Karachun V.V, Mel’niñk V. N.
National Technical University
of Ukraine «KPI»
REPRODUCTION
OF EXPECTED FREQUENCY
SPECTRUM
BANDS
If the number of pleces is m = 18 (fig. 1) in the
spectrum of siren it can be observed clearly outlined three frequency bands –
0...20, 35…55, 75…95, and in areas 25...35, 55...75 ³
95...100 – dip. In fact, these forms
are missing in the spectrum. Thus, the rotor of siren with the number of places
m = 18 is convenient to use for reproduction of expected frequency spectrum
bands. Values m = 59, spectrum is similar to the spectrum of siren, in which
the modulation function is quasi-trapezoid form. They, apparently, almost
coincide.
Provided that the number of places m = 276, or higher, for example, m =
1528, spectrum of siren tends to increase amplitudes of harmonics with
increasing of their numbers (fig.2). This feature, along with white noise is a significant interest
for the practice, because allows to evaluate the acoustic compliance of
construction and on-board equipment, which frequencies are very large. In this
case, the siren with the number of places m = 59, for example, quite unsuitable
because the amplitude of harmonics with numbers higher than 120, almost equal
to zero, and all the energy of acoustic emission is concentrated at low
frequencies.
With increasing number of places m in the rotor the characteristics of the spectrum is more steeply
against the axis of frequencies (fig. 3 dotted line).
As already noted, the most dangerous, in terms of
occurrence of the phenomenon of sonic fatique in material is a broadband sound
load. Generating a lot of fluctuations in the details and components of
products, acoustic radiation may cause irreversible deformities due to spatial
or spatial-frequency resonance. So, it is undoubted interest to studying the
issue of creation of broadband acoustic radiation using monorotor siren to
reproduce conditions close to operational.

For definition, let’s outline the bandwidth of frequency
with number of forms equal to 100, ie, let’s take
n = 100.
Spectrum optimization problem for these conditions can
be reduced to analyze the expression:
. (1)
Let’s analyze, in which the values of m, λk
and φi amplitude of
spectral components of generable noise will be constant.
The solution of the assigned task will be illustrated
as a modulation in a form of rectangular pulses, analytically shown by the
expression:
(2)
whence it easily may be defined the amplitude of components of the
spectrum:
. (3)
Replacement of quazi-trapezoid form of modulation
functions into rectangular, as shown further calculation, do not make
substantial differences in the assessment of structure of spectrum. At the same
time achieve significant simplification of mathematical apparatus of problem
witch is being solved. On the other hand, to determine the power of acoustic
radiation it is not so only important the form of modulation function but also
the maximum expenditure of air. In consideration of expressions (2) (3),
formula (1) has a form:



. (4)
Here m – the number of equal parts in which the circle
of rotor is broken into; f(t) = λkf0 (0≤ λk ≤1,
k – number of area) - modulation
function on those areas where windows are put; f0 – amplitude; φ³ - angle of
displacement of windows relatively to the basis radial line equidistant from
the center of the stator disc, the sum
means that the value
of parameter k is not used in
succession, but only for areas with pulses; p
– number of individual pulses per unit time T, therefore 1 <p ≤ m.