Learning Objectives
Distinguish between scalar and vector quantities.
Express a vector as two perpendicular components using unit‑vector notation.
Add and subtract coplanar vectors:
Graphically – tip‑to‑tail and parallelogram methods.
Analytically – component (algebraic) method.
Convert between magnitude‑direction form and component form, and interpret the resulting angle correctly.
Scalars and Vectors
Quantity Definition Example
Scalar
A physical quantity described by a magnitude only (single number + unit).
Mass \(m = 2\;\text{kg}\), Temperature \(T = 25^{\circ}\text{C}\)
Vector
A physical quantity described by a magnitude **and** a direction. It can be written in terms of two perpendicular components.
Displacement \(\mathbf{s}\), Force \(\mathbf{F}\)
Reminder – Unit Vectors
\(\hat{\mathbf i}\) and \(\hat{\mathbf j}\) are unit vectors along the chosen x ‑ and y ‑axes:
\(|\hat{\mathbf i}| = |\hat{\mathbf j}| = 1\)
\(\hat{\mathbf i}\perp\hat{\mathbf j}\) (they are orthogonal)
Representing Vectors
Graphical Representation
An arrow whose length is proportional to the magnitude and whose orientation shows the direction.
Typical vector drawn on a 2‑D coordinate system.
Algebraic (Component) Representation
For a vector \(\mathbf{A}\) in the plane:
\[
\mathbf{A}=A_x\hat{\mathbf i}+A_y\hat{\mathbf j}
\]
where \(A_x\) and \(A_y\) are the components along the x ‑ and y -axes respectively.
Sign Conventions (2‑D Plane)
East (right) = + \(x\)
West (left) = – \(x\)
North (up) = + \(y\)
South (down) = – \(y\)
Conversion Between Forms
If a vector has magnitude \(A\) and makes an angle \(\theta\) measured anticlockwise from the positive x -axis:
\[
A_x = A\cos\theta,\qquad A_y = A\sin\theta
\]
Conversely, given components \(A_x\) and \(A_y\):
\[
A = \sqrt{A_x^{2}+A_y^{2}},\qquad
\theta = \tan^{-1}\!\left(\frac{A_y}{A_x}\right)
\]
Use the signs of \(A_x\) and \(A_y\) (or a calculator’s “atan2” function) to place \(\theta\) in the correct quadrant.
Adding Coplanar Vectors
1. Graphical Methods
Method Steps (quick‑check) Illustration
Tip‑to‑Tail (Polygon)
Draw the first vector \(\mathbf{A}\) with its tail at the origin.
Place the tail of \(\mathbf{B}\) at the tip of \(\mathbf{A}\) (keep length and direction unchanged).
Draw the resultant \(\mathbf{R}\) from the origin to the tip of \(\mathbf{B}\).
Parallelogram
Draw \(\mathbf{A}\) and \(\mathbf{B}\) with a common tail at the origin.
Complete the parallelogram by drawing lines parallel to each vector through the tip of the other.
The diagonal from the origin gives the resultant \(\mathbf{R}\).
2. Component (Algebraic) Method
For \(\mathbf{A}=A_x\hat{\mathbf i}+A_y\hat{\mathbf j}\) and \(\mathbf{B}=B_x\hat{\mathbf i}+B_y\hat{\mathbf j}\):
\[
\boxed{\mathbf{R}= \mathbf{A}+\mathbf{B}= (A_x+B_x)\hat{\mathbf i}+ (A_y+B_y)\hat{\mathbf j}}
\]
Find the magnitude and direction of \(\mathbf{R}\) with the conversion formulas given above.
Subtracting Coplanar Vectors
Graphical Approach
Subtracting \(\mathbf{B}\) from \(\mathbf{A}\) is equivalent to adding the **negative** of \(\mathbf{B}\) (same length, opposite direction).
Step Description Illustration
1. Reverse \(\mathbf{B}\)
Draw a vector \(-\mathbf{B}\) with the same magnitude as \(\mathbf{B}\) but pointing opposite to \(\mathbf{B}\).
2. Add \(\mathbf{A}\) and \(-\mathbf{B}\)
Use either tip‑to‑tail or parallelogram method as for addition.
Component Approach
\[
\boxed{\mathbf{A}-\mathbf{B}= (A_x-B_x)\hat{\mathbf i}+ (A_y-B_y)\hat{\mathbf j}}
\]
Again use the magnitude‑direction formulas to obtain the resultant’s size and angle.
Worked Example – Vector Addition
Problem: Two forces act in the horizontal plane.
\(\mathbf{F}_1 = 30\;\text{N}\) at \(30^{\circ}\) north of east.
\(\mathbf{F}_2 = 40\;\text{N}\) at \(120^{\circ}\) measured anticlockwise from east.
Find the resultant \(\mathbf{F}_R = \mathbf{F}_1+\mathbf{F}_2\).
Resolve each force into components (east = + \(x\), north = + \(y\)):
\[
\begin{aligned}
F_{1x}&=30\cos30^{\circ}=30(0.866)=25.98\;\text{N}\\
F_{1y}&=30\sin30^{\circ}=30(0.5)=15.00\;\text{N}\\[4pt]
F_{2x}&=40\cos120^{\circ}=40(-0.5)=-20.0\;\text{N}\\
F_{2y}&=40\sin120^{\circ}=40(0.866)=34.64\;\text{N}
\end{aligned}
\]
Add the components :
\[
F_{Rx}=F_{1x}+F_{2x}=25.98-20.0=5.98\;\text{N}
\]
\[
F_{Ry}=F_{1y}+F_{2y}=15.00+34.64=49.64\;\text{N}
\]
Resultant magnitude :
\[
F_R=\sqrt{F_{Rx}^{2}+F_{Ry}^{2}}=\sqrt{(5.98)^{2}+(49.64)^{2}}=50.0\;\text{N}
\]
Resultant direction (measured anticlockwise from east):
\[
\theta_R=\tan^{-1}\!\left(\frac{F_{Ry}}{F_{Rx}}\right)=\tan^{-1}\!\left(\frac{49.64}{5.98}\right)=83.1^{\circ}
\]
Both components are positive → first quadrant → “\(83.1^{\circ}\) north of east”.
Worked Example – Vector Subtraction
Problem: A displacement \(\mathbf{d}_1 = 12\;\text{m}\) at \(40^{\circ}\) east of north is followed by a displacement \(\mathbf{d}_2 = 5\;\text{m}\) due south. Find the net displacement \(\mathbf{d} = \mathbf{d}_1-\mathbf{d}_2\).
Choose north = + \(y\), east = + \(x\):
\[
\begin{aligned}
d_{1x}&=12\sin40^{\circ}=12(0.643)=7.72\;\text{m}\\
d_{1y}&=12\cos40^{\circ}=12(0.766)=9.19\;\text{m}\\
d_{2x}&=0\\
d_{2y}&=-5\;\text{m}\quad(\text{south is –\(y\)})
\end{aligned}
\]
Subtract components :
\[
d_x = d_{1x}-d_{2x}=7.72-0=7.72\;\text{m}
\]
\[
d_y = d_{1y}-d_{2y}=9.19-(-5)=14.19\;\text{m}
\]
Resultant magnitude :
\[
d=\sqrt{d_x^{2}+d_y^{2}}=\sqrt{7.72^{2}+14.19^{2}}=16.2\;\text{m}
\]
Resultant direction** (east of north):
\[
\theta=\tan^{-1}\!\left(\frac{d_x}{d_y}\right)=\tan^{-1}\!\left(\frac{7.72}{14.19}\right)=28.6^{\circ}
\]
Net displacement: \(16.2\;\text{m}\) at \(28.6^{\circ}\) east of north.
Summary Table
Operation
Graphical Method (steps)
Component Formula
Resultant Magnitude
Resultant Direction
\(\mathbf{A}+\mathbf{B}\)
Tip‑to‑tail or parallelogram.
Draw resultant from origin (or from first tail).
\((A_x+B_x)\hat{\mathbf i}+(A_y+B_y)\hat{\mathbf j}\)
\(\sqrt{(A_x+B_x)^2+(A_y+B_y)^2}\)
\(\tan^{-1}\!\bigl((A_y+B_y)/(A_x+B_x)\bigr)\) (adjust quadrant)
\(\mathbf{A}-\mathbf{B}\)
Reverse \(\mathbf{B}\) to obtain \(-\mathbf{B}\).
Add \(\mathbf{A}\) and \(-\mathbf{B}\) using tip‑to‑tail or parallelogram.
\((A_x-B_x)\hat{\mathbf i}+(A_y-B_y)\hat{\mathbf j}\)
\(\sqrt{(A_x-B_x)^2+(A_y-B_y)^2}\)
\(\tan^{-1}\!\bigl((A_y-B_y)/(A_x-B_x)\bigr)\) (adjust quadrant)
Key Points to Remember
Scalars have magnitude only; vectors have magnitude + direction.
State your coordinate axes and sign convention before resolving any vector.
\(\hat{\mathbf i}\) and \(\hat{\mathbf j}\) are unit vectors of length 1 and are perpendicular.
When converting components to an angle, always check the signs of the components to place the angle in the correct quadrant.
Graphical methods help visualise the result; the component method is faster for calculations and is required in exam questions.
Both addition and subtraction obey the same algebraic rules: add the components, then recombine into magnitude‑direction form.