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Modelling the motion of a projectile

The principle of superposition of motions

One motion, two independent directions

A projectile is an object thrown into the air that is subject (in the simplified high-school model) only to its weight, once it has left the hand or the device that launched it. This is the case for a tennis ball after being hit, a cannonball, or a thrown stone.

The key idea, due to Galileo, is that we can study the horizontal motion and the vertical motion separately, as if they had no influence on each other. We say that we decompose the motion along two perpendicular axes, x (horizontal) and y (vertical).

Why this decomposition works

The weight P = m*g is a vertical force, directed downward. In the absence of air friction (the simplified model's assumption), there is no horizontal force. Consequence:

  • On the horizontal axis (x): no force -> constant speed -> uniform rectilinear motion.
  • On the vertical axis (y): only gravity acts -> uniformly accelerated motion (like free fall).

Concrete example

A ball is thrown horizontally from a roof with a speed v0 = 5 m/s. Even as it falls, its horizontal speed stays at 5 m/s throughout the fall (as long as we neglect air resistance). Its vertical speed, meanwhile, increases steadily due to g (about 9.8 m/s^2 on Earth).

Axis Force Type of motion
Horizontal (x) none uniform rectilinear
Vertical (y) weight uniformly accelerated

Common pitfall

Never confuse the two axes: many students think the horizontal speed decreases "because the object is falling." This is wrong in this model: the fall (y axis) and the forward motion (x axis) are completely independent as long as there is no air friction.