Resolve vectors into components, add vectors algebraically in two dimensions, and apply the triangle and parallelogram laws to find resultants.
A scalar has magnitude only (e.g. speed, mass, temperature). A vector has both magnitude and direction (e.g. force, velocity, displacement, acceleration).
Vectors are written in bold (F) or with an arrow overhead (F⃗). The magnitude is written as |F| or simply F (italic).
Any vector F at angle θ from the positive x-axis can be broken into perpendicular components:
The components are scalars (can be positive or negative). Always draw a sketch first to identify which quadrant θ falls in.
To add multiple vectors algebraically:
| Symbol | Meaning | Unit |
|---|---|---|
| F | Magnitude of force vector | N |
| Fx | x-component of force | N |
| Fy | y-component of force | N |
| R | Magnitude of resultant | N |
| θ | Direction angle from positive x-axis | ° |
| ΣFx | Sum of all x-components | N |
| ΣFy | Sum of all y-components | N |
Triangle law: Draw vectors head-to-tail (one after the other). The resultant is the vector drawn from the tail of the first to the head of the last, closing the triangle.
Parallelogram law: Draw both vectors from the same point. Complete the parallelogram. The resultant is the diagonal from the common point.
An object is in equilibrium when the net force on it is zero. For 2D problems this means:
A closed vector diagram (the tail of the last vector meets the head of the first) indicates equilibrium.
The equilibrant is the single force that would bring a system into equilibrium. It is equal in magnitude but opposite in direction to the resultant.
Three forces act on an object: F₁ = 40 N at 0°, F₂ = 30 N at 90°, F₃ = 50 N at 210°. Find the resultant.
When three concurrent coplanar forces are in equilibrium, Lami's Theorem states:
where α, β, γ are the angles opposite each force (i.e. the angle between the other two forces). This is a quick method when three forces meet at a point and are in equilibrium — no need to resolve into components.
In three dimensions, a vector has three mutually perpendicular components: Fx, Fy, Fz. The magnitude is R = √(Fx² + Fy² + Fz²). Direction is specified by angles to each axis. IEB may present introductory problems where a force in a plane tilted in 3D must be resolved into horizontal and vertical components first, then further resolved.
| Cable | Force (N) | Angle (° from +x-axis) |
|---|---|---|
| A | 100 | 0° |
| B | 80 | 90° |
| C | 60 | 200° |
| D | 40 | 300° |