Last section we studied head on collisions, in which both objects move on a line. Most natural collisions, however, are not head on, instead causing objects to move at an angle to their original trajectory. Consider a game of pool, in which balls are frequently hit at an angle to get them in the pockets. These kinds of collisions, though more complicated, can be solved using the same methods as those used in one dimension. An elastic collision still conserves kinetic energy and, of course, any collision conserves linear momentum. We shall examine the elastic and completely inelastic case, and show how each of these cases can be solved.
Since the theory behind solving two dimensional collisions problems is the same as the one dimensional case, we will simply take a general example of a two dimensional collision, and show how to solve it. Consider two particles, m1 and m2, moving toward each other with velocity v1o and v2o, respectively. They hit in an elastic collision at an angle, and both particles travel off at an angle to their original displacement, as shown below:
|v1o2 + v2o2 = v1f2 + v2f2|
Let's start with the x-component. Our initial momentum in the x direction is given by: m1v1o - m2v2o. Note the minus sign, as the two particles are moving in opposite directions. After the collision, each particle maintains a component of their velocity in the x direction, which can be calculated using trigonometry. Thus our equation for the conservation of linear momentum in the x-direction is:
|m1v1o - m2v2o||=||m1v1fcosθ1 + m2v2fcosθ2|
|0||=||m1v1fsinθ1 + m2v2fsinθ2|
Surprisingly enough, the completely inelastic case is easier to solve in two dimensions than the completely elastic one. To see why, we shall examine a general example of a completely inelastic collision. As we've done previously, we will count equations and variables and show that it is solvable.
The most general case of a completely inelastic collision is two particles m1 and m2 moving at an angle of θ1 to each other with velocities v1 and v2, respectively. They undergo a completely inelastic collision, and form a single mass M with velocity vf, as shown below.
|x component:||m1v1 + m2v2cosθ1 =||Mvfcosθ2|
|y component:||m2v2sinθ1 =||Mvfsinθ2|
Our entire study of collision can be seen as simply an application of the conservation of linear momentum. So much time is spent on this topic, however, because it is such a common one, both in physics and in practical life. Collisions occur in particle physics, pool halls, car accidents, sports, and just about anything else you can think of. A thorough study of the topic will be well rewarded in practical use.