42!−⋯e^{-x^2} = 1 - x^2 + \dfrac{x^4}{2!} - \cdots:

∫00.1e−x2 dx≈∫00.1(1−x2+x42)dx=[x−x33+x510]00.1\int_0^{0.1} e^{-x^2}\,dx \approx \int_0^{0.1}\left(1 - x^2 + \frac{x^4}{2}\right)dx = \left[x - \frac{x^3}{3} + \frac{x^5}{10}\right]_0^{0.1}

=0.1−0.0013+0.0000110≈0.1−0.000333+0.000001=0.099668= 0.1 - \frac{0.001}{3} + \frac{0.00001}{10} \approx 0.1 - 0.000333 + 0.000001 = 0.099668

Maclaurin series for ln⁡(1+x)\ln(1+x) converges only for −1<x≤1-1 < x \leq 1. At x=1x = 1: the alternating harmonic series converges conditionally to ln⁡2\ln 2. At x=−1x = -1: it diverges. Always state the interval of validity when writing the series. Applying the series outside its radius gives nonsensical results.

Maclaurin Series Multiplication

Find the Maclaurin series for sin⁡x⋅ex\sin x \cdot e^x up to and including the x3x^3 term.

sin⁡x≈x−x36+⋯ex≈1+x+x22+x36+⋯\sin x \approx x - \frac{x^3}{6} + \cdots \qquad e^x \approx 1 + x + \frac{x^2}{2} + \frac{x^3}{6} + \cdots

Multiply term by term, collecting up to x3x^3:

x1:  x⋅1=xx^1: \; x \cdot 1 = x x2:  x⋅x=x2x^2: \; x \cdot x = x^2 x3:  x⋅x22+(−x36)⋅1=x32−x36=x33x^3: \; x \cdot \frac{x^2}{2} + \left(-\frac{x^3}{6}\right) \cdot 1 = \frac{x^3}{2} - \frac{x^3}{6} = \frac{x^3}{3}

sin⁡x⋅ex≈x+x2+x33+⋯\sin x \cdot e^x \approx x + x^2 + \frac{x^3}{3} + \cdots


Section 8: MCQ Practice

Q1. The derivative of f(x)=ln⁡(sin⁡x)f(x) = \ln(\sin x) is:

(A) cos⁡x\cos x \quad (B) cot⁡x\cot x \quad (C) tan⁡x\tan x \quad (D) 1sin⁡x\dfrac{1}{\sin x}

Answer: (B) Chain rule: f′(x)=1sin⁡x⋅cos⁡x=cos⁡xsin⁡x=cot⁡xf'(x) = \dfrac{1}{\sin x} \cdot \cos x = \dfrac{\cos x}{\sin x} = \cot x.

Q2. ∫0π/2sin⁡2x dx=\displaystyle\int_0^{\pi/2} \sin^2 x\,dx =

(A) 00 \quad (B) π4\dfrac{\pi}{4} \quad (C) π2\dfrac{\pi}{2} \quad (D) 11

Answer: (B) Use sin⁡2x=1−cos⁡2x2\sin^2 x = \dfrac{1 - \cos 2x}{2}:

∫0π/21−cos⁡2x2 dx=[x2−sin⁡2x4]0π/2=π4−0=π4\int_0^{\pi/2} \frac{1-\cos 2x}{2}\,dx = \left[\frac{x}{2} - \frac{\sin 2x}{4}\right]_0^{\pi/2} = \frac{\pi}{4} - 0 = \frac{\pi}{4}

Q3. If y=xxy = x^x, then dydx=\dfrac{dy}{dx} =

(A) x⋅xx−1x \cdot x^{x-1} \quad (B) xxln⁡xx^x \ln x \quad (C) xx(1+ln⁡x)x^x(1 + \ln x) \quad (D) xx⋅xx^x \cdot x

Answer: (C) Use logarithmic differentiation: ln⁡y=xln⁡x\ln y = x \ln x.

1ydydx=ln⁡x+x⋅1x=ln⁡x+1\frac{1}{y}\frac{dy}{dx} = \ln x + x \cdot \frac{1}{x} = \ln x + 1

dydx=y(ln⁡x+1)=xx(1+ln⁡x)\frac{dy}{dx} = y(\ln x + 1) = x^x(1 + \ln x)

Q4. The value of lim⁡x→01−cos⁡xx2\displaystyle\lim_{x \to 0} \dfrac{1 - \cos x}{x^2} is:

(A) 00 \quad (B) 14\dfrac{1}{4} \quad (C) 12\dfrac{1}{2} \quad (D) 11

Answer: (C) Using the Maclaurin series cos⁡x=1−x22+⋯\cos x = 1 - \dfrac{x^2}{2} + \cdots:

1−cos⁡xx2=x2/2−⋯x2→12\frac{1 - \cos x}{x^2} = \frac{x^2/2 - \cdots}{x^2} \to \frac{1}{2}

Alternatively, apply L’Hôpital’s rule twice: sin⁡x2x→cos⁡x2→12\dfrac{\sin x}{2x} \to \dfrac{\cos x}{2} \to \dfrac{1}{2}.

Q5. The function f(x)=x3−6x2+9xf(x) = x^3 - 6x^2 + 9x has an inflection point at:

(A) x=1x = 1 \quad (B) x=2x = 2 \quad (C) x=3x = 3 \quad (D) x=0x = 0

Answer: (B) f′(x)=3x2−12x+9f'(x) = 3x^2 - 12x + 9, f′′(x)=6x−12=6(x−2)f''(x) = 6x - 12 = 6(x-2).

f′′(x)=0f''(x) = 0 at x=2x = 2. Sign change: f′′(1)=−6<0f''(1) = -6 < 0 and f′′(3)=6>0f''(3) = 6 > 0 — confirmed sign change from negative to positive. Therefore x=2x = 2 is the only inflection point.

Q6. ∫xln⁡x dx=\displaystyle\int x \ln x\,dx =

(A) x22ln⁡x−x24+C\dfrac{x^2}{2}\ln x - \dfrac{x^2}{4} + C \quad (B) x2ln⁡x2+C\dfrac{x^2 \ln x}{2} + C \quad (C) xln⁡x−x+Cx\ln x - x + C \quad (D) x24(ln⁡x−1)+C\dfrac{x^2}{4}(\ln x - 1) + C

Answer: (A) IBP with u=ln⁡xu = \ln x, dv=x dxdv = x\,dx:

∫xln⁡x dx=x22ln⁡x−∫x22⋅1x dx=x22ln⁡x−x24+C\int x\ln x\,dx = \frac{x^2}{2}\ln x - \int\frac{x^2}{2} \cdot \frac{1}{x}\,dx = \frac{x^2}{2}\ln x - \frac{x^2}{4} + C

Q7. The general solution of dydx=2y\dfrac{dy}{dx} = 2y is:

(A) y=Cexy = Ce^x \quad (B) y=Ce2xy = Ce^{2x} \quad (C) y=2Cexy = 2Ce^x \quad (D) y=x2+Cy = x^2 + C

Answer: (B) Separate: dyy=2 dx⇒ln⁡∣y∣=2x+k⇒y=Ce2x\dfrac{dy}{y} = 2\,dx \Rightarrow \ln\lvert y\rvert = 2x + k \Rightarrow y = Ce^{2x}.

Q8. Which of the following is the correct Maclaurin expansion of cos⁡(2x)\cos(2x) up to the x4x^4 term?

(A) 1−2x2+2x431 - 2x^2 + \dfrac{2x^4}{3} \quad (B) 1−2x2+x431 - 2x^2 + \dfrac{x^4}{3} \quad (C) 1−x2+x461 - x^2 + \dfrac{x^4}{6} \quad (D) 1−4x2+8x431 - 4x^2 + \dfrac{8x^4}{3}

Answer: (A) Substitute 2x2x into the standard cos⁡x\cos x series:

cos⁡(2x)=1−(2x)22!+(2x)44!=1−4x22+16x424=1−2x2+2x43\cos(2x) = 1 - \frac{(2x)^2}{2!} + \frac{(2x)^4}{4!} = 1 - \frac{4x^2}{2} + \frac{16x^4}{24} = 1 - 2x^2 + \frac{2x^4}{3}

Common error: substituting x→2xx \to 2x but forgetting to apply the exponents — writing 2x22\frac{2x^2}{2} instead of (2x)22=4x22\frac{(2x)^2}{2} = \frac{4x^2}{2}.

Q9. If f′′(x)>0f''(x) > 0 on (a,b)(a, b) then on (a,b)(a, b), ff is:

(A) decreasing \quad (B) increasing \quad (C) concave down \quad (D) concave up

Answer: (D) f′′>0f'' > 0 means the gradient f′f' is increasing, which is the definition of concave up. The sign of f′′f'' says nothing directly about whether ff is increasing or decreasing (that depends on f′f').

Q10. A particle moves with v(t)=t2−3tv(t) = t^2 - 3t. The particle first comes to rest at t=t =

(A) 00 \quad (B) 11 \quad (C) 33 \quad (D) 1.51.5

Answer: (C) v(t)=0⇒t(t−3)=0⇒t=0v(t) = 0 \Rightarrow t(t-3) = 0 \Rightarrow t = 0 or t=3t = 3. At t=0t = 0 the particle starts from rest, so the first time it comes to rest again is at t=3t = 3.

Q11. The area enclosed by y=exy = e^x and the lines x=0x = 0, x=1x = 1, y=0y = 0 is:

(A) ee \quad (B) e−1e - 1 \quad (C) e+1e + 1 \quad (D) 11

Answer: (B) ∫01ex dx=[ex]01=e1−e0=e−1\displaystyle\int_0^1 e^x\,dx = [e^x]_0^1 = e^1 - e^0 = e - 1.

Q12. The volume generated by rotating y=2xy = 2x, 0≤x≤30 \leq x \leq 3, about the xx-axis is:

(A) 12π12\pi \quad (B) 24π24\pi \quad (C) 36π36\pi \quad (D) 72π72\pi

Answer: (C) V=π∫03(2x)2 dx=π∫034x2 dx=4π[x33]03=4π⋅9=36πV = \pi\displaystyle\int_0^3 (2x)^2\,dx = \pi\int_0^3 4x^2\,dx = 4\pi\left[\dfrac{x^3}{3}\right]_0^3 = 4\pi \cdot 9 = 36\pi.

Q13. The partial fraction decomposition of 5(x−1)(x+4)\dfrac{5}{(x-1)(x+4)} is:

(A) 1x−1−1x+4\dfrac{1}{x-1} - \dfrac{1}{x+4} \quad (B) 1x−1+1x+4\dfrac{1}{x-1} + \dfrac{1}{x+4} \quad (C) 5x−1−5x+4\dfrac{5}{x-1} - \dfrac{5}{x+4} \quad (D) 1x−1+4x+4\dfrac{1}{x-1} + \dfrac{4}{x+4}

Answer: (A) Let 5(x−1)(x+4)=Ax−1+Bx+4\dfrac{5}{(x-1)(x+4)} = \dfrac{A}{x-1} + \dfrac{B}{x+4}.

5=A(x+4)+B(x−1)5 = A(x+4) + B(x-1). Set x=1x=1: 5=5A⇒A=15 = 5A \Rightarrow A = 1. Set x=−4x=-4: 5=−5B⇒B=−15 = -5B \Rightarrow B = -1.

Q14. If ∫0ax2 dx=9\displaystyle\int_0^a x^2\,dx = 9, then a=a =

(A) 33 \quad (B) 3\sqrt{3} \quad (C) 273\sqrt[3]{27} \quad (D) 99

Answer: (A) [x33]0a=a33=9⇒a3=27⇒a=3\left[\dfrac{x^3}{3}\right]_0^a = \dfrac{a^3}{3} = 9 \Rightarrow a^3 = 27 \Rightarrow a = 3.

Note: (C) is also equal to 3, since 273=3\sqrt[3]{27} = 3 — but (A) is the standard form.

Q15. Using the Maclaurin series for ln⁡(1+x)\ln(1+x), the approximate value of ln⁡(1.1)\ln(1.1) to 4 decimal places (using up to the x4x^4 term) is:

(A) 0.09530.0953 \quad (B) 0.10000.1000 \quad (C) 0.09000.0900 \quad (D) 0.09090.0909

Answer: (A) With x=0.1x = 0.1:

ln⁡(1.1)≈0.1−(0.1)22+(0.1)33−(0.1)44=0.1−0.005+0.000333−0.000025=0.095308\ln(1.1) \approx 0.1 - \frac{(0.1)^2}{2} + \frac{(0.1)^3}{3} - \frac{(0.1)^4}{4} = 0.1 - 0.005 + 0.000333 - 0.000025 = 0.095308

Rounded to 4 d.p.: 0.09530.0953.

Q16. For f(x)=x3−3xf(x) = x^3 - 3x, the local minimum value is:

(A) −2-2 \quad (B) 00 \quad (C) 22 \quad (D) 33

Answer: (A) f′(x)=3x2−3=3(x−1)(x+1)=0⇒x=±1f'(x) = 3x^2 - 3 = 3(x-1)(x+1) = 0 \Rightarrow x = \pm 1.

f′′(x)=6xf''(x) = 6x. At x=1x = 1: f′′=6>0f'' = 6 > 0 (local min). f(1)=1−3=−2f(1) = 1 - 3 = -2.

Q17. Given the implicit equation x2y+y3=2xx^2y + y^3 = 2x, find dydx\dfrac{dy}{dx} at the point (1,1)(1, 1).

(A) 14\dfrac{1}{4} \quad (B) 00 \quad (C) −14-\dfrac{1}{4} \quad (D) −1-1

Answer: (B) Differentiate both sides with respect to xx:

ddx(x2y+y3)=ddx(2x)\frac{d}{dx}(x^2y + y^3) = \frac{d}{dx}(2x)

Using product rule on x2yx^2y and chain rule on y3y^3:

2xy+x2dydx+3y2dydx=22xy + x^2\frac{dy}{dx} + 3y^2\frac{dy}{dx} = 2

Collect terms with dydx\dfrac{dy}{dx}:

dydx(x2+3y2)=2−2xy\frac{dy}{dx}(x^2 + 3y^2) = 2 - 2xy

dydx=2−2xyx2+3y2\frac{dy}{dx} = \frac{2 - 2xy}{x^2 + 3y^2}

At (1,1)(1, 1): dydx=2−2(1)(1)12+3(1)2=04=0\dfrac{dy}{dx} = \dfrac{2 - 2(1)(1)}{1^2 + 3(1)^2} = \dfrac{0}{4} = 0

Common error: Forgetting to apply the product rule to x2yx^2y, leading to option (C).

Q18. A ladder 5 m long leans against a vertical wall. The bottom of the ladder slides away from the wall at 1 m/s. How fast is the top of the ladder sliding down the wall when the bottom is 3 m from the wall?

(A) −38-\dfrac{3}{8} m/s \quad (B) −12-\dfrac{1}{2} m/s \quad (C) −23-\dfrac{2}{3} m/s \quad (D) −34-\dfrac{3}{4} m/s

Answer: (D) Let xx = distance from wall to bottom of ladder, yy = height of top of ladder.

By Pythagoras: x2+y2=25x^2 + y^2 = 25

Given: dxdt=1\dfrac{dx}{dt} = 1 m/s. Find: dydt\dfrac{dy}{dt} when x=3x = 3.

When x=3x = 3: 9+y2=25⇒y=49 + y^2 = 25 \Rightarrow y = 4 m.

Differentiate the constraint with respect to time:

2xdxdt+2ydydt=02x\frac{dx}{dt} + 2y\frac{dy}{dt} = 0

dydt=−xydxdt\frac{dy}{dt} = -\frac{x}{y}\frac{dx}{dt}

Substitute x=3x = 3, y=4y = 4, and dxdt=1\dfrac{dx}{dt} = 1:

dydt=−34(1)=−34 m/s\frac{dy}{dt} = -\frac{3}{4}(1) = -\frac{3}{4} \text{ m/s}

The negative sign indicates the ladder is sliding down.

Common error: Forgetting the negative sign from differentiation, leading to option (C) with positive value, or incorrectly computing xy\dfrac{x}{y} as 43\dfrac{4}{3}, leading to option (B).


Key Formulas

Complete Calculus Formula Reference

Limits

FormulaNotes
lim⁡x→0sin⁡xx=1\displaystyle\lim_{x \to 0}\dfrac{\sin x}{x} = 1Fundamental limit
lim⁡x→0ex−1x=1\displaystyle\lim_{x \to 0}\dfrac{e^x - 1}{x} = 1Derived from series
L’Hôpital: lim⁡x→af(x)g(x)=lim⁡x→af′(x)g′(x)\displaystyle\lim_{x \to a}\dfrac{f(x)}{g(x)} = \lim_{x \to a}\dfrac{f'(x)}{g'(x)}Only for 00\frac{0}{0} or ∞∞\frac{\infty}{\infty}

Differentiation Rules

RuleFormula
Powerddx[xn]=nxn−1\frac{d}{dx}[x^n] = nx^{n-1}
Productddx[uv]=u′v+uv′\frac{d}{dx}[uv] = u'v + uv'
Quotientddx ⁣[uv]=u′v−uv′v2\frac{d}{dx}\!\left[\frac{u}{v}\right] = \frac{u'v - uv'}{v^2}
Chainddx[f(g(x))]=f′(g(x))⋅g′(x)\frac{d}{dx}[f(g(x))] = f'(g(x)) \cdot g'(x)
Implicit: yny^nnyn−1dydxny^{n-1}\frac{dy}{dx}

Key Derivatives

f(x)f(x)f′(x)f'(x)
sin⁡x\sin xcos⁡x\cos x
cos⁡x\cos x−sin⁡x-\sin x
tan⁡x\tan xsec⁡2x\sec^2 x
exe^xexe^x
ln⁡x\ln x1/x1/x
arcsin⁡x\arcsin x1/1−x21/\sqrt{1-x^2}
arctan⁡x\arctan x1/(1+x2)1/(1+x^2)

Integration

Rule / FormulaNotes
∫xn dx=xn+1n+1+C\int x^n\,dx = \frac{x^{n+1}}{n+1} + Cn≠−1n \neq -1
∫1x dx=ln⁡∣x∣+C\int \frac{1}{x}\,dx = \ln\lvert x\rvert + CAbsolute value required
∫ex dx=ex+C\int e^x\,dx = e^x + C
∫sin⁡x dx=−cos⁡x+C\int \sin x\,dx = -\cos x + CNote sign
∫cos⁡x dx=sin⁡x+C\int \cos x\,dx = \sin x + C
∫sec⁡2x dx=tan⁡x+C\int \sec^2 x\,dx = \tan x + C
∫u dv=uv−∫v du\int u\,dv = uv - \int v\,duIntegration by parts
Substitution: ∫f(g(x))g′(x) dx=∫f(u) du\int f(g(x))g'(x)\,dx = \int f(u)\,duu=g(x)u = g(x)
∫1x2+a2 dx=1aarctan⁡ ⁣(xa)+C\int \frac{1}{x^2+a^2}\,dx = \frac{1}{a}\arctan\!\left(\frac{x}{a}\right) + C
∫1a2−x2 dx=arcsin⁡ ⁣(xa)+C\int \frac{1}{\sqrt{a^2-x^2}}\,dx = \arcsin\!\left(\frac{x}{a}\right) + C

Applications

QuantityFormula
Tangent gradient at x=ax=am=f′(a)m = f'(a)
Normal gradient at x=ax=am=−1/f′(a)m = -1/f'(a)
Area under curveA=∫ab∣f(x)∣ dxA = \int_a^b \lvert f(x)\rvert\,dx
Area between curvesA=∫ab[f(x)−g(x)] dxA = \int_a^b [f(x)-g(x)]\,dx
Volume of revolution (xx-axis)V=π∫ab[f(x)]2 dxV = \pi\int_a^b [f(x)]^2\,dx
Displacement from vvs=∫v dts = \int v\,dt
Distance from vvd=∫∣v∣ dtd = \int \lvert v\rvert\,dt

Differential Equations

TypeMethod
Separable: dydx=f(x)g(y)\frac{dy}{dx} = f(x)g(y)∫dyg(y)=∫f(x) dx\int\frac{dy}{g(y)} = \int f(x)\,dx
Exponential growth/decayN=N0e±ktN = N_0 e^{\pm kt}
Newton’s cooling: dθdt=−kθ\frac{d\theta}{dt} = -k\thetaθ=θ0e−kt\theta = \theta_0 e^{-kt}, θ=T−Tenv\theta = T - T_{\text{env}}

Maclaurin Series

FunctionSeriesInterval
exe^x∑n=0∞xnn!=1+x+x22!+⋯\displaystyle\sum_{n=0}^{\infty}\frac{x^n}{n!} = 1 + x + \frac{x^2}{2!} + \cdotsAll xx
sin⁡x\sin x∑n=0∞(−1)nx2n+1(2n+1)!=x−x36+x5120−⋯\displaystyle\sum_{n=0}^{\infty}\frac{(-1)^n x^{2n+1}}{(2n+1)!} = x - \frac{x^3}{6} + \frac{x^5}{120} - \cdotsAll xx
cos⁡x\cos x∑n=0∞(−1)nx2n(2n)!=1−x22+x424−⋯\displaystyle\sum_{n=0}^{\infty}\frac{(-1)^n x^{2n}}{(2n)!} = 1 - \frac{x^2}{2} + \frac{x^4}{24} - \cdotsAll xx
ln⁡(1+x)\ln(1+x)∑n=1∞(−1)n+1xnn=x−x22+x33−⋯\displaystyle\sum_{n=1}^{\infty}\frac{(-1)^{n+1}x^n}{n} = x - \frac{x^2}{2} + \frac{x^3}{3} - \cdots−1<x≤1-1 < x \leq 1

Mixed Practice — Exam Style

How to use this section: Unlike topic-specific practice, these questions are interleaved — they mix all topics from this guide in random order. Before answering, identify which concept or topic area the question is testing. This is exactly the skill you need on Paper 2 and Paper 3, where you don’t know in advance which topic each question covers.

  1. [Integration] Evaluate ∫01xex2 dx\displaystyle\int_0^1 x e^{x^2}\,dx.

    A. e−12\dfrac{e-1}{2}

    B. e−1e - 1

    C. 12\dfrac{1}{2}

    D. e2−1e^2 - 1

  2. [Limits] Evaluate lim⁡x→0sin⁡3x5x\displaystyle\lim_{x \to 0} \dfrac{\sin 3x}{5x}.

    A. 00

    B. 35\dfrac{3}{5}

    C. 11

    D. 53\dfrac{5}{3}

  3. [Differential Equations] The rate of change of a population PP satisfies dPdt=0.04P\dfrac{dP}{dt} = 0.04P. If P(0)=500P(0) = 500, find P(10)P(10).

    A. 500+0.04(10)500 + 0.04(10)

    B. 500e0.4500 e^{0.4}

    C. 500e4500 e^{4}

    D. 500(1.04)10500(1.04)^{10}

  4. [Applications of Derivatives] A function ff has f′(x)=(x−2)2(x+1)f'(x) = (x-2)^2(x+1). Which statement is correct?

    A. ff has a local minimum at x=2x = 2 and a local maximum at x=−1x = -1

    B. ff has a local minimum at x=−1x = -1 only; x=2x = 2 is a stationary point of inflection

    C. ff has local minima at both x=−1x = -1 and x=2x = 2

    D. ff has a local maximum at x=−1x = -1 and no stationary point at x=2x = 2

  5. [Maclaurin Series] The first three non-zero terms of the Maclaurin series of cos⁡(2x)\cos(2x) are:

    A. 1−2x2+2x431 - 2x^2 + \dfrac{2x^4}{3}

    B. 1−2x+2x21 - 2x + 2x^2

    C. 2x−8x36+32x51202x - \dfrac{8x^3}{6} + \dfrac{32x^5}{120}

    D. 1+2x2−2x431 + 2x^2 - \dfrac{2x^4}{3}

  6. [Differentiation Rules] Find dydx\dfrac{dy}{dx} if y=ln⁡(sin⁡x)y = \ln(\sin x).

    A. 1sin⁡x\dfrac{1}{\sin x}

    B. cos⁡x\cos x

    C. cot⁡x\cot x

    D. −cot⁡x-\cot x

  7. [Volumes of Revolution] The region bounded by y=xy = \sqrt{x}, the xx-axis, and x=4x = 4 is rotated 2π2\pi radians about the xx-axis. The exact volume is:

    A. 4π4\pi

    B. 8π8\pi

    C. 16π16\pi

    D. 32π32\pi

  8. [Limits — L’Hôpital] Use L’Hôpital’s rule to evaluate lim⁡x→0ex−1−xx2\displaystyle\lim_{x \to 0} \dfrac{e^x - 1 - x}{x^2}.

    A. 00

    B. 14\dfrac{1}{4}

    C. 12\dfrac{1}{2}

    D. 11

  9. [Differential Equations] The general solution of dydx=xy\dfrac{dy}{dx} = \dfrac{x}{y} is:

    A. y=x+Cy = x + C

    B. y2=x2+Cy^2 = x^2 + C

    C. y=x22+Cy = \dfrac{x^2}{2} + C

    D. ln⁡y=ln⁡x+C\ln y = \ln x + C

  10. [Integration by Parts] Evaluate ∫xcos⁡x dx\displaystyle\int x \cos x\,dx.

    A. xsin⁡x+cos⁡x+Cx \sin x + \cos x + C

    B. xsin⁡x−cos⁡x+Cx \sin x - \cos x + C

    C. −xsin⁡x+cos⁡x+C-x \sin x + \cos x + C

    D. sin⁡x−xcos⁡x+C\sin x - x\cos x + C

Show Answers
  1. A — e−12\dfrac{e-1}{2}. Substitute u=x2u = x^2, du=2x dxdu = 2x\,dx, so the integral becomes 12∫01eu du=12[eu]01=e−12\dfrac{1}{2}\int_0^1 e^u\,du = \dfrac{1}{2}[e^u]_0^1 = \dfrac{e-1}{2}. B is a common error from forgetting the factor of 12\frac{1}{2}.

  2. B — 35\dfrac{3}{5}. Use the standard limit lim⁡u→0sin⁡uu=1\lim_{u\to 0}\frac{\sin u}{u}=1: rewrite as 35⋅sin⁡3x3x→35\frac{3}{5}\cdot\frac{\sin 3x}{3x}\to\frac{3}{5}. C (answer of 1) is the trap when students forget to account for the coefficient 3 in the numerator.

  3. B — 500e0.4500e^{0.4}. Exponential growth P=P0ektP = P_0 e^{kt}, so P(10)=500e0.04×10=500e0.4P(10) = 500e^{0.04 \times 10} = 500e^{0.4}. D uses compound interest formula — a distractor for students who confuse continuous and discrete growth.

  4. B — Local minimum at x=−1x = -1 only; x=2x = 2 is a stationary point of inflection. At x=−1x=-1, f′f' changes from negative to positive (local min). At x=2x=2, f′=0f' = 0 but (x−2)2≥0(x-2)^2 \geq 0 on both sides, so f′f' does not change sign — it is a stationary point of inflection.

  5. A — 1−2x2+2x431 - 2x^2 + \dfrac{2x^4}{3}. Substitute 2x2x into cos⁡u=1−u22!+u44!−⋯\cos u = 1 - \frac{u^2}{2!} + \frac{u^4}{4!} - \cdots: 1−(2x)22+(2x)424=1−2x2+2x431 - \frac{(2x)^2}{2} + \frac{(2x)^4}{24} = 1 - 2x^2 + \frac{2x^4}{3}.

  6. C — cot⁡x\cot x. Chain rule: ddx[ln⁡(sin⁡x)]=cos⁡xsin⁡x=cot⁡x\frac{d}{dx}[\ln(\sin x)] = \frac{\cos x}{\sin x} = \cot x. D is a trap — the derivative of ln⁡(cos⁡x)\ln(\cos x) is −tan⁡x-\tan x, not −cot⁡x-\cot x here.

  7. B — 8π8\pi. V=π∫04(x)2 dx=π∫04x dx=π[x22]04=π⋅8=8πV = \pi\int_0^4 (\sqrt{x})^2\,dx = \pi\int_0^4 x\,dx = \pi\left[\frac{x^2}{2}\right]_0^4 = \pi \cdot 8 = 8\pi.

  8. C — 12\dfrac{1}{2}. lim⁡x→0ex−1−xx2\lim_{x\to 0}\frac{e^x - 1 - x}{x^2}: first application of L’Hôpital gives ex−12x\frac{e^x - 1}{2x} (00\frac{0}{0} still), apply again: ex2→12\frac{e^x}{2}\to\frac{1}{2}. Students who apply L’Hôpital only once get 00\frac{0}{0} and may incorrectly conclude the limit is 0.

  9. B — y2=x2+Cy^2 = x^2 + C. Separate: y dy=x dxy\,dy = x\,dx, integrate both sides: y22=x22+C1\frac{y^2}{2} = \frac{x^2}{2} + C_1, multiply by 2: y2=x2+Cy^2 = x^2 + C. Note the constant absorbs the factor of 2.

  10. A — xsin⁡x+cos⁡x+Cx\sin x + \cos x + C. Let u=xu = x, dv=cos⁡x dxdv = \cos x\,dx; then du=dxdu = dx, v=sin⁡xv = \sin x. IBP: xsin⁡x−∫sin⁡x dx=xsin⁡x+cos⁡x+Cx\sin x - \int\sin x\,dx = x\sin x + \cos x + C. B has the wrong sign on cos⁡x\cos x.


IB Math IA Ideas — Calculus

Exploration topics from this chapter:

  • Modelling drug concentration — Use a first-order differential equation dCdt=−kC\frac{dC}{dt} = -kC to model how a drug is eliminated from the bloodstream. Investigate how the elimination constant kk varies across drugs, optimise dosing intervals to keep concentration within a therapeutic window, and compare your model against real pharmacokinetic data.

  • Lorenz curves and the Gini coefficient — A Lorenz curve L(x)L(x) describes income distribution; the Gini coefficient G=1−2∫01L(x) dxG = 1 - 2\int_0^1 L(x)\,dx measures inequality. Download World Bank income-share data for two countries and use numerical integration to calculate and compare their Gini coefficients. Extend by fitting a functional form to the curve.

  • The Brachistochrone problem — Find the curve of fastest descent between two points under gravity. Derive the cycloid parametrically and verify it is faster than a straight line by comparing definite integrals of travel time. This connects differentiation, integration, and parametric equations in one elegant problem.

  • Population growth: logistic vs exponential — The logistic model dPdt=rP(1−PK)\frac{dP}{dt} = rP\left(1 - \frac{P}{K}\right) accounts for carrying capacity. Source census data for a real population, solve both ODEs analytically, and use least-squares or residual analysis to determine which model fits better.

  • Optimising packaging — Minimise the surface area of a cylindrical tin for a fixed volume using dSdr=0\frac{dS}{dr} = 0. Extend to elliptical cross-sections, conical lids, or prism shapes, and compare your theoretical optimum against the dimensions of real commercial products.

  • Volumes of revolution in architecture — Model a dome, arch, or vase using a curve y=f(x)y = f(x) and compute the volume using V=π∫ab[f(x)]2 dxV = \pi\int_a^b [f(x)]^2\,dx. Photograph a real object, digitise its profile, fit a function, and compare the calculated volume to the manufacturer’s stated capacity.

  • The Mean Value Theorem and speed cameras — Prove rigorously that if a car’s average speed between two cameras exceeds the limit, then by the Mean Value Theorem it must have instantaneously exceeded the limit at some point. Extend to discuss the mathematics behind average-speed enforcement and how it differs from point-speed checks.

Tip: A strong IA has a clear personal engagement angle. Pick a topic that connects to something you genuinely find interesting — sports, medicine, economics, or architecture — and let the mathematics serve your question, not the other way around.


November 2026 Prediction Questions

These are NOT official IB questions. These are trend-based practice questions written to reflect the topic areas and question styles most likely to appear on the November 2026 IB Math AA HL Paper 2. Based on recent exam patterns (2022–2025), expect heavy weighting on: integration techniques, differential equations, optimization, and Maclaurin series.


Question 1 [Integration by Parts] [~7 marks]

Evaluate the definite integral

∫0πxsin⁡x dx\int_0^{\pi} x \sin x \, dx

showing all working. State the integration technique used.

Show Solution

Technique: Integration by parts — ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du

Step 1: Choose uu and dvdv.

Let u=xu = x and dv=sin⁡x dxdv = \sin x \, dx.

Then du=dxdu = dx and v=−cos⁡xv = -\cos x.

Step 2: Apply the integration by parts formula.

∫0πxsin⁡x dx=[−xcos⁡x]0π−∫0π(−cos⁡x) dx\int_0^{\pi} x \sin x \, dx = \Bigl[-x\cos x\Bigr]_0^{\pi} - \int_0^{\pi}(-\cos x)\,dx

=[−xcos⁡x]0π+∫0πcos⁡x dx= \Bigl[-x\cos x\Bigr]_0^{\pi} + \int_0^{\pi}\cos x\,dx

Step 3: Evaluate the remaining integral.

∫0πcos⁡x dx=[sin⁡x]0π=sin⁡π−sin⁡0=0−0=0\int_0^{\pi}\cos x\,dx = \Bigl[\sin x\Bigr]_0^{\pi} = \sin\pi - \sin 0 = 0 - 0 = 0

Step 4: Evaluate the boundary term.

[−xcos⁡x]0π=(−πcos⁡π)−(−0⋅cos⁡0)=(−π)(−1)−0=π\Bigl[-x\cos x\Bigr]_0^{\pi} = (-\pi\cos\pi) - (-0\cdot\cos 0) = (-\pi)(-1) - 0 = \pi

Step 5: Combine.

∫0πxsin⁡x dx=π+0=π\int_0^{\pi} x \sin x \, dx = \pi + 0 = \pi

Answer: ∫0πxsin⁡x dx=π\displaystyle\int_0^{\pi} x \sin x \, dx = \pi


Question 2 [Optimization] [~8 marks]

A closed cylindrical tin has a fixed volume of V=250π cm3V = 250\pi \text{ cm}^3. The total surface area of the tin is SS.

(a) Show that S=2πr2+500πrS = 2\pi r^2 + \dfrac{500\pi}{r}, where rr is the radius of the base in cm.

(b) Find the value of rr that minimizes SS, and verify it is a minimum.

(c) Find the minimum surface area, giving your answer in exact form.

Show Solution

Part (a) — Setting up the expression for SS

A closed cylinder has surface area S=2πr2+2πrhS = 2\pi r^2 + 2\pi r h.

Volume constraint: πr2h=250π\pi r^2 h = 250\pi, so h=250r2h = \dfrac{250}{r^2}.

Substitute:

S=2πr2+2πr⋅250r2=2πr2+500πr✓S = 2\pi r^2 + 2\pi r \cdot \frac{250}{r^2} = 2\pi r^2 + \frac{500\pi}{r} \qquad \checkmark

Part (b) — Minimizing SS

Step 1: Differentiate with respect to rr.

dSdr=4πr−500πr2\frac{dS}{dr} = 4\pi r - \frac{500\pi}{r^2}

Step 2: Set dSdr=0\dfrac{dS}{dr} = 0.

4πr=500πr24\pi r = \frac{500\pi}{r^2}

4r3=5004r^3 = 500

r3=125  ⟹  r=5 cmr^3 = 125 \implies r = 5 \text{ cm}

Step 3: Verify it is a minimum using the second derivative.

d2Sdr2=4π+1000πr3\frac{d^2S}{dr^2} = 4\pi + \frac{1000\pi}{r^3}

At r=5r = 5:

d2Sdr2=4π+1000π125=4π+8π=12π>0\frac{d^2S}{dr^2} = 4\pi + \frac{1000\pi}{125} = 4\pi + 8\pi = 12\pi > 0

Since d2Sdr2>0\dfrac{d^2S}{dr^2} > 0, this is a local (and global) minimum.

Part (c) — Minimum surface area

Smin⁡=2π(5)2+500π5=50π+100π=150π cm2S_{\min} = 2\pi(5)^2 + \frac{500\pi}{5} = 50\pi + 100\pi = 150\pi \text{ cm}^2

Answer: r=5r = 5 cm gives minimum surface area Smin⁡=150π cm2≈471 cm2S_{\min} = 150\pi \text{ cm}^2 \approx 471 \text{ cm}^2.


Question 3 [Separable Differential Equation] [~7 marks]

Consider the differential equation

dydx=2xy+1,y>−1\frac{dy}{dx} = \frac{2x}{y+1}, \quad y > -1

(a) Find the general solution, expressing yy explicitly in terms of xx.

(b) Find the particular solution satisfying y(0)=2y(0) = 2.

Show Solution

Part (a) — General solution

Step 1: Separate variables.

(y+1) dy=2x dx(y + 1)\,dy = 2x\,dx

Step 2: Integrate both sides.

∫(y+1) dy=∫2x dx\int (y+1)\,dy = \int 2x\,dx

(y+1)22=x2+C1\frac{(y+1)^2}{2} = x^2 + C_1

(y+1)2=2x2+Cwhere C=2C1(y+1)^2 = 2x^2 + C \quad \text{where } C = 2C_1

Step 3: Solve for yy (using y>−1y > -1).

y+1=2x2+Cy + 1 = \sqrt{2x^2 + C}

y=2x2+C−1y = \sqrt{2x^2 + C} - 1

Part (b) — Particular solution

Apply initial condition y(0)=2y(0) = 2:

2=2(0)2+C−12 = \sqrt{2(0)^2 + C} - 1

3=C  ⟹  C=93 = \sqrt{C} \implies C = 9

Answer: The particular solution is y=2x2+9−1y = \sqrt{2x^2 + 9} - 1.

Verification: At x=0x = 0: y=9−1=2y = \sqrt{9} - 1 = 2 ✓


Question 4 [Maclaurin Series] [~7 marks]

(a) Write down the Maclaurin series for sin⁡u\sin u up to and including the term in u5u^5.

(b) Hence find the first three non-zero terms of the Maclaurin series for sin⁡(x2)\sin(x^2).

(c) State the interval of validity of the series in part (b).

(d) Use the series from part (b) to find an approximation for ∫00.5sin⁡(x2) dx\displaystyle\int_0^{0.5} \sin(x^2)\,dx, giving your answer to 4 significant figures.

Show Solution

Part (a) — Maclaurin series for sin⁡u\sin u

sin⁡u=u−u33!+u55!−⋯=u−u36+u5120−⋯\sin u = u - \frac{u^3}{3!} + \frac{u^5}{5!} - \cdots = u - \frac{u^3}{6} + \frac{u^5}{120} - \cdots

Part (b) — Series for sin⁡(x2)\sin(x^2)

Substitute u=x2u = x^2:

sin⁡(x2)=x2−(x2)36+(x2)5120−⋯\sin(x^2) = x^2 - \frac{(x^2)^3}{6} + \frac{(x^2)^5}{120} - \cdots

sin⁡(x2)=x2−x66+x10120−⋯\sin(x^2) = x^2 - \frac{x^6}{6} + \frac{x^{10}}{120} - \cdots

Part (c) — Interval of validity

The Maclaurin series for sin⁡u\sin u converges for all u∈Ru \in \mathbb{R}. Since u=x2u = x^2 is defined for all x∈Rx \in \mathbb{R}, the series for sin⁡(x2)\sin(x^2) is valid for all x∈Rx \in \mathbb{R}.

Part (d) — Approximation of the integral

∫00.5sin⁡(x2) dx≈∫00.5(x2−x66+x10120)dx\int_0^{0.5}\sin(x^2)\,dx \approx \int_0^{0.5}\left(x^2 - \frac{x^6}{6} + \frac{x^{10}}{120}\right)dx

=[x33−x742+x111320]00.5= \left[\frac{x^3}{3} - \frac{x^7}{42} + \frac{x^{11}}{1320}\right]_0^{0.5}

Evaluate at x=0.5x = 0.5:

=(0.5)33−(0.5)742+(0.5)111320= \frac{(0.5)^3}{3} - \frac{(0.5)^7}{42} + \frac{(0.5)^{11}}{1320}

=0.1253−0.007812542+0.000488…1320= \frac{0.125}{3} - \frac{0.0078125}{42} + \frac{0.000488\ldots}{1320}

≈0.041667−0.000186+0.0000004\approx 0.041667 - 0.000186 + 0.0000004

≈0.04148\approx 0.04148

Answer: ∫00.5sin⁡(x2) dx≈0.04148\displaystyle\int_0^{0.5}\sin(x^2)\,dx \approx 0.04148 (to 4 s.f.)


Question 5 [Area Between Curves] [~8 marks]

The curves f(x)=x2−2xf(x) = x^2 - 2x and g(x)=4−x2g(x) = 4 - x^2 intersect at two points.

(a) Find the xx-coordinates of the two intersection points.

(b) Find the exact area of the region enclosed between the two curves.

Show Solution

Part (a) — Intersection points

Set f(x)=g(x)f(x) = g(x):

x2−2x=4−x2x^2 - 2x = 4 - x^2

2x2−2x−4=02x^2 - 2x - 4 = 0

x2−x−2=0x^2 - x - 2 = 0

(x−2)(x+1)=0(x-2)(x+1) = 0

x=2orx=−1x = 2 \quad \text{or} \quad x = -1

The curves intersect at x=−1x = -1 and x=2x = 2.

Part (b) — Area between the curves

Step 1: Determine which curve is on top on [−1,2][-1, 2].

Test x=0x = 0: f(0)=0f(0) = 0, g(0)=4g(0) = 4. Since g(0)>f(0)g(0) > f(0), we have g(x)≥f(x)g(x) \geq f(x) on [−1,2][-1, 2].

Step 2: Set up the integral.

A=∫−12[g(x)−f(x)] dx=∫−12[(4−x2)−(x2−2x)] dxA = \int_{-1}^{2}\bigl[g(x) - f(x)\bigr]\,dx = \int_{-1}^{2}\bigl[(4 - x^2) - (x^2 - 2x)\bigr]\,dx

=∫−12(4−2x2+2x) dx= \int_{-1}^{2}(4 - 2x^2 + 2x)\,dx

Step 3: Integrate.

=[4x−2x33+x2]−12= \left[4x - \frac{2x^3}{3} + x^2\right]_{-1}^{2}

Step 4: Evaluate at the bounds.

At x=2x = 2:

4(2)−2(8)3+4=8−163+4=12−163=36−163=2034(2) - \frac{2(8)}{3} + 4 = 8 - \frac{16}{3} + 4 = 12 - \frac{16}{3} = \frac{36 - 16}{3} = \frac{20}{3}

At x=−1x = -1:

4(−1)−2(−1)3+1=−4+23+1=−3+23=−9+23=−734(-1) - \frac{2(-1)}{3} + 1 = -4 + \frac{2}{3} + 1 = -3 + \frac{2}{3} = \frac{-9 + 2}{3} = -\frac{7}{3}

Step 5: Subtract.

A=203−(−73)=203+73=273=9A = \frac{20}{3} - \left(-\frac{7}{3}\right) = \frac{20}{3} + \frac{7}{3} = \frac{27}{3} = 9

Answer: The exact area enclosed between the two curves is 99 square units.

IB Formula Booklet — Complex Numbers

Modulus & Polar Form

GIVENz = r(cosθ + i sinθ) = r cis θ
GIVENz = reiθ (Euler form)
MEMORISE|z| = √(a² + b²)
MEMORISEarg(z) — sketch point, use quadrant formula

Polar Multiplication & Division

GIVENz&sub1;z&sub2; = r&sub1;r&sub2; cis(θ&sub1; + θ&sub2;)
GIVENz&sub1;/z&sub2; = (r&sub1;/r&sub2;) cis(θ&sub1; − θ&sub2;)

De Moivre's Theorem

GIVEN(r cis θ)n = rn cis(nθ)
MEMORISEz + 1/z = 2cosθ (when |z|=1)
MEMORISEz − 1/z = 2i sinθ (when |z|=1)

nth Roots

GIVENw1/n = r1/n cis((θ + 2πk)/n), k=0..n-1
MEMORISESum of nth roots of unity = 0
MEMORISE1 + ω + ω² = 0 (cube roots)

Conjugate & Arithmetic

MEMORISEz* = a − bi
MEMORISEz · z* = |z|² (always real)
MEMORISEz + z* = 2Re(z)
MEMORISEz − z* = 2i Im(z)

Loci

MEMORISE|z − a| = r → Circle, centre a, radius r
MEMORISE|z − a| = |z − b| → Perpendicular bisector
MEMORISEarg(z − a) = θ → Ray from a

Vieta's Formulas

MEMORISEz² + az + b = 0: sum = −a, product = b
MEMORISEConjugate root theorem: real coeff → roots come in conjugate pairs