The energy of sound waves in gases consists of two components: the potential energy, which is due to the magnitude of the relative elastic strain, and the component of the kinetic energy of the oscillatory movement of gas molecules. Adiabatic compression and rarefaction have to change the gas temperature in the wave disturbance areas. However, since in the sound waves these zones alternate, the net effect is zero. | The component, which is due to the kinetic energy of the oscillatory movement of gas molecules, is absent in the energy of PGEWs.The energy of the PGEW consists of two components: the energy of starting sound disturbances, including the component associated with the change in temperature and pressure of the disturbance area, and the energy equivalent of the work done by pressure forces creating pressure gradient, which compresses and rarefies the wave fronts. |
Inside a bonded space, the sound waves are reflected from the walls. | Inside a bonded space, the compressed and rarefied fronts of PGEWs are reflected from the walls but immediately are extinguished by next fronts du to interference. The effect is equivalent to absorption, and the entire energy of the wave is transferred to the walls in the form of heat or cold.The PGEW cannot pass through an extremum point, thus if the function of the pressure gradient has an extremum (the centre of rotation), the PGEW is dissipated in this place. |