To
the point, in Fig. 4 we see that for a single pulsing sphere the field pattern in the near
field is also progressive and distinguishes from the far field only by the velocity of its
amplitude variation with the distance. Thus, on the basis of conventional mathematical
formalism there exists no region of the standing field. And all attempts to substantiate
this field, e.g. in [5], are based on an incorrect approximation of conventional equations
for the case r << . The incorrectness is first of all in ignoring the
spatial phase delay of the process, in comparison with the time characteristic. As the
indicated terms are arguments of a trigonometric function, the value equal to the integer
number of periods can be deleted from the momentary time phase of process t without
any consequence. The rest value will vary in limits from 0 to 2 . Thus, however near distance from the
source we take, we can always find the time intervals in which the time phase of process
is less than that spatial. It is clear that this will violate the rigour of inequality
r << , the result of this we see in Fig. 4. Though visually the
dynamics of this process can be delusively seen as a standing wave near the source,
because of moving surface of the pulsing sphere. In case of few sources superposition the
near field will form and the interference will be seen in it. Now we can study it on the
basis worked out in this investigation.
5. Conclusions
In this investigation we have ascertained that the
non-conformal mapping of a semi-belt of the plane Z into the uniform radial
metric of the plane W models in the best way the processes in an acoustic
field produced by a single pulsing sphere.
On the basis of carried out construction of dynamical
non-conformal mapping we have ascertained that with the correct application of
conventional mathematical formalism the standing wave in the near field does not form, and
all attempts to describe it in the region r << are the consequence of incorrectly
taken into account relationship of time and spatial phases of process in the argument of
trigonometric function.
References:
- Karavashkin, S.B. and Karavashkina, O.N. Theoretical substantiation and experimental
corroboration of existence of transverse acoustic wave in gas. SELF Transactions,
2 (2002), 1, p. 3- 16 3-16.
- Karavashkin, S.B. and Karavashkina, O.N. Theorem of curl of a potential vector in dynamical
fields. SELF Transactions, 2 (2002), 2, p. 1-
9
- Karavashkin, S.B. Some
peculiarities of derivative of complex function with respect
to complex variable. SELF Transactions, 1 (1994), pp. 77-95. Eney (Ukraine,
in English).
- Polyakova, A.L. Acoustic radiator. Physical encyclopaedia, vol.1. Sovetskaya
Encyclopedia, Moscow, 1960 (Russian).
- Doak, P.E. Noise and acoustic fatigue in aeronautics, An introduction to sound
radiation and its sources. John Wiley & Sons Ltd., 1968.
- Rusakov, I.G. Impedance acoustical. Physical encyclopaedia, vol.2. Sovetskaya
Encyclopedia, Moscow, 1962 (Russian).
- Korn, G.A. and Korn, T.M. Mathematical handbook for scientists and engineers.
MGraw-Hill, New York - Toronto -
London, 1961, 720 pp. (Russian)
- Lavrentiev, M.A. and Shabat, B.V. Methods of theory of function of complex variable.
Nauka, Moscow, 1973, 736 pp. (Russian).
- Sveshnikov, A.G. and Tikhonov, A.N. Theory of functions of complex variable. In: The
course of higher mathematics and mathematical physics, edited by Tikhonov, A.N.,
Ilyin, V.A. and Sveshnikov, A.G. Nauka, Moscow, 1967.
|