Gravity on a slope
The steeper the slope, the bigger the share of your weight that pulls you down it.
On a slope at angle θ, your weight mg splits in two: mg sin θ along the slope, pulling you downhill, and mg cos θ into the snow, pressing you onto it. Subtract snow friction (Ch 2) and you get the acceleration: a = g (sin θ − μ cos θ). Slopes are often quoted as a percentage: gradient = tan θ × 100.
| Slope | Gradient | Pull down the slope | Acceleration | Speed after 50 m straight |
|---|---|---|---|---|
| 5° | 9% | 64 N | 0.37 m/s² | ≈ 22 km/h |
| 15° | 27% | 190 N | 2.07 m/s² | ≈ 52 km/h |
| 25° | 47% | 311 N | 3.70 m/s² | ≈ 69 km/h |
| 35° | 70% | 422 N | 5.22 m/s² | ≈ 82 km/h |
15°: 75 × 9.81 × sin 15° ≈ 190 N; a = 9.81 × (0.259 − 0.05 × 0.966) ≈ 2.07 m/s²; v = √(2 × 2.07 × 50) ≈ 14.4 m/s ≈ 52 km/h. Without drag, mass cancels: heavy and light skiers accelerate alike.
Why beginners start on gentle slopes
On a 5° nursery slope, speed builds slowly enough to practise the snow plough. Below about 3° on groomed snow, gravity barely beats friction and you'll hardly move at all: try it in the Slope Lab.
What's the gradient of a 20° slope, and the pull on a 60 kg skier?
tan 20° ≈ 0.36, so 36%; pull = 60 × 9.81 × sin 20° ≈ 201 N.