Abstract
In this paper the author proves that the propagation velocity of an acoustic velocity wave in the near field differs from the velocity of a pressure wave, while both differ from c_0 in d'Alambert's equation. The velocity of an acoustic velocity wave was calculated for a point source, for a cylindrical source of zero order and for a circular piston and ring in a baffle.References
[1] M. ABRAMOWITZ, I. A. STEGUN, Handbook of mathematical functions, Dover Publications, New York 1963.
[2] F. JANKE, F. EMDE, F. LOACH, Tafeln horerer funktionen, B. 6. Teubner velagagesellschaft, Stuttgard 1960.
[3] M. KWIEK, Laboratory acoustics, PWN, Poznań-Warszawa 1968 (in Polish).
[4] I. MALECKI, Theory, of acoustic waves and systems, IFTR PAS, Warszawa 1964 (in Polish).
[2] F. JANKE, F. EMDE, F. LOACH, Tafeln horerer funktionen, B. 6. Teubner velagagesellschaft, Stuttgard 1960.
[3] M. KWIEK, Laboratory acoustics, PWN, Poznań-Warszawa 1968 (in Polish).
[4] I. MALECKI, Theory, of acoustic waves and systems, IFTR PAS, Warszawa 1964 (in Polish).