Comprehensive Guide to Two-Dimensional Vectors and Foundations for 3D Vector Calculus

Overview and Study Recommendations for Two-Dimensional Vectors

  • Two-dimensional (2D2\text{D}) vector operations serve as the primary conceptual foundation required for transitioning into three-dimensional (3D3\text{D}) vector applications.
  • Recommended student workflow when working through practice problems:
    • Pause before attempting each problem.
    • Solve the problem independently.
    • Review the step-by-step solution to confirm both the final result and the conceptual approach.
    • Pay close attention to conceptual remarks and structural techniques, as these extend directly to higher dimensions where visual diagrams are no longer feasible.

Displacement Vectors and Position Vectors Between Points

  • Position Vectors:
    • The position vector of a point A(x,y)A(x, y) relative to the origin O(0,0)O(0, 0) is denoted as OA=(xy)OA = \begin{pmatrix} x \\ y \end{pmatrix}.
  • Displacement Vector Between Two Points Formula:
    • Given two points AA and BB with position vectors OAOA and OBOB:     AB=OB−OAAB = OB - OA
    • Rule of thumb: Subtract the position vector of the first point (start point) from the position vector of the second point (end point) — "second letter minus first letter".
  • Vector Reversal Property:
    • Reversing the direction of a displacement vector negates its components:     BA=−ABBA = -ABCO=−OCCO = -OC
  • Comprehensive Worked Example with Given Points:
    • Given points: O(0,0)O(0, 0), A(1,−2)A(1, -2), B(3,0)B(3, 0), and C(2,−3)C(2, -3).
    • Position vector OAOA:     OA=(1−2)OA = \begin{pmatrix} 1 \\ -2 \end{pmatrix}
    • Finding vector ABAB:     AB=OB−OA=(30)−(1−2)=(3−10−(−2))=(22)AB = OB - OA = \begin{pmatrix} 3 \\ 0 \end{pmatrix} - \begin{pmatrix} 1 \\ -2 \end{pmatrix} = \begin{pmatrix} 3 - 1 \\ 0 - (-2) \end{pmatrix} = \begin{pmatrix} 2 \\ 2 \end{pmatrix}
    • Visual Verification: Moving from point A(1,−2)A(1, -2) to point B(3,0)B(3, 0) requires moving 2 units2\,\text{units} right (+2+2) and 2 units2\,\text{units} up (+2+2).
    • Finding vector BCBC:     BC=OC−OB=(2−3)−(30)=(2−3−3−0)=(−1−3)BC = OC - OB = \begin{pmatrix} 2 \\ -3 \end{pmatrix} - \begin{pmatrix} 3 \\ 0 \end{pmatrix} = \begin{pmatrix} 2 - 3 \\ -3 - 0 \end{pmatrix} = \begin{pmatrix} -1 \\ -3 \end{pmatrix}
    • Visual Verification: Moving from point B(3,0)B(3, 0) to point C(2,−3)C(2, -3) requires moving 1 unit1\,\text{unit} left (−1-1) and 3 units3\,\text{units} down (−3-3).
    • Finding vector COCO:     CO=−OC=−(2−3)=(−23)CO = -OC = -\begin{pmatrix} 2 \\ -3 \end{pmatrix} = \begin{pmatrix} -2 \\ 3 \end{pmatrix}
    • Finding vector CBCB:
    • Method 1: CB=OB−OC=(30)−(2−3)=(13)CB = OB - OC = \begin{pmatrix} 3 \\ 0 \end{pmatrix} - \begin{pmatrix} 2 \\ -3 \end{pmatrix} = \begin{pmatrix} 1 \\ 3 \end{pmatrix}
    • Method 2: CB=−BC=−(−1−3)=(13)CB = -BC = -\begin{pmatrix} -1 \\ -3 \end{pmatrix} = \begin{pmatrix} 1 \\ 3 \end{pmatrix}

Vector Operations: Addition, Subtraction, and Scalar Multiplication

  • Vector Addition:
    • Performed component-wise:     (a1a2)+(b1b2)=(a1+b1a2+b2)\begin{pmatrix} a_1 \\ a_2 \end{pmatrix} + \begin{pmatrix} b_1 \\ b_2 \end{pmatrix} = \begin{pmatrix} a_1 + b_1 \\ a_2 + b_2 \end{pmatrix}
    • Example: Given a=(12)a = \begin{pmatrix} 1 \\ 2 \end{pmatrix} and b=(1−3)b = \begin{pmatrix} 1 \\ -3 \end{pmatrix}:     a+b=(1+12+(−3))=(2−1)a + b = \begin{pmatrix} 1 + 1 \\ 2 + (-3) \end{pmatrix} = \begin{pmatrix} 2 \\ -1 \end{pmatrix}
  • Scalar Multiplication and Subtraction Combined:
    • Given a=(12)a = \begin{pmatrix} 1 \\ 2 \end{pmatrix} and b=(−21)b = \begin{pmatrix} -2 \\ 1 \end{pmatrix}:
    • Evaluate 2b−a2b - a:     2b=2(−21)=(−42)2b = 2 \begin{pmatrix} -2 \\ 1 \end{pmatrix} = \begin{pmatrix} -4 \\ 2 \end{pmatrix}2b−a=(−42)−(12)=(−4−12−2)=(−50)2b - a = \begin{pmatrix} -4 \\ 2 \end{pmatrix} - \begin{pmatrix} 1 \\ 2 \end{pmatrix} = \begin{pmatrix} -4 - 1 \\ 2 - 2 \end{pmatrix} = \begin{pmatrix} -5 \\ 0 \end{pmatrix}

Vector Geometry and Geometric Proofs in Two Dimensions

  • Vector Addition and Midpoint Traversal:
    • Vectors can be expressed in terms of defined side vectors in geometric figures.
    • Opposite sides of a parallelogram are equal in both magnitude and direction, representing identical vectors.
  • Worked Example:
    • Let quadrilateral ABCDABCD have side vectors AB=aAB = a and AD=bAD = b.
    • Let MM be the midpoint of side ABAB.
    • Express vector MDMD in terms of aa and bb:
    • Traversal path from MM to DD:
      • Travel from MM to AA: Since MM is the midpoint of ABAB, vector MA=−12aMA = -\frac{1}{2}a
      • Travel from AA to DD: Vector AD=bAD = b
    • Summing the path:       MD=MA+AD=−12a+bMD = MA + AD = -\frac{1}{2}a + b
    • Express vector MNMN (where NN is the midpoint of side DCDC) in terms of aa and bb:
    • Traversal path from MM to NN:
      • Travel from MM to AA: −12a-\frac{1}{2}a
      • Travel from AA to DD: bb
      • Travel from DD to NN: +12a+\frac{1}{2}a (since side DCDC is parallel and equal to AB=aAB = a)
    • Summing and simplifying:       MN=−12a+b+12a=bMN = -\frac{1}{2}a + b + \frac{1}{2}a = b

Component Form and Vector Magnitude

  • Unit Vector Bracket Notation (i,ji, j Form):
    • Any 2D2\text{D} vector can be expressed in terms of orthogonal unit vectors ii (1 unit1\,\text{unit} along xx-axis) and jj (1 unit1\,\text{unit} along yy-axis):     v=vxi+vyjv = v_x i + v_y j
    • Subtraction with Brackets Warning:
    • When computing AB=OB−OAAB = OB - OA, always enclose OAOA in brackets to distribute the negative sign to both components.
    • Example: Given OA=i+2jOA = i + 2j and OB=3i−5jOB = 3i - 5j:       AB=(3i−5j)−(i+2j)=3i−5j−i−2j=2i−7jAB = (3i - 5j) - (i + 2j) = 3i - 5j - i - 2j = 2i - 7j
    • Verification: Starting at x=1x = 1 to x=3x = 3 is +2 units+2\,\text{units}; starting at y=2y = 2 down to y=−5y = -5 is −7 units-7\,\text{units}.
  • Vector Magnitude Formula:
    • The magnitude (length) of vector v=vxi+vyjv = v_x i + v_y j is denoted by ∣v∣|v|:     ∣v∣=vx2+vy2|v| = \sqrt{v_x^2 + v_y^2}
    • Important Calculator Caveat: Always enclose negative components inside parentheses prior to squaring (e.g., (−5)2(-5)^2) to avoid evaluation errors.
  • Worked Examples for Magnitude:
    • Example 1: Given vector v=12i−5jv = 12i - 5j:     ∣v∣=122+(−5)2=144+25=169=13|v| = \sqrt{12^2 + (-5)^2} = \sqrt{144 + 25} = \sqrt{169} = 13
    • Example 2: Find ABAB and ∣AB∣|AB| for A(2,3)A(2, 3) and B(5,1)B(5, 1):     AB=(51)−(23)=(3−2)=3i−2jAB = \begin{pmatrix} 5 \\ 1 \end{pmatrix} - \begin{pmatrix} 2 \\ 3 \end{pmatrix} = \begin{pmatrix} 3 \\ -2 \end{pmatrix} = 3i - 2j∣AB∣=32+(−2)2=9+4=13|AB| = \sqrt{3^2 + (-2)^2} = \sqrt{9 + 4} = \sqrt{13}
    • Note on Exact Values: Keep answers in exact surd form (13\sqrt{13}) rather than converting to decimals.
    • Reasonableness Check: Since 9<13<16\sqrt{9} < \sqrt{13} < \sqrt{16}, the length must lie between 33 and 44, which matches a displacement of 3 units3\,\text{units} across and 2 units2\,\text{units} down.

Unit Vectors

  • Definition:
    • A unit vector is a vector scaled to have a magnitude of exactly 1 unit1\,\text{unit} while preserving its original direction.
    • Designated using a hat symbol: b^\hat{b} or v^\hat{v}.
  • Formula:   b^=1∣b∣b\hat{b} = \frac{1}{|b|} b
  • Worked Examples:
    • Example 1: Find the unit vector for b=3i−jb = 3i - j:
    • Step 1: Calculate magnitude:       ∣b∣=32+(−1)2=9+1=10|b| = \sqrt{3^2 + (-1)^2} = \sqrt{9 + 1} = \sqrt{10}
    • Step 2: Apply unit vector formula:       b^=110(3i−j)=310i−110j\hat{b} = \frac{1}{\sqrt{10}}(3i - j) = \frac{3}{\sqrt{10}}i - \frac{1}{\sqrt{10}}j
    • Example 2: Find the unit vector for b=6i−4jb = 6i - 4j:
    • Step 1: Calculate magnitude:       ∣b∣=62+(−4)2=36+16=52=4×13=213|b| = \sqrt{6^2 + (-4)^2} = \sqrt{36 + 16} = \sqrt{52} = \sqrt{4 \times 13} = 2\sqrt{13}
    • Step 2: Apply unit vector formula:       b^=1213(6i−4j)=6213i−4213j\hat{b} = \frac{1}{2\sqrt{13}}(6i - 4j) = \frac{6}{2\sqrt{13}}i - \frac{4}{2\sqrt{13}}j
    • Step 3: Simplify fractions:       b^=313i−213j\hat{b} = \frac{3}{\sqrt{13}}i - \frac{2}{\sqrt{13}}j

Polar Form and Component Form Conversions

  • Converting Polar Form (r∠θ)(r \angle \theta) to Component Form (i,ji, j Form):
    • General Formula:     u=∣u∣cos⁡(θ)i+∣u∣sin⁡(θ)ju = |u|\cos(\theta)i + |u|\sin(\theta)j
    • Derivation: Right-angled triangle trigonometry where the adjacent side along xx is ∣u∣cos⁡(θ)|u|\cos(\theta) and the opposite side along yy is ∣u∣sin⁡(θ)|u|\sin(\theta).
    • Advantage of Using Direct Rotational Angle: Substituting the full angle θ\theta (including negative signs for clockwise rotation) automatically determines both the magnitude and correct sign (+ or −+\text{ or }-) for each component.
  • Conversion Examples:
    • Example 1: Magnitude ∣u∣=4|u| = 4, angle θ=−120∘\theta = -120^\circ:
    • Formula setup:       u=4cos⁡(−120∘)i+4sin⁡(−120∘)ju = 4\cos(-120^\circ)i + 4\sin(-120^\circ)j
    • Reference angle analysis:
      • Quadrant III (both cosine and sine are negative). Reference angle =60∘= 60^\circ.
      • Standard 30∘−60∘−90∘30^\circ-60^\circ-90^\circ triangle sides: 1,2,31, 2, \sqrt{3}.       cos⁡(−120∘)=−cos⁡(60∘)=−12\cos(-120^\circ) = -\cos(60^\circ) = -\frac{1}{2}sin⁡(−120∘)=−sin⁡(60∘)=−32\sin(-120^\circ) = -\sin(60^\circ) = -\frac{\sqrt{3}}{2}
    • Component substitution:       u=4(−12)i+4(−32)j=−2i−23ju = 4\left(-\frac{1}{2}\right)i + 4\left(-\frac{\sqrt{3}}{2}\right)j = -2i - 2\sqrt{3}j
    • Example 2: Magnitude ∣v∣=4|v| = 4, angle θ=150∘\theta = 150^\circ:
    • Formula setup:       v=4cos⁡(150∘)i+4sin⁡(150∘)jv = 4\cos(150^\circ)i + 4\sin(150^\circ)j
    • Reference angle analysis:
      • Quadrant II (cosine negative, sine positive). Reference angle =30∘= 30^\circ.       cos⁡(150∘)=−cos⁡(30∘)=−32\cos(150^\circ) = -\cos(30^\circ) = -\frac{\sqrt{3}}{2}sin⁡(150∘)=sin⁡(30∘)=12\sin(150^\circ) = \sin(30^\circ) = \frac{1}{2}
    • Component substitution:       v=4(−32)i+4(12)j=−23i+2jv = 4\left(-\frac{\sqrt{3}}{2}\right)i + 4\left(\frac{1}{2}\right)j = -2\sqrt{3}i + 2j
  • Converting Component Form to Polar Form:
    • Example 1: Convert v=−23i+2jv = -2\sqrt{3}i + 2j into polar form:
    • Magnitude:       ∣v∣=(−23)2+22=4×3+4=12+4=16=4|v| = \sqrt{(-2\sqrt{3})^2 + 2^2} = \sqrt{4 \times 3 + 4} = \sqrt{12 + 4} = \sqrt{16} = 4
    • Angle determination:
      • Plotting components places vector in Quadrant II (−x,+y-x, +y).       tan⁡(θref)=∣y∣∣x∣=223=13\tan(\theta_{\text{ref}}) = \frac{|y|}{|x|} = \frac{2}{2\sqrt{3}} = \frac{1}{\sqrt{3}}θref=tan⁡−1(13)=30∘\theta_{\text{ref}} = \tan^{-1}\left(\frac{1}{\sqrt{3}}\right) = 30^\circθ=180∘−30∘=150∘\theta = 180^\circ - 30^\circ = 150^\circ
    • Polar form result: 4∠150∘4 \angle 150^\circ
    • Example 2: Convert v=−5i−12jv = -5i - 12j into polar form:
    • Magnitude:       ∣v∣=(−5)2+(−12)2=25+144=169=13|v| = \sqrt{(-5)^2 + (-12)^2} = \sqrt{25 + 144} = \sqrt{169} = 13
    • Angle determination:
      • Vector lies in Quadrant III (−x,−y-x, -y).       tan⁡(θref)=125\tan(\theta_{\text{ref}}) = \frac{12}{5}θref=tan⁡−1(125)≈67.38∘\theta_{\text{ref}} = \tan^{-1}\left(\frac{12}{5}\right) \approx 67.38^\circθ=180∘−67.38∘=112.62∘\theta = 180^\circ - 67.38^\circ = 112.62^\circ
    • Polar form result: 13∠112.62∘13 \angle 112.62^\circ

The Dot Product (Scalar Product)

  • Algebraic Definition (Component Form):
    • For two vectors a=axi+ayja = a_x i + a_y j and b=bxi+byjb = b_x i + b_y j:     a⋅b=axbx+aybya \cdot b = a_x b_x + a_y b_y
    • The dot product always yields a scalar quantity (a real number), not a vector.
  • Algebraic Examples:
    • Example 1: Given a=2i−ja = 2i - j and b=3i−2jb = 3i - 2j:     a⋅b=(2)(3)+(−1)(−2)=6+2=8a \cdot b = (2)(3) + (-1)(-2) = 6 + 2 = 8
    • Example 2: Given a=2i−ja = 2i - j and c=−i+3jc = -i + 3j:     a⋅c=(2)(−1)+(−1)(3)=−2+(−3)=−5a \cdot c = (2)(-1) + (-1)(3) = -2 + (-3) = -5
  • Geometric Definition:
    • Formula:     a⋅b=∣a∣∣b∣cos⁡(θ)a \cdot b = |a||b|\cos(\theta)     where θ\theta is the angle between vectors aa and b$.\n * Example: Given |a||b| = 30andangleand angle\theta = 45^\circ:\n    a \cdot b = 30 \times \cos(45^\circ) = 30 \times \frac{\sqrt{2}}{2} = 15\sqrt{2}\n\n# Angles Between Vectors\n\n* Derivation:\n * Equating algebraic and geometric dot products:\n    u \cdot v = |u||v|\cos(\theta)\n    \cos(\theta) = \frac{u \cdot v}{|u||v|}\n    \theta = \cos^{-1}\left(\frac{u \cdot v}{|u||v|}\right)\n * This method is essential for 3\text{D} vector calculations where geometric drawing is impossible.\n* Worked Examples:\n * Example 1: Find angle \thetabetweenbetweenu = i + 2jandandv = i - 4j:\n * Step 1: Dot product:\n      u \cdot v = (1)(1) + (2)(-4) = 1 - 8 = -7\n * Step 2: Magnitudes:\n      |u| = \sqrt{1^2 + 2^2} = \sqrt{5}\n      |v| = \sqrt{1^2 + (-4)^2} = \sqrt{17}\n * Step 3: Cosine equation:\n      \cos(\theta) = \frac{-7}{\sqrt{5}\sqrt{17}} = \frac{-7}{\sqrt{85}}\n      \theta = \cos^{-1}\left(\frac{-7}{\sqrt{85}}\right) \approx 139.40^\circ\n * Example 2: Find angle \thetabetweenbetweenu = -2i + jandandv = -2i - 2j:\n * Step 1: Dot product:\n      u \cdot v = (-2)(-2) + (1)(-2) = 4 - 2 = 2\n * Step 2: Magnitudes:\n      |u| = \sqrt{(-2)^2 + 1^2} = \sqrt{5}\n      |v| = \sqrt{(-2)^2 + (-2)^2} = \sqrt{8}\n * Step 3: Cosine equation:\n      \cos(\theta) = \frac{2}{\sqrt{5}\sqrt{8}} = \frac{2}{\sqrt{40}}\n      \theta = \cos^{-1}\left(\frac{2}{\sqrt{40}}\right) \approx 71.57^\circ\n\n# Perpendicular Vectors and Orthogonality\n\n* Condition for Orthogonality:\n * Two non-zero vectors uandandv are perpendicular (orthogonal) if and only if their dot product equals zero:\n    u \cdot v = 0 \iff u \perp v\n * Reason: \cos(90^\circ) = 0,making, making|u||v|\cos(90^\circ) = 0$.
  • Worked Example:
    • Given u=2i+3ju = 2i + 3j and v=xi+18jv = xi + 18j, find xx such that u⊥vu \perp v:
    • Step 1: Set dot product to zero:       u⋅v=2(x)+3(18)=0u \cdot v = 2(x) + 3(18) = 0
    • Step 2: Solve linear equation:       2x+54=02x + 54 = 02x=−542x = -54x=−27x = -27
    • Geometric check confirms that v=−27i+18jv = -27i + 18j forms an exact 90∘90^\circ angle with u = 2i + 3j$.\n\n# Vector Projections and Vector Resolutes\n\n* Definition and Formulas:\n * The vector resolute of ainthedirectionofin the direction ofb(denoted(denoteda_{\text{on } b})isthevectorcomponentof) is the vector component ofaparalleltoparallel tob$.
    • Primary Formula:     Resolute a on b=(a⋅b^)b^\text{Resolute } a \text{ on } b = (a \cdot \hat{b})\hat{b}     where b^=b∣b∣\hat{b} = \frac{b}{|b|} is the unit vector of b$.\n * Computational Simplified Form:\n    \text{Resolute } a \text{ on } b = \left(\frac{a \cdot b}{|b|^2}\right)b\n * Note: (a \cdot \hat{b})producesascalarmagnitude,whichisthenmultipliedbydirectionvectorproduces a scalar magnitude, which is then multiplied by direction vector\hat{b}.\n* Worked Examples:\n * Example 1: Find vector resolute of a = i + 3jinthedirectionofin the direction ofb = i - 4j:\n * Step 1: Find unit vector \hat{b}:\n      |b| = \sqrt{1^2 + (-4)^2} = \sqrt{17}\n      \hat{b} = \frac{1}{\sqrt{17}}(i - 4j)\n * Step 2: Calculate dot product factor (a \cdot b):\n      a \cdot b = (1)(1) + (3)(-4) = 1 - 12 = -11\n * Step 3: Combine scalar projection and unit vector:\n      \text{Resolute } a \text{ on } b = \left(\frac{-11}{\sqrt{17}}\right) \frac{1}{\sqrt{17}}(i - 4j) = -\frac{11}{17}(i - 4j)\n * Step 4: Expand components:\n      \text{Resolute } a \text{ on } b = -\frac{11}{17}i + \frac{44}{17}j\n * Example 2: Find vector resolute of a = 3i + jinthedirectionofin the direction ofb = i + j:\n * Step 1: Find magnitude and unit vector \hat{b}:\n      |b| = \sqrt{1^2 + 1^2} = \sqrt{2}\n      \hat{b} = \frac{1}{\sqrt{2}}(i + j)\n * Step 2: Calculate dot product (a \cdot b):\n      a \cdot b = (3)(1) + (1)(1) = 3 + 1 = 4\n * Step 3: Evaluate vector projection:\n      \text{Resolute } a \text{ on } b = \left(\frac{a \cdot b}{|b|^2}\right) b = \left(\frac{4}{2}\right)(i + j) = 2(i + j) = 2i + 2j$$