Classical Velocity Addition
Classical Velocity Addition
For simplicity, we restrict our consideration of velocity addition to one-dimensional motion. Classically, velocities add like regular numbers in one-dimensional motion. (See this figure.) Suppose, for example, a girl is riding in a sled at a speed 1.0 m/s relative to an observer. She throws a snowball first forward, then backward at a speed of 1.5 m/s relative to the sled. We denote direction with plus and minus signs in one dimension; in this example, forward is positive. Let \(v\) be the velocity of the sled relative to the Earth, \(u\) the velocity of the snowball relative to the Earth-bound observer, and \(u\prime \) the velocity of the snowball relative to the sled.
Classical Velocity Addition
\(\text{u=v+u}\prime \)
Thus, when the girl throws the snowball forward, \(u=1.0 m/s+1.5 m/s=2.5 m/s\). It makes good intuitive sense that the snowball will head towards the Earth-bound observer faster, because it is thrown forward from a moving vehicle. When the girl throws the snowball backward, \(u=1.0 m/s+(-1.5 m/s)=-0.5 m/s\). The minus sign means the snowball moves away from the Earth-bound observer.
This lesson is part of:
Special Relativity