We have already seen that motion in more than one dimension that undergoes constant acceleration is given by the vector equation:
Simply stated, projectile motion is just the motion of an object near the earth's surface which experiences acceleration only due to the earth's gravitational pull. In the section on one-dimensional motion with constant acceleration, we learned that this acceleration is given by g = 9.8 m/s2. Using a three-dimensional coordinate system, with the z-axis pointing upwards to the sky, the corresponding acceleration vector becomes a = (0, 0, - g). This turns out to be the only piece of information we need to write down the general vector equation for projectile motion.
As an example, consider a creature fired out of a canon with speed v at an angle θ from the earth's surface. How far away will the creature be when it falls back down to earth? To answer this question we must first determine the position function, x(t), which means we must find v0 and x0. We can choose the x-axis to point in the direction of the creature's horizontal movement across the earth. This means that the creature's movement will be constrained to the x-z plane, and so we can completely ignore the y-direction, effectively reducing our problem to two dimensions. (In fact, using this kind of trick we can always reduce projectile motion problems to two dimensions!) From the initial speed and angle of projection, we can determine that v0 = (v cosθ, 0, v sinθ). Since the canon is fired from the surface of the earth, we can set x0 = 0 (where 0 = (0, 0, 0), the zero-vector). This leaves us with the position function:
|z(t)||=||v sinθt - gt2|