Notes on Acoustics

In Chapters. 2 and 3, complex amplitudes were gradually introduced in the analysis of simple problems and it was mentioned that with increased problem complexity, the advantage of complex variables becomes more apparent. This will be further illustrated in this and subsequent chapters. Actually, after having become used to solving problems in this manner, it often becomes difficult to do it any other way.
A ball thrown against a rigid wall bounces back with the same speed as the incident if the collision is elastic. This reflection is not unlike what happens when a sound wave strikes a rigid, impervious wall; it is reflected with no change in strength.
Consider next a head-on collision between an incident ball, the projectile, and a stationary ball, the target. The masses and initial velocities of these balls are M 1, M 2, and U 1, U 2. It is well known (from billiards, for example) that if the masses are the same, the projectile comes to rest after the collision and the target acquires the velocity of the projectile. [1] If the masses are not the same, we find the velocities
and
of the projectile and the target after the collision to be such that
These results follow from the equations for conservation of momentum and energy (see Problem 1). The quantities R U and T U can be considered to be reflection and transmission...