\(F_{\text{net}} = ma\)
\(F_{\text{net}}\): net (resultant) force in N · \(m\): mass in kg · \(a\): acceleration in m/s²
| mass ↓ force → | pull 10 N | pull 20 N | spring 30 N | pull 50 N, friction 20 N |
no horizontal force |
|---|---|---|---|---|---|
| 1 kg | |||||
| 2 kg | |||||
| 5 kg | |||||
| 10 kg |
Notice: Down a column, the mass doubles, so the acceleration . Compare the spring and friction columns.
| mass ↓ accel. → | at rest: 0 m/s² | 2 m/s² | lifted up: 3 m/s² | 4 m/s² | 5 m/s² |
|---|---|---|---|---|---|
| 1 kg | |||||
| 2 kg | |||||
| 3 kg | |||||
| 5 kg |
Notice: “At rest” means \(F_{\text{net}}=0\), not “no forces”. For “lifted up”, \(F\) is the net force, not the string’s pull.
| accel. ↓ force → | pull 10 N | pull 20 N | spring 30 N | pull 40 N (left) | pull 50 N, friction 20 N |
|---|---|---|---|---|---|
| 1 m/s² | |||||
| 2 m/s² | |||||
| 5 m/s² | |||||
| 10 m/s² |
Notice: Put grid C next to grid A. Which answers appear in both? Why?
Concept: net force and constant velocity
1. A box is pushed along the floor at constant velocity. Which is true?
Constant velocity → \(a = 0\) → \(F_{\text{net}} = 0\): push = friction. Forces still act; they cancel.
Concept: how \(a\) depends on \(m\)
2. The same net force acts on X and Y. X has twice the mass of Y. Then \(a_X\) is
\(a = F/m\): with \(F\) fixed, \(a \propto 1/m\). Double the mass → half the acceleration (look down a column of grid A).
Concept: velocity vs. acceleration
3. A ball is thrown straight up. At the top, the net force on it is
The velocity is zero for an instant, but the acceleration is not: only gravity acts, so \(F_{\text{net}} = mg\) downward.