Practical aspects of increasing workers efficient work time in a high noise level industrial area.
Mikalauskas, R. ; Volkovas, V.
1. Introduction
In the modern world there exists a lot of negative impacts on human
health, including acoustic noise in a technical environment surrounding
the individual. That noise is usually being emitted by various equipment
at a workplace, outside or in a household.
Today the problem of fighting the noise is widely discussed; it is
named as priority in order to ensure human safety and health,
appropriate work environment and prevention of professional diseases.
The base of human protection from the risk due to noise in many
European countries is on the number of European Parliament and Council
Directives: 2000/14/EC, 2003/10/EC, 2002/44/EC, the occupational
exposure standards of the countries [1-3]. These requirements impelled
two directions of studies in solving the industrial noise problem and
human health protection: identification and assessment of acoustic
fields; environmental acoustic field control and insurance of optimal
working conditions for the personnel. The first direction focuses more
on acoustic fields modelling [4, 5] and prediction, where the second
direction focuses on creating means and tools [4] for reducing noise
levels, as well as their implementation outdoors [6, 7], in buildings
[8] and industrial environment. Research in the aforementioned second
direction and other known methods for reducing nose create a path for
studying the possibility of increasing staff work time until a
permissible noise exposure dose is accumulated. The effectiveness of
such methods can be evaluated with an effective work time [T.sub.e]
which characterises the amount of time a staff member can work in a
noisy environment so that the noise exposure value [L.sub.EX,8h] = 85
dB(A) [1] is not exceeded. This paper studies a group of noise sources
that generate high level (up to 110 dB) level noise--specific acoustic
fields in an enclosed space, as well as methodology for effectively
increasing the work time in such environment until a permissible daily
noise exposure dose is accumulated.
The investigation of acoustic fields, generated by various sources
is a specific and complex problem, which needs application of complex
solutions that are presented in this paper as practical methodology for
increasing time duration, until a permissible noise doze for workers
would be achieved. To characterize and define this problem a number of
questions were answered. Among them we can mention an analysis of
acoustic fields' specific features that helps us to designate a
corresponding investigation and create practical methodology for
enclosed spaces with wideband acoustic field control generated from
multiple sources for the aim of efficient and practical noise reduction
in the denoted place.
While solving various aspects of the acoustical problem, many
researches have been done [9-13], but there is a lack of systematic
view, to suggest general investigation methodology, which could be used
to evaluate specific characteristic of the acoustic field and would
allow to achieve an efficient and economically competitive solution for
increasing the time duration until an allowable noise dose for workers
will be reached.
For that purpose an optimization analysis was conducted by using a
limited number of experimental data as well as modelling the acoustic
power and directivity for some noise sources. With the help of this
analysis, the acoustic field in an enclosed space with a complicated
acoustic excitation was successfully simulated and an optimal passive
noise reduction screen system was selected. The noise passive reduction
results ~5-6 dB were the same as achieved from modifying the structures
of some working units responsible for the noise level [14].
This paper investigates specific acoustical fields in systematic
point of view that are generated by several turbine compressors in an
enclosed space as well as general methodology of reducing noise levels
in a denoted place of an industrial shop room. Practical aspects for
applying this approach are connected with increasing the staff work time
until a maximum accumulated noise exposure dose is reached, by more than
six times.
2. Principles of acoustic field control and measurement quantities
Efficient noise reduction in industrial premises is possible only
by assessing the problem from systematic positions. The formulation of
noise control strategy and application of acoustic field's
measurement for such premises requires particular steps. According the
requirements of the series of standards ISO 11690 [15-17] they can be
described as:
a) formulation of purposes and criteria;
b) evaluation and identification of noise;
c) noise control;
d) composition of control program;
e) use of measurements;
f) evaluation of noise reduction efficiency.
The sound noise control can be distinguished into two levels as
illustrated in Fig. 1.
[FIGURE 1 OMITTED]
In a general practical situation we have noise sources that can be
identified and impacted only so that there would be no changes in the
construction, negative impacts on technological process and suggested
solutions would not require large capital investments. In this work it
was investigated how and by what principles it is possible to control
and purposefully reduce emitted acoustic field level in compressors room
premises with 8 high output turbo compressors (Fig. 2).
The mentioned European directives define the measurement quantities
of acoustic fields, that is: A--weighted average time acoustic noise
pressure [L.sub.Aeq] and C--weighted maximum (peak) sound presser level
[L.sub.Cpk]. Thus in practice methodically it is correct to measure
these quantities, or if the purpose requires measuring another quantity,
the results still can be provided as [L.sub.Aeq] and [L.sub.Cpk]. This
is necessary when the intensimetry is applied to the measurements, which
allows determining the intensity and propagation direction of the sound.
But the results of the methods application for comparative analysis
still have to be delivered by mentioned quantities.
The sound pressure level measurements are useful if the
measurements can be made for one or for at least part of sources. While
localising in sources particular emitted noise points, it is purposeful
to use intensimetry.
[FIGURE 2 OMITTED]
For the measurement of the mentioned features of the acoustic field
parameters and analysis B&K (Denmark) sound pressure meter 2260
Investigator, equipment Pulse 3600C and sound intensity microphone
antenna of type 3599 were used.
3. The stages for reduction of sound pressure level in closed space
The general procedure for sound pressure level reduction can be
explained by below presented scheme (Fig. 3), where using systematic
approach main stages are distinguished.
[FIGURE 3 OMITTED]
The reduction of noise, in the limits of systematic understanding
requires data accumulation and investigation of specificity of acoustic
fields, composition of mathematical models and modelling of acoustic
fields, result analysis and decision making. This would be quite
universal way both for formulation of the purpose and naming aimed sound
pressure level we have to investigate the nature of acoustic field and
define its specific features. The obtained results can be used for the
formulation of protective means principal solutions, selection of sound
absorbing material, numerical modelling of acoustic fields and physical
protective means and optimization of constructional solutions. In our
opinion, this direction is most promising for enhancing operating
conditions in a particular space (compression room premises) and to
increase efficient work time [T.sub.e] for workers who are repairing one
of the turbo compressors in the mentioned compression room. Then we need
to describe some specific aspects of problem solution direction and the
potential effect of procedure realization.
3.1. Analysis of noise nature
The nature of the noise was determined by measuring the change of
acoustic noise parameters in time. With the help of particular examples
of turbo compressors in compression room we will show how noise nature
assessment procedure is applied.
[FIGURE 4 OMITTED]
[FIGURE 5 OMITTED]
The noise was measured in the height of 1.5 m from the floor of
turbo compressor turbine zone (about 3.5 m from the end of the turbo
compressor) within 1 m ... 1.3 m distance from the aggregate. The
measurement quantities were: A-weighted average time acoustic noise
sound pressure level [L.sub.Aeq] and C-weighted maximum (peak) sound
pressure level [L.sub.Cpk]. The results of the measurements are provided
in Figs. 4 and 5.
The Fig. 4 presents variation of equivalent sound presser level
parameters [L.sub.Aeq] and [L.sub.Cpk] in time. The 1/3 octave
characteristic spectrum of acoustic noise is provided in Fig. 5. Using
Figs. 4 and 5 and definitions of hygiene norms [3] the nature of noise
emitted by turbo compressors in the workshop room can be defined as
constant broadband noise.
3.2. Estimation of extreme acoustic field criteria
The measurements of turbo compressor emitted noise intensity for
the investigation of the features of noise sources acoustic field were
made. To determine turbo compressors emitted noise acoustic field
extreme zones the separate nodes emitted noise was measured. In order to
localize extreme zones as precisely as possible, the measurements were
made within 0.25 m distance from investigated node surface. The noise of
turbo compressor was measured in five longitudinal sections.
Using intensimetry principle the noise emitted by turbo compressor
and distribution pipes were applied. Fig. 7 presents the turbo
compressors measured surface involute (without right plane). The
Selected dimensions for measured surface segments were 1 m x 1 m.
[FIGURE 6 OMITTED]
When analysing measurement results, the maximum noise emission
zones were determined. In Fig. 6 these zones are indicated by arrows:
* at the axial compressor back next to oil pump in a centre part
(pos. 1);
* in the area of axial joint plane of compressor and gas turbine
(pos. 2);
* next to the speed-reducer/gear unit (box) (pos. 3);
* next to the air press (4 and 5 pos.).
[FIGURE 7 OMITTED]
On the base of the results obtained after investigation of noise
nature, the acoustic screen material was selected and they covered the
maximum noise emission zones. The results of such noise reduction
physical modelling are presented in Fig. 8.
[FIGURE 8 OMITTED]
The provided results show that by covering the area of the turbo
compressor zone next the axial compressor with sound absorbing plates,
the acoustic noise level is significantly reduced in that zone. It is
possible that by covering all eight separate zones of turbo compressors
with optimal size easily removable acoustic screens will reduce total
acoustic noise level in the machine premises.
The performed investigation shows that acoustic fields can be
reduced by using passive means made of sound absorbing material.
Acoustic material must feature particular characteristics, which are
determined by using sound noise measurement spectral analysis and
physical modelling. For appropriate and optimal use of the means in
particular technical environment the results provided in this study are
essential. If the experiments require a lot of resources and the
obtained information is insufficient to make conclusions about the
characteristics of the technical environment--it is possible to apply
mathematical modelling. In this case there is a need to choose the
assumptions which would ensure the adequacy of the models for the real
acoustic fields. The model identification by using physical experiment
data might be useful.
3.3. Mathematical modelling of acoustical fields
In order to reproduce adequately the acoustic field in technical
environment, the acoustic excitation modelling is very important. The
variety of maintained equipment in technical environments both in the
sense of frequency spectrum and emitted power requires separate
investigation of separate source acoustic parameters. In this study the
noise emitted by maintained turbo compressor was modelled (Fig. 2, a).
For this purpose when measuring sound intensity according the above
described methodology the zones in the turbo compressor where the
maximum noise was emitted (extreme zones). Similar noise measurements
were made for all eight turbo compressors exploited in compression
section of the machine room.
The data obtained from the turbo compressor emitted noise were used
for theoretical 2D sources model by using finite elements method (FEM).
The excitation source was modelled by distinguishing five circular
zones, their size the same as extreme zones of the turbo compressors:
axial compressor, gas turbine, reducer and air press. In these zones
specific values for acoustic pressure were set. It is known [18], that
intensity which characterizes the directivity of acoustic power and
sound pressure are related:
I = W/S = [p.sup.2]/[rho]c , (1)
here I is sound pressure intensity, W/[m.sup.2]; W is acoustic
power, W; S is surface area through which during particular time
acoustic power permeates, [m.sup.2]; p is sound pressure in specific
point; [rho] is air density, kg/[m.sup.3]; c is the speed of sound wave,
m/s. The sound pressure values had to be set such that acoustic power
emitted by every separately modelled turbo compressor and its
directivity would comply with the values determined experimentally. For
this purpose optimisation analysis was performed with objective function
of turbo compressors emitted acoustic power, state variables--acoustic
intensity in front, back, left and right plane directions, designed
variables--sound pressure values in extreme zones. The optimization
analysis was performed using subproblem approximation method [19]. Thus
by using penalty functions the minimizing is performed:
[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] (2)
here F(x, [p.sub.k]) is unconstrained objective function (also
termed a response surface); [bar.x] is design variable vector; [p.sub.k]
is a response surface parameter; [f.sub.0] is reference objective
function value; [??] is approximated objective function; X is penalty
function of the designed variable; R, B, L and G are penalty functions
of state variables, in front, back, left and right planes directions,
respectively; [MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] are
state variables, acoustic intensity in the front, back, left and right
plane directions, respectively (Fig. 1, b). The optimization analysis
led to obtaining values of designed variables, i.e. sound pressure in
the extreme zones of every turbine.
The adequacy of the modelled excitation source was tested
experimentally. During the experiment the acoustic field of the
maintained turbo compressor was measured without sound absorbing screens
and when maximum noise emission zone next to axial compressor is covered
with screens and sound intensity in four directions is calculated. The
division of measured surface into segments is presented in Fig. 7.
The values of sound intensity level, measured experimentally and
calculated using theoretically modelled excitation source, using FEM
model in four directions is provided in Fig. 9.
The obtained results of the modelled noise source acoustic field
show that by applying mathematical modelling the adequate reconstruction
of exploited turbo compressors acoustic field sound intensity and
evaluation of its acoustic power are possible when the sound absorbing
screens are used. By comparing sound intensity level for different
cases: with sound absorbing planes and without them it can be seen that
in first case it was reduced in left and backplane direction by 14%.
[FIGURE 9 OMITTED]
3.4. Evaluation of efficiency of methodology application
The efficiency of suggested methodology was executed according the
decrease of [L.sub.Aeq] and correspondingly increase of [T.sub.e].
Fourteen acoustic screens arrangement model were tested totally. Their
main feature was that by optimizing arrangement of the screens the
minimal sound pressure level next to one of idle (being repaired)
compressor. In practice it was accomplished by using procedure presented
in Fig. 10. The Fig. 11 summarizes the results of methodology
realization prototype model according the decrease of [L.sub.Aeq] and
correspondingly the increase of [T.sub.e].
The tendency of increment of prototype model efficiency was
obtained by comparing [L.sub.Aeq] decrease and respective [T.sub.e]
increase with initial noise level in compression room turbo compressors
hall. It shows that all the means increase efficiency, but the influence
of the means is different. The biggest influence is obtained by covering
compressors' air presses and axial compressors with casings made of
ISOTEC KVL-100 acoustic panels and covering the floors. Other applied
means did not cause any significant changes in the values criteria.
[FIGURE 10 OMITTED]
The efficiency of technology was evaluated by comparing with
alternative noise reduction technology by using absorbance screens,
often used in practice [4, 8]. The analysis shows that in order to reach
the result of the prototype ([L.sub.Aeq] reduction from 110 dBA to 95
dBA) in case of alternative technology very big investment is required
(30 ... 40 times larger than suggested technologies). Moreover, by
applying some other suggested technological means, the efficiency would
increase and [L.sub.Aeq] decrease even more and in such case the area of
the whole shop machine hall ceilings and walls is not sufficient to
apply absorbance screens used in alternative technology.
[FIGURE 11 OMITTED]
4. Conclusions
The executed investigations allowed creating strategy for reduction
of noise emitted in closed space by several sources and approve its
elements. The main idea of the suggested strategy--by using passive
acoustic screen identify and acoustic separate the zones of aggregate
which emitted sound in machinery hall in shop's compression section
and thus reduce general sound pressure level. There were noise reduction
models suggested and corresponding practical cases for noise level
optimization technology.
For the optimization the most efficient--the third technology
prototype (Fig. 11) realization model was selected as its optimization
need and efficiency of actions can be evaluated according the increment
of efficient work time [T.sub.e]:
* for non-optimized prototype of the third model the [T.sub.e]
increased 4 times;
* for optimized prototype of the third model--6 times.
When comparing suggested technology with widely used absorbance
screens technology [7] the effect is as follows:
* the current sound pressure level decrease effect (in repair zone)
was achieved with 40 times lesser investments for acoustic materials
than covering shop ceilings and walls with acoustic panels (the sound
pressure reduction method by using absorbance screens);
* my applying the above mentioned method even by covering the whole
area of the shop ceiling and walls with absorbance screens, the sound
pressure level decreases only to 94 dB.
http://dx.doi.org/10.5755/j01.mech.21.6.13240
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Received September 29, 2015
Accepted November 12, 2015
R. Mikalauskas*, V. Volkovas**
* Kaunas University of Technology, Technological System Diagnostic
Institute Kcstucio str. 27, 44312 Kaunas, Lithuania, E-mail: robertas.
mikalauskas@ktu.lt
** Kaunas University of Technology, Technological System Diagnostic
Institute Kcstucio str. 27, 44312 Kaunas, Lithuania, E-mail:
vitalijus.volkovas@ktu.lt