IB HL

IB Math AA HL Topic 3: Geometry and Trigonometry

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IB Math AA HL — Geometry & Trigonometry

Complete Study Guide

Topics Covered

  1. 3D Geometry — distance, midpoint, volume, surface area
  2. Right-Angle and Non-Right-Angle Trigonometry — sine rule, cosine rule, area
  3. Applications — bearings, angles of elevation and depression
  4. Radian Measure, Arc Length, Sector Area
  5. The Unit Circle and Exact Trigonometric Values
  6. Trigonometric Identities — Pythagorean, double angle, compound angle HL
  7. Trigonometric Functions and Their Graphs
  8. Solving Trigonometric Equations
  9. Reciprocal and Inverse Trigonometric Functions HL
  10. Vector Algebra — notation, addition, dot product, cross product HL
  11. Vector Equations of Lines in 2D and 3D HL
  12. Vector Equations of Planes HL
  13. Intersections of Lines and Planes HL
  14. Practice Exam Questions

Topic 3 of the IB Math AA HL syllabus — 25 SL hours, 51 HL hours — Paper 1 and Paper 2

Why this topic matters: Topic 3 has the most HL teaching hours (51) of any topic in Math AA HL. Vectors alone regularly appear as a 15–20 mark extended-response question on Paper 2, and trig identities appear almost every year on Paper 1 (no calculator). Mastering this topic is essential for a 6 or 7.

What is and is not in the formula booklet: The sine rule, cosine rule, area of a triangle formula, arc length and sector area formulas, the Pythagorean identity, double angle formulas, and compound angle formulas are all given. The unit circle exact values are NOT given — you must know sin\sin, cos\cos, and tan\tan of 00, π6\frac{\pi}{6}, π4\frac{\pi}{4}, π3\frac{\pi}{3}, π2\frac{\pi}{2} from memory. The cross product formula is given. Vector line and plane equations follow from definitions you must know.


Section 1: 3D Geometry

1.1 Distance and Midpoint in 3D

In three-dimensional space, points are described by coordinates (x,y,z)(x, y, z). The distance between points A(x1,y1,z1)A(x_1, y_1, z_1) and B(x2,y2,z2)B(x_2, y_2, z_2) is a direct extension of the 2D Pythagorean theorem:

d=(x2x1)2+(y2y1)2+(z2z1)2d = \sqrt{(x_2 - x_1)^2 + (y_2 - y_1)^2 + (z_2 - z_1)^2}

The midpoint MM of segment ABAB is:

M=(x1+x22, y1+y22, z1+z22)M = \left(\frac{x_1 + x_2}{2},\ \frac{y_1 + y_2}{2},\ \frac{z_1 + z_2}{2}\right)

Distance in 3D

Find the distance between P(1,2,4)P(1, -2, 4) and Q(5,0,1)Q(5, 0, 1), and the midpoint of PQPQ.

d=(51)2+(0(2))2+(14)2=16+4+9=29d = \sqrt{(5-1)^2 + (0-(-2))^2 + (1-4)^2} = \sqrt{16 + 4 + 9} = \sqrt{29}

M=(1+52, 2+02, 4+12)=(3, 1, 52)M = \left(\frac{1+5}{2},\ \frac{-2+0}{2},\ \frac{4+1}{2}\right) = \left(3,\ -1,\ \frac{5}{2}\right)

1.2 Volumes and Surface Areas of 3D Solids

The IB expects you to apply standard formulae to composite 3D problems. All the following formulas are in the formula booklet.

Key 3D Solid Formulas

SolidVolumeSurface Area
Cuboid (l×w×hl \times w \times h)lwhlwh2(lw+lh+wh)2(lw + lh + wh)
Cylinder (radius rr, height hh)πr2h\pi r^2 h2πr2+2πrh2\pi r^2 + 2\pi r h
Cone (radius rr, height hh, slant ll)13πr2h\dfrac{1}{3}\pi r^2 hπr2+πrl\pi r^2 + \pi r l
Sphere (radius rr)43πr3\dfrac{4}{3}\pi r^34πr24\pi r^2
Pyramid (base area AA, height hh)13Ah\dfrac{1}{3}AhBase + lateral faces

Note: slant height of cone l=r2+h2l = \sqrt{r^2 + h^2}.

Composite solids: Many IB questions join two solids (e.g., a cone on top of a cylinder). For volume, add the parts. For surface area, subtract any internal faces that are no longer external. A cone sitting on a cylinder shares a circular face — the base circle of the cone and the top circle of the cylinder cancel each other from the surface area count.

Composite Solid — Cone on Cylinder

A solid consists of a cylinder of radius 4 cm and height 6 cm, with a cone of the same base radius and height 3 cm placed on top. Find the total volume and the total surface area.

Volume:

V=π(4)2(6)+13π(4)2(3)=96π+16π=112π352 cm3V = \pi(4)^2(6) + \frac{1}{3}\pi(4)^2(3) = 96\pi + 16\pi = 112\pi \approx 352 \text{ cm}^3

Surface area: The solid has a circular base (bottom of cylinder), the curved lateral surface of the cylinder, and the curved lateral surface of the cone. The circle where cylinder meets cone is internal — it does not contribute.

Slant height of cone: l=42+32=25=5l = \sqrt{4^2 + 3^2} = \sqrt{25} = 5 cm

SA=π(4)2+2π(4)(6)+π(4)(5)=16π+48π+20π=84π264 cm2SA = \pi(4)^2 + 2\pi(4)(6) + \pi(4)(5) = 16\pi + 48\pi + 20\pi = 84\pi \approx 264 \text{ cm}^2


Quick Recall — Section 1

Try to answer without scrolling up:

  1. Write the distance formula between (x1,y1,z1)(x_1, y_1, z_1) and (x2,y2,z2)(x_2, y_2, z_2).
  2. What is the volume of a cone with base radius rr and height hh?
  3. Why is the shared circle between a cone and a cylinder not counted in surface area?
Reveal answers
  1. d=(x2x1)2+(y2y1)2+(z2z1)2d = \sqrt{(x_2-x_1)^2+(y_2-y_1)^2+(z_2-z_1)^2}
  2. V=13πr2hV = \dfrac{1}{3}\pi r^2 h
  3. That circle is an internal face — it lies inside the composite solid and is not exposed to the exterior.

Section 2: Right-Angle and Non-Right-Angle Trigonometry

2.1 Right-Triangle Trigonometry (SOH CAH TOA)

For a right-angled triangle with acute angle θ\theta, hypotenuse hh, opposite side oo, and adjacent side aa:

sinθ=ohcosθ=ahtanθ=oa\sin\theta = \frac{o}{h} \qquad \cos\theta = \frac{a}{h} \qquad \tan\theta = \frac{o}{a}

These definitions apply directly to right-triangle problems (ladders, building heights, simple bearings).

2.2 The Sine Rule

For any triangle with sides aa, bb, cc opposite to angles AA, BB, CC respectively:

asinA=bsinB=csinC\frac{a}{\sin A} = \frac{b}{\sin B} = \frac{c}{\sin C}

Use the sine rule when you know:

  • Two angles and one side (AAS or ASA), or
  • Two sides and a non-included angle (SSA — watch for the ambiguous case)

The ambiguous case (SSA): When you are given two sides and a non-included angle, the equation sinBb=sinAa\frac{\sin B}{b} = \frac{\sin A}{a} can sometimes give two valid solutions for angle BB (one acute, one obtuse — supplementary angles have the same sine). Always check whether B=180°BB' = 180° - B also produces a valid triangle before concluding there is only one solution.

Sine Rule — Finding a Side

In triangle ABCABC, angle A=35°A = 35°, angle B=72°B = 72°, and side a=8.4a = 8.4 cm. Find side bb.

First find C=180°35°72°=73°C = 180° - 35° - 72° = 73°.

bsinB=asinA\frac{b}{\sin B} = \frac{a}{\sin A}

b=8.4×sin72°sin35°=8.4×0.95110.573613.9 cmb = \frac{8.4 \times \sin 72°}{\sin 35°} = \frac{8.4 \times 0.9511}{0.5736} \approx 13.9 \text{ cm}

2.3 The Cosine Rule

For a triangle with sides aa, bb, cc and angle CC opposite side cc:

c2=a2+b22abcosCc^2 = a^2 + b^2 - 2ab\cos C

Rearranged to find angle CC when all three sides are known:

cosC=a2+b2c22ab\cos C = \frac{a^2 + b^2 - c^2}{2ab}

Use the cosine rule when you know:

  • Two sides and the included angle (SAS), or
  • All three sides (SSS)

Cosine Rule — Finding an Angle

A triangle has sides a=7a = 7, b=5b = 5, c=9c = 9. Find angle CC.

cosC=72+52922(7)(5)=49+258170=770=0.1\cos C = \frac{7^2 + 5^2 - 9^2}{2(7)(5)} = \frac{49 + 25 - 81}{70} = \frac{-7}{70} = -0.1

C=arccos(0.1)95.7°C = \arccos(-0.1) \approx 95.7°

Since cosC<0\cos C < 0, the angle CC is obtuse — this is consistent with cc being the longest side.

2.4 Area of a Triangle

Area=12absinC\text{Area} = \frac{1}{2}ab\sin C

where aa and bb are two sides and CC is the included angle between them.

When to use which formula: If you have base and height, use 12bh\frac{1}{2}bh. If you have two sides and the included angle, use 12absinC\frac{1}{2}ab\sin C. If you have all three sides, use Heron’s formula (though this is less common on IB exams). The formula 12absinC\frac{1}{2}ab\sin C is the most useful in non-right-angle contexts.


Quick Recall — Section 2

Try to answer without scrolling up:

  1. State the sine rule.
  2. State the cosine rule (finding side cc).
  3. What is the area of a triangle with sides aa and bb and included angle CC?
  4. Under what two conditions do you use the cosine rule (not the sine rule)?
Reveal answers
  1. asinA=bsinB=csinC\dfrac{a}{\sin A} = \dfrac{b}{\sin B} = \dfrac{c}{\sin C}
  2. c2=a2+b22abcosCc^2 = a^2 + b^2 - 2ab\cos C
  3. 12absinC\dfrac{1}{2}ab\sin C
  4. SAS (two sides and included angle) or SSS (all three sides known).

Section 3: Applications — Bearings and Angles of Elevation/Depression

3.1 Bearings

A bearing is a direction measured as a three-digit angle clockwise from North. For example, a bearing of 065°065° means 65°65° clockwise from North (i.e., roughly north-east).

Key conventions:

  • Bearings are always measured clockwise from North
  • They are written as three digits: 005°005°, 090°090°, 180°180°, 270°270°
  • A bearing of 090°090° is due East; 180°180° is due South; 270°270° is due West

Reverse bearing: If the bearing from AA to BB is θ\theta, the bearing from BB to AA is θ+180°\theta + 180° (mod 360°360°).

Bearings Problem

A ship travels 12 km on a bearing of 050°050°, then 9 km on a bearing of 140°140°. Find the distance and bearing back to the start.

The two legs form a triangle. The angle between the directions 050°050° and 140°140° is 140°50°=90°140° - 50° = 90° (the turn at the intermediate point is 90°90°, making the paths perpendicular).

d=122+92=144+81=225=15 kmd = \sqrt{12^2 + 9^2} = \sqrt{144 + 81} = \sqrt{225} = 15 \text{ km}

The angle at the start satisfies tanθ=912=0.75\tan\theta = \frac{9}{12} = 0.75, so θ=36.87°36.9°\theta = 36.87° \approx 36.9°.

Bearing from start to final position: 050°+36.9°=086.9°087°050° + 36.9° = 086.9° \approx 087°.

Return bearing: 087°+180°=267°087° + 180° = 267°.

3.2 Angles of Elevation and Depression

  • Angle of elevation: The angle measured upward from the horizontal to a line of sight.
  • Angle of depression: The angle measured downward from the horizontal to a line of sight.

These angles are equal when the observer and the object are at the same horizontal level for alternate interior angles, but in general they are supplementary parts of the right-angle trig setup.

Common setup: The angle of depression from the top of a cliff to a boat is equal to the angle of elevation from the boat to the top of the cliff (alternate angles with parallel horizontal lines). Labelling a clear diagram always prevents errors in these problems. Always draw and label a diagram before writing any equation.


Section 4: Radian Measure, Arc Length, and Sector Area

4.1 Radian Measure

One radian is the angle subtended at the centre of a circle by an arc equal in length to the radius.

π radians=180°\pi \text{ radians} = 180°

Conversions:

θ (radians)=θ (degrees)×π180°θ (degrees)=θ (radians)×180°π\theta\text{ (radians)} = \theta\text{ (degrees)} \times \frac{\pi}{180°} \qquad \theta\text{ (degrees)} = \theta\text{ (radians)} \times \frac{180°}{\pi}

Common angle conversions

DegreesRadians
0°00
30°30°π6\dfrac{\pi}{6}
45°45°π4\dfrac{\pi}{4}
60°60°π3\dfrac{\pi}{3}
90°90°π2\dfrac{\pi}{2}
120°120°2π3\dfrac{2\pi}{3}
135°135°3π4\dfrac{3\pi}{4}
150°150°5π6\dfrac{5\pi}{6}
180°180°π\pi
270°270°3π2\dfrac{3\pi}{2}
360°360°2π2\pi

4.2 Arc Length and Sector Area

For a circle of radius rr and a sector with central angle θ\theta (in radians):

Arc lengthl=rθ\text{Arc length} \quad l = r\theta

Sector areaA=12r2θ\text{Sector area} \quad A = \frac{1}{2}r^2\theta

Segment area = Sector area - Triangle area:

Asegment=12r2θ12r2sinθ=12r2(θsinθ)A_{\text{segment}} = \frac{1}{2}r^2\theta - \frac{1}{2}r^2\sin\theta = \frac{1}{2}r^2(\theta - \sin\theta)

These formulas only work when θ\theta is in radians. If the angle is given in degrees, convert first. A common exam trap is to leave the angle in degrees and use the arc length formula directly — this will always give the wrong answer.

Arc Length and Sector Area

A sector of a circle has radius 8 cm and central angle 5π6\dfrac{5\pi}{6} radians. Find the arc length, the sector area, and the area of the corresponding minor segment.

Arc length: l=rθ=8×5π6=40π6=20π320.9l = r\theta = 8 \times \dfrac{5\pi}{6} = \dfrac{40\pi}{6} = \dfrac{20\pi}{3} \approx 20.9 cm

Sector area: A=12r2θ=12(64)(5π6)=320π12=80π383.8A = \dfrac{1}{2}r^2\theta = \dfrac{1}{2}(64)\left(\dfrac{5\pi}{6}\right) = \dfrac{320\pi}{12} = \dfrac{80\pi}{3} \approx 83.8 cm2^2

Segment area: Aseg=12r2(θsinθ)=32(5π6sin ⁣5π6)=32 ⁣(5π612)32(2.6180.5)67.8A_{\text{seg}} = \dfrac{1}{2}r^2(\theta - \sin\theta) = 32\left(\dfrac{5\pi}{6} - \sin\!\dfrac{5\pi}{6}\right) = 32\!\left(\dfrac{5\pi}{6} - \dfrac{1}{2}\right) \approx 32(2.618 - 0.5) \approx 67.8 cm2^2


Quick Recall — Section 4

Try to answer without scrolling up:

  1. Convert 240°240° to radians.
  2. Write the arc length formula.
  3. Write the sector area formula.
  4. What is the area of a circular segment?
Reveal answers
  1. 240°×π180°=4π3240° \times \dfrac{\pi}{180°} = \dfrac{4\pi}{3} radians
  2. l=rθl = r\theta (with θ\theta in radians)
  3. A=12r2θA = \dfrac{1}{2}r^2\theta (with θ\theta in radians)
  4. Asegment=12r2(θsinθ)A_{\text{segment}} = \dfrac{1}{2}r^2(\theta - \sin\theta)

Section 5: The Unit Circle and Exact Trigonometric Values

5.1 The Unit Circle

The unit circle has centre (0,0)(0, 0) and radius 1. For any angle θ\theta measured anticlockwise from the positive xx-axis, the point on the unit circle is (cosθ,sinθ)(\cos\theta, \sin\theta).

This gives a definition of sin\sin and cos\cos that extends beyond right triangles to all real angles.

cosθ=x-coordinatesinθ=y-coordinatetanθ=sinθcosθ=yx\cos\theta = x\text{-coordinate} \qquad \sin\theta = y\text{-coordinate} \qquad \tan\theta = \frac{\sin\theta}{\cos\theta} = \frac{y}{x}

5.2 Signs in Each Quadrant (CAST)

QuadrantAnglesPositive functions
1st (00 to π2\frac{\pi}{2})0° to 90°90°All (sin\sin, cos\cos, tan\tan)
2nd (π2\frac{\pi}{2} to π\pi)90°90° to 180°180°sin\sin only
3rd (π\pi to 3π2\frac{3\pi}{2})180°180° to 270°270°tan\tan only
4th (3π2\frac{3\pi}{2} to 2π2\pi)270°270° to 360°360°cos\cos only

The acronym CAST (reading quadrants 4–1–2–3 anticlockwise) is a mnemonic: Cos, All, Sin, Tan.

5.3 Exact Trigonometric Values

Exact values — must know from memory

θ\thetasinθ\sin\thetacosθ\cos\thetatanθ\tan\theta
00001100
π6\dfrac{\pi}{6}12\dfrac{1}{2}32\dfrac{\sqrt{3}}{2}13=33\dfrac{1}{\sqrt{3}} = \dfrac{\sqrt{3}}{3}
π4\dfrac{\pi}{4}22\dfrac{\sqrt{2}}{2}22\dfrac{\sqrt{2}}{2}11
π3\dfrac{\pi}{3}32\dfrac{\sqrt{3}}{2}12\dfrac{1}{2}3\sqrt{3}
π2\dfrac{\pi}{2}1100undefined

Memory trick for sin\sin: The values for sin\sin at 0,π6,π4,π3,π20, \frac{\pi}{6}, \frac{\pi}{4}, \frac{\pi}{3}, \frac{\pi}{2} are 02,12,22,32,42\dfrac{\sqrt{0}}{2}, \dfrac{\sqrt{1}}{2}, \dfrac{\sqrt{2}}{2}, \dfrac{\sqrt{3}}{2}, \dfrac{\sqrt{4}}{2} — a neat pattern under the square root.

5.4 Symmetry and Reference Angles

For any angle θ\theta in quadrants 2, 3, or 4, find the reference angle α\alpha (the acute angle to the nearest xx-axis), then apply the sign from CAST.

  • Quadrant 2: α=πθ\alpha = \pi - \theta
  • Quadrant 3: α=θπ\alpha = \theta - \pi
  • Quadrant 4: α=2πθ\alpha = 2\pi - \theta

Example: sin ⁣(5π6)=sin ⁣(ππ6)=sin ⁣π6=12\sin\!\left(\dfrac{5\pi}{6}\right) = \sin\!\left(\pi - \dfrac{\pi}{6}\right) = \sin\!\dfrac{\pi}{6} = \dfrac{1}{2} (positive in Q2).


Section 6: Trigonometric Identities

6.1 Pythagorean Identity

From the unit circle definition (cos2θ+sin2θ=1\cos^2\theta + \sin^2\theta = 1 is immediate from x2+y2=1x^2 + y^2 = 1):

sin2θ+cos2θ=1\sin^2\theta + \cos^2\theta = 1

Two derived forms (divide through by cos2θ\cos^2\theta or sin2θ\sin^2\theta):

1+tan2θ=sec2θcot2θ+1=csc2θ1 + \tan^2\theta = \sec^2\theta \qquad \cot^2\theta + 1 = \csc^2\theta

6.2 Double Angle Identities

sin2θ=2sinθcosθ\sin 2\theta = 2\sin\theta\cos\theta

cos2θ=cos2θsin2θ=2cos2θ1=12sin2θ\cos 2\theta = \cos^2\theta - \sin^2\theta = 2\cos^2\theta - 1 = 1 - 2\sin^2\theta

tan2θ=2tanθ1tan2θ\tan 2\theta = \frac{2\tan\theta}{1 - \tan^2\theta}

The three forms of cos2θ\cos 2\theta are all in the booklet, but knowing when to use each saves time. Use 2cos2θ12\cos^2\theta - 1 when you want to eliminate sin\sin; use 12sin2θ1 - 2\sin^2\theta when you want to eliminate cos\cos; use cos2θsin2θ\cos^2\theta - \sin^2\theta as the starting point for proofs.

6.3 Compound Angle Identities HL

sin(A±B)=sinAcosB±cosAsinB\sin(A \pm B) = \sin A\cos B \pm \cos A\sin B

cos(A±B)=cosAcosBsinAsinB\cos(A \pm B) = \cos A\cos B \mp \sin A\sin B

tan(A±B)=tanA±tanB1tanAtanB\tan(A \pm B) = \frac{\tan A \pm \tan B}{1 \mp \tan A\tan B}

Note the sign convention: for cos\cos, the signs are opposite to the signs in the angle.

Compound Angle Identity — Exact Value

Show that sin75°=6+24\sin 75° = \dfrac{\sqrt{6} + \sqrt{2}}{4}.

Write 75°=45°+30°75° = 45° + 30°:

sin(45°+30°)=sin45°cos30°+cos45°sin30°\sin(45° + 30°) = \sin 45°\cos 30° + \cos 45°\sin 30°

=2232+2212= \frac{\sqrt{2}}{2} \cdot \frac{\sqrt{3}}{2} + \frac{\sqrt{2}}{2} \cdot \frac{1}{2}

=64+24=6+24= \frac{\sqrt{6}}{4} + \frac{\sqrt{2}}{4} = \frac{\sqrt{6} + \sqrt{2}}{4} \qquad \checkmark

Identity Proof

Prove that sin2θ1+cos2θ=tanθ\dfrac{\sin 2\theta}{1 + \cos 2\theta} = \tan\theta.

Starting from the left-hand side:

sin2θ1+cos2θ=2sinθcosθ1+(2cos2θ1)=2sinθcosθ2cos2θ=sinθcosθ=tanθ\frac{\sin 2\theta}{1 + \cos 2\theta} = \frac{2\sin\theta\cos\theta}{1 + (2\cos^2\theta - 1)} = \frac{2\sin\theta\cos\theta}{2\cos^2\theta} = \frac{\sin\theta}{\cos\theta} = \tan\theta \qquad \checkmark

Identity proofs: Always start from one side (usually the more complex side) and work towards the other. Never manipulate both sides simultaneously — the IB mark scheme expects a one-directional chain of equalities. Write “LHS ==== \cdots = \cdots = RHS” explicitly. Starting from the left and reaching the right shows the most logical flow.


Quick Recall — Section 6

Try to answer without scrolling up:

  1. State the Pythagorean identity.
  2. Write all three forms of cos2θ\cos 2\theta.
  3. State the compound angle identity for sin(A+B)\sin(A + B).
  4. State the compound angle identity for cos(AB)\cos(A - B).
Reveal answers
  1. sin2θ+cos2θ=1\sin^2\theta + \cos^2\theta = 1
  2. cos2θ=cos2θsin2θ=2cos2θ1=12sin2θ\cos 2\theta = \cos^2\theta - \sin^2\theta = 2\cos^2\theta - 1 = 1 - 2\sin^2\theta
  3. sin(A+B)=sinAcosB+cosAsinB\sin(A+B) = \sin A\cos B + \cos A\sin B
  4. cos(AB)=cosAcosB+sinAsinB\cos(A-B) = \cos A\cos B + \sin A\sin B

Section 7: Trigonometric Functions and Their Graphs

7.1 Graphs of sin, cos, and tan

The three basic trig functions have the following key features:

Featurey=sinxy = \sin xy=cosxy = \cos xy=tanxy = \tan x
Period2π2\pi2π2\piπ\pi
Amplitude1111undefined
DomainR\mathbb{R}R\mathbb{R}xπ2+nπx \neq \frac{\pi}{2} + n\pi, nZn \in \mathbb{Z}
Range[1,1][-1, 1][1,1][-1, 1]R\mathbb{R}
yy-intercept001100
Zerosnπn\piπ2+nπ\frac{\pi}{2} + n\pinπn\pi

7.2 Transformations of Trig Functions

The general form is y=asin(b(xc))+dy = a\sin(b(x - c)) + d (and similarly for cos and tan):

  • a|a| = amplitude (vertical stretch/compression; if a<0a < 0, reflection in xx-axis)
  • 2πb\dfrac{2\pi}{|b|} = period (for sin\sin and cos\cos); πb\dfrac{\pi}{|b|} for tan\tan
  • cc = horizontal shift (phase shift; positive cc shifts right)
  • dd = vertical shift (midline is at y=dy = d)

Graph Transformations

Describe the transformations of y=3cos ⁣(2xπ3)+1y = -3\cos\!\left(2x - \dfrac{\pi}{3}\right) + 1 and state the amplitude, period, phase shift, and range.

Rewrite as y=3cos ⁣(2 ⁣(xπ6))+1y = -3\cos\!\left(2\!\left(x - \dfrac{\pi}{6}\right)\right) + 1.

  • a=3a = -3: amplitude 33, reflected in xx-axis
  • b=2b = 2: period =2π2=π= \dfrac{2\pi}{2} = \pi
  • c=π6c = \dfrac{\pi}{6}: shifted right by π6\dfrac{\pi}{6}
  • d=1d = 1: shifted up by 11; midline y=1y = 1

Range: [13, 1+3]=[2,4][1 - 3,\ 1 + 3] = [-2, 4]

Factoring bb before reading the phase shift: You must write b(xc)b(x - c), not bxkbx - k. To find the phase shift from y=cos(2xπ3)y = \cos(2x - \frac{\pi}{3}), factor out the 22: y=cos ⁣(2 ⁣(xπ6))y = \cos\!\left(2\!\left(x - \frac{\pi}{6}\right)\right), so the phase shift is π6\frac{\pi}{6}, not π3\frac{\pi}{3}. This is one of the most common errors in trig graph questions.


Section 8: Solving Trigonometric Equations

8.1 General Strategy

To solve a trig equation on a given interval:

  1. Isolate the trig function (e.g., sinx=12\sin x = \frac{1}{2})
  2. Find the principal value using inverse trig
  3. Use the unit circle or CAST diagram to find all solutions in the interval
  4. Check that all solutions satisfy any restrictions

General solutions (all solutions, no interval restriction):

sinx=k    x=arcsink+2nπorx=πarcsink+2nπ,nZ\sin x = k \implies x = \arcsin k + 2n\pi \quad \text{or} \quad x = \pi - \arcsin k + 2n\pi, \quad n \in \mathbb{Z}

cosx=k    x=±arccosk+2nπ,nZ\cos x = k \implies x = \pm\arccos k + 2n\pi, \quad n \in \mathbb{Z}

tanx=k    x=arctank+nπ,nZ\tan x = k \implies x = \arctan k + n\pi, \quad n \in \mathbb{Z}

Solving a Trig Equation on an Interval

Solve 2cos2xcosx1=02\cos^2 x - \cos x - 1 = 0 for 0x2π0 \leq x \leq 2\pi.

Step 1: Factorise — treat cosx\cos x as the variable.

2cos2xcosx1=(2cosx+1)(cosx1)=02\cos^2 x - \cos x - 1 = (2\cos x + 1)(\cos x - 1) = 0

Step 2: Set each factor to zero.

cosx=12\cos x = -\dfrac{1}{2} or cosx=1\cos x = 1

Step 3: Solve each case on [0,2π][0, 2\pi].

For cosx=1\cos x = 1: x=0x = 0 (and x=2πx = 2\pi, but check interval is 0x2π0 \leq x \leq 2\pi, so x=0x = 0 and x=2πx = 2\pi are both valid endpoints).

For cosx=12\cos x = -\dfrac{1}{2}: reference angle =π3= \dfrac{\pi}{3}; cosine is negative in Q2 and Q3.

x=ππ3=2π3orx=π+π3=4π3x = \pi - \frac{\pi}{3} = \frac{2\pi}{3} \qquad \text{or} \qquad x = \pi + \frac{\pi}{3} = \frac{4\pi}{3}

Solutions: x{0, 2π3, 4π3, 2π}x \in \left\{0,\ \dfrac{2\pi}{3},\ \dfrac{4\pi}{3},\ 2\pi\right\}

Trig Equation Requiring an Identity

Solve sin2x=sinx\sin 2x = \sin x for 0x<2π0 \leq x < 2\pi.

Step 1: Apply the double angle identity: sin2x=2sinxcosx\sin 2x = 2\sin x\cos x.

2sinxcosx=sinx2\sin x\cos x = \sin x

Step 2: Rearrange (do not divide by sinx\sin x — you would lose solutions!).

2sinxcosxsinx=02\sin x\cos x - \sin x = 0

sinx(2cosx1)=0\sin x(2\cos x - 1) = 0

Step 3: Solve each factor.

sinx=0    x=0, π\sin x = 0 \implies x = 0,\ \pi

cosx=12    x=π3, 5π3\cos x = \dfrac{1}{2} \implies x = \dfrac{\pi}{3},\ \dfrac{5\pi}{3}

Solutions: x{0, π3, π, 5π3}x \in \left\{0,\ \dfrac{\pi}{3},\ \pi,\ \dfrac{5\pi}{3}\right\}

Never divide both sides of a trig equation by a trig function (e.g., dividing sinx(2cosx1)=0\sin x(2\cos x - 1) = 0 by sinx\sin x). Dividing loses the solutions where sinx=0\sin x = 0. Always factorise and set each factor to zero instead.


Section 9: Reciprocal and Inverse Trigonometric Functions HL

9.1 Reciprocal Trig Functions

cscθ=1sinθsecθ=1cosθcotθ=1tanθ=cosθsinθ\csc\theta = \frac{1}{\sin\theta} \qquad \sec\theta = \frac{1}{\cos\theta} \qquad \cot\theta = \frac{1}{\tan\theta} = \frac{\cos\theta}{\sin\theta}

These are defined wherever the denominator is non-zero. Key identities:

1+tan2θ=sec2θcot2θ+1=csc2θ1 + \tan^2\theta = \sec^2\theta \qquad \cot^2\theta + 1 = \csc^2\theta

Graphs of reciprocal functions: Each has vertical asymptotes wherever the original function equals zero.

  • y=cscxy = \csc x: asymptotes at x=nπx = n\pi; range (,1][1,)(-\infty, -1] \cup [1, \infty)
  • y=secxy = \sec x: asymptotes at x=π2+nπx = \frac{\pi}{2} + n\pi; range (,1][1,)(-\infty, -1] \cup [1, \infty)
  • y=cotxy = \cot x: asymptotes at x=nπx = n\pi; period π\pi; range R\mathbb{R}

9.2 Inverse Trigonometric Functions HL

To make trig functions invertible, their domains are restricted:

FunctionRestricted domainRange (principal values)
arcsinx=sin1x\arcsin x = \sin^{-1} x[1,1][-1, 1][π2,π2]\left[-\dfrac{\pi}{2}, \dfrac{\pi}{2}\right]
arccosx=cos1x\arccos x = \cos^{-1} x[1,1][-1, 1][0,π][0, \pi]
arctanx=tan1x\arctan x = \tan^{-1} xR\mathbb{R}(π2,π2)\left(-\dfrac{\pi}{2}, \dfrac{\pi}{2}\right)

Inverse trig outputs principal values only. Your calculator gives one answer. When solving equations, use the principal value to find all solutions with the unit circle — do not assume the calculator output is the only answer. For example, arcsin(0.5)=π6\arcsin(0.5) = \frac{\pi}{6}, but the equation sinx=0.5\sin x = 0.5 has infinitely many solutions.

Reciprocal Trig Identity Proof

Prove that cscθcotθ+tanθ=cosθ\dfrac{\csc\theta}{\cot\theta + \tan\theta} = \cos\theta.

LHS:

cscθcotθ+tanθ=1sinθcosθsinθ+sinθcosθ\frac{\csc\theta}{\cot\theta + \tan\theta} = \frac{\dfrac{1}{\sin\theta}}{\dfrac{\cos\theta}{\sin\theta} + \dfrac{\sin\theta}{\cos\theta}}

Simplify the denominator using a common denominator of sinθcosθ\sin\theta\cos\theta:

=1sinθcos2θ+sin2θsinθcosθ=1sinθ1sinθcosθ=1sinθ×sinθcosθ=cosθ= \frac{\dfrac{1}{\sin\theta}}{\dfrac{\cos^2\theta + \sin^2\theta}{\sin\theta\cos\theta}} = \frac{\dfrac{1}{\sin\theta}}{\dfrac{1}{\sin\theta\cos\theta}} = \frac{1}{\sin\theta} \times \sin\theta\cos\theta = \cos\theta \qquad \checkmark


Section 10: Vector Algebra HL

10.1 Vector Notation and Basic Operations

A vector has both magnitude and direction. In 2D and 3D, vectors are written as column vectors or using unit vector notation:

v=(v1v2v3)=v1i+v2j+v3k\mathbf{v} = \begin{pmatrix} v_1 \\ v_2 \\ v_3 \end{pmatrix} = v_1\,\mathbf{i} + v_2\,\mathbf{j} + v_3\,\mathbf{k}

where i=(1,0,0)\mathbf{i} = (1, 0, 0), j=(0,1,0)\mathbf{j} = (0, 1, 0), k=(0,0,1)\mathbf{k} = (0, 0, 1) are standard unit vectors.

Magnitude (modulus):

v=v12+v22+v32|\mathbf{v}| = \sqrt{v_1^2 + v_2^2 + v_3^2}

Unit vector in the direction of v\mathbf{v}:

v^=vv\hat{\mathbf{v}} = \frac{\mathbf{v}}{|\mathbf{v}|}

Vector between two points: AB=BA=(b1a1b2a2b3a3)\overrightarrow{AB} = B - A = \begin{pmatrix} b_1 - a_1 \\ b_2 - a_2 \\ b_3 - a_3 \end{pmatrix}

10.2 Vector Addition and Scalar Multiplication

u+v=(u1+v1u2+v2u3+v3)kv=(kv1kv2kv3)\mathbf{u} + \mathbf{v} = \begin{pmatrix} u_1 + v_1 \\ u_2 + v_2 \\ u_3 + v_3 \end{pmatrix} \qquad k\mathbf{v} = \begin{pmatrix} kv_1 \\ kv_2 \\ kv_3 \end{pmatrix}

Geometrically, vector addition follows the triangle or parallelogram law. Scalar multiplication stretches or compresses the vector (and flips it if k<0k < 0).

Parallel vectors: u\mathbf{u} and v\mathbf{v} are parallel if u=kv\mathbf{u} = k\mathbf{v} for some scalar kk.

10.3 The Dot Product (Scalar Product)

uv=u1v1+u2v2+u3v3=uvcosθ\mathbf{u} \cdot \mathbf{v} = u_1 v_1 + u_2 v_2 + u_3 v_3 = |\mathbf{u}||\mathbf{v}|\cos\theta

where θ\theta is the angle between the vectors. Rearranging gives:

cosθ=uvuv\cos\theta = \frac{\mathbf{u} \cdot \mathbf{v}}{|\mathbf{u}||\mathbf{v}|}

Key property: uv=0\mathbf{u} \cdot \mathbf{v} = 0 if and only if u\mathbf{u} and v\mathbf{v} are perpendicular (provided both are non-zero).

Dot Product — Angle Between Vectors

Find the angle between u=(213)\mathbf{u} = \begin{pmatrix} 2 \\ -1 \\ 3 \end{pmatrix} and v=(142)\mathbf{v} = \begin{pmatrix} 1 \\ 4 \\ -2 \end{pmatrix}.

uv=(2)(1)+(1)(4)+(3)(2)=246=8\mathbf{u} \cdot \mathbf{v} = (2)(1) + (-1)(4) + (3)(-2) = 2 - 4 - 6 = -8

u=4+1+9=14v=1+16+4=21|\mathbf{u}| = \sqrt{4 + 1 + 9} = \sqrt{14} \qquad |\mathbf{v}| = \sqrt{1 + 16 + 4} = \sqrt{21}

cosθ=81421=8294\cos\theta = \frac{-8}{\sqrt{14}\cdot\sqrt{21}} = \frac{-8}{\sqrt{294}}

θ=arccos ⁣(8294)117.8°\theta = \arccos\!\left(\frac{-8}{\sqrt{294}}\right) \approx 117.8°

10.4 The Cross Product (Vector Product) HL

The cross product u×v\mathbf{u} \times \mathbf{v} produces a vector perpendicular to both u\mathbf{u} and v\mathbf{v}.

u×v=ijku1u2u3v1v2v3=(u2v3u3v2u3v1u1v3u1v2u2v1)\mathbf{u} \times \mathbf{v} = \begin{vmatrix} \mathbf{i} & \mathbf{j} & \mathbf{k} \\ u_1 & u_2 & u_3 \\ v_1 & v_2 & v_3 \end{vmatrix} = \begin{pmatrix} u_2 v_3 - u_3 v_2 \\ u_3 v_1 - u_1 v_3 \\ u_1 v_2 - u_2 v_1 \end{pmatrix}

Magnitude of the cross product:

u×v=uvsinθ|\mathbf{u} \times \mathbf{v}| = |\mathbf{u}||\mathbf{v}|\sin\theta

This equals the area of the parallelogram formed by u\mathbf{u} and v\mathbf{v}. The area of the triangle formed by u\mathbf{u} and v\mathbf{v} is 12u×v\dfrac{1}{2}|\mathbf{u} \times \mathbf{v}|.

Key property: u×v=0\mathbf{u} \times \mathbf{v} = \mathbf{0} if and only if u\mathbf{u} and v\mathbf{v} are parallel.

Cross product is not commutative: u×v=(v×u)\mathbf{u} \times \mathbf{v} = -(\mathbf{v} \times \mathbf{u}). The direction of the result follows the right-hand rule. On IB exams, the question will often ask for a normal vector to a plane — the cross product of two vectors in the plane gives exactly that.

Cross Product — Normal Vector and Area

Given A(1,0,2)A(1, 0, 2), B(3,1,0)B(3, 1, 0), C(0,2,1)C(0, 2, 1), find a vector normal to the plane ABCABC and the area of triangle ABCABC.

AB=(212)AC=(121)\overrightarrow{AB} = \begin{pmatrix} 2 \\ 1 \\ -2 \end{pmatrix} \qquad \overrightarrow{AC} = \begin{pmatrix} -1 \\ 2 \\ -1 \end{pmatrix}

AB×AC=((1)(1)(2)(2)(2)(1)(2)(1)(2)(2)(1)(1))=(1+42+24+1)=(345)\overrightarrow{AB} \times \overrightarrow{AC} = \begin{pmatrix} (1)(-1) - (-2)(2) \\ (-2)(-1) - (2)(-1) \\ (2)(2) - (1)(-1) \end{pmatrix} = \begin{pmatrix} -1 + 4 \\ 2 + 2 \\ 4 + 1 \end{pmatrix} = \begin{pmatrix} 3 \\ 4 \\ 5 \end{pmatrix}

Normal vector: n=(345)\mathbf{n} = \begin{pmatrix} 3 \\ 4 \\ 5 \end{pmatrix}

Area of triangle: A=12(345)=129+16+25=502=522A = \dfrac{1}{2}\left|\begin{pmatrix} 3 \\ 4 \\ 5 \end{pmatrix}\right| = \dfrac{1}{2}\sqrt{9 + 16 + 25} = \dfrac{\sqrt{50}}{2} = \dfrac{5\sqrt{2}}{2}


Quick Recall — Section 10

Try to answer without scrolling up:

  1. How do you find the angle between two vectors?
  2. What does uv=0\mathbf{u} \cdot \mathbf{v} = 0 tell you (assuming both vectors are non-zero)?
  3. What is the geometric interpretation of u×v|\mathbf{u} \times \mathbf{v}|?
  4. How do you find a normal vector to a plane containing points AA, BB, CC?
Reveal answers
  1. cosθ=uvuv\cos\theta = \dfrac{\mathbf{u} \cdot \mathbf{v}}{|\mathbf{u}||\mathbf{v}|}, then θ=arccos()\theta = \arccos(\cdots).
  2. u\mathbf{u} and v\mathbf{v} are perpendicular (orthogonal).
  3. The area of the parallelogram formed by u\mathbf{u} and v\mathbf{v}.
  4. Compute AB×AC\overrightarrow{AB} \times \overrightarrow{AC}.

Section 11: Vector Equations of Lines HL

11.1 Vector Equation of a Line

A line in 2D or 3D is determined by a point on the line and a direction vector. If the line passes through point AA with position vector a\mathbf{a} and has direction vector d\mathbf{d}, then any point PP on the line satisfies:

r=a+td,tR\mathbf{r} = \mathbf{a} + t\mathbf{d}, \qquad t \in \mathbb{R}

where tt is a scalar parameter. In component form (3D):

(xyz)=(a1a2a3)+t(d1d2d3)\begin{pmatrix} x \\ y \\ z \end{pmatrix} = \begin{pmatrix} a_1 \\ a_2 \\ a_3 \end{pmatrix} + t\begin{pmatrix} d_1 \\ d_2 \\ d_3 \end{pmatrix}

11.2 Parametric and Cartesian Forms

Parametric equations:

x=a1+td1y=a2+td2z=a3+td3x = a_1 + td_1 \qquad y = a_2 + td_2 \qquad z = a_3 + td_3

Cartesian (symmetric) form (provided di0d_i \neq 0):

xa1d1=ya2d2=za3d3=t\frac{x - a_1}{d_1} = \frac{y - a_2}{d_2} = \frac{z - a_3}{d_3} = t

11.3 Angle Between Two Lines

The angle θ\theta between lines with direction vectors d1\mathbf{d}_1 and d2\mathbf{d}_2:

cosθ=d1d2d1d2\cos\theta = \frac{|\mathbf{d}_1 \cdot \mathbf{d}_2|}{|\mathbf{d}_1||\mathbf{d}_2|}

The absolute value ensures θ[0°,90°]\theta \in \left[0°, 90°\right] (we take the acute angle between lines).

11.4 Relationships Between Lines

Two lines can be:

  • Parallel: direction vectors are scalar multiples; lines do not intersect (unless they are the same line)
  • Intersecting: lines meet at a unique point (solve simultaneously for parameters)
  • Skew: lines are not parallel and do not intersect (only possible in 3D)

To check if two lines intersect: set the parametric equations equal and solve for the parameters ss and tt. If all three equations are consistent with specific values of ss and tt, the lines intersect. If the system is inconsistent, the lines are skew (or parallel).

Line Intersection in 3D

Line L1L_1: r=(120)+s(112)\mathbf{r} = \begin{pmatrix} 1 \\ 2 \\ 0 \end{pmatrix} + s\begin{pmatrix} 1 \\ -1 \\ 2 \end{pmatrix} and line L2L_2: r=(304)+t(110)\mathbf{r} = \begin{pmatrix} 3 \\ 0 \\ 4 \end{pmatrix} + t\begin{pmatrix} -1 \\ 1 \\ 0 \end{pmatrix}. Determine whether the lines intersect, are parallel, or are skew.

Step 1: Check if direction vectors are parallel. (1,1,2)(1, -1, 2) and (1,1,0)(-1, 1, 0) are not scalar multiples (since 11=1\frac{1}{-1} = -1 but 20\frac{2}{0} is undefined), so the lines are not parallel.

Step 2: Set corresponding components equal.

1+s=3ts+t=2(i)1 + s = 3 - t \quad \Rightarrow \quad s + t = 2 \qquad (i) 2s=ts+t=2(ii)2 - s = t \quad \Rightarrow \quad s + t = 2 \qquad (ii) 0+2s=4s=2(iii)0 + 2s = 4 \quad \Rightarrow \quad s = 2 \qquad (iii)

From (iii)(iii): s=2s = 2. From (i)(i): t=0t = 0.

Step 3: Verify in the zz-component of L2L_2: z=4+0(0)=4z = 4 + 0(0) = 4. For L1L_1: z=0+2(2)=4z = 0 + 2(2) = 4. Consistent.

The lines intersect at the point: L1L_1 at s=2s = 2: (1+2,22,0+4)=(3,0,4)(1+2, 2-2, 0+4) = (3, 0, 4). Intersection point: (3,0,4)(3, 0, 4).

Skew lines: After finding ss and tt from two components, always verify in the third component. If the third equation is inconsistent, the lines are skew — not parallel and not intersecting. This check is essential and frequently omitted by students, leading to incorrect conclusions.


Section 12: Vector Equations of Planes HL

12.1 Equation of a Plane

A plane is determined by a point and a normal vector perpendicular to it.

If n=(abc)\mathbf{n} = \begin{pmatrix} a \\ b \\ c \end{pmatrix} is the normal vector and the plane passes through point (x0,y0,z0)(x_0, y_0, z_0), the Cartesian equation is:

a(xx0)+b(yy0)+c(zz0)=0a(x - x_0) + b(y - y_0) + c(z - z_0) = 0

Expanded as ax+by+cz=dax + by + cz = d where d=ax0+by0+cz0d = ax_0 + by_0 + cz_0.

Vector form: rn=an\mathbf{r} \cdot \mathbf{n} = \mathbf{a} \cdot \mathbf{n}, or equivalently nr=d\mathbf{n} \cdot \mathbf{r} = d.

Parametric form: Using two non-parallel vectors b\mathbf{b} and c\mathbf{c} in the plane:

r=a+sb+tc,s,tR\mathbf{r} = \mathbf{a} + s\mathbf{b} + t\mathbf{c}, \qquad s, t \in \mathbb{R}

12.2 Finding the Equation of a Plane

Given a normal vector and a point: Substitute directly into ax+by+cz=dax + by + cz = d.

Given three points: Find two vectors in the plane, take their cross product to get the normal, then use one point to find dd.

Equation of a Plane Through Three Points

Find the Cartesian equation of the plane through P(1,0,2)P(1, 0, 2), Q(3,1,0)Q(3, 1, 0), R(0,2,1)R(0, 2, 1).

Step 1: Find two vectors in the plane.

PQ=(212)PR=(121)\overrightarrow{PQ} = \begin{pmatrix} 2 \\ 1 \\ -2 \end{pmatrix} \qquad \overrightarrow{PR} = \begin{pmatrix} -1 \\ 2 \\ -1 \end{pmatrix}

Step 2: Cross product gives the normal.

n=PQ×PR=((1)(1)(2)(2)(2)(1)(2)(1)(2)(2)(1)(1))=(345)\mathbf{n} = \overrightarrow{PQ} \times \overrightarrow{PR} = \begin{pmatrix} (1)(-1)-(-2)(2) \\ (-2)(-1)-(2)(-1) \\ (2)(2)-(1)(-1) \end{pmatrix} = \begin{pmatrix} 3 \\ 4 \\ 5 \end{pmatrix}

Step 3: Use point P(1,0,2)P(1, 0, 2) to find dd.

d=3(1)+4(0)+5(2)=3+0+10=13d = 3(1) + 4(0) + 5(2) = 3 + 0 + 10 = 13

Equation of the plane: 3x+4y+5z=133x + 4y + 5z = 13

Verification with Q(3,1,0)Q(3,1,0): 9+4+0=139 + 4 + 0 = 13 ✓. With R(0,2,1)R(0,2,1): 0+8+5=130 + 8 + 5 = 13 ✓.

12.3 Angle Between a Line and a Plane

Let d\mathbf{d} be the direction of the line and n\mathbf{n} be the normal to the plane. The angle ϕ\phi between the line and the plane satisfies:

sinϕ=dndn\sin\phi = \frac{|\mathbf{d} \cdot \mathbf{n}|}{|\mathbf{d}||\mathbf{n}|}

(Note: this is the complement of the angle between the line and the normal.)

12.4 Angle Between Two Planes

The angle between two planes is the angle between their normal vectors:

cosθ=n1n2n1n2\cos\theta = \frac{|\mathbf{n}_1 \cdot \mathbf{n}_2|}{|\mathbf{n}_1||\mathbf{n}_2|}

Normal vector reading: From a Cartesian plane equation ax+by+cz=dax + by + cz = d, the normal vector is immediately n=(abc)\mathbf{n} = \begin{pmatrix} a \\ b \\ c \end{pmatrix}. You do not need to find two vectors in the plane and cross them — just read the coefficients. This saves significant time on exams.


Quick Recall — Section 12

Try to answer without scrolling up:

  1. What is the normal vector of the plane 2xy+3z=72x - y + 3z = 7?
  2. Given three points in a plane, how do you find the normal vector?
  3. How do you find the angle between two planes?
  4. A line has direction d\mathbf{d} and a plane has normal n\mathbf{n}. How do you find the angle between the line and the plane?
Reveal answers
  1. n=(213)\mathbf{n} = \begin{pmatrix} 2 \\ -1 \\ 3 \end{pmatrix}
  2. Find two vectors in the plane (using the points), then take their cross product.
  3. cosθ=n1n2n1n2\cos\theta = \dfrac{|\mathbf{n}_1 \cdot \mathbf{n}_2|}{|\mathbf{n}_1||\mathbf{n}_2|}
  4. sinϕ=dndn\sin\phi = \dfrac{|\mathbf{d} \cdot \mathbf{n}|}{|\mathbf{d}||\mathbf{n}|}

Section 13: Intersections of Lines and Planes HL

13.1 Line and Plane Intersection

To find where a line r=a+td\mathbf{r} = \mathbf{a} + t\mathbf{d} meets a plane ax+by+cz=kax + by + cz = k:

  1. Substitute the parametric equations of the line into the plane equation
  2. Solve for tt
  3. Substitute tt back to find the intersection point

If dn=0\mathbf{d} \cdot \mathbf{n} = 0, the line is parallel to the plane (no intersection unless the line lies in the plane).

Line-Plane Intersection

Find the point where LL: r=(121)+t(213)\mathbf{r} = \begin{pmatrix} 1 \\ 2 \\ -1 \end{pmatrix} + t\begin{pmatrix} 2 \\ -1 \\ 3 \end{pmatrix} meets the plane Π\Pi: x+2yz=5x + 2y - z = 5.

Parametric equations of LL: x=1+2t, y=2t, z=1+3tx = 1 + 2t,\ y = 2 - t,\ z = -1 + 3t

Substitute into plane equation:

(1+2t)+2(2t)(1+3t)=5(1 + 2t) + 2(2 - t) - (-1 + 3t) = 5

1+2t+42t+13t=51 + 2t + 4 - 2t + 1 - 3t = 5

63t=5    t=136 - 3t = 5 \implies t = \frac{1}{3}

Intersection point: x=1+23=53x = 1 + \frac{2}{3} = \frac{5}{3}, y=213=53y = 2 - \frac{1}{3} = \frac{5}{3}, z=1+1=0z = -1 + 1 = 0.

Point of intersection: (53, 53, 0)\left(\dfrac{5}{3},\ \dfrac{5}{3},\ 0\right)

13.2 Intersection of Two Planes

Two non-parallel planes intersect in a line. The line’s direction is given by n1×n2\mathbf{n}_1 \times \mathbf{n}_2 (normal vectors of the two planes). To find a specific point on the line, set one variable to 00 and solve the two plane equations simultaneously.

13.3 Intersection of Three Planes

Three planes can intersect in:

  • A unique point (most common exam case — solve the 3×33 \times 3 system)
  • A line (two planes have the same intersection line, and the third contains it)
  • No point (inconsistent system — parallel planes or other configurations)

Use row reduction (Gaussian elimination) to solve the 3×33 \times 3 system. The number of solutions corresponds to the rank of the augmented matrix.

Intersection of Three Planes

Find the intersection of the planes Π1:x+y+z=6\Pi_1: x + y + z = 6, Π2:2xy+z=3\Pi_2: 2x - y + z = 3, Π3:x+2yz=4\Pi_3: x + 2y - z = 4.

Set up the system:

x+y+z=62xy+z=3x+2yz=4\begin{aligned} x + y + z &= 6 \\ 2x - y + z &= 3 \\ x + 2y - z &= 4 \end{aligned}

Eliminate xx: Using R2R22R1R_2 \leftarrow R_2 - 2R_1 and R3R3R1R_3 \leftarrow R_3 - R_1:

x+y+z=63yz=9y2z=2\begin{aligned} x + y + z &= 6 \\ -3y - z &= -9 \\ y - 2z &= -2 \end{aligned}

From row 2: 3y+z=93y + z = 9 so z=93yz = 9 - 3y.

Substitute into row 3: y2(93y)=2    y18+6y=2    7y=16    y=167y - 2(9 - 3y) = -2 \implies y - 18 + 6y = -2 \implies 7y = 16 \implies y = \dfrac{16}{7}

Then: z=93 ⁣(167)=9487=157z = 9 - 3\!\left(\dfrac{16}{7}\right) = 9 - \dfrac{48}{7} = \dfrac{15}{7}, x=6yz=6167157=6317=117x = 6 - y - z = 6 - \dfrac{16}{7} - \dfrac{15}{7} = 6 - \dfrac{31}{7} = \dfrac{11}{7}

Intersection point: (117, 167, 157)\left(\dfrac{11}{7},\ \dfrac{16}{7},\ \dfrac{15}{7}\right)

Inconsistency check: When solving three plane equations, if elimination leads to a contradiction like 0=50 = 5, the system is inconsistent — the planes do not all meet at a common point (they form a prism or triangular arrangement). If elimination produces 0=00 = 0, the planes all contain a common line. Always interpret the geometric meaning of the outcome in your written answer.


Section 14: Practice Exam Questions

Exam strategy for Topic 3: In Papers 1 and 2, trig identities and solving trig equations appear on Paper 1 (no calculator). Use exact values. Vectors, 3D geometry, and applications appear on Paper 2. Always show full working, including labelled diagrams for geometry problems. Vectors questions often follow a chain: find a normal, write a plane equation, find an intersection — plan the whole question before starting.


Question 1 [Non-Right-Angle Trig and Sector] [~8 marks]

Triangle ABCABC has AB=10AB = 10 cm, AC=7AC = 7 cm, and angle BAC=1.2BAC = 1.2 radians.

(a) Find the area of triangle ABCABC.

(b) Find the length BCBC.

(c) A sector of a circle has the same area as triangle ABCABC and a radius of 5 cm. Find the central angle of the sector in radians.

Show Solution

Part (a) — Area of triangle

Area=12(10)(7)sin(1.2)=35sin(1.2)35×0.932032.6 cm2\text{Area} = \frac{1}{2}(10)(7)\sin(1.2) = 35\sin(1.2) \approx 35 \times 0.9320 \approx 32.6 \text{ cm}^2

Part (b) — Length BCBC using cosine rule

BC2=AB2+AC22(AB)(AC)cos(BAC)BC^2 = AB^2 + AC^2 - 2(AB)(AC)\cos(\angle BAC)

=100+492(10)(7)cos(1.2)=149140cos(1.2)= 100 + 49 - 2(10)(7)\cos(1.2) = 149 - 140\cos(1.2)

cos(1.2)0.3624\cos(1.2) \approx 0.3624

BC214950.74=98.26    BC9.91 cmBC^2 \approx 149 - 50.74 = 98.26 \implies BC \approx 9.91 \text{ cm}

Part (c) — Central angle of sector

Sector area =12r2θ=12(25)θ=25θ2= \dfrac{1}{2}r^2\theta = \dfrac{1}{2}(25)\theta = \dfrac{25\theta}{2}

Set equal to triangle area:

25θ2=32.6    θ=65.2252.61 rad\frac{25\theta}{2} = 32.6 \implies \theta = \frac{65.2}{25} \approx 2.61 \text{ rad}


Question 2 [Trig Identity Proof and Equation] [~9 marks]

(a) Prove that cos2θ+2sin2θ=1\cos 2\theta + 2\sin^2\theta = 1.

(b) Hence, or otherwise, solve cos4x+2sin22x1=0\cos 4x + 2\sin^2 2x - 1 = 0 for 0xπ0 \leq x \leq \pi.

Show Solution

Part (a) — Identity proof

Starting from the LHS:

cos2θ+2sin2θ=(12sin2θ)+2sin2θ=1\cos 2\theta + 2\sin^2\theta = (1 - 2\sin^2\theta) + 2\sin^2\theta = 1 \qquad \checkmark

Part (b) — Solving the equation

Apply the identity in part (a) with θ=2x\theta = 2x:

cos4x+2sin22x=1\cos 4x + 2\sin^2 2x = 1

So the equation cos4x+2sin22x1=0\cos 4x + 2\sin^2 2x - 1 = 0 becomes 11=01 - 1 = 0, i.e., 0=00 = 0.

This is an identity — it is true for all xx. Therefore every x[0,π]x \in [0, \pi] is a solution.

Note: The question becomes: “find all xx such that the equation holds,” and since it is an identity on R\mathbb{R}, the answer is all x[0,π]x \in [0, \pi].


Question 3 [Compound Angle — HL] [~9 marks]

(a) Given that sinα=35\sin\alpha = \dfrac{3}{5} and cosβ=513\cos\beta = \dfrac{5}{13}, where α\alpha and β\beta are both acute angles, find the exact value of cos(α+β)\cos(\alpha + \beta).

(b) Show that cos(α+β)=cos(αβ)2sinαsinβ\cos(\alpha + \beta) = \cos(\alpha - \beta) - 2\sin\alpha\sin\beta.

Show Solution

Part (a)

Since α\alpha is acute and sinα=35\sin\alpha = \dfrac{3}{5}: cosα=45\cos\alpha = \dfrac{4}{5} (Pythagorean triple 3-4-5).

Since β\beta is acute and cosβ=513\cos\beta = \dfrac{5}{13}: sinβ=1213\sin\beta = \dfrac{12}{13} (Pythagorean triple 5-12-13).

cos(α+β)=cosαcosβsinαsinβ=45513351213\cos(\alpha + \beta) = \cos\alpha\cos\beta - \sin\alpha\sin\beta = \frac{4}{5}\cdot\frac{5}{13} - \frac{3}{5}\cdot\frac{12}{13}

=20653665=1665= \frac{20}{65} - \frac{36}{65} = -\frac{16}{65}

Part (b)

Starting from RHS:

cos(αβ)2sinαsinβ=(cosαcosβ+sinαsinβ)2sinαsinβ\cos(\alpha - \beta) - 2\sin\alpha\sin\beta = (\cos\alpha\cos\beta + \sin\alpha\sin\beta) - 2\sin\alpha\sin\beta

=cosαcosβsinαsinβ=cos(α+β)= \cos\alpha\cos\beta - \sin\alpha\sin\beta = \cos(\alpha + \beta) \qquad \checkmark


Question 4 [Vectors — Lines and Planes] [~15 marks] HL

The plane Π1\Pi_1 passes through the points A(2,0,1)A(2, 0, 1), B(1,3,1)B(1, 3, -1), and C(0,1,2)C(0, 1, 2).

(a) Find the equation of plane Π1\Pi_1 in the form ax+by+cz=dax + by + cz = d.

A second plane Π2\Pi_2 has equation 2xy+z=42x - y + z = 4.

(b) Find the angle between Π1\Pi_1 and Π2\Pi_2.

(c) Find the vector equation of the line LL of intersection of Π1\Pi_1 and Π2\Pi_2.

A point PP lies on LL with x=0x = 0.

(d) Find the coordinates of PP.

Show Solution

Part (a) — Equation of Π1\Pi_1

AB=(132)\overrightarrow{AB} = \begin{pmatrix} -1 \\ 3 \\ -2 \end{pmatrix}, AC=(211)\overrightarrow{AC} = \begin{pmatrix} -2 \\ 1 \\ 1 \end{pmatrix}

n1=AB×AC=((3)(1)(2)(1)(2)(2)(1)(1)(1)(1)(3)(2))=(3+24+11+6)=(555)\mathbf{n}_1 = \overrightarrow{AB} \times \overrightarrow{AC} = \begin{pmatrix} (3)(1)-(-2)(1) \\ (-2)(-2)-(-1)(1) \\ (-1)(1)-(3)(-2) \end{pmatrix} = \begin{pmatrix} 3+2 \\ 4+1 \\ -1+6 \end{pmatrix} = \begin{pmatrix} 5 \\ 5 \\ 5 \end{pmatrix}

We can simplify to n1=(111)\mathbf{n}_1 = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}.

Using point A(2,0,1)A(2,0,1): d=1(2)+1(0)+1(1)=3d = 1(2) + 1(0) + 1(1) = 3.

Equation of Π1\Pi_1: x+y+z=3x + y + z = 3

Verification with BB: 1+31=31+3-1=3 ✓. With CC: 0+1+2=30+1+2=3 ✓.

Part (b) — Angle between planes

n1=(111)\mathbf{n}_1 = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}, n2=(211)\mathbf{n}_2 = \begin{pmatrix} 2 \\ -1 \\ 1 \end{pmatrix}

cosθ=n1n2n1n2=21+136=218=232=23\cos\theta = \frac{|\mathbf{n}_1 \cdot \mathbf{n}_2|}{|\mathbf{n}_1||\mathbf{n}_2|} = \frac{|2 - 1 + 1|}{\sqrt{3}\cdot\sqrt{6}} = \frac{2}{\sqrt{18}} = \frac{2}{3\sqrt{2}} = \frac{\sqrt{2}}{3}

θ=arccos ⁣(23)61.9°\theta = \arccos\!\left(\frac{\sqrt{2}}{3}\right) \approx 61.9°

Part (c) — Line of intersection

The direction of LL is d=n1×n2\mathbf{d} = \mathbf{n}_1 \times \mathbf{n}_2:

d=(111)×(211)=((1)(1)(1)(1)(1)(2)(1)(1)(1)(1)(1)(2))=(213)\mathbf{d} = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} \times \begin{pmatrix} 2 \\ -1 \\ 1 \end{pmatrix} = \begin{pmatrix} (1)(1)-(1)(-1) \\ (1)(2)-(1)(1) \\ (1)(-1)-(1)(2) \end{pmatrix} = \begin{pmatrix} 2 \\ 1 \\ -3 \end{pmatrix}

Part (d) — Point on LL with x=0x = 0

Substitute x=0x = 0 into both plane equations:

Π1\Pi_1: 0+y+z=3    y+z=30 + y + z = 3 \implies y + z = 3

Π2\Pi_2: 0y+z=4    y+z=40 - y + z = 4 \implies -y + z = 4

Adding: 2z=7    z=722z = 7 \implies z = \dfrac{7}{2}, y=372=12y = 3 - \dfrac{7}{2} = -\dfrac{1}{2}

Point PP: (0, 12, 72)\left(0,\ -\dfrac{1}{2},\ \dfrac{7}{2}\right)

Vector equation of LL:

r=(01272)+t(213),tR\mathbf{r} = \begin{pmatrix} 0 \\ -\frac{1}{2} \\ \frac{7}{2} \end{pmatrix} + t\begin{pmatrix} 2 \\ 1 \\ -3 \end{pmatrix}, \quad t \in \mathbb{R}


Question 5 [3D Trig Application] [~9 marks]

A vertical tower ABAB stands on horizontal ground at AA. From a point CC on the ground, the angle of elevation of the top BB is 42°42°. The bearing of AA from CC is 325°325°, and CA=80CA = 80 m. A second point DD on the ground is 50 m due East of CC.

(a) Find the height ABAB of the tower.

(b) Find the angle of elevation of BB from DD.

(c) Find the bearing of AA from DD.

Show Solution

Part (a) — Height of tower

From the right triangle CABCAB:

tan42°=ABCA    AB=80tan42°80×0.900472.0 m\tan 42° = \frac{AB}{CA} \implies AB = 80\tan 42° \approx 80 \times 0.9004 \approx 72.0 \text{ m}

Part (b) — Angle of elevation from DD

Set up a coordinate system with CC at the origin, East as +x+x, North as +y+y.

DD is 50 m due East of CC: D=(50,0)D = (50, 0).

Bearing of AA from CC is 325°325° (clockwise from North), so the bearing is 325°325°.

Direction from CC to AA: angle from East (standard) =90°325°=235°= 90° - 325° = -235°, equivalently 125°125° (i.e., North 235°-235° or bearing 325°325° means roughly North-West).

Converting bearing 325°325° to standard angle: standard angle=90°325°=235°\text{standard angle} = 90° - 325° = -235°, add 360°360°: 125°125° from East.

A=80(cos125°,sin125°)80(0.5736,0.8192)(45.9,65.5)A = 80(\cos 125°, \sin 125°) \approx 80(-0.5736, 0.8192) \approx (-45.9, 65.5)

DA=AD=(45.950,65.50)=(95.9,65.5)DA = A - D = (-45.9 - 50, 65.5 - 0) = (-95.9, 65.5)

Horizontal distance DA=95.92+65.529196.8+4290.313487116.1DA = \sqrt{95.9^2 + 65.5^2} \approx \sqrt{9196.8 + 4290.3} \approx \sqrt{13487} \approx 116.1 m

tan(elevation from D)=72.0116.10.620    elevation31.8°\tan(\text{elevation from }D) = \frac{72.0}{116.1} \approx 0.620 \implies \text{elevation} \approx 31.8°

Part (c) — Bearing of AA from DD

Vector DA=(95.9,65.5)\overrightarrow{DA} = (-95.9, 65.5).

Bearing = angle clockwise from North. DA\overrightarrow{DA} points West and North.

α=arctan ⁣(95.965.5)arctan(1.464)55.6°\alpha = \arctan\!\left(\frac{95.9}{65.5}\right) \approx \arctan(1.464) \approx 55.6°

Since DA\overrightarrow{DA} has a negative xx-component (West) and positive yy-component (North), bearing =360°55.6°=304°= 360° - 55.6° = 304°.

Bearing of AA from D304°D \approx 304°


Topic 3 Quick-Reference Summary

ConceptKey Formula / Fact
Distance in 3Dd=(x2x1)2+(y2y1)2+(z2z1)2d = \sqrt{(x_2-x_1)^2+(y_2-y_1)^2+(z_2-z_1)^2}
Sine ruleasinA=bsinB=csinC\dfrac{a}{\sin A} = \dfrac{b}{\sin B} = \dfrac{c}{\sin C}
Cosine rulec2=a2+b22abcosCc^2 = a^2 + b^2 - 2ab\cos C
Triangle area12absinC\dfrac{1}{2}ab\sin C
Arc lengthl=rθl = r\theta (θ\theta in radians)
Sector areaA=12r2θA = \dfrac{1}{2}r^2\theta
Segment area12r2(θsinθ)\dfrac{1}{2}r^2(\theta - \sin\theta)
sin2θ+cos2θ\sin^2\theta + \cos^2\theta=1= 1
cos2θ\cos 2\theta (3 forms)cos2θsin2θ=2cos2θ1=12sin2θ\cos^2\theta - \sin^2\theta = 2\cos^2\theta - 1 = 1-2\sin^2\theta
sin2θ\sin 2\theta2sinθcosθ2\sin\theta\cos\theta
sin(A±B)\sin(A \pm B)sinAcosB±cosAsinB\sin A\cos B \pm \cos A\sin B
cos(A±B)\cos(A \pm B)cosAcosBsinAsinB\cos A\cos B \mp \sin A\sin B
Dot productuv=u1v1+u2v2+u3v3=uvcosθ\mathbf{u}\cdot\mathbf{v} = u_1v_1+u_2v_2+u_3v_3 = \lvert\mathbf{u}\rvert\lvert\mathbf{v}\rvert\cos\theta
Perpendicular vectorsuv=0\mathbf{u}\cdot\mathbf{v} = 0
Angle between vectorscosθ=uvuv\cos\theta = \dfrac{\mathbf{u}\cdot\mathbf{v}}{\lvert\mathbf{u}\rvert\lvert\mathbf{v}\rvert}
Plane from normal n=(a,b,c)\mathbf{n} = (a,b,c)ax+by+cz=dax + by + cz = d
Line equationr=a+td\mathbf{r} = \mathbf{a} + t\mathbf{d}
Normal to plane ABCABCAB×AC\overrightarrow{AB} \times \overrightarrow{AC}
Angle between planescosθ=n1n2n1n2\cos\theta = \dfrac{\lvert\mathbf{n}_1\cdot\mathbf{n}_2\rvert}{\lvert\mathbf{n}_1\rvert\lvert\mathbf{n}_2\rvert}

IB Formula Booklet — Complex Numbers

Modulus & Polar Form

GIVENz = r(cosθ + i sinθ) = r cis θ
GIVENz = re (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