Study of Parameter Influence of the Basic Cylinder of Rotary Screw
Propulsion Units on Noise Level during Locomotion on Ice
Umar Vahidov
1a
, Dmitriy Mokerov
2
, Roman Dorofeev
1
, Vladimir Belyakov
1
,
Vladimir Makarov
1b
and Yuri Molev
1c
1
Nizhny Novgorod State Technical University n.a. R.E. Alekseev, Minin Str., 24, Nizhny Novgorod, Russian Federation
2
Nizhny Novgrod State Pedagogical University n.a. K. Minin, Uyanova str., 1, Nizhny Novgorod, Russian Federation
Keywords: Basic Cylinder of Rotary Screw Propulsion Unit, Ice, Noise Level, Area of Deformation.
Abstract: The paper presents deformation calculations of the basic cylinder of the rotary screw propulsion unit under
external load. The influence of such basic parameters of the rotary screw propulsion unit as basic cylinder
diameter, its length and wall thickness on its deformation area, and, as a consequence, the generated noise
level has been demonstrated. The basis for the method development were studies by scientists who were
studying the sound wave generation by the deformation of different structural elements, parts and assemblies.
The contribution of each of the parameters of the basic cylinder to the general level of the generated sound
pressure was analyzed. It was determined that the magnitude of the noise level is mostly dependent on the
length of the basic cylinder, then, to a less extent, on the cylinder wall thickness, and, to the least extent, on
its diameter. A correlation was revealed between the oscillations power of the propulsion unit and their
correlation with their generated noise level. The results and conclusions obtained during the described study
allow for a more solid-based approach to the parameter selection of the rotary-screw propulsion unit for
improved acoustic comfort, also for improved driver's work conditions, including the relief of his/her nervous
system, sharpening of his/her attention during the operation, accident reduction. Beside the design of
structures with the least possible noise, the proposed method allows also for selection of a rational propulsion
unit design achieving a compromise between vehicle's noise specifications and its off-road ability.
1 INTRODUCTION
Currently, the main way to develop all-terrain
vehicles is to ensure their mobility (Belyaeva and
Evseev, 2020, Diakov, 2018, Klubnichkin, 2019,
Manianin, 2019). However, the study of the noise
level generated by all-terrain vehicles was not given
sufficient attention.
One of the factors worsening the work condition
of all-terrain vehicle drivers is the high noise level in
the cabin, which both affects the driver's well-being
and detracts him/her. Numerous researchers have
proven that the increased noise level (more than 55-
65dB) significantly affects human health (Parma
Declaration on Environment and Health, 2010)
(Fritsch, 2011, Lercher, 2007). Exceeding the noise
level by 10-20dB relative to the background leads to
a
https://orcid.org/0000-0003-4109-8406
b
https://orcid.org/0000-0002-4423-5042
c
https://orcid.org/0000-0002-0429-4590
panic in fish (Effects of Noise on Fish, Fisheries, and
Invertebrates in the U.S. Atlantic and Arctic from
Energy Industry Sound-Generating Activities, 2012).
The same excess of the noise level by 10 relative to
the background leads to a decrease in the bird
population by 90%. (Harbrow, 2010)
The noise generated by off-road vehicles is mainly
generated by the engine, transmission, as well as
vibrations caused by the interaction of the propulsion
unit with the road surface. The most noisy is the rotary
screw propulsion unit. Let us consider in more detail
how noise is generated in this propulsion.
The purpose of this study is to develop the
requirements for the operation of all-terrain vehicles
with a rotary-screw propulsion units and the choice of
their design parameters that ensure the movement of
vehicles with a generated sound level less than 65dB.
714
Vahidov, U., Mokerov, D., Dorofeev, R., Belyakov, V., Makarov, V. and Molev, Y.
Study of Parameter Influence of the Basic Cylinder of Rotary Screw Propulsion Units on Noise Level during Locomotion on Ice.
DOI: 10.5220/0010526807140719
In Proceedings of the 7th International Conference on Vehicle Technology and Intelligent Transport Systems (VEHITS 2021), pages 714-719
ISBN: 978-989-758-513-5
Copyright
c
2021 by SCITEPRESS – Science and Technology Publications, Lda. All rights reserved
2 THEORETICAL RESEARCH
A most complete description of the influence of the
screw blade on the total noise in a vehicle's cabin can
be found in studies by (Nikitin, 2004, Shashurin,
2010, Pokachalov, 2003) providing evidence that the
acoustic power of any sound source can be obtained
from the following equation:
𝑊
=𝜌𝑐𝑠
𝑣
𝑆
,
(1)
where - is the air density, 𝑐 – is the sonic speed,
-
is the oscillation velocity of the surface radiating the
acoustic oscillations, 𝑠
– is the power conversion ratio
of the mechanical oscillations to the acoustic ones,
whereas 𝑆
is the acoustic radiant surface. From this
equation, it is obvious that the design-stipulated
acoustic power 𝑈 is dependent on the acoustic radiant
surface and the surface oscillation velocity:
𝑈 =𝐾𝑊
= 𝐾𝑣
𝑆
,
(2)
where K is the generalized conversion ratio of the
mechanical oscillation energy into the acoustic one.
Under recognition that the oscillation velocity is
related to the amplitude and the locomotion velocity
by the following dependency:
=2𝐴

𝐿 𝑉

,
where 𝐴

is the maximum oscillation amplitude,
and 0.5 𝐿 𝑉

is the cycling time of such oscillation
equal to the rotor length divided by the vehicle's
locomotion speed (since the oscillation cycle consists
of the maximum displacement of the point under test
and its return in its initial position, then, during the
rotor travel all-along its length, the surface of the
basic cylinder will be displaced by 𝐴

, first, to the
one side, and then to the other side, that is, the total
displacement is 2𝐴

, stipulating the presence of
the factor 2 in the presented dependency.
In general appearance, the loading diagram of the
rotary screw propulsion unit from the travel surface
in form of ice (Belyakov, 2020, 2021) leading to the
basic cylinder deformation can be presented as shown
in Figure 1.
Figure 1: Basic cylinder loading diagram due to external
loads.
The problem can be solved by means of Autodesk
Simulation Mechanical design software package. The
problem was solved in quasi-static statement with
linear elastic and plastic material properties.
As material, the basic rotor cylinder adopts St3sp
steel grade, see specifications in Table 1.
Table 1: Physical and mechanical properties of St3sp steel
grade.
ρ,
t/m
3
σ
т
,
МPа
σ
0.2
,
МPа
δ
5
,
%
E,
N/mm
2
v
7,858 245 370 23 200*10
3
0,3
We obtained the sag of the basic cylinder walls as
delta of the load value 𝑅, the basic cylinder length 𝐿,
the basic cylinder diameter 𝐷 and the wall thickness
. The obtained values are unambiguous evidence of
the fact that as the wall thickness , and the diameter
of the basic cylinder grow, whereas its length get
shorter, the deformation magnitude is reduced. In the
graphic appearance, the results of the obtained
calculations are presented in Figures 2 - 4, whereas
the numeric values of the sag are listed in Table 2.
Figure 2: Design case of short basic cylinder loading (1200
mm length) with large diameter (800 mm) and thick wall (5
mm).
Figure 3: Design case of long basic cylinder loading (1800
mm length) with Large diameter (800 mm) and thick wall
(5 mm).
Study of Parameter Influence of the Basic Cylinder of Rotary Screw Propulsion Units on Noise Level during Locomotion on Ice
715
Figure 4: Design case of short basic cylinder loading (1200
mm length) with Average diameter (600 mm) and thin wall
(2 mm).
Having obtained the deformation values of the
basic cylinder surface, at known speed of locomotion
and geometry of the basic cylinder, based on
equations 1 and 2 we can easily determine the energy
of the mechanical oscillations of the system under
analysis. In order to determine the acoustic radiation
power, it is important to find out the values of factor
К from dependency 2. The simplest method of its
determining is the comparison of the power of the
mechanical oscillations with the actual generated
sound power of the experimental propulsion works.
3 EXPERIMENTAL RESEARCH
To determine this parameter, a test bench was
developed (Figure 6) consisting of two semi-rotors
assembled with a two-shaft counter-rotating gear
reducer, with mutually balanced ice penetration of the
screw blades, and two adjustable height vertical
columns for ice penetration depth adjustment of the
screw blades. The rotation of the rotors was obtained
via belt transmission generating torque from a
vertically traveling weight.
Figure 6 shows: 1 – two balanced semi-rotors; 2
two-shaft counter-rotation gear reducer; 3 belt
transmission; 4 column; 5 meter weight; 6 ice
penetration depth adjustment column.
Figure 5: Design case of long basic cylinder loading (1800 mm length) with small diameter (400 mm) and thin wall (2 mm).
Table 2: Test results of sound generated by basic cylinder of rotary screw propulsion unit during its deformation.
Item No. D, mm L, mm l, mm
δ, mm
R, kN ∆, mm*10
-3
Design level of
generated sound, dB
1
600 1200 1000
3
100
48 20
*
2 600 1800 1500 127 30
3 400 1200 1000 125 30
4 400 1800 1500 410 75
5 600 1200 1000
2
60 20
6 600 1800 1500 180 40
7 400 1200 1000 162 40
8 400 1800 1500 485 75
9 800 1200 1000
5
18 10
10 800 1800 1500 36 15
*
the sound level equal to 20 dB marked in test No. 1 is not the design value, but an experimental one obtained in the scope
of the conducted studies.
VEHITS 2021 - 7th International Conference on Vehicle Technology and Intelligent Transport Systems
716
Figure 6: Test bench for determining of the relationship
between the generated sound level and the deformation
force magnitude of the basic cylinder.
The experimental data demonstrate that the re-
distribution of the mechanical energy of the basic
cylinder oscillations into acoustic oscillations with
1/10 ratio. The obtained data allow for the
modification of equation 2 to a dependency of the
following appearance:
𝑈 =0.4
𝐴

𝑉
𝜋 𝐷.
(3)
4 ANALYSIS OF RESULTS
The analysis of the obtained results demonstrates that
the design of the rotary screw propulsion units in
general and that of the basic cylinder, in particular,
will be the less capable of radiating the acoustic
energy, the less the deformation magnitude and the
locomotion speed of the vehicle are. The rotor length
change reduces, on the one side, the oscillation
velocity, on the other side, it leads to sag growth.
Thereby, in spite of the fact that the power of the
generated acoustic radiation (based on dependency 3)
is directly proportional to the rotor diameter and
inversely proportional to its length, the total noise
level will grow with the increase of the length and
with the diameter reduction, since these parameters
influence the sag magnitude stipulating, in equation
3, the noise level growth not in linear, but in
quadratical dependency.
The reduction in the length of the base cylinder is
limited by the need to ensure such a length of contact
of the screw blade with the ice, at which the necessary
reserve of thrust force of the vehicle under study
would be provided. The diameter of the rotor is
limited exclusively by the dimensions of the vehicle.
In papers (Vakhidov, 2020a, Vakhidov, 2020b,
Lipin, 2019, Mokerov, 2019), noises generated by
rotary screw propulsion units were analyzed, the
structure of which is shown in Figure 7.
Figure 7: Components of noise generated by rotary screw
propulsion unit during all-terrain vehicle locomotion on ice
(see paper (Vakhidov, 2020a)). 1 – noise generated by
screw blade penetration into ice; 2 noise generated by
base cylinder shell deformation; 3 noise generated by base
cylinder friction over ice surface.
Thereby, in previous works, no difference based
on the basic cylinder sag and shell deformation was
made. The data provided herein allow for finalizing
the contribution of the processes associated exactly
with the basic cylinder shell deformation of the rotary
screw propulsion unit to the total noise level. As a
result, it was found out that it is exactly the
deformation under analysis which is "liable" for 80%
of the generated acoustic radiation, and it is exactly
the basic cylinder wall thickness change and the
reduction of the radiant area (e.g. by means of the
basic cylinder internal surface sound insulation for
single-time radiant area and the radiated noise
reduction by 50%) is the most promising
development direction of low-noise rotary screw
propulsion units.
Figure 8: Finalized components of noise generated by
rotary screw propulsion unit during all-terrain vehicle
locomotion on ice. 1– noise generated by screw blade
penetration into ice; 2 noise generated by base cylinder
shell deformation; 3 noise generated by basic cylinder
deflection; 4 noise generated by basic cylinder friction
over ice surface.
Study of Parameter Influence of the Basic Cylinder of Rotary Screw Propulsion Units on Noise Level during Locomotion on Ice
717
5 CONCLUSIONS
The obtained data made it possible to develop
requirements to rotary screw propulsion units to
provide for its proper operation on ice with acoustic
radiation level. It was found out that the basic
cylinder should have as large diameter as possible
(restricted only by the overall vehicle dimensions)
and as less length as possible (restricted by the
necessity of the presence of at least two turns of the
screw blade winding). The basic cylinder wall should
feature a wall thickness of at least 5 mm.
The results obtained in this work clearly indicate
that the use of 4 short rotors from the point of view of
acoustic radiation is the most promising way to
develop vehicles of this class.
The difference in the designs of these vehicles is
shown in Figure 9 and 10.
Figure 9: Classic line-up of a special all-terrain vehicle.
Figure 10: The proposed design, which provides noise
reduction when driving a special all-terrain vehicle.
A further direction to reduce the noise of the
machine is to replace the front rotors with skis or
skates. However, this approach significantly reduces
the scope of this technique, including making it
impossible for it to move on water.
ACKNOWLEDGEMENTS
This study was conducted in continuation of the
research conducted in the Nizhny Novgorod scientific
and practical school of transport snow and with
financial support of the grants of the President of the
Russian Federation № MD-226.2020.8.
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