The equations of uniformly accelerated motion extend naturally to the two-dimensional case by replacing scalars with vectors:
Equations of accelerated motion in 2D
In components, the equation of motion becomes a pair of independent equations:
The trajectory of a 2D motion with constant acceleration is a parabola. The most important case is projectile motion (oblique launch), in which the acceleration is entirely vertical, directed downwards:
Here lies the key to projectile motion: along there is no acceleration, so the horizontal motion is uniform; along only gravity acts, so the vertical motion is free fall. The two components are independent and combine into the curved trajectory.
Velocity and acceleration, distinct roles
The velocity vector is always tangent to the trajectory at point A, while the acceleration vector “curves” the trajectory, bending it towards itself. In projectile motion always points downwards, even while the body is rising.
Projectile motion: the velocity is tangent to the trajectory, gravity always points downwards.
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Collegamenti
Argomenti: Vettori Concetti: Moto parabolico · Caduta libera Metodi: Scomposizione in componenti cartesiane
Esercizi collegati: Caduta libera in due dimensioni · Calciatore gittata e altezza massima · Esercizio svolto — Gittata di un proiettile