\(E_k = \tfrac12 mv^2\)
\(E_k\): kinetic energy in J · \(m\): mass in kg · \(v\): speed in m/s
| mass ↓ velocity → | 1 m/s | 2 m/s | 3 m/s | 4 m/s | −2 m/s |
|---|---|---|---|---|---|
| 1 kg | |||||
| 2 kg | |||||
| 4 kg | |||||
| 10 kg |
Notice: Across a row, \(v\) doubles (1 → 2 m/s), so \(E_k\) becomes times larger. Why is the last column positive?
| mass ↓ \(E_k\) → | 4 J | 16 J | 36 J | 100 J | 1.6 kJ |
|---|---|---|---|---|---|
| 0.5 kg | |||||
| 2 kg | |||||
| 8 kg | |||||
| 50 kg |
Notice: Down a column, the mass is ×4 (0.5 → 2 → 8 kg) and the speed is ÷.
| velocity ↓ \(E_k\) → | 10 J | 50 J | 100 J | 200 J | 1 kJ |
|---|---|---|---|---|---|
| 1 m/s | |||||
| 2 m/s | |||||
| 5 m/s | |||||
| 10 m/s |
Notice: From 1 m/s to 2 m/s, the mass for the same energy is ÷. Speed matters more than mass.
Concept: how \(E_k\) depends on \(v\)
1. The speed of a car doubles. Its kinetic energy becomes
\(E_k \propto v^2\): \(2^2 = 4\). This is why speed matters so much in crashes.
Concept: energy is a scalar
2. Two identical cars move at 10 m/s, one north and one south. Their kinetic energies are
\(v^2\) is always positive, and energy has no direction. Both cars have the same \(E_k\).
Concept: the unit of energy
3. Using \(E_k = \tfrac12 mv^2\), the joule is equal to
kg × (m/s)² = kg·m²/s² = (kg·m/s²)·m = N·m = J.