Components of Projection
A projectile follows a parabolic path because its motion can be split into two independent vectors: a constant horizontal velocity and a vertical motion subject to constant gravitational acceleration.
Vertical: y = u sin(θ)t - ½gt²
1. Independence of Motion
The key principle of projectile motion is that the horizontal and vertical motions do not affect each other. Gravity only acts vertically, meaning the horizontal velocity uₓ = u cos(θ) remains constant throughout the flight.
2. The Trajectory Equation
By eliminating time (t) from the horizontal and vertical equations, we get the parabolic equation for any point (x,y) in the flight path:
Deep Dive: Worked Examples
✅ Example 1: Basic Ground-to-Ground
A football is kicked at 20 m/s at an angle of 30°. Calculate the horizontal range.
uᵧ = 20 sin 30 = 10.00 m/s
Total Time T = 2 × 1.02 = 2.04s
✅ Example 2: Velocity at a Certain Time
A projectle is fired at 25 m/s at 40°. Find its velocity vector after 1.5 seconds.
vᵧ = 25 sin 40 - (9.81)(1.5) = 16.07 - 14.72 = 1.35 m/s
✅ Example 3: Horizontal Launch
A stone is thrown horizontally from a cliff 45m high at 15 m/s. How far from the base does it land?
t = √(90 / 9.81) = 3.03s
✅ Example 4: Uneven Ground
A golf ball is hit from a tee 5m above the fairway. u = 30 m/s, θ = 20°. Find the total horizontal distance.
Solving quadratic: t ≈ 2.50s
✅ Example 5: Angle for Specified Range
At what angle should a ball be thrown at 15 m/s to hit a target 20m away on ground level?