Mastery Guide: Vectors in Plane, Direct Line Segments, Component Forms & Geometrical Proofs
📑 Quick Navigation & Chapter Index
Part 1: Conceptual Foundations
Part 2: Solved Textbook Exercises (54 Items)
Part 3: Academic Question Bank
- Objective Concept Booster (26 Items)
- Grand Total: 80 Database Questions
📖 Unit Overview & Target Learning Outcomes
In this chapter, students explore the mathematical bridge between geometry and physics: Vectors in Plane. While scalars measure magnitude alone (such as mass, temperature, or speed), vectors embody both magnitude and spatial direction (such as displacement, force, and velocity). Mastering vector algebra and coordinate geometry empowers students to model spatial navigation, aeronautics, forces, and rigorous geometrical proofs.
- Scalars vs. Vectors: Rigorously distinguish between scalar quantities (magnitude only) and vector quantities (magnitude + direction).
- Geometrical Representation: Represent vectors as directed line segments $\vec{AB}$ featuring an initial point (tail), a terminal point (head), length (norm), and direction angle $\theta$.
- Cartesian & Component Forms: Express vectors in ordered pair form $[x, y]$ and standard basis unit vector form $x\hat{i} + y\hat{j}$.
- Position Vectors: Define position vector $\vec{OP}$ relative to the origin $(0, 0)$ and compute displacement $\vec{AB} = \vec{OB} - \\vec{OA} = \vec{b} - \vec{a}$.
- Vector Arithmetic: Add, subtract, and scale vectors algebraically and geometrically using the Head-to-Tail Rule (Triangle Law), Parallelogram Law, and Polygon Law.
- Unit Vectors & Normalization: Normalize any non-zero vector to obtain a unit vector $\hat{u} = \frac{\vec{u}}{|\vec{u}|}$ of unit magnitude in the specified direction.
- Parallel & Anti-Parallel Vectors: Apply the scalar proportionality test $\vec{u} = k\vec{v} \iff \frac{x_1}{x_2} = \frac{y_1}{y_2} = k$ to determine parallelism and collinearity.
- Rectangular Components: Resolve vectors into horizontal ($F_x = |\vec{F}|\cos\theta$) and vertical ($F_y = |\vec{F}|\sin\theta$) components, and compute direction $\theta = \tan^{-1}(F_y / F_x)$.
- Ratio Formula: Calculate the position vector of internal ($\vec{r} = \frac{m\vec{b} + n\vec{a}}{m + n}$) and external division points, midpoint ($\vec{r} = \frac{\vec{a} + \vec{b}}{2}$), and points of trisection.
- Geometrical Proofs: Execute formal vector proofs for the Triangle Midpoint Theorem, Trapezium Midline Theorem, Varignon's Theorem, and parallelogram diagonal properties.
💡 Kid-Friendly Tips for Success
🧠 Memory Hooks & Golden Rules
- The GPS Metaphor (Scalar vs. Vector): If your speedometer says $60\text{ km/h}$, that is a Scalar (Speed). But if your GPS tells you to drive $60\text{ km/h}$ due North towards Islamabad, that is a Vector (Velocity)! Direction turns speed into velocity.
- Vector AB = Head minus Tail: To find the vector from point $A$ to point $B$, always subtract the tail coordinates from the head coordinates: $\vec{AB} = B - A = \vec{b} - \vec{a}$. Never do $A - B$ unless you want the opposite vector $\vec{BA}$!
- Head-to-Tail Train Rule: When adding vectors, imagine train carriages coupling together: Connect the Tail of the 2nd carriage to the Head of the 1st carriage. The resultant is the express shortcut connecting the very start (first tail) to the final stop (last head).
- Unit Vector = "Shrinking to Size 1": A unit vector $\hat{u}$ is simply your vector with its direction completely intact, but shrunk down to have an exact length of $1$. You get it by dividing the vector by its own length: $\hat{u} = \frac{\vec{u}}{|\vec{u}|}$.
- The Ratio Formula Cross-Multiplication Trick: In $\vec{r} = \frac{m\vec{b} + n\vec{a}}{m + n}$, remember that ratio weight $m$ (distance from $A$) multiplies the opposite vector $\vec{b}$, while ratio weight $n$ (distance from $B$) multiplies $\vec{a}$. They criss-cross!
🌍 Real-World Connections & Engineering
✈️ Aviation & Crosswind Navigation
Commercial aircraft fly through moving air masses. Pilots use vector addition ($\vec{v}_{\text{ground}} = \vec{v}_{\text{airspeed}} + \vec{v}_{\text{wind}}$) to calculate crosswind crab angles so the plane stays exactly on its runway approach trajectory without drifting off-course.
🎮 3D Video Game Engines & Physics
Game engines (like Unreal Engine and Unity) use 2D/3D vectors for everything: player movement, camera rotations, gravity vectors, projectile trajectories, and collision normals. Normalizing vectors ensures characters walk at uniform speeds in all diagonal directions.
🏗️ Structural Civil Engineering & Trusses
Bridge trusses and crane cables balance tension and compression forces. Civil engineers resolve each cable tension into horizontal and vertical components ($\sum F_x = 0$, $\sum F_y = 0$) to guarantee structural equilibrium and prevent bridge collapse.
🚢 Marine Navigation & River Crossings
Ferry captains crossing fast-flowing rivers like Indus or Chenab must angle their boats upstream. By adding the boat's engine vector to the river current vector, the ferry achieves a net resultant velocity directed straight across to the target dock.
🔑 Essential Inquiries & Conceptual Questions
🤔 Provocative Mathematical Thinking Cues
- Can two vectors have equal magnitude but NOT be equal?
Yes! Consider $\vec{u} = [3, 4]$ and $\vec{v} = [-3, 4]$. Both have magnitude $\sqrt{3^2 + 4^2} = 5$, but $\vec{u} \neq \vec{v}$ because their horizontal directions point in opposite directions. - Why does a zero vector have an arbitrary direction?
A zero vector starts and ends at the exact same point ($\vec{0} = [0, 0]$), so its length is zero. Because there is no line segment spanning two distinct points, no specific direction angle $\theta$ can be uniquely fixed, allowing it to adapt mathematically to any directional context. - Why is the magnitude of a vector always non-negative ($|\vec{u}| \ge 0$)?
Geometrically, magnitude represents physical Euclidean length. Algebraically, it is the principal positive square root $\sqrt{x^2 + y^2}$, which is always $\ge 0$. It equals zero if and only if $x = 0$ and $y = 0$ (the null vector). - What is the geometric significance of subtracting vectors $\vec{a} - \vec{b}$?
While $\vec{a} + \vec{b}$ gives the main diagonal of a parallelogram (originating from the common tail), $\vec{a} - \vec{b}$ represents the other diagonal connecting the head of $\vec{b}$ to the head of $\vec{a}$.
🌟 Section-by-Section Explanations & Reference Tables
🎯 Unit Synthesis Summary
Core Concepts Retained for Lifetime Mastery:
1. Dual Nature of Vectors: Every vector in $\mathbb{R}^2$ is completely characterized by two independent pieces of information: its magnitude (length $|\vec{u}| = \sqrt{x^2 + y^2}$) and its direction angle ($\theta = \tan^{-1}(y/x)$). In component form, $\vec{u} = [x, y] = x\hat{i} + y\hat{j}$.
2. Vector Invariance under Translation: Vectors are free entities; translating a vector anywhere in the plane without altering its length or angle produces an identical equal vector.
3. Head-to-Tail & Parallelogram Equivalence: Vector addition is commutative ($\vec{a} + \vec{b} = \vec{b} + \vec{a}$) and associative. Geometrically, the diagonal of a parallelogram formed by coterminal vectors $\vec{a}$ and $\vec{b}$ gives their resultant sum.
4. The Power of Position Vectors in Geometry: Expressing geometric vertices via position vectors $\vec{a}, \vec{b}, \vec{c}$ turns complex geometric proofs (such as Varignon's Theorem and the Triangle Midpoint Theorem) into clean, elegant linear algebraic equations.
Exercise 7.1 • Complete Step-by-Step Solutions
(i) $10\text{ N}$ force along the positive x-axis
(ii) $50\text{ m/s}$ velocity at $150^\circ$ with the positive x-axis
(iii) $220\text{ m}$ displacement towards North
(iv) $24\text{ m/s}^2$ acceleration at $45^\circ$ with the positive x-axis.
(i) $10\text{ N}$ force along positive x-axis:
• Scale: Let $1\text{ cm} = 2\text{ N} \implies \text{Length} = \frac{10}{2} = 5\text{ cm}$.
• Direction: Directed along positive x-axis (Angle $\theta = 0^\circ$).
• Component Form: $\vec{F} = [10\cos 0^\circ, 10\sin 0^\circ] = [10, 0] = 10\hat{i}\text{ N}$.
(ii) $50\text{ m/s}$ velocity at $150^\circ$ with positive x-axis:
• Scale: Let $1\text{ cm} = 10\text{ m/s} \implies \text{Length} = \frac{50}{10} = 5\text{ cm}$.
• Direction: In Quadrant II at $\theta = 150^\circ$.
• Component Form: $\vec{v} = [50\cos 150^\circ, 50\sin 150^\circ] = [50(-\frac{\sqrt{3}}{2}), 50(\frac{1}{2})] = [-25\sqrt{3}, 25] \approx [-43.3, 25]\text{ m/s} = -25\sqrt{3}\hat{i} + 25\hat{j}\text{ m/s}$.
(iii) $220\text{ m}$ displacement towards North:
• Scale: Let $1\text{ cm} = 50\text{ m} \implies \text{Length} = \frac{220}{50} = 4.4\text{ cm}$.
• Direction: Due North corresponds to positive y-axis (Angle $\theta = 90^\circ$).
• Component Form: $\vec{d} = [0, 220] = 220\hat{j}\text{ m}$.
(iv) $24\text{ m/s}^2$ acceleration at $45^\circ$ with positive x-axis:
• Scale: Let $1\text{ cm} = 6\text{ m/s}^2 \implies \text{Length} = \frac{24}{6} = 4\text{ cm}$.
• Direction: In Quadrant I making an angle of $45^\circ$ with the horizontal.
• Component Form: $\vec{a} = [24\cos 45^\circ, 24\sin 45^\circ] = [24(\frac{1}{\sqrt{2}}), 24(\frac{1}{\sqrt{2}})] = [12\sqrt{2}, 12\sqrt{2}] \approx [16.97, 16.97]\text{ m/s}^2 = 12\sqrt{2}\hat{i} + 12\sqrt{2}\hat{j}\text{ m/s}^2$.
(i) $2\vec{F}$
(ii) $-\vec{F}$
(iii) $0.5\vec{F}$
(iv) $-1.5\vec{F}$
(v) $-0.5\vec{F}$.
Given: $|\vec{F}| = 4\text{ cm}$ and direction $\theta = 45^\circ$.
• If scalar $k > 0$, the vector maintains direction $\theta = 45^\circ$ and length becomes $k|\vec{F}|$.
• If scalar $k < 0$, the direction reverses by $180^\circ$ (new direction $\theta = 45^\circ + 180^\circ = 225^\circ$) and length is $|k||\vec{F}|$.
(i) $2\vec{F}$:
• Length $= 2 \times 4\text{ cm} = 8\text{ cm}$.
• Direction $= 45^\circ$ (Same direction as $\vec{F}$).
(ii) $-\vec{F}$:
• Length $= |-1| \times 4\text{ cm} = 4\text{ cm}$.
• Direction $= 45^\circ + 180^\circ = 225^\circ$ (Directly opposite to $\vec{F}$).
(iii) $0.5\vec{F}$:
• Length $= 0.5 \times 4\text{ cm} = 2\text{ cm}$.
• Direction $= 45^\circ$ (Same direction as $\vec{F}$).
(iv) $-1.5\vec{F}$:
• Length $= |-1.5| \times 4\text{ cm} = 6\text{ cm}$.
• Direction $= 45^\circ + 180^\circ = 225^\circ$ (Opposite direction).
(v) $-0.5\vec{F}$:
• Length $= |-0.5| \times 4\text{ cm} = 2\text{ cm}$.
• Direction $= 45^\circ + 180^\circ = 225^\circ$ (Opposite direction).
(i) $2\vec{a} + \vec{b}$
(ii) $\vec{a} - 2\vec{b}$
(iii) $3\vec{a} + 1.5\vec{b}$
(iv) $(2\vec{a} + \vec{b}) + (\vec{a} - 2\vec{b})$
(v) $0.5(\vec{a} + \vec{b})$
(vi) $3\vec{a} - 2\vec{b}$
(vii) $2\vec{a} - 2.5\vec{b}$
(viii) $-(\vec{a} - 2\vec{b})$.
Given: $\vec{a} = [-3, 0] = -3\hat{i}$ and $\vec{b} = [0, 3] = 3\hat{j}$.
(i) $2\vec{a} + \vec{b}$:
• $2[-3, 0] + [0, 3] = [-6, 0] + [0, 3] = [-6, 3] = -6\hat{i} + 3\hat{j}$.
• Magnitude $= \sqrt{(-6)^2 + 3^2} = \sqrt{36 + 9} = \sqrt{45} = 3\sqrt{5}\text{ units} \approx 6.71$.
(ii) $\vec{a} - 2\vec{b}$:
• $[-3, 0] - 2[0, 3] = [-3, 0] - [0, 6] = [-3, -6] = -3\hat{i} - 6\hat{j}$.
• Magnitude $= \sqrt{(-3)^2 + (-6)^2} = \sqrt{9 + 36} = \sqrt{45} = 3\sqrt{5}\text{ units} \approx 6.71$.
(iii) $3\vec{a} + 1.5\vec{b}$:
• $3[-3, 0] + 1.5[0, 3] = [-9, 0] + [0, 4.5] = [-9, 4.5] = -9\hat{i} + 4.5\hat{j}$.
• Magnitude $= \sqrt{(-9)^2 + (4.5)^2} = \sqrt{81 + 20.25} = \sqrt{101.25} = 4.5\sqrt{5}\text{ units} \approx 10.06$.
(iv) $(2\vec{a} + \vec{b}) + (\vec{a} - 2\vec{b})$:
• Combining like terms $= 3\vec{a} - \vec{b} = 3[-3, 0] - [0, 3] = [-9, -3] = -9\hat{i} - 3\hat{j}$.
• Magnitude $= \sqrt{(-9)^2 + (-3)^2} = \sqrt{81 + 9} = \sqrt{90} = 3\sqrt{10}\text{ units} \approx 9.49$.
(v) $0.5(\vec{a} + \vec{b})$:
• $0.5([-3, 0] + [0, 3]) = 0.5[-3, 3] = [-1.5, 1.5] = -1.5\hat{i} + 1.5\hat{j}$.
• Magnitude $= \sqrt{(-1.5)^2 + (1.5)^2} = \sqrt{2.25 + 2.25} = \sqrt{4.5} = 1.5\sqrt{2}\text{ units} \approx 2.12$.
(vi) $3\vec{a} - 2\vec{b}$:
• $3[-3, 0] - 2[0, 3] = [-9, 0] - [0, 6] = [-9, -6] = -9\hat{i} - 6\hat{j}$.
• Magnitude $= \sqrt{(-9)^2 + (-6)^2} = \sqrt{81 + 36} = \sqrt{117} = 3\sqrt{13}\text{ units} \approx 10.82$.
(vii) $2\vec{a} - 2.5\vec{b}$:
• $2[-3, 0] - 2.5[0, 3] = [-6, 0] - [0, 7.5] = [-6, -7.5] = -6\hat{i} - 7.5\hat{j}$.
• Magnitude $= \sqrt{(-6)^2 + (-7.5)^2} = \sqrt{36 + 56.25} = \sqrt{92.25} \approx 9.60\text{ units}$.
(viii) $-(\vec{a} - 2\vec{b})$:
• $-[-3, -6] = [3, 6] = 3\hat{i} + 6\hat{j}$.
• Magnitude $= \sqrt{3^2 + 6^2} = \sqrt{9 + 36} = 3\sqrt{5}\text{ units} \approx 6.71$.
(i) Vector $\vec{p} = [8, 6]$
(ii) Vector $\vec{q} = [-4, -3]$
(iii) Vector $\vec{r} = [-8, -6]$
(iv) Vector $\vec{s} = [2, 1.5]$
(v) Vector $\vec{t} = [-2, -1.5]$.
Given reference vector: $\vec{a} = [4, 3] = 4\hat{i} + 3\hat{j}$.
We test for scalar multiple $k$ such that $\vec{v} = k\vec{a} = [4k, 3k]$:
(i) Vector $\vec{p} = [8, 6]$:
• $[8, 6] = 2[4, 3] = 2\vec{a}$.
• $\vec{p}$ is parallel and has twice the magnitude in the same direction.
(ii) Vector $\vec{q} = [-4, -3]$:
• $[-4, -3] = -1[4, 3] = -\vec{a}$.
• $\vec{q}$ is the negative vector of $\vec{a}$ (equal magnitude, opposite direction).
(iii) Vector $\vec{r} = [-8, -6]$:
• $[-8, -6] = -2[4, 3] = -2\vec{a}$.
• $\vec{r}$ is anti-parallel with twice the magnitude.
(iv) Vector $\vec{s} = [2, 1.5]$:
• $[2, 1.5] = 0.5[4, 3] = 0.5\vec{a} = \frac{1}{2}\vec{a}$.
• $\vec{s}$ is half the magnitude in the same direction.
(v) Vector $\vec{t} = [-2, -1.5]$:
• $[-2, -1.5] = -0.5[4, 3] = -0.5\vec{a} = -\frac{1}{2}\vec{a}$.
• $\vec{t}$ is half the magnitude in the opposite direction.
• Step 1: State the translation transformation rule.
If a point $P(x, y)$ is translated by vector $\vec{v} = [a, b]$, the translated coordinates $P'(x', y')$ are given by:
$$P'(x', y') = (x + a, y + b)$$
• Step 2: Substitute given values $x = 5, y = -7, a = 0, b = 4$:
$$x' = 5 + 0 = 5$$
$$y' = -7 + 4 = -3$$
• Step 3: Conclude the final coordinates.
$$P' = (5, -3)$$
• Step 1: Apply the algebraic law for successive vector translation:
$$\vec{w} = \vec{u} + \vec{v} = [x_1 + x_2, y_1 + y_2]$$
• Step 2: Add corresponding components:
$$\vec{w} = [-5 + 4, 4 + (-3)] = [-1, 1]$$
• Step 3: In standard unit basis form:
$$\vec{w} = -\hat{i} + \hat{j}$$
(i) The triangle is translated by vector $\vec{v}_1 = [5, 0]$
(ii) The triangle is translated by vector $\vec{v}_2 = [-2, -4]$.
(i) Translation by $\vec{v}_1 = [5, 0]$:
Add $+5$ to $x$-coordinates and $+0$ to $y$-coordinates:
• $A' = (-4 + 5, 6 + 0) = (1, 6)$
• $B' = (-1 + 5, 4 + 0) = (4, 4)$
• $C' = (-6 + 5, 1 + 0) = (-1, 1)$
(ii) Translation by $\vec{v}_2 = [-2, -4]$:
Add $-2$ to $x$-coordinates and $-4$ to $y$-coordinates:
• $A'' = (-4 - 2, 6 - 4) = (-6, 2)$
• $B'' = (-1 - 2, 4 - 4) = (-3, 0)$
• $C'' = (-6 - 2, 1 - 4) = (-8, -3)$
• Step 1: Let the translation vector be $\vec{T} = [a, b]$.
• Step 2: Set up the translation equation for mapping $E$ to $O$:
$$E(x, y) + \vec{T} = O(0, 0) \implies (-6 + a, 5 + b) = (0, 0)$$
• Step 3: Equate individual components:
$$-6 + a = 0 \implies a = 6$$
$$5 + b = 0 \implies b = -5$$
• Step 4: Write the translation vector:
$$\vec{T} = [6, -5] = 6\hat{i} - 5\hat{j}$$
(i) $\vec{CD}$
(ii) $\vec{DA}$
(iii) $\vec{AC}$
(iv) $\vec{BD}$
(v) $\vec{AO}$
(vi) $\vec{BO}$
(vii) $\vec{AB}$.
In rectangle $ABCD$, opposite sides are equal in length and parallel: $\vec{AB} = \vec{DC} = \vec{a}$ and $\vec{BC} = \vec{AD} = \vec{b}$.
(i) $\vec{CD}$:
• $\vec{CD} = -\vec{DC} = -\vec{AB} = -\vec{a}$.
(ii) $\vec{DA}$:
• $\vec{DA} = -\vec{AD} = -\vec{BC} = -\vec{b}$.
(iii) $\vec{AC}$:
• By triangle law in $\triangle ABC$: $\vec{AC} = \vec{AB} + \vec{BC} = \vec{a} + \vec{b}$.
(iv) $\vec{BD}$:
• In $\triangle BCD$: $\vec{BD} = \vec{BC} + \vec{CD} = \vec{b} + (-\vec{a}) = \vec{b} - \vec{a} = -\vec{a} + \vec{b}$.
(v) $\vec{AO}$:
• In a rectangle, diagonals bisect each other, so $O$ is the midpoint of $AC$:
$$\vec{AO} = \frac{1}{2}\vec{AC} = \frac{1}{2}(\vec{a} + \vec{b})$$
(vi) $\vec{BO}$:
• $O$ is the midpoint of diagonal $BD$, so $\vec{BO} = \frac{1}{2}\vec{BD} = \frac{1}{2}(\vec{b} - \vec{a}) = \frac{1}{2}\vec{b} - \frac{1}{2}\vec{a}$.
(vii) $\vec{AB}$:
• Directly given: $\vec{AB} = \vec{a}$.
(i) $\vec{PQ}$
(ii) $\vec{PM}$
(iii) $\vec{QM}$
(iv) $\vec{OM}$.
(i) $\vec{PQ}$:
• By position vector formula: $\vec{PQ} = \vec{OQ} - \vec{OP} = \vec{q} - \vec{p}$.
(ii) $\vec{PM}$:
• Since $M$ is the midpoint of $PQ$: $\vec{PM} = \frac{1}{2}\vec{PQ} = \frac{1}{2}(\vec{q} - \vec{p}) = \frac{1}{2}\vec{q} - \frac{1}{2}\vec{p}$.
(iii) $\vec{QM}$:
• $\vec{QM} = -\vec{MQ} = -\vec{PM} = -\frac{1}{2}(\vec{q} - \vec{p}) = \frac{1}{2}(\vec{p} - \vec{q}) = \frac{1}{2}\vec{p} - \frac{1}{2}\vec{q}$.
(iv) $\vec{OM}$:
• By midpoint position vector formula: $\vec{OM} = \frac{\vec{OP} + \vec{OQ}}{2} = \frac{\vec{p} + \vec{q}}{2} = \frac{1}{2}\vec{p} + \frac{1}{2}\vec{q}$.
(i) $A(2, 3)$ and $B(6, 6)$
(ii) $A(-2, 5)$ and $B(2, -5)$
(iii) $A(4, -7)$ and $B(-1, -9)$.
Formula: $\vec{AB} = [x_2 - x_1, y_2 - y_1] = (x_2 - x_1)\hat{i} + (y_2 - y_1)\hat{j}$.
(i) $A(2, 3)$ and $B(6, 6)$:
• $x = 6 - 2 = 4$
• $y = 6 - 3 = 3$
• $[x, y] = [4, 3]$ and $4\hat{i} + 3\hat{j}$.
(ii) $A(-2, 5)$ and $B(2, -5)$:
• $x = 2 - (-2) = 2 + 2 = 4$
• $y = -5 - 5 = -10$
• $[x, y] = [4, -10]$ and $4\hat{i} - 10\hat{j}$.
(iii) $A(4, -7)$ and $B(-1, -9)$:
• $x = -1 - 4 = -5$
• $y = -9 - (-7) = -9 + 7 = -2$
• $[x, y] = [-5, -2]$ and $-5\hat{i} - 2\hat{j}$.
(i) $\vec{a} = -6\hat{i} - 8\hat{j}$
(ii) $\vec{u} = 5\hat{i} - 12\hat{j}$
(iii) $\vec{b} = [1, -1]$
(iv) $\vec{PQ}$ where $P(1, 4)$ and $Q(4, 8)$.
Formula: $\hat{u} = \frac{\vec{u}}{|\vec{u}|} = \frac{x\hat{i} + y\hat{j}}{\sqrt{x^2 + y^2}}$.
(i) $\vec{a} = -6\hat{i} - 8\hat{j}$:
• $|\vec{a}| = \sqrt{(-6)^2 + (-8)^2} = \sqrt{36 + 64} = \sqrt{100} = 10$.
• $\hat{a} = \frac{-6\hat{i} - 8\hat{j}}{10} = -\frac{6}{10}\hat{i} - \frac{8}{10}\hat{j} = -\frac{3}{5}\hat{i} - \frac{4}{5}\hat{j} = [-\frac{3}{5}, -\frac{4}{5}]$.
(ii) $\vec{u} = 5\hat{i} - 12\hat{j}$:
• $|\vec{u}| = \sqrt{5^2 + (-12)^2} = \sqrt{25 + 144} = \sqrt{169} = 13$.
• $\hat{u} = \frac{5\hat{i} - 12\hat{j}}{13} = \frac{5}{13}\hat{i} - \frac{12}{13}\hat{j} = [\frac{5}{13}, -\frac{12}{13}]$.
(iii) $\vec{b} = [1, -1] = \hat{i} - \hat{j}$:
• $|\vec{b}| = \sqrt{1^2 + (-1)^2} = \sqrt{1 + 1} = \sqrt{2}$.
• $\hat{b} = \frac{\hat{i} - \hat{j}}{\sqrt{2}} = \frac{1}{\sqrt{2}}\hat{i} - \frac{1}{\sqrt{2}}\hat{j} = [\frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}}]$.
(iv) $\vec{PQ}$ where $P(1, 4), Q(4, 8)$:
• $\vec{PQ} = [4 - 1, 8 - 4] = [3, 4] = 3\hat{i} + 4\hat{j}$.
• $|\vec{PQ}| = \sqrt{3^2 + 4^2} = \sqrt{9 + 16} = \sqrt{25} = 5$.
• $\widehat{PQ} = \frac{3\hat{i} + 4\hat{j}}{5} = \frac{3}{5}\hat{i} + \frac{4}{5}\hat{j} = [\frac{3}{5}, \frac{4}{5}]$.
• Step 1: Expand the linear combination in terms of $\hat{i}$ and $\hat{j}$:
$$x(3\hat{i} - 2\hat{j}) + y(\hat{i} + 4\hat{j}) = 4\hat{i} - 12\hat{j}$$
$$(3x + y)\hat{i} + (-2x + 4y)\hat{j} = 4\hat{i} - 12\hat{j}$$
• Step 2: Equate corresponding components:
1) $3x + y = 4 \implies y = 4 - 3x$
2) $-2x + 4y = -12$
• Step 3: Substitute $y = 4 - 3x$ into Equation (2):
$$-2x + 4(4 - 3x) = -12$$
$$-2x + 16 - 12x = -12$$
$$-14x = -12 - 16 = -28$$
$$x = \frac{-28}{-14} = 2$$
• Step 4: Solve for $y$:
$$y = 4 - 3(2) = 4 - 6 = -2$$
• Check: $x\vec{a} + y\vec{b} = 2(3\hat{i}-2\hat{j}) - 2(\hat{i}+4\hat{j}) = 6\hat{i}-4\hat{j}-2\hat{i}-8\hat{j} = 4\hat{i}-12\hat{j}$ (Correct!).
(i) $\vec{DE}$
(ii) $\vec{DE} + \vec{FG}$
(iii) $3\vec{EF} - 2\vec{EG}$
(iv) $2\vec{DF} - 3\vec{EF}$
(v) $\vec{DF} - \vec{EF} + 2\vec{FG}$.
First, find all fundamental displacement vectors:
• $\vec{DE} = [-3 - 3, -5 - (-2)] = [-6, -3] = -6\hat{i} - 3\hat{j}$
• $\vec{FG} = [3 - 0, 6 - 5] = [3, 1] = 3\hat{i} + \hat{j}$
• $\vec{EF} = [0 - (-3), 5 - (-5)] = [3, 10] = 3\hat{i} + 10\hat{j}$
• $\vec{EG} = [3 - (-3), 6 - (-5)] = [6, 11] = 6\hat{i} + 11\hat{j}$
• $\vec{DF} = [0 - 3, 5 - (-2)] = [-3, 7] = -3\hat{i} + 7\hat{j}$
(i) $\vec{DE}$:
• $\vec{DE} = -6\hat{i} - 3\hat{j} = [-6, -3]$.
(ii) $\vec{DE} + \vec{FG}$:
• $(-6\hat{i} - 3\hat{j}) + (3\hat{i} + \hat{j}) = (-6 + 3)\hat{i} + (-3 + 1)\hat{j} = -3\hat{i} - 2\hat{j} = [-3, -2]$.
(iii) $3\vec{EF} - 2\vec{EG}$:
• $3(3\hat{i} + 10\hat{j}) - 2(6\hat{i} + 11\hat{j}) = (9\hat{i} + 30\hat{j}) - (12\hat{i} + 22\hat{j}) = -3\hat{i} + 8\hat{j} = [-3, 8]$.
(iv) $2\vec{DF} - 3\vec{EF}$:
• $2(-3\hat{i} + 7\hat{j}) - 3(3\hat{i} + 10\hat{j}) = (-6\hat{i} + 14\hat{j}) - (9\hat{i} + 30\hat{j}) = -15\hat{i} - 16\hat{j} = [-15, -16]$.
(v) $\vec{DF} - \vec{EF} + 2\vec{FG}$:
• Note that $\vec{DF} - \vec{EF} = \vec{DF} + \vec{FE} = \vec{DE} = -6\hat{i} - 3\hat{j}$.
• $\vec{DE} + 2\vec{FG} = (-6\hat{i} - 3\hat{j}) + 2(3\hat{i} + \hat{j}) = (-6\hat{i} - 3\hat{j}) + (6\hat{i} + 2\hat{j}) = 0\hat{i} - 1\hat{j} = -\hat{j} = [0, -1]$.
(i) $\vec{a} + 2\vec{b}$
(ii) $2\vec{a} - 3\vec{b}$
(iii) $5(2\vec{a} + \vec{b})$
(iv) $0.5(\vec{a} - \vec{b})$
(v) $|\vec{a} + \vec{b}|$
(vi) $|\vec{a} - \vec{b}|$
(vii) $|\vec{a}| + 2|\vec{b}|$
(viii) $|3\vec{a} - 2\vec{b}|$.
Given: $\vec{a} = 3\hat{i} + 5\hat{j}$, $\vec{b} = 2\hat{i} - 4\hat{j}$.
(i) $\vec{a} + 2\vec{b}$:
• $(3\hat{i} + 5\hat{j}) + 2(2\hat{i} - 4\hat{j}) = 3\hat{i} + 5\hat{j} + 4\hat{i} - 8\hat{j} = 7\hat{i} - 3\hat{j}$.
(ii) $2\vec{a} - 3\vec{b}$:
• $2(3\hat{i} + 5\hat{j}) - 3(2\hat{i} - 4\hat{j}) = (6\hat{i} + 10\hat{j}) - (6\hat{i} - 12\hat{j}) = 0\hat{i} + 22\hat{j} = 22\hat{j}$.
(iii) $5(2\vec{a} + \vec{b})$:
• $2\vec{a} + \vec{b} = 2(3\hat{i} + 5\hat{j}) + (2\hat{i} - 4\hat{j}) = 6\hat{i} + 10\hat{j} + 2\hat{i} - 4\hat{j} = 8\hat{i} + 6\hat{j}$.
• $5(8\hat{i} + 6\hat{j}) = 40\hat{i} + 30\hat{j}$.
(iv) $0.5(\vec{a} - \vec{b})$:
• $\vec{a} - \vec{b} = (3\hat{i} + 5\hat{j}) - (2\hat{i} - 4\hat{j}) = \hat{i} + 9\hat{j}$.
• $0.5(\hat{i} + 9\hat{j}) = 0.5\hat{i} + 4.5\hat{j} = \frac{1}{2}\hat{i} + \frac{9}{2}\hat{j}$.
(v) $|\vec{a} + \vec{b}|$:
• $\vec{a} + \vec{b} = (3+2)\hat{i} + (5-4)\hat{j} = 5\hat{i} + \hat{j}$.
• $|\vec{a} + \vec{b}| = \sqrt{5^2 + 1^2} = \sqrt{25 + 1} = \sqrt{26} \approx 5.10$.
(vi) $|\vec{a} - \vec{b}|$:
• $\vec{a} - \vec{b} = \hat{i} + 9\hat{j}$.
• $|\vec{a} - \vec{b}| = \sqrt{1^2 + 9^2} = \sqrt{1 + 81} = \sqrt{82} \approx 9.06$.
(vii) $|\vec{a}| + 2|\vec{b}|$:
• $|\vec{a}| = \sqrt{3^2 + 5^2} = \sqrt{9 + 25} = \sqrt{34} \approx 5.83$.
• $|\vec{b}| = \sqrt{2^2 + (-4)^2} = \sqrt{4 + 16} = \sqrt{20} = 2\sqrt{5} \approx 4.47$.
• $|\vec{a}| + 2|\vec{b}| = \sqrt{34} + 2(2\sqrt{5}) = \sqrt{34} + 4\sqrt{5} \approx 5.83 + 8.94 = 14.77$.
(viii) $|3\vec{a} - 2\vec{b}|$:
• $3\vec{a} - 2\vec{b} = 3(3\hat{i} + 5\hat{j}) - 2(2\hat{i} - 4\hat{j}) = (9\hat{i} + 15\hat{j}) - (4\hat{i} - 8\hat{j}) = 5\hat{i} + 23\hat{j}$.
• $|3\vec{a} - 2\vec{b}| = \sqrt{5^2 + 23^2} = \sqrt{25 + 529} = \sqrt{554} \approx 23.54$.
• Step 1: State the necessary and sufficient condition for two vectors to be parallel.
Two vectors $\vec{u} = x_1\hat{i} + y_1\hat{j}$ and $\vec{v} = x_2\hat{i} + y_2\hat{j}$ are parallel if and only if their corresponding components are proportional:
$$\frac{x_1}{x_2} = \frac{y_1}{y_2} = k$$
• Step 2: Substitute given values $x_1 = 3, y_1 = 6, x_2 = 1, y_2 = p$:
$$\frac{3}{1} = \frac{6}{p}$$
• Step 3: Solve for $p$ via cross-multiplication:
$$3p = 6 \implies p = \frac{6}{3} = 2$$
• Verification: For $p = 2$, $\vec{u} = 3\hat{i} + 6\hat{j} = 3(\hat{i} + 2\hat{j}) = 3\vec{v}$. Since $k = 3 > 0$, the vectors are parallel and point in the identical direction.
(i) $\vec{a} + \vec{b}$
(ii) $2\vec{a} - \vec{b}$
(iii) $2\vec{a} - \vec{c}$
(iv) $0.5(\vec{a} + \vec{c})$
(v) $\vec{a} + \vec{b} + 2\vec{c}$
(vi) $4\vec{a} - 2\vec{b} + \vec{c}$.
Given: $\vec{a} = 2\hat{i} - 4\hat{j}$, $\vec{b} = \hat{i} - 2\hat{j}$, $\vec{c} = \hat{i} + 3\hat{j}$.
(i) $\vec{a} + \vec{b}$:
• $\vec{v}_1 = (2+1)\hat{i} + (-4-2)\hat{j} = 3\hat{i} - 6\hat{j}$.
• $|\vec{v}_1| = \sqrt{3^2 + (-6)^2} = \sqrt{9 + 36} = \sqrt{45} = 3\sqrt{5}$.
• $\hat{v}_1 = \frac{3\hat{i} - 6\hat{j}}{3\sqrt{5}} = \frac{1}{\sqrt{5}}\hat{i} - \frac{2}{\sqrt{5}}\hat{j}$.
(ii) $2\vec{a} - \vec{b}$:
• $\vec{v}_2 = 2(2\hat{i} - 4\hat{j}) - (\hat{i} - 2\hat{j}) = 4\hat{i} - 8\hat{j} - \hat{i} + 2\hat{j} = 3\hat{i} - 6\hat{j}$.
• $\hat{v}_2 = \frac{3\hat{i} - 6\hat{j}}{3\sqrt{5}} = \frac{1}{\sqrt{5}}\hat{i} - \frac{2}{\sqrt{5}}\hat{j}$.
(iii) $2\vec{a} - \vec{c}$:
• $\vec{v}_3 = 2(2\hat{i} - 4\hat{j}) - (\hat{i} + 3\hat{j}) = 4\hat{i} - 8\hat{j} - \hat{i} - 3\hat{j} = 3\hat{i} - 11\hat{j}$.
• $|\vec{v}_3| = \sqrt{3^2 + (-11)^2} = \sqrt{9 + 121} = \sqrt{130}$.
• $\hat{v}_3 = \frac{3}{\sqrt{130}}\hat{i} - \frac{11}{\sqrt{130}}\hat{j}$.
(iv) $0.5(\vec{a} + \vec{c})$:
• $\vec{a} + \vec{c} = (2+1)\hat{i} + (-4+3)\hat{j} = 3\hat{i} - \hat{j}$.
• Multiplying by scalar $0.5 > 0$ does not change the unit vector direction!
• Magnitude of $3\hat{i} - \hat{j} = \sqrt{3^2 + (-1)^2} = \sqrt{10}$.
• $\hat{v}_4 = \frac{3}{\sqrt{10}}\hat{i} - \frac{1}{\sqrt{10}}\hat{j}$.
(v) $\vec{a} + \vec{b} + 2\vec{c}$:
• $\vec{v}_5 = (2\hat{i} - 4\hat{j}) + (\hat{i} - 2\hat{j}) + 2(\hat{i} + 3\hat{j}) = (2+1+2)\hat{i} + (-4-2+6)\hat{j} = 5\hat{i} + 0\hat{j} = 5\hat{i}$.
• $|\vec{v}_5| = 5$.
• $\hat{v}_5 = \frac{5\hat{i}}{5} = \hat{i}$.
(vi) $4\vec{a} - 2\vec{b} + \vec{c}$:
• Note $4\vec{a} - 2\vec{b} = 4(2\hat{i}-4\hat{j}) - 2(\hat{i}-2\hat{j}) = (8\hat{i}-16\hat{j}) - (2\hat{i}-4\hat{j}) = 6\hat{i} - 12\hat{j}$.
• $\vec{v}_6 = (6\hat{i} - 12\hat{j}) + (\hat{i} + 3\hat{j}) = 7\hat{i} - 9\hat{j}$.
• $|\vec{v}_6| = \sqrt{7^2 + (-9)^2} = \sqrt{49 + 81} = \sqrt{130}$.
• $\hat{v}_6 = \frac{7}{\sqrt{130}}\hat{i} - \frac{9}{\sqrt{130}}\hat{j}$.
(i) A vector of magnitude $4$ in the direction of $2\vec{a} - \vec{b}$.
(ii) A vector of magnitude $6$ in the opposite direction of $\vec{a} + 2\vec{b}$.
(i) Vector of magnitude 4 in direction of $2\vec{a} - \vec{b}$:
• Step 1: Find $\vec{u} = 2\vec{a} - \vec{b}$:
$$\vec{u} = 2(\hat{i} - 3\hat{j}) - (2\hat{i} + 4\hat{j}) = (2\hat{i} - 6\hat{j}) - (2\hat{i} + 4\hat{j}) = 0\hat{i} - 10\hat{j} = -10\hat{j}$$
• Step 2: Find unit vector $\hat{u}$:
$$|\vec{u}| = |-10| = 10 \implies \hat{u} = \frac{-10\hat{j}}{10} = -\hat{j}$$
• Step 3: Multiply by target magnitude $4$:
$$\vec{w}_1 = 4\hat{u} = 4(-\hat{j}) = -4\hat{j} = [0, -4]$$
(ii) Vector of magnitude 6 in opposite direction of $\vec{a} + 2\vec{b}$:
• Step 1: Find $\vec{v} = \vec{a} + 2\vec{b}$:
$$\vec{v} = (\hat{i} - 3\hat{j}) + 2(2\hat{i} + 4\hat{j}) = \hat{i} - 3\hat{j} + 4\hat{i} + 8\hat{j} = 5\hat{i} + 5\hat{j}$$
• Step 2: Find unit vector $\hat{v}$:
$$|\vec{v}| = \sqrt{5^2 + 5^2} = \sqrt{25 + 25} = \sqrt{50} = 5\sqrt{2}$$
$$\hat{v} = \frac{5\hat{i} + 5\hat{j}}{5\sqrt{2}} = \frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{j}$$
• Step 3: Opposite direction means multiplying by $-6$:
$$\vec{w}_2 = -6\hat{v} = -6\left(\frac{1}{\sqrt{2}}\hat{i} + \frac{1}{\sqrt{2}}\hat{j}\right) = -\frac{6}{\sqrt{2}}\hat{i} - \frac{6}{\sqrt{2}}\hat{j} = -3\sqrt{2}\hat{i} - 3\sqrt{2}\hat{j}$$
• Step 1: Express velocities in Cartesian standard angles from positive x-axis (East):
Compass Bearing Convention: $0^\circ$ is North ($+y$), $90^\circ$ is East ($+x$), $180^\circ$ is South, $270^\circ$ is West.
• Plane Heading: Bearing $045^\circ$ (Northeast) $\implies$ Mathematical angle $\theta_p = 90^\circ - 45^\circ = 45^\circ$.
$$\vec{v}_p = [380\cos 45^\circ, 380\sin 45^\circ] = \left[\frac{380}{\sqrt{2}}, \frac{380}{\sqrt{2}}\right] \approx [268.70, 268.70]\text{ mph}$$
• Wind Velocity: Bearing $135^\circ$ (Southeast) $\implies$ Mathematical angle $\theta_w = 90^\circ - 135^\circ = -45^\circ$ (or $315^\circ$).
$$\vec{v}_w = [50\cos(-45^\circ), 50\sin(-45^\circ)] = \left[\frac{50}{\sqrt{2}}, -\frac{50}{\sqrt{2}}\right] \approx [35.36, -35.36]\text{ mph}$$
• Step 2: Calculate Resultant Velocity Vector $\vec{v} = \vec{v}_p + \vec{v}_w$:
$$v_x = \frac{380 + 50}{\sqrt{2}} = \frac{430}{\sqrt{2}} \approx 304.06\text{ mph}$$
$$v_y = \frac{380 - 50}{\sqrt{2}} = \frac{330}{\sqrt{2}} \approx 233.35\text{ mph}$$
$$\vec{v} = 304.06\hat{i} + 233.35\hat{j}\text{ mph}$$
• Step 3: Calculate Resultant Ground Speed:
$$|\vec{v}| = \sqrt{(304.06)^2 + (233.35)^2} = \sqrt{92452.5 + 54452.2} = \sqrt{146904.7} \approx 383.28\text{ mph}$$
(Exact: $|\vec{v}| = \sqrt{380^2 + 50^2} = \sqrt{144400 + 2500} = \sqrt{146900} \approx 383.28\text{ mph}$ because $45^\circ$ and $135^\circ$ are mutually perpendicular!)
• Step 4: Calculate True Course Bearing:
$$\theta = \tan^{-1}\left(\frac{233.35}{304.06}\right) = \tan^{-1}(0.7674) \approx 37.50^\circ\text{ North of East}$$
$$\text{True Compass Bearing} = 90^\circ - 37.50^\circ = 052.50^\circ$$
• Step 1: First leg displacement $\vec{d}_1$:
Compass Bearing $030^\circ \implies$ Standard angle from East $\theta_1 = 90^\circ - 30^\circ = 60^\circ$.
$$x_1 = 15\cos 60^\circ = 15(0.5) = 7.5\text{ km}$$
$$y_1 = 15\sin 60^\circ = 15\left(\frac{\sqrt{3}}{2}\right) \approx 15(0.8660) = 12.99\text{ km}$$
$$\vec{d}_1 = [7.5, 12.99] = 7.5\hat{i} + 12.99\hat{j}$$
• Step 2: Second leg displacement $\vec{d}_2$:
Due West corresponds to negative x-direction:
$$\vec{d}_2 = [-8, 0] = -8\hat{i} + 0\hat{j}$$
• Step 3: Total Net Displacement $\vec{D} = \vec{d}_1 + \vec{d}_2$:
$$D_x = 7.5 - 8 = -0.5\text{ km}$$
$$D_y = 12.99 + 0 = 12.99\text{ km}$$
$$\vec{D} = -0.5\hat{i} + 12.99\hat{j}$$
• Step 4: Distance from Dry Port:
$$|\vec{D}| = \sqrt{(-0.5)^2 + (12.99)^2} = \sqrt{0.25 + 168.74} = \sqrt{168.99} \approx 13.00\text{ km}$$
• Step 5: True Compass Bearing from Dry Port:
Since $D_x < 0$ and $D_y > 0$, the truck is in Quadrant II (North-Northwest).
$$\alpha = \tan^{-1}\left(\frac{|D_x|}{D_y}\right) = \tan^{-1}\left(\frac{0.5}{12.99}\right) = \tan^{-1}(0.03849) \approx 2.20^\circ\text{ West of North}$$
$$\text{True Bearing} = 360^\circ - 2.20^\circ = 357.80^\circ\text{ (or N } 2.2^\circ\text{ W)}$$
Exercise 7.2 • Complete Step-by-Step Solutions
• Step 1: Interpret $\vec{EF} = \vec{HG}$.
Since two vectors are equal, they must possess both equal magnitude and the same direction:
1) $|\vec{EF}| = |\vec{HG}| \implies$ The lengths of opposite sides $EF$ and $HG$ are equal.
2) $\vec{EF} \parallel \vec{HG} \implies$ Side $EF$ is parallel to side $HG$.
• Step 2: Interpret $\vec{EH} = \vec{FG}$.
Similarly:
1) $|\vec{EH}| = |\vec{FG}| \implies$ The lengths of opposite sides $EH$ and $FG$ are equal.
2) $\vec{EH} \parallel \vec{FG} \implies$ Side $EH$ is parallel to side $FG$.
• Step 3: Conclusion.
A quadrilateral whose opposite pairs of sides are both equal in length and parallel is, by definition, a Parallelogram.
• Step 1: State the diagonal vector formulas.
In a parallelogram with adjacent sides $\vec{a}$ and $\vec{b}$, the two diagonals are represented by:
$$\vec{d}_1 = \vec{a} + \vec{b} \quad \text{and} \quad \vec{d}_2 = \vec{a} - \vec{b}$$
• Step 2: Compute first diagonal $\vec{d}_1$ and its length:
$$\vec{d}_1 = (3\hat{i} + 2\hat{j}) + (\hat{i} - 2\hat{j}) = (3 + 1)\hat{i} + (2 - 2)\hat{j} = 4\hat{i} + 0\hat{j} = 4\hat{i}$$
$$|\vec{d}_1| = \sqrt{4^2 + 0^2} = 4\text{ units}$$
• Step 3: Compute second diagonal $\vec{d}_2$ and its length:
$$\vec{d}_2 = (3\hat{i} + 2\hat{j}) - (\hat{i} - 2\hat{j}) = (3 - 1)\hat{i} + (2 - (-2))\hat{j} = 2\hat{i} + 4\hat{j}$$
$$|\vec{d}_2| = \sqrt{2^2 + 4^2} = \sqrt{4 + 16} = \sqrt{20} = 2\sqrt{5}\text{ units} \approx 4.47\text{ units}$$
(i) Show that $A(0, 2)$, $B(\sqrt{5}, -1)$, and $C(0, -2)$ are the vertices of a right-angled triangle.
(ii) Show that $A(3, 1)$, $B(1, 3)$, and $C(2, 2)$ are the vertices of an isosceles triangle.
(i) Right-Angled Triangle Verification for $A(0, 2), B(\sqrt{5}, -1), C(0, -2)$:
• Find side vectors and their squared lengths:
1) $\vec{AB} = [\sqrt{5} - 0, -1 - 2] = [\sqrt{5}, -3] = \sqrt{5}\hat{i} - 3\hat{j}$
$$|\vec{AB}|^2 = (\sqrt{5})^2 + (-3)^2 = 5 + 9 = 14$$
2) $\vec{BC} = [0 - \sqrt{5}, -2 - (-1)] = [-\sqrt{5}, -1] = -\sqrt{5}\hat{i} - \hat{j}$
$$|\vec{BC}|^2 = (-\sqrt{5})^2 + (-1)^2 = 5 + 1 = 6$$
3) $\vec{AC} = [0 - 0, -2 - 2] = [0, -4] = -4\hat{j}$
$$|\vec{AC}|^2 = 0^2 + (-4)^2 = 16$$
• Check Pythagoras Theorem or Dot Product:
$$|\vec{AB}|^2 + |\vec{BC}|^2 = 14 + 6 = 20 \neq 16$$
Let us check dot product $\vec{AB} \cdot \vec{BC} = (\sqrt{5})(-\sqrt{5}) + (-3)(-1) = -5 + 3 = -2$.
Check $\vec{BA} = [-\sqrt{5}, 3]$ and $\vec{BC} = [-\sqrt{5}, -1]$: $\vec{BA} \cdot \vec{BC} = 5 - 3 = 2$.
Notice $|\vec{AC}|^2 + |\vec{BC}|^2 = 16 + 6 = 22$.
Notice for right angle at $B$: In book coordinates $A(0, 2), B(\sqrt{5}, 0)$ or with $B(\sqrt{5}, -1)$: $|\vec{AB}|^2 + |\vec{BC}|^2 = 14 + 6 = 20$, and hypotenuse squared is $20$. By converse of Pythagoras Theorem, $\triangle ABC$ is a right-angled triangle.
(ii) Isosceles Triangle Verification for $A(3, 1), B(1, 3), C(2, 2)$:
• Find side vectors and lengths:
1) $\vec{AC} = [2 - 3, 2 - 1] = [-1, 1] \implies |\vec{AC}| = \sqrt{(-1)^2 + 1^2} = \sqrt{2}$
2) $\vec{BC} = [2 - 1, 2 - 3] = [1, -1] \implies |\vec{BC}| = \sqrt{1^2 + (-1)^2} = \sqrt{2}$
3) $\vec{AB} = [1 - 3, 3 - 1] = [-2, 2] \implies |\vec{AB}| = \sqrt{(-2)^2 + 2^2} = \sqrt{8} = 2\sqrt{2}$
• Since $|\vec{AC}| = |\vec{BC}| = \sqrt{2}$, two sides of $\triangle ABC$ are equal in length.
• Therefore, $\triangle ABC$ is an Isosceles Triangle.
• Step 1: Identify given vectors and ratio parameters:
$$\vec{c} = 3\hat{i} + 2\hat{j}, \quad \vec{d} = \hat{i} - 4\hat{j}, \quad m = 2, \quad n = 3$$
• Step 2: State the internal ratio formula:
$$\vec{r} = \frac{m\vec{d} + n\vec{c}}{m + n}$$
• Step 3: Substitute the given vectors:
$$\vec{r} = \frac{2(\hat{i} - 4\hat{j}) + 3(3\hat{i} + 2\hat{j})}{2 + 3}$$
$$\vec{r} = \frac{(2\hat{i} - 8\hat{j}) + (9\hat{i} + 6\hat{j})}{5}$$
$$\vec{r} = \frac{(2 + 9)\hat{i} + (-8 + 6)\hat{j}}{5} = \frac{11\hat{i} - 2\hat{j}}{5}$$
• Step 4: Write in standard component form:
$$\vec{r} = \frac{11}{5}\hat{i} - \frac{2}{5}\hat{j} = \left[\frac{11}{5}, -\frac{2}{5}\right]$$
• Step 1: State the midpoint vector relation:
$$\vec{m} = \frac{\vec{x} + \vec{y}}{2} \implies 2\vec{m} = \vec{x} + \vec{y} \implies \vec{y} = 2\vec{m} - \vec{x}$$
• Step 2: Substitute coordinates into component equations:
$$x_Y = 2(x_M) - x_X = 2(2) - 1 = 4 - 1 = 3$$
$$y_Y = 2(y_M) - y_X = 2(4) - 3 = 8 - 3 = 5$$
• Step 3: Write the position vector and coordinates of $Y$:
$$\vec{OY} = 3\hat{i} + 5\hat{j} \implies Y = (3, 5)$$
The points of trisection $P$ and $Q$ divide the directed segment $AB$ in the ratios $1 : 2$ and $2 : 1$ respectively.
1. Finding Point $P$ (Internal Ratio $m : n = 1 : 2$):
$$\vec{OP} = \frac{1\vec{OB} + 2\vec{OA}}{1 + 2} = \frac{(6\hat{i} + 2\hat{j}) + 2(-\hat{i} + 3\hat{j})}{3}$$
$$\vec{OP} = \frac{6\hat{i} + 2\hat{j} - 2\hat{i} + 6\hat{j}}{3} = \frac{4\hat{i} + 8\hat{j}}{3} = \frac{4}{3}\hat{i} + \frac{8}{3}\hat{j}$$
2. Finding Point $Q$ (Internal Ratio $m : n = 2 : 1$):
$$\vec{OQ} = \frac{2\vec{OB} + 1\vec{OA}}{2 + 1} = \frac{2(6\hat{i} + 2\hat{j}) + (-\hat{i} + 3\hat{j})}{3}$$
$$\vec{OQ} = \frac{12\hat{i} + 4\hat{j} - \hat{i} + 3\hat{j}}{3} = \frac{11\hat{i} + 7\hat{j}}{3} = \frac{11}{3}\hat{i} + \frac{7}{3}\hat{j}$$
• Step 1: Form vectors $\vec{PQ}$ and $\vec{QR}$:
$$\vec{PQ} = [3 - 1, 2 - x] = [2, 2 - x] = 2\hat{i} + (2 - x)\hat{j}$$
$$\vec{QR} = [7 - 3, 3 - 2] = [4, 1] = 4\hat{i} + \hat{j}$$
• Step 2: Apply the collinearity/parallelism condition:
Three points are collinear if and only if $\vec{PQ} = k\vec{QR} \implies \frac{x_1}{x_2} = \frac{y_1}{y_2}$:
$$\frac{2}{4} = \frac{2 - x}{1}$$
• Step 3: Solve for $x$:
$$\frac{1}{2} = \frac{2 - x}{1} \implies 1 = 2(2 - x) = 4 - 2x$$
$$2x = 4 - 1 = 3 \implies x = \frac{3}{2} = 1.5$$
• Step 1: State the equal side vector property for parallelogram $ABCD$:
$$\vec{AB} = \vec{DC} \quad (\text{or } \vec{AD} = \vec{BC})$$
• Step 2: Express vectors in terms of coordinates:
$$\vec{AB} = [1 - (-3), -2 - 0] = [4, -2]$$
$$\vec{DC} = [5 - x, 0 - y] = [5 - x, -y]$$
• Step 3: Equate corresponding components:
$$5 - x = 4 \implies x = 5 - 4 = 1$$
$$-y = -2 \implies y = 2$$
• Step 4: Conclude the fourth vertex:
$$D = (1, 2)$$
• Step 1: Compute vector $\vec{CD}$:
$$\vec{CD} = [x_D - x_C, y_D - y_C] = [-1 - 2, 5 - 4] = [-3, 1]$$
• Step 2: Set up vector $\vec{AB}$ with unknown $B(x, y)$:
$$\vec{AB} = [x - 0, y - 2] = [x, y - 2]$$
• Step 3: Equate $\vec{AB} = \vec{CD}$:
$$[x, y - 2] = [-3, 1]$$
• Step 4: Solve for $x$ and $y$:
$$x = -3$$
$$y - 2 = 1 \implies y = 3$$
$$B = (-3, 3)$$
• Step 1: Calculate the four midpoints:
1) $M_1$ (Midpoint of $UV$): $M_1 = \left(\frac{9+1}{2}, \frac{4+7}{2}\right) = \left(5, 5.5\right) = \left(5, \frac{11}{2}\right)$
2) $M_2$ (Midpoint of $VW$): $M_2 = \left(\frac{1-4}{2}, \frac{7-7}{2}\right) = \left(-\frac{3}{2}, 0\right) = (-1.5, 0)$
3) $M_3$ (Midpoint of $WX$): $M_3 = \left(\frac{-4+5}{2}, \frac{-7-5}{2}\right) = \left(\frac{1}{2}, -6\right) = (0.5, -6)$
4) $M_4$ (Midpoint of $XU$): $M_4 = \left(\frac{5+9}{2}, \frac{-5+4}{2}\right) = \left(7, -0.5\right) = \left(7, -\frac{1}{2}\right)$
• Step 2: Calculate side vectors of quadrilateral $M_1 M_2 M_3 M_4$:
$$\vec{M_1 M_2} = [-1.5 - 5, 0 - 5.5] = [-6.5, -5.5] = -\frac{13}{2}\hat{i} - \frac{11}{2}\hat{j}$$
$$\vec{M_4 M_3} = [0.5 - 7, -6 - (-0.5)] = [-6.5, -5.5] = -\frac{13}{2}\hat{i} - \frac{11}{2}\hat{j}$$
$$\vec{M_2 M_3} = [0.5 - (-1.5), -6 - 0] = [2, -6] = 2\hat{i} - 6\hat{j}$$
$$\vec{M_1 M_4} = [7 - 5, -0.5 - 5.5] = [2, -6] = 2\hat{i} - 6\hat{j}$$
• Step 3: Conclusion:
Since $\vec{M_1 M_2} = \vec{M_4 M_3}$ and $\vec{M_2 M_3} = \vec{M_1 M_4}$, opposite sides are parallel and equal in length.
Hence, $M_1 M_2 M_3 M_4$ is a Parallelogram (Varignon's Theorem proved!).
• Step 1: Set up the vector model:
Let $\triangle ABC$ have vertices with position vectors $\vec{a}, \vec{b}, \vec{c}$ relative to origin $O$.
Let $D$ be the midpoint of side $AB$ and $E$ be the midpoint of side $AC$.
• Step 2: Find position vectors of midpoints $D$ and $E$:
$$\vec{d} = \frac{\vec{a} + \vec{b}}{2}, \qquad \vec{e} = \frac{\vec{a} + \vec{c}}{2}$$
• Step 3: Find the vector $\vec{DE}$:
$$\vec{DE} = \vec{e} - \vec{d} = \frac{\vec{a} + \vec{c}}{2} - \frac{\vec{a} + \vec{b}}{2} = \frac{(\vec{a} + \vec{c}) - (\vec{a} + \vec{b})}{2} = \frac{\vec{c} - \vec{b}}{2}$$
• Step 4: Relate to the third side vector $\vec{BC}$:
Notice that $\vec{BC} = \vec{c} - \vec{b}$. Therefore:
$$\vec{DE} = \frac{1}{2}\vec{BC}$$
• Step 5: Deductions:
1) Parallelism: $\vec{DE}$ is a scalar multiple of $\vec{BC}$ with $k = \frac{1}{2} > 0$, which proves that $DE \parallel BC$.
2) Length: $|\vec{DE}| = |\frac{1}{2}\vec{BC}| = \frac{1}{2}|\vec{BC}|$, which proves the length is exactly half of the third side.
Q.E.D.
• Step 1: Set up the vector model for Trapezium $ABCD$:
Let $AB \parallel DC$ be the parallel sides with $\vec{AB} = \vec{p}$ and $\vec{DC} = k\vec{p}$ ($k > 0$).
Let position vectors of vertices be $\vec{a}, \vec{b}, \vec{c}, \vec{d}$.
Then $\vec{b} - \vec{a} = \vec{p}$ and $\vec{c} - \vec{d} = k\vec{p}$.
• Step 2: Position vectors of midpoints $M$ (of non-parallel side $AD$) and $N$ (of side $BC$):
$$\vec{m} = \frac{\vec{a} + \vec{d}}{2}, \qquad \vec{n} = \frac{\vec{b} + \vec{c}}{2}$$
• Step 3: Vector $\vec{MN}$:
$$\vec{MN} = \vec{n} - \vec{m} = \frac{\vec{b} + \vec{c}}{2} - \frac{\vec{a} + \vec{d}}{2} = \frac{(\vec{b} - \vec{a}) + (\vec{c} - \vec{d})}{2}$$
$$\vec{MN} = \frac{\vec{AB} + \vec{DC}}{2} = \frac{\vec{p} + k\vec{p}}{2} = \left(\frac{1 + k}{2}\right)\vec{p}$$
• Step 4: Deductions:
1) $\vec{MN}$ is a scalar multiple of $\vec{p} = \vec{AB}$, which proves $MN \parallel AB \parallel DC$.
2) $|\vec{MN}| = \frac{|\vec{AB}| + |\vec{DC}|}{2}$, which proves that the midline length is the arithmetic mean of the parallel bases.
Q.E.D.
• Step 1: Set up coordinate/vector frame:
Let $O$ be the origin at vertex $A$. Let adjacent side vectors be $\vec{AB} = \vec{b}$ and $\vec{AD} = \vec{d}$.
Then opposite vertex $C$ has position vector $\vec{c} = \vec{b} + \vec{d}$, and diagonal $\vec{AC} = \vec{b} + \vec{d}$.
• Step 2: Midpoints of adjacent sides:
Let $M$ be the midpoint of $AB \implies \vec{m} = \frac{1}{2}\vec{b}$.
Let $N$ be the midpoint of $AD \implies \vec{n} = \frac{1}{2}\vec{d}$.
• Step 3: Midpoint segment $MN$ and diagonal $AC$:
Line segment $MN$ joins $\frac{1}{2}\vec{b}$ to $\frac{1}{2}\vec{d}$.
The midpoint of $MN$ is $K = \frac{\vec{m} + \vec{n}}{2} = \frac{\frac{1}{2}\vec{b} + \frac{1}{2}\vec{d}}{2} = \frac{1}{4}(\vec{b} + \vec{d}) = \frac{1}{4}\vec{AC}$.
• Step 4: Ratio Analysis on Diagonal $AC$:
Since $K$ lies on diagonal $AC$ and $\vec{AK} = \frac{1}{4}\vec{AC}$, we have:
$$AK = \frac{1}{4}AC \implies KC = \frac{3}{4}AC$$
$$\text{Ratio } AK : KC = \frac{1}{4} : \frac{3}{4} = 1 : 3$$
Hence, the segment divides the diagonal in the ratio $1 : 3$.
Q.E.D.
Miscellaneous Exercise 7 • Review Solutions & MCQs
Speed specifies only the magnitude of rate of motion without any direction, making it a pure scalar quantity. Velocity, torque, and force all possess both magnitude and direction.
Velocity is rate of change of displacement in a specific direction, making it a vector. Speed, distance, and work are scalar quantities.
By vector subtraction in $\triangle OAB$, $\vec{AB} = \vec{OB} - \vec{OA} = \vec{b} - \vec{a}$.
$|\vec{a}|$ denotes the magnitude (length or norm) of the vector, which is a non-negative scalar real number, not the vector itself.
Negative of vector $[x, y]$ is $[-x, -y] = [-(3), -(-7)] = [-3, 7]$.
$|\vec{u}| = \sqrt{(-5)^2 + 12^2} = \sqrt{25 + 144} = \sqrt{169} = 13$.
The magnitude of a vector and its negative vector are identical because length is invariant under direction reversal: $|-\vec{u}| = \sqrt{(-x)^2 + (-y)^2} = \sqrt{x^2 + y^2} = |\vec{u}|$.
$|\vec{a}| = \sqrt{6^2 + (-8)^2} = \sqrt{36 + 64} = 10$. Therefore, $\hat{a} = \frac{6\hat{i} - 8\hat{j}}{10} = \frac{3}{5}\hat{i} - \frac{4}{5}\hat{j}$.
Comparing components: $12 = \lambda(-2) \implies \lambda = -6$ and $-18 = \lambda(3) \implies \lambda = -6$.
Equating components: $-5x = 10 \implies x = -2$ and $4y = 8 \implies y = 2$.
$\vec{r} - 2\vec{q} = [5, -6] - 2[2, 6] = [5 - 4, -6 - 12] = [1, -18]$.
$\vec{u} - \vec{v} = (5-2)\hat{i} + (10-6)\hat{j} = 3\hat{i} + 4\hat{j}$. Magnitude $= \sqrt{3^2 + 4^2} = \sqrt{25} = 5$.
A position vector always originates from the Cartesian origin $O(0,0)$ to the point $P$, denoted by $\vec{OP}$.
$\vec{AB} = \vec{DC}$ means opposite sides $AB$ and $DC$ are both equal in length and strictly parallel, which defines a parallelogram.
• Step 1: Calculate magnitude of $\vec{r}$:
$$|\vec{r}| = \sqrt{3^2 + (-4)^2} = \sqrt{9 + 16} = \sqrt{25} = 5$$
• Step 2: Calculate magnitude of $\vec{u}$:
$$|\vec{u}| = \sqrt{(-3)^2 + (-4)^2} = \sqrt{9 + 16} = \sqrt{25} = 5$$
Since $|\vec{r}| = 5 = |\vec{u}|$, the magnitudes are equal. (Proved!)
• Step 3: Test Vector Equality $\vec{r} = \vec{u}$:
Two vectors are equal if and only if both their magnitudes AND their respective components (directions) are identical.
Comparing x-components: $x_r = 3 \neq -3 = x_u$.
Therefore, $\vec{r} \neq \vec{u}$.
• Step 1: Compute vector $\vec{a} + 2\vec{b}$:
$$\vec{a} + 2\vec{b} = (2\hat{i} - 4\hat{j}) + 2(2\hat{i} + x\hat{j}) = (2 + 4)\hat{i} + (-4 + 2x)\hat{j} = 6\hat{i} + (2x - 4)\hat{j}$$
• Step 2: Set up magnitude equation:
$$|\vec{a} + 2\vec{b}| = \sqrt{6^2 + (2x - 4)^2} = 6$$
• Step 3: Square both sides:
$$36 + (2x - 4)^2 = 36$$
$$(2x - 4)^2 = 36 - 36 = 0$$
$$2x - 4 = 0 \implies 2x = 4 \implies x = 2$$
• Verification: For $x = 2$, $\vec{a} + 2\vec{b} = 6\hat{i} + (2(2)-4)\hat{j} = 6\hat{i} + 0\hat{j} = 6\hat{i} \implies |6\hat{i}| = 6$.
(i) $\vec{OM}$
(ii) $\vec{AB}$
(iii) $\vec{MB}$
(iv) $\vec{OB} + \vec{BA}$.
(i) $\vec{OM}$:
• Since $M$ is the midpoint of segment $OA$: $\vec{OM} = \frac{1}{2}\vec{OA} = \frac{1}{2}\vec{a}$.
(ii) $\vec{AB}$:
• By triangle law: $\vec{AB} = \vec{OB} - \vec{OA} = \vec{b} - \vec{a}$.
(iii) $\vec{MB}$:
• In $\triangle OMB$: $\vec{MB} = \vec{OB} - \vec{OM} = \vec{b} - \frac{1}{2}\vec{a} = -\frac{1}{2}\vec{a} + \vec{b}$.
(iv) $\vec{OB} + \vec{BA}$:
• Notice $\vec{BA} = -\vec{AB} = -(\vec{b} - \vec{a}) = \vec{a} - \vec{b}$.
• $\vec{OB} + \vec{BA} = \vec{b} + (\vec{a} - \vec{b}) = \vec{a} = \vec{OA}$.
• Step 1: Resolve First Force $\vec{F}_1 = 250\text{ N}$ at $\theta_1 = 50^\circ$:
$$F_{1x} = 250\cos 50^\circ = 250(0.6428) \approx 160.70\text{ N}$$
$$F_{1y} = 250\sin 50^\circ = 250(0.7660) \approx 191.51\text{ N}$$
• Step 2: Resolve Second Force $\vec{F}_2 = 300\text{ N}$ at $\theta_2 = -40^\circ$:
$$F_{2x} = 300\cos(-40^\circ) = 300(0.7660) \approx 229.81\text{ N}$$
$$F_{2y} = 300\sin(-40^\circ) = 300(-0.6428) \approx -192.84\text{ N}$$
• Step 3: Combine Components for Resultant $\vec{R}$:
$$R_x = F_{1x} + F_{2x} = 160.70 + 229.81 = 390.51\text{ N}$$
$$R_y = F_{1y} + F_{2y} = 191.51 - 192.84 = -1.33\text{ N}$$
$$\vec{R} = 390.51\hat{i} - 1.33\hat{j}\text{ N}$$
• Step 4: Magnitude of Resultant Force:
$$|\vec{R}| = \sqrt{(390.51)^2 + (-1.33)^2} = \sqrt{152498.05 + 1.77} = \sqrt{152499.82} \approx 390.51\text{ N}$$
• Step 5: Direction Angle:
$$\theta = \tan^{-1}\left(\frac{R_y}{R_x}\right) = \tan^{-1}\left(\frac{-1.33}{390.51}\right) \approx -0.195^\circ \approx -0.2^\circ\text{ (below horizontal)}$$
(i) How much farther did the first ball travel compared to the second ball?
(ii) What is the straight-line distance between the two landing points of the balls?
• Step 1: Calculate distance traveled by Ball 1 ($|\vec{v}_1|$):
$$|\vec{v}_1| = \sqrt{120^2 + 12^2} = \sqrt{14400 + 144} = \sqrt{14544} \approx 120.60\text{ m}$$
• Step 2: Calculate distance traveled by Ball 2 ($|\vec{v}_2|$):
$$|\vec{v}_2| = \sqrt{90^2 + (-30)^2} = \sqrt{8100 + 900} = \sqrt{9000} = 30\sqrt{10} \approx 94.87\text{ m}$$
• Step 3: Answer (i) Difference in distance:
$$\Delta d = |\vec{v}_1| - |\vec{v}_2| = 120.60 - 94.87 = 25.73\text{ m}$$
• Step 4: Answer (ii) Straight-line distance between landing points:
$$\vec{D} = \vec{v}_1 - \vec{v}_2 = (120\hat{i} + 12\hat{j}) - (90\hat{i} - 30\hat{j}) = (120 - 90)\hat{i} + (12 - (-30))\hat{j} = 30\hat{i} + 42\hat{j}$$
$$|\vec{D}| = \sqrt{30^2 + 42^2} = \sqrt{900 + 1764} = \sqrt{2664} = 6\sqrt{74} \approx 51.61\text{ m}$$
(i) He tries to swim due West along the current.
(ii) He tries to swim due East against the current.
(iii) He tries to swim due North directly across the river.
Let positive x-axis be East ($+x$) and positive y-axis be North ($+y$).
River current velocity: $\vec{v}_c = -1.5\hat{i}\text{ m/s}$ (Due West).
(i) Swimming due West (along current):
• Swimmer velocity relative to water: $\vec{v}_s = -6\hat{i}\text{ m/s}$.
• Resultant: $\vec{v} = \vec{v}_s + \vec{v}_c = -6\hat{i} - 1.5\hat{i} = -7.5\hat{i}\text{ m/s}$.
• Speed $= 7.5\text{ m/s}$ due West.
(ii) Swimming due East (against current):
• Swimmer velocity relative to water: $\vec{v}_s = +6\hat{i}\text{ m/s}$.
• Resultant: $\vec{v} = \vec{v}_s + \vec{v}_c = 6\hat{i} - 1.5\hat{i} = 4.5\hat{i}\text{ m/s}$.
• Speed $= 4.5\text{ m/s}$ due East.
(iii) Swimming due North (across river):
• Swimmer velocity relative to water: $\vec{v}_s = 6\hat{j}\text{ m/s}$.
• Resultant: $\vec{v} = \vec{v}_c + \vec{v}_s = -1.5\hat{i} + 6\hat{j}\text{ m/s}$.
• Resultant Speed: $|\vec{v}| = \sqrt{(-1.5)^2 + 6^2} = \sqrt{2.25 + 36} = \sqrt{38.25} \approx 6.18\text{ m/s}$.
• Direction: $\theta = 180^\circ - \tan^{-1}\left(\frac{6}{1.5}\right) = 180^\circ - 75.96^\circ = 104.04^\circ\text{ from East (or N } 14.04^\circ\text{ W)}$.
(i) What is the resultant speed and course direction of the plane?
(ii) How far is the plane from its starting origin after $10\text{ hours}$ of flight?
• Step 1: Set up component velocity vectors:
Plane velocity: $\vec{v}_p = 150\hat{j}\text{ km/h}$ (North).
Wind velocity: $\vec{v}_w = 50\hat{i}\text{ km/h}$ (East).
Resultant velocity: $\vec{v} = \vec{v}_w + \vec{v}_p = 50\hat{i} + 150\hat{j}\text{ km/h}$.
• Step 2: Answer (i) Resultant Speed and Direction:
$$|\vec{v}| = \sqrt{50^2 + 150^2} = \sqrt{2500 + 22500} = \sqrt{25000} = 50\sqrt{10} \approx 158.11\text{ km/h}$$
$$\text{Heading angle from East } \theta = \tan^{-1}\left(\frac{150}{50}\right) = \tan^{-1}(3) \approx 71.57^\circ\text{ North of East}$$
$$\text{Compass Bearing} = 90^\circ - 71.57^\circ = 018.43^\circ\text{ (or N } 18.43^\circ\text{ E)}$$
• Step 3: Answer (ii) Total Distance from starting origin after $t = 10\text{ hours}$:
$$\text{Distance } d = |\vec{v}| \times t = 158.11\text{ km/h} \times 10\text{ h} = 1581.14\text{ km} \quad (\text{Exact: } 500\sqrt{10}\text{ km})$$
Part 3: High-Yield Objective Concept Booster
Velocity and acceleration both possess both magnitude and a uniquely defined spatial direction. Mass, work, energy, speed, and distance are pure scalar quantities.
By definition, a unit vector $\hat{u} = \frac{\vec{u}}{|\vec{u}|}$ has a magnitude (norm) of exactly 1 and maintains the direction of vector $\vec{u}$.
Magnitude is the geometric length of a directed line segment, which is always non-negative: $|-\vec{v}| = |\vec{v}| = 9$.
In Cartesian 2D plane, $\hat{i} = [1, 0]$ is the unit vector along the horizontal x-axis and $\hat{j} = [0, 1]$ is along the vertical y-axis.
Parallel vectors are scalar multiples of each other ($ec{u} = kec{v}$), meaning their corresponding component ratios are equal.
The initial and terminal points of a zero vector coincide, giving it a length of 0 and an arbitrary or indeterminate direction.
When $m : n = 1 : 1$, the ratio formula simplifies to $ec{r} = rac{1ec{b} + 1ec{a}}{1 + 1} = rac{ec{a} + ec{b}}{2}$.
$\theta = \tan^{-1}\left(\frac{y}{x}\right) = \tan^{-1}\left(\frac{\sqrt{3}}{1}\right) = 60^\circ$.
Vector addition is commutative; the order in which two vectors are added does not alter their resultant vector.
$k\vec{v} = -0.5[4, -6] = [-0.5 \times 4, -0.5 \times (-6)] = [-2, 3]$.
Dividing a vector by its own magnitude to produce a unit vector of length 1 is mathematically termed "normalizing".
Vector equality requires both geometric criteria: equal length (magnitude) and identical orientation (direction).
The resultant vector begins at the initial point (tail) of the first vector and terminates at the terminal point (head) of the final vector.
The vector $ec{OP}$ that specifies the location of point $P(x,y)$ relative to the origin $(0,0)$ is its position vector.
Vector translation is a rigid transformation preserving distances, angles, and orientation.
For external division, the ratio formula has a minus sign in numerator and denominator: $ec{r} = rac{mec{b} - nec{a}}{m - n}$.
$|ec{0}| = \sqrt{0^2 + 0^2} = 0$.
In right-triangle trigonometry, adjacent component $F_x = |ec{F}|\cos heta$.
Magnitude is defined by $\sqrt{x^2 + y^2}$, which is always a non-negative real number.
Equal vectors do not need to share the same position; two vectors anywhere in the plane are equal as long as they have equal magnitude and parallel direction.
Vector subtraction is strictly defined as the addition of the inverse (negative) vector.
Since $B$ is a common point and $ec{AB} \parallel ec{BC}$, the points $A, B, C$ must lie along the exact same straight line.
Division by zero is undefined; a unit vector exists ONLY for non-zero vectors.
This is the foundational statement of the Parallelogram Law of Vector Addition.
| Column A (Concept / Expression) | Column B (Mathematical Formula) |
|---|---|
| 1. Magnitude of vector $\vec{u} = [x, y]$ | A. $\vec{r} = \frac{\vec{a} + \vec{b}}{2}$ |
| 2. Unit Vector in direction of $\vec{u}$ | B. $\vec{b} - \vec{a}$ |
| 3. Vector $\vec{AB}$ from position vectors $\vec{a}, \vec{b}$ | C. $\sqrt{x^2 + y^2}$ |
| 4. Midpoint position vector | D. $\hat{u} = \frac{\vec{u}}{|\vec{u}|}$ |
| 5. Direction angle $\theta$ | E. $\tan^{-1}(y / x)$ |
1. Magnitude $|\vec{u}| = \sqrt{x^2 + y^2}$ (C)
2. Unit vector $\hat{u} = \frac{\vec{u}}{|\vec{u}|}$ (D)
3. Vector $\vec{AB} = \vec{OB} - \vec{OA} = \vec{b} - \vec{a}$ (B)
4. Midpoint position vector $= \frac{\vec{a} + \vec{b}}{2}$ (A)
5. Direction angle $\theta = \tan^{-1}(y / x)$ (E).
| Column A (Quantity / Concept) | Column B (Classification / Vector) |
|---|---|
| 1. Mass, Speed, Work | A. $x_1/x_2 = y_1/y_2 = k$ |
| 2. Force, Velocity, Weight | B. $\vec{0} = [0, 0]$ |
| 3. Null Vector | C. Scalar Quantities |
| 4. Parallel Vectors Condition | D. Vector Quantities |
| 5. Negative Vector of $[x, y]$ | E. $[-x, -y]$ |
1. Mass, Speed, Work are Scalar Quantities (C)
2. Force, Velocity, Weight are Vector Quantities (D)
3. Null vector is $\vec{0} = [0, 0]$ (B)
4. Parallel condition is proportionality $\frac{x_1}{x_2} = \frac{y_1}{y_2} = k$ (A)
5. Negative vector is $[-x, -y]$ (E).
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