Comprehensive Guide to Two-Dimensional Vectors and Foundations for 3D Vector Calculus
Overview and Study Recommendations for Two-Dimensional Vectors
Two-dimensional (2D) vector operations serve as the primary conceptual foundation required for transitioning into three-dimensional (3D) 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) relative to the origin O(0,0) is denoted as OA=(xy).
Displacement Vector Between Two Points Formula:
Given two points A and B with position vectors OA and OB:
AB=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=−ABCO=−OC
Comprehensive Worked Example with Given Points:
Given points: O(0,0), A(1,−2), B(3,0), and C(2,−3).
Step 2: Apply unit vector formula:
b^=2131(6i−4j)=2136i−2134j
Step 3: Simplify fractions:
b^=133i−132j
Polar Form and Component Form Conversions
Converting Polar Form (r∠θ) to Component Form (i,j Form):
General Formula:
u=∣u∣cos(θ)i+∣u∣sin(θ)j
Derivation: Right-angled triangle trigonometry where the adjacent side along x is ∣u∣cos(θ) and the opposite side along y is ∣u∣sin(θ).
Advantage of Using Direct Rotational Angle: Substituting the full angle θ (including negative signs for clockwise rotation) automatically determines both the magnitude and correct sign (+ or −) for each component.
Conversion Examples:
Example 1: Magnitude ∣u∣=4, angle θ=−120∘:
Formula setup:
u=4cos(−120∘)i+4sin(−120∘)j
Reference angle analysis:
Quadrant III (both cosine and sine are negative). Reference angle =60∘.
Standard 30∘−60∘−90∘ triangle sides: 1,2,3.
cos(−120∘)=−cos(60∘)=−21sin(−120∘)=−sin(60∘)=−23
Plotting components places vector in Quadrant II (−x,+y).
tan(θref)=∣x∣∣y∣=232=31θref=tan−1(31)=30∘θ=180∘−30∘=150∘
Polar form result: 4∠150∘
Example 2: Convert v=−5i−12j into polar form:
Magnitude:
∣v∣=(−5)2+(−12)2=25+144=169=13
Angle determination:
Vector lies in Quadrant III (−x,−y).
tan(θref)=512θref=tan−1(512)≈67.38∘θ=180∘−67.38∘=112.62∘
Polar form result: 13∠112.62∘
The Dot Product (Scalar Product)
Algebraic Definition (Component Form):
For two vectors a=axi+ayj and b=bxi+byj:
a⋅b=axbx+ayby
The dot product always yields a scalar quantity (a real number), not a vector.
Algebraic Examples:
Example 1: Given a=2i−j and b=3i−2j:
a⋅b=(2)(3)+(−1)(−2)=6+2=8
Example 2: Given a=2i−j and c=−i+3j:
a⋅c=(2)(−1)+(−1)(3)=−2+(−3)=−5
Geometric Definition:
Formula:
a⋅b=∣a∣∣b∣cos(θ)
where θ is the angle between vectors a and b$.\n * Example: Given |a||b| = 30andangle\theta = 45^\circ:\n a \cdot b = 30 \times \cos(45^\circ) = 30 \times \frac{\sqrt{2}}{2} = 15\sqrt{2}\n\n# Angles Between Vectors\n\n* Derivation:\n * Equating algebraic and geometric dot products:\n u \cdot v = |u||v|\cos(\theta)\n \cos(\theta) = \frac{u \cdot v}{|u||v|}\n \theta = \cos^{-1}\left(\frac{u \cdot v}{|u||v|}\right)\n * This method is essential for 3\text{D} vector calculations where geometric drawing is impossible.\n* Worked Examples:\n * Example 1: Find angle \thetabetweenu = i + 2jandv = i - 4j:\n * Step 1: Dot product:\n u \cdot v = (1)(1) + (2)(-4) = 1 - 8 = -7\n * Step 2: Magnitudes:\n |u| = \sqrt{1^2 + 2^2} = \sqrt{5}\n |v| = \sqrt{1^2 + (-4)^2} = \sqrt{17}\n * Step 3: Cosine equation:\n \cos(\theta) = \frac{-7}{\sqrt{5}\sqrt{17}} = \frac{-7}{\sqrt{85}}\n \theta = \cos^{-1}\left(\frac{-7}{\sqrt{85}}\right) \approx 139.40^\circ\n * Example 2: Find angle \thetabetweenu = -2i + jandv = -2i - 2j:\n * Step 1: Dot product:\n u \cdot v = (-2)(-2) + (1)(-2) = 4 - 2 = 2\n * Step 2: Magnitudes:\n |u| = \sqrt{(-2)^2 + 1^2} = \sqrt{5}\n |v| = \sqrt{(-2)^2 + (-2)^2} = \sqrt{8}\n * Step 3: Cosine equation:\n \cos(\theta) = \frac{2}{\sqrt{5}\sqrt{8}} = \frac{2}{\sqrt{40}}\n \theta = \cos^{-1}\left(\frac{2}{\sqrt{40}}\right) \approx 71.57^\circ\n\n# Perpendicular Vectors and Orthogonality\n\n* Condition for Orthogonality:\n * Two non-zero vectors uandv are perpendicular (orthogonal) if and only if their dot product equals zero:\n u \cdot v = 0 \iff u \perp v\n * Reason: \cos(90^\circ) = 0,making|u||v|\cos(90^\circ) = 0$.
Worked Example:
Given u=2i+3j and v=xi+18j, find x such that u⊥v:
Step 1: Set dot product to zero:
u⋅v=2(x)+3(18)=0
Step 2: Solve linear equation:
2x+54=02x=−54x=−27
Geometric check confirms that v=−27i+18j forms an exact 90∘ angle with u = 2i + 3j$.\n\n# Vector Projections and Vector Resolutes\n\n* Definition and Formulas:\n * The vector resolute of ainthedirectionofb(denoteda_{\text{on } b})isthevectorcomponentofaparalleltob$.
Primary Formula:
Resolute a on b=(a⋅b^)b^
where b^=∣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,whichisthenmultipliedbydirectionvector\hat{b}.\n* Worked Examples:\n * Example 1: Find vector resolute of a = i + 3jinthedirectionofb = 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 + jinthedirectionofb = 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$$