A shell is fired from a cannon and follows a somewhat parabolic path until it returns to the ground.
At a certain instant the horizontal component of its velocity are, respectively, 1.21 meters per second and 2.54 meters per second.
We could sketch a triangle to depict 1 second's worth of motion, which will be 1.21 meters horizontally and 2.54 meters vertically. The horizontal leg of the triangle will represent a displacement vector of 1.21 meters; the vertical leg will represent a displacement vector of 2.54 meters, which will be placed with its initial point at the terminal point of the first.
- The velocity will be the magnitude of this vector, in meters, divided by 1 second, giving velocity in m/s.
We could equivalently just sketch a similar triangle whose legs represent the 1.21 m/s and 2.54 m/s velocities. The hypotenuse will represent the velocity of the projectile.
We regard the horizontal and vertical velocities vx and vy as the velocity components vx and vy of a velocity vector.
- v = `sqrt(vx^2 + vy^2)
- tan-1(vy / vx), or tan-1(vy / vx) + 180 deg if vx is negative.
The figure below depicts the velocity components vx and vy and the vector velocity resulting from the combination of these horizontal and vertical velocities.
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