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Projectile motion

Beginner

A launched body follows a parabola under gravity.

Key relationy = x tanθ − gx²/(2u²cos²θ)

A projectile has constant horizontal velocity and constant downward acceleration g, so its path is a parabola. Split the initial velocity: ux = u cosθ, uy = u sinθ.

Worked example

Launched at 20 m/s at 30°: ux = 17.3, uy = 10 m/s.

Common mistake

Acceleration is g everywhere, including the top, where only the vertical velocity is zero.

In more detail

Projectile motion is motion under gravity with an initial velocity. Horizontal velocity stays constant, while vertical velocity changes at g, giving a parabolic path.

Real-world uses

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Frequently asked questions

What shape is the path of a projectile?

A parabola, if air resistance is ignored.

Does the horizontal velocity change?

No, not if air resistance is ignored, since there is no horizontal force.

Why is the path of a projectile a parabola?

The horizontal motion is uniform and the vertical is uniformly accelerated, so eliminating time gives y as a quadratic in x.

Related topics in Kinematics

Motion graphs from calculus · Terminal velocity · Two-dimensional motion · Time of flight · Maximum height · Horizontal range

← All Kinematics topics