1.1Key terms1.2Laws and key relationships1.3Rigorous Derivation of Reciprocal Trigonometric Functions1.4Logarithmic and General Exponential Differentiation Techniques1.5Parametric and Implicit Second-Order Derivatives1.6Worked examples1.7Exam tips1.8Real-world applications1.9Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula1.10📌 Comprehensive Scientific Terminology Dictionary:1.11🔍 In-Depth Explanations, Deductions & Multi-Book Insights:1.12Lesson summary1.1The counting principle1.2Permutations (nPr)1.3Combinations (nCr)1.4Worked examples on counting, permutations and combinations1.5Recall: counting principle, permutations and combinations1.61-1 (a) Pascal's triangle and the binomial expansion1.71-1 (b) The general term1.81-1 (c) The middle term1.91-2 The term containing xk and the term free of x1.101-3 (a) The ratio between two consecutive terms1.111-3 (b) The greatest term1.12Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula1.13Lesson 1 - Counting Principle, Permutations and Combinations and the Binomial Theorem1.14Lesson summary1.1Key terms1.2Laws and key relationships1.3Geometry of 3D Vectors and Scalar/Cross Product Physics1.4Equations of Straight Lines in Three Dimensions1.5Equations of Planes and Perpendicular Distance Formulas1.6Worked examples1.7Exam tips1.8Real-world applications1.9Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula1.10📌 Comprehensive Scientific Terminology Dictionary:1.11⚖️ Governing Physical Laws & Mathematical Relations:1.12🔍 In-Depth Explanations, Deductions & Multi-Book Insights:1.13Lesson summary1.11 Smooth and rough surfaces1.22 Properties of the static friction force1.33 Kinetic friction force1.44 The resultant reaction R′1.55 The angle of friction1.66 Equilibrium of a body on a rough horizontal plane1.77 Equilibrium of a body on a rough inclined plane1.88 Conditions of equilibrium and rigid bodies with friction1.13-1 (a) Indefinite integrals of exponential functions1.23-1 (b) Indefinite integrals of logarithmic functions1.33-2 (a) The differential and the standard integrals1.43-2 (b) Integration by substitution1.53-2 (c) Integration by parts1.63-2 (d) Applications of the indefinite integral1.73-3 (a) The definite integral and the fundamental theorem of calculus1.83-3 (b) Properties of the definite integral1.93-3 (c) Definite integral by substitution, odd and even functions1.103-4 (a) Area of a plane region1.113-4 (b) Volumes of solids of revolution1.12Key Scientific Tables & Anatomical Diagrams Extracted from Official Curricula1.12-1 (a) Polar coordinates and the Argand plane1.22-1 (b) Modulus, amplitude and principal amplitude1.32-1 (c) The trigonometric (polar) form of a complex number1.42-1 (d) Product and quotient in trigonometric form1.52-1 (e) The exponential (Euler) form1.62-2 (a) De Moivre's theorem for a positive integer power1.72-2 (b) De Moivre's theorem for a rational power and the roots of a complex number1.82-3 The cube roots of unity1.11 Momentum and its change1.22 Newton's first law, inertia and force1.33 Newton's second law, the equation of motion and variable mass1.44 Newton's third law, lifts and scales1.55 Bodies connected by a string over a smooth pulley1.66 Impulse1.77 Work1.88 Kinetic energy and the work-energy principle1.99 Potential energy and conservation of energy1.1010 Power| Comparison aspect | Main idea | Example | Keywords |
|---|---|---|---|
| • |
| — | stationarypointcurvetangent |
| Local maximum | f′ changes from positive to negative as x increases through the point (the curve rises then falls) | — | changespositivenegativeincreases |
| Local minimum | f′ changes from negative to positive | — | changesnegativepositive |
| Point of inflection (stationary) | f′ does not change sign — it keeps the same sign on both sides | f(x) = x3 at x = 0 | doeschangesignkeeps |
| Curve Behaviour |
| — | wirelikehillvalley |

| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Domain |
| valuesexcludeddenominatorseven |
| Intercepts | set x = 0 for the y-intercept and solve f(x) = 0 for the x-intercepts | solve |
| Symmetry |
| evenfunctionsymmetricaxis |
| Asymptotes |
| verticaldenominatorvanisheshorizontal |
| Stationary points |
| nature |
| Points of inflection | and the concavity on each side | concavityside |
| End behaviour |
| signleadingtermthen |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| Fencing |
| rectangularfieldareafenced |
| Open box |
| squaresquaressidefold |
| Closest point |
| nearestminimisepointsdistance |
| Revenue |
| 100xunitsprice |
| Comparison aspect | Main idea | Keywords |
|---|---|---|
| f′ = 0 is necessary, not sufficient. |
| Everystationarypointmaximum |
| f″ = 0 is not an inflection point. | It must be accompanied by a change of concavity (x4 is the standard counter-example) | mustaccompaniedchangeconcavity |
| Endpoints of a closed interval. |
| absolutegreatestleastvalue |
| Maximum value versus point. |
| questionabscissaAnswerexactly |
| Constant of integration when reconstructing f. |
| Givenpointfindbefore |
| Units and “in words”. |
| Optimisationanswerslosemarks |
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