Teaching
Projectile motion
A kicked ball, a jet of water, a stone thrown from a bridge: they all follow the same law. Set up the throw, then compare trajectories.
Controls
- Current throw
Results
- Flight time
- 1.44 s
- Range
- 10.2 m
- Maximum height
- 2.55 m
- Impact speed
- 10.0 m/s
The equations
Axes: origin on the ground, directly below the launch point; x-axis horizontal, y-axis pointing up.
- Equations of motion
x(t) = v0 cos α · t
y(t) = −½ g t2 + v0 sin α · t + h0
x(t) = 7.07 t
y(t) = −4.90 t2 + 7.07 t
- Trajectory (a parabola)
y = −g x2 / (2 v02 cos2 α) + x tan α + h0
y = −0.0980 x2 + 1.00 x
- Maximum height
H = h0 + v02 sin2 α / (2g)
H = 2.55 m
- Flight time
tv = [v0 sin α + √(v02 sin2 α + 2 g h0)] / g
tv = 1.44 s
- Range
R = v0 cos α · tv
with no launch height, R = v02 sin 2α / g
R = 10.2 m
- Impact speed
v = √(v02 + 2 g h0)
v = 10.0 m/s
Assumptions
The projectile is treated as a point mass, and the Earth’s frame of reference as inertial. Air resistance is neglected: only its weight acts on it, so its acceleration is g, pointing straight down.
Try this
With no launch height, throw at 30° and then at 60° at the same speed. What do you notice?
Show the explanation
the range is v₀² sin 2α / g, and sin 60° = sin 120°. Two complementary angles give the same range.
Still with no launch height, find the angle that gives the longest range.
Show the explanation
45°, because sin 2α is at most 1, when 2α = 90°.
Make the same throw on Earth and then on the Moon, with no launch height. By how much is the range multiplied?
Show the explanation
by 9.8 / 1.6 ≈ 6.1. With no launch height, the range is inversely proportional to g.