Kinematics of motion in a straight line: displacement, velocity, acceleration, equations of motion
🚀 Mechanics (M1): Kinematics of Motion in a Straight Line
📍 Displacement
Displacement, denoted by $\Delta \mathbf{s}$, is the change in position of an object. It is a vector quantity, meaning it has both magnitude and direction. Analogy: Think of a runner on a straight track. If they start at the 0 m mark and finish at the 30 m mark, their displacement is +30 m in the direction of the track. If they finish at the 10 m mark, the displacement is +10 m. If they finish at the -5 m mark (behind the start), the displacement is –5 m.
📈 Velocity
Velocity is the rate of change of displacement. It is also a vector.
$$\mathbf{v} = \frac{d\mathbf{s}}{dt}$$If an object moves at a constant speed of 5 m s⁻¹ to the right, its velocity is $\mathbf{v}=+5\,\text{m\,s}^{-1}$. Example: A cyclist travels 20 km east in 2 h. $$\mathbf{v} = \frac{20\,\text{km}}{2\,\text{h}} = 10\,\text{km\,h}^{-1}\text{ east}$$
⚡ Acceleration
Acceleration is the rate of change of velocity. It is also a vector.
$$\mathbf{a} = \frac{d\mathbf{v}}{dt}$$If a car speeds up from 0 to 20 m s⁻¹ in 5 s, its average acceleration is $$\mathbf{a}_{\text{avg}} = \frac{20\,\text{m\,s}^{-1} - 0}{5\,\text{s}} = 4\,\text{m\,s}^{-2}$$
📐 Equations of Motion (Constant Acceleration)
When acceleration is constant, the following equations hold (often called the “SUVAT” equations).
- $\displaystyle \mathbf{v} = \mathbf{u} + \mathbf{a}t$ – Final velocity after time $t$.
- $\displaystyle \mathbf{s} = \mathbf{u}t + \tfrac{1}{2}\mathbf{a}t^2$ – Displacement after time $t$.
- $\displaystyle \mathbf{v}^2 = \mathbf{u}^2 + 2\mathbf{a}\mathbf{s}$ – Relates velocities and displacement without time.
- $\mathbf{u}$ – Initial velocity
- $\mathbf{v}$ – Final velocity
- $\mathbf{a}$ – Acceleration
- $t$ – Time
- $\mathbf{s}$ – Displacement
| Equation | Use |
|---|---|
| $\,\mathbf{v} = \mathbf{u} + \mathbf{a}t$ | Find final velocity when time and acceleration are known. |
| $\,\mathbf{s} = \mathbf{u}t + \tfrac{1}{2}\mathbf{a}t^2$ | Find displacement when time, initial velocity and acceleration are known. |
| $\,\mathbf{v}^2 = \mathbf{u}^2 + 2\mathbf{a}\mathbf{s}$ | Find final velocity or displacement when time is not needed. |
🏃♂️ Example Problem
A skateboarder starts from rest and accelerates at $2\,\text{m\,s}^{-2}$ for $10\,\text{s}$.
- Find the final velocity.
- Find the displacement.
1. $\displaystyle \mathbf{v} = 0 + (2\,\text{m\,s}^{-2})(10\,\text{s}) = 20\,\text{m\,s}^{-1}$ 2. $\displaystyle \mathbf{s} = 0 \times 10\,\text{s} + \tfrac{1}{2}(2\,\text{m\,s}^{-2})(10\,\text{s})^2 = 100\,\text{m}$So the skateboarder reaches 20 m s⁻¹ and travels 100 m in 10 s.
💡 Key Takeaways
- Displacement, velocity, and acceleration are all vectors.
- Use the correct sign (positive or negative) to indicate direction.
- For constant acceleration, the SUVAT equations give a quick way to solve problems.
- Always check units – they must be consistent across all quantities.
Revision
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