[0001] The present invention relates to an acoustic panel for noise barriers and to a noise
barrier provided with such a panel.
[0002] More in detail, the present invention relates to a sound-absorbent acoustic panel
for noise barriers adapted to obstruct the propagation of polluting acoustic waves
in open spaces, to which use explicit reference will be made in the following description
without therefore loosing in generality.
[0003] As known, the propagation of polluting acoustic waves in open spaces, such as sections
of highways or railways, construction sites or industrial plants, is normally controlled
by a series of acoustic panels of substantially rectangular shape, which are mounted
side-by-side on a specific support frame so as to form a substantially vertical wall,
which generally in seamless manner surrounds the polluting acoustic source.
[0004] The most common sound-absorbent acoustic panels have a rectangular shape and are
generally essentially formed by two rigid half-shells made of metallic material, which
are essentially shaped as a shallow rectangular bowl and which are reciprocally coupled
so as to form a box-like containment of flat parallelepiped shape; and by a layer
of rock or glass wool, which completely fills the interspace inside the box-like container.
[0005] The outer box-like container mainly performs a sound-proofing action, while the filling
material mainly performs a sound-absorbent action.
[0006] The main drawback of the acoustic panels described above is that of not being adaptable,
or rather "tuned", to the features of the polluting acoustic wave, i.e. to the frequency
spectrum of the incident acoustic wave, so as to maximize the shielding capacity of
the noise barrier.
[0007] The features of the polluting acoustic wave indeed vary according to the type of
polluting acoustic source (moving motor vehicles, moving trains, operating machinery
etc.), while in the above-described acoustic panels the attenuation curve of the incident
acoustic wave according to frequency has a substantially bell/wave shape which offers
very narrow possibility of adjustment/adaptation.
[0008] Experimental tests have indeed shown that major variations of acoustic panel size
and/or constructive materials produce only minor variations to the incident acoustic
wave attenuation curve pattern.
[0009] It is the object of the present invention to make an acoustic panel for noise barriers
which offers a better possibility of adapting to the features of the incident acoustic
wave and which is additionally cost-effective to produce.
[0010] In accordance with such objectives, in conformity to the present invention, an acoustic
panel for noise barriers is made as disclosed in claim 1 and preferably, but not necessarily,
in any one of the dependent claims.
[0011] According to the invention, a noise barrier is further made as disclosed in claim
16.
[0012] The present invention will now be described with reference to the accompanying drawings,
which illustrate a non-limitative embodiment thereof, in which:
- figure 1 shows an axonometric view, with parts removed for clarity, of a noise barrier
comprising acoustic panels made according to the dictates of the present invention;
- figure 2 is an exploded perspective view of one of the acoustic panels shown in figure
1;
- figure 3 is a section view of the upper part of the acoustic panels shown in figure
2; while
- figures 4, 5, 6 and 7 show on enlarged scale four different diffusion profiles which
may be adopted on the front face of the reverberating plate of the acoustic panel
shown in figures 2 and 3.
[0013] With reference to figures 1, 2 and 3, numeral 1 indicates as a whole a sound-absorbent
acoustic panel, particularly suited for making a noise barrier 2 adapted to obstruct
the propagation of polluting acoustic waves in open or closed spaces.
[0014] In the illustrated example, in particular, the noise barrier 2 is preferably, but
not necessarily constituted by a series of acoustic panels 1 of preferably, but not
necessarily rectangular shape, which are arranged side-by-side on a support frame
3, so as to form a preferably, but not necessarily vertical shielding frame.
[0015] More in detail, with reference to figure 1, in the illustrated example, the support
frame 3 preferably, but not necessarily consists of a base 4 made preferably, but
not necessarily of reinforced concrete, and by at least one pair of vertical supporting
uprights 5, which overhangingly extend from the base 4 itself, parallel and mutually
side-by-side. Each acoustic panel 1 is arranged straddling two consecutive vertical
uprights 5 so as to have one of the two faces facing the source of the polluting acoustic
waves.
[0016] In the illustrated example, in particular, the vertical uprights 5 of the support
frame 3 preferably, but not necessarily consist of a series of rectilinear metallic
profiles 5 with H-shape cross section, which overhangingly extend from the base 4
in vertical direction, and are arranged in pairs parallel and mutually side-by-side,
so as to have the longitudinal grooves 5a locally and substantially coplanar with
the laying plane of the acoustic panel 1, which is positioned straddling the rectilinear
metallic profiles 5 themselves. Furthermore, the rectilinear metallic profiles 5,
which form each pair of vertical uprights 5, are reciprocally distanced so that the
two vertical side edges of the corresponding central acoustic panel 1 engage the longitudinal
grooves 5a of the rectilinear metallic profiles 5 themselves.
[0017] With reference to figures 2 and 3, the acoustic panel 1 has, as mentioned, a preferably,
but not necessarily rectangular shape and essentially consists of a reverberating
plate 6 of preferably, but not necessarily rectangular shape, which is made of a rigid,
compact material having a nominal density higher than 200 kg/m
3 (kilograms per cubic meter), and which has, on one of the two faces, a stepped-profile
surface 6a, which is dimensioned so as to reflect at least one incident acoustic wave
with predetermined reference frequency or "band center" in "diffused" manner and with
destructive interference; and by a layer 7 of sound-absorbent material, which has
a peripheral edge that essentially follows the shape of the reverberating plate 6,
and is coupled to the reverberating plate 6 so as to completely cover the stepped-profile
surface 6a, so as to be crossed by the acoustic wave reflected in "diffused" manner
by such a surface.
[0018] In other words, the stepped-profile surface 6a is dimensioned to "diffuse" acoustic
waves of frequency and intensity different from the incident acoustic wave in all
directions; such diffused waves may also cause a destructive interference with the
other acoustic waves arriving towards the panel. By virtue of the two combined phenomena,
a reduction of the acoustic wave amplitude is obtained.
[0019] Such a physical phenomenon is radially different from the reflection which occurs
on the surface of traditional acoustic panels and is not sufficiently appreciable
(in terms of reflected sound energy reduction) in presence of a constant, repetitive
panel surface morphology pattern. A monotonous repetition of the "fretting" of the
surface of the panel indeed reflects only one frequency, and thus the phenomenon of
the diffusion distributed in frequency and of the destructive inference would be drastically
reduced.
[0020] Instead, the layer 7 of sound-absorbent material systematically attenuates the intensity
of the reflected acoustic waves working in parallel to the "diffused reflection with
destructive interference" phenomenon because it can work for the entire length of
the layer itself; the diffusion indeed "distributes" the waves in all directions after
the impact of the direct wave, causing a much longer return path (and thus more effective
sound-absorption) within the layer itself.
[0021] In the illustrated example, in particular, the shape of the stepped-profile surface
6a is determined on the basis of the "Quadratic Residue" or "Schroeder's" mathematical
model, which was developed by mathematician Manfred SCHROEDER.
[0022] In other words, the number of steps, the width of each step and the distances between
the various steps are determined on the bases of the "Quadratic Residue" or "Schroeder's"
mathematical model, so as to reflect in "diffused" manner with destructive interference
at least one incident acoustic wave having a reference frequency or predetermined
"band center".
[0023] In the illustrated example, in particular, the reverberating plate 6 has a thickness
preferably, but not necessarily comprised between 4 and 50 cm (centimetres), and a
nominal density preferably, but not necessarily comprised between 300 and 8000 kg/m
3 (kilograms per cubic meter); while the stepped-profile surface 6a is preferably,
but not necessarily shaped so as to copy a Schroeder profile optimized to reflect
at least one acoustic wave having reference frequency or "band center" preferably,
but not necessarily comprised between 500 and 4000 Hz (Hertz) in "diffused" manner.
[0024] More in detail, the stepped-profile surface 6a of the reverberating plate 6 is preferably,
but not necessarily optimized according to the "Quadratic Residue" mathematical model,
so as to reflect in "diffused" manner at least one first acoustic wave with reference
frequency or "band center" preferably, but not necessarily equal to 500 Hz, 1000 Hz,
2000 Hz, or 4000 Hz; and at least one second acoustic wave with reference frequency
or "band center" different from that of the first acoustic wave, and preferably, but
not necessarily equal to 500 Hz, 1000 Hz, 2000 Hz, or 4000 Hz.
[0025] The layer 7 of sound-absorbent material has instead a nominal thickness preferably,
but not necessarily comprised between 1 and 50 centimetres, and is made with a sound-absorbent
material having a nominal density preferably, but not necessarily comprised between
5 and 150 kg/m
3 (kilograms per cubic meter). Such sound-absorbent material further has a porosity
preferably, but not necessarily higher than 0.9; and/or a resistivity of the air flow
preferably, but not necessarily comprised between 1 and 100 KN/s/m
4; and/or an acoustic path greater than 1.
[0026] With reference to figures 2 and 3, the acoustic panel 1 is further preferably, but
not necessarily provided with an outer protective half-shell 8 substantially rigid,
which is shaped so as to be fitted on the body of the reverberating plate 6, over
the sound-absorbent material layer 7, so as to form an interspace which accommodates
and at the same time maintains the sound-absorbent material layer 7 abutting on the
stepped-profile surface 6a of the reverberating plate 6.
[0027] Furthermore, preferably, but not necessarily, in the illustrated example, the portion
of the protective half-shell 8 which is faced/aligned to the stepped-profile surface
6a of the reverberating plate 6, is appropriately pierced so as to make a series of
Helmholtz resonators along with the interspace which accommodates the layer 7 made
of sound-absorbent material.
[0028] With reference to figures 2 and 3, in the illustrated example, in particular, the
reverberating plate 6 has preferably, but not necessarily a normal thickness comprised
between 10 and 25 cm (centimetres) and is preferably, but not necessarily made of
cement, metal, marble or other compact high density material.
[0029] The shape of the stepped-profile surface 6a of the reverberating plate 6 is instead
preferably, but not necessarily optimized on the basis of the "Quadratic Residue"
mathematical model so as to be able to reflect two different incident acoustic waves
in "diffused" manner. The reference frequency or "band center" of the first incident
acoustic wave is preferably, but not necessarily equal to 1000 Hz (Hertz), while the
reference frequency or "band center" of the second incident acoustic wave is preferably,
but not necessarily equal to 2000 Hz (Hertz).
[0030] Furthermore, in the illustrated example, the reverberating plate 6 preferably, but
not necessarily consists of a series of modular reverberating boards or panels 9 of
preferably, but not necessarily elongated rectangular shape (two in the illustrated
example), which are fixed sideways to one another so as to form single, substantially
rigid, indeformable flat body 6. The front face of the reverberating boards or panels
9 is obviously stepped-profiled so to form the stepped-profile surface of the "Quadratic
Residue" mathematical model 6a on a same face of the flat body 6.
[0031] More in detail, with reference to figure 2, in the example shown, each reverberating
panel 9 preferably, but not necessarily consists of a containment basin or framework
10 of elongated regular shape, which has a bottom shaped so as to copy, at least in
part, the surface of the stepped-profile surface 6a of the reverberating plate 6,
and of a filling core 11, made of concrete, which completely fills the containment
basin or framework 10.
[0032] Preferably, but not necessarily, the reverberating panel 9 may further also comprise
a stiffening armature (not shown), either completely or partially embedded in the
filling core 11.
[0033] The containment basin or formwork 10 may be made either of plastic, metal or composite
material. In the first case, the containment basin or formwork 10 may be advantageously
made either by means of an injection molding procedure or by means of thermoforming
of a sheet of plastic material of suitable thickness. In the second case, instead,
the containment basin or formwork 10 may be advantageously made by means of a cold
molding procedure starting from a sheet of suitable thickness.
[0034] Obviously, the reverberating plate 6 may be also formed by only one reverberating
panel 9 made preferably, but not necessarily with the methods described above.
[0035] With reference to figures 2 and 3, the layer 7 of sound-absorbent material has instead
a thickness preferably, but not necessarily comprised between 3 and 15 centimetres,
and is made preferably, but not necessarily of open cell polyurethane foam with nominal
density preferably, but not necessarily comprised between 30 and 60 kg/m
3, or other cell material, preferably, but not necessarily open, with sound-absorbent
properties.
[0036] Alternatively, the sound-absorbent material layer 7 made also be made of mineral
fiber, either synthetic or natural, with nominal density preferably, but not necessarily
comprised between 15 and 45 kg/m
3.
[0037] With reference to figures 2 and 3, in the illustrated example, the protective half-shell
8 is instead preferably, but not necessarily made of metal material and essentially
consists of a rectangular basin 8 dimensioned to be fitted on the reverberating plate
6. Obviously, the protective half-shell 8 may be made of plastic or composite material.
[0038] The bottom of such a basin 8 is further provided with a multitude of through holes
so as to form a series of Helmholtz resonators when the basin 8 is coupled to the
reverberating plate 6.
[0039] The protective half-shell 8 may be advantageously made by means of a cold molding
procedure starting from a flat or fretted plate of suitable thickness.
[0040] Instead, as mentioned, the shape of the reverberating plate 6 with stepped-profile
surface 6a is determined on the basis of "Schroeder's" mathematical model, and in
the illustrated example consists of an elementary diffusion profile which is repeated
cyclically substantially along the entire face of the reverberating plate 6.
[0041] With reference to figures from 4 to 7, if dimensioned to reflect only one incident
acoustic wave with predetermined reference frequency or "band center" in "diffused"
manner, the steps which form the elementary diffusion profile have all the same width
and spatial distribution, which is determined directly by "Schroeder's" mathematical
model.
[0042] More in detail, according to "Schroeder's" mathematical model, in order to reflect
the sound in "diffused" manner, the profile of the surface must copy the mathematical
sequence QRS so as to obtain diffusers having diffraction lobes with the same energy,
operating with propagation waves of flat type. The mathematic sequence QRS is given
by the ratio:

where n is number of sequence of steps, and N is a prime number, the choice of which
is bound to the modularity of the panels, as described below.
[0043] The size of the "steps" (width w and height d
n) which form the various diffusers are determined by means of mathematical ratios:

and

where λ
min is the minimum design wavelength, and λ
0 is the maximum design wavelength (the two frequencies must not necessarily have the
same value).
[0044] Obviously, the lower the reference frequency or "band center", the higher will be
the overall size of the diffuser in terms of both length and thickness needed to reflect
the incident acoustic wave in "diffused" manner.
[0045] Thus, having chosen the reference frequency or "band center", and consequently the
corresponding minimum wavelength λ
min, and having fixed the maximum length L that the elementary diffusion profile must
have, the maximum number of steps n
s which form the elementary diffusion profile is obtained on the basic of the equation:

[0046] For determining the steps the prime number N closest to n
s is considered, and from this the sequence s
n is then determined by means of the first formula shown above.
[0047] If instead it must be dimensioned to reflect incident acoustic waves which have two
different reference frequencies or "band centers" (see figures 2 and 3) in "diffused"
manner, the steps which form the elementary diffusion profile generally have a mutually
different length, and the spatial distribution of the steps is determined by combining
to each other the two elementary diffusion profiles determined directly by "Schroeder's"
mathematical model with reference to the two required reference frequencies or "band
center".
[0048] More in detail, the elementary diffusion profile dimensioned to reflect incident
acoustic waves with two different reference frequencies or "band center" in "diffused"
manner may be obtained by combining the sequence of the widths of the steps formed
by "Schroeder's" mathematical model with reference to the first reference frequency
or "band center" with the sequence of distances or heights between the tops of the
various steps provided with "Schroeder's" mathematical model with reference to the
second reference frequency or "band center".
[0049] In other words, a single reference frequency or "band center" is fixed to determine
the width of the step (
w), and then the various heights of the steps are calculated according to the different
frequency values (
di). Alternatively, it is also possible to use a single reference frequency or "band
center" for calculating the sequence of the step heights (
d) and determine the different widths of the steps (
wi) according to different reference frequency or "band center" values.
[0050] In the illustrated example, in particular, having decided to maintain the width of
the reverberating panel 9 equal to 100 cm (centimeters), a maximum number of steps
equal to 6 result for each elementary diffusion profile "tuned" to a single reference
frequency or "band center", therefore the QRS sequence which is obtained (for N=7)
is the following: sn={0, 1, 4, 2, 2, 4, 1}.
[0051] Furthermore, in order to dimension the reverberating panel 9 to work in the typical
road and railway traffic frequency spectrum, and since the dimensional limit fixed
for the thickness of the reverberating plate 6 (for example 10 cm) cannot be exceeded,
a sequence of steps of variable width and fixed height has been chosen.
[0052] In the case of an elementary diffusion profile "tuned" onto two different reference
frequencies or "band centers", the same dimensional constraints require choosing a
number of steps equal to 12.
[0053] Figure 4, for example, shows an elementary diffusion profile optimized to reflect
the incident acoustic waves with reference frequency or "band center" equal to approximately
1000 Hz (Hertz) in "diffused" manner.
[0054] Such an elementary diffusion profile preferably, but not necessarily consists of
6 steps, each of which has a length l
1 equal to approximately 17 cm (centimeters). Consequently, the first elementary diffusion
profile has a total width l
0 preferably, but not necessarily equal to 102 cm (centimeters).
[0055] In this first elementary diffusion profile, the flat top of the first step a1 lays
on the reference plane P of the profile, while the flat top of the second step a2
is positioned behind (under) the reference plane P, at a distance d
2 from the flat top of the first step a1 preferably, but not necessarily equal to approximately
2.45 cm (centimeters). The flat top of the third step a3 is instead positioned in
front of (over) the reference plate P, at a distance d
3 from the flat top of the second step a2 preferably, but not necessarily equal to
approximately 9.8 cm (centimeters).
[0056] The flat top of the fourth step a4 is still positioned in front of the reference
plane P, but closer to the reference plane P than the flat top of the third step a3,
and is at a distance d
4 from the flat top of the fourth step a3 preferably, but not necessarily equal to
4.9 cm (centimeters).
[0057] The flat top of the fifth step a5 is still positioned in front of the reference plane
P, but closer to the reference plane P than the flat top of the fourth step a4, and
is at a distance d
5 from the flat top of the fourth step a4 preferably, but not necessarily equal to
4.9 cm (centimeters).
[0058] The flat top of the sixth and last step a6 is instead positioned behind the reference
plane P, at a distance d
6 from the flat top of the fifth step a5 preferably, but not necessarily equal to approximately
9.8 cm (centimetres).
[0059] In the case of an elementary diffusion profile optimized to reflect the acoustic
waves with frequency equal to 2000 Hz (Hertz) in "diffused" manner, the nominal length
11 of each step should be equal to approximately 9.5 cm (centimeters), while the total
length 10 of the diffusion profile should be equal to approximately 54 cm (centimeters).
[0060] With regards instead to the distance between the flat tops of the various steps,
the distance d
2 between the flat top of the second step a2 and the second flat of the first step
a1 should be equal to approximately 1.23 cm (centimeters); the distance d
3 between the flat top of the third step a3 and the flat top of the second step a2
should be equal to approximately 4.9 cm (centimeter); the distance d
4 between the flat top of the fourth step a4 and the flat top of the third step a3
should be equal to approximately 2.45 cm (centimeters); the distance d
5 between the flat top of the fifth step a5 and the flat top of the fourth step a4
should be equal to approximately 2.45 cm (centimeters); while the distance d
6 between the flat top of the sixth step a6 and the flat top of the fifth step a5 should
be equal to approximately 4.9 cm (centimeters).
[0061] More in general, the six-step elementary diffusion profile described above may be
used to reflect an incident acoustic wave with reference frequency or "band center"
different from 1000 Hz (Hertz) in "diffused" manner, taking the measure of decreasing
the nominal widths of the steps and the distances between the flat tops of the various
steps in manner reversely proportional to the ratio between the old reference frequency
or "band center" (1000 Hz) and the new reference frequency or "band center" of the
incident acoustic wave which is reflected in "diffused" manner, leaving substantially
unchanged the dimensional ratios between the various portions of the elementary six-step
diffusion profile.
[0062] Obviously, the elementary diffusion profile could have a number of steps higher than
six, providing that the nominal width of the steps and the distances between the various
steps comply with the "Quadratic Residue" mathematical model.
[0063] Figure 5, instead, shows a second elementary diffusion profile optimized to reflect
the incident acoustic waves with reference frequency or "band center" equal to approximately
1000 Hz (Hertz) in "diffused" manner, and with reference frequency or "band center"
equal to approximately 2000 Hz (Hertz).
[0064] Such a second elementary profile preferably, but not necessarily consists of 12 steps
of different length from each other, and has a total width f
0 preferably, but not necessarily equal to approximately 100.2 cm (centimeter).
[0065] In this second elementary diffusion profile, the flat top of the first step c1 has
a width f
1 equal to approximately 15.5 cm (centimeters) and lays on a reference plane P of the
profile, while the flat top of the second step c2 has a width f
2 equal to approximately 5.4 cm (centimeters) and is positioned in front (over) the
reference plane P, at a distance h
2 from the top of the first step c1 equal to approximately 1.23 cm (centimeters).
[0066] Instead, the flat top of the third step c3 has a width f3 equal to approximately
4.3 cm (centimeters) and lays behind (under) the reference plane P of the profile,
at a distance h
3 from the flat top of the second step c2 equal to approximately 4.9 cm (centimeters).
[0067] Furthermore, the flat top of the fourth step c4 has a width f
4 equal to approximately 3.4 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but closer to the reference plane P than the flat top of the
third step c3, at a distance h
4 from the flat top of the third step c3 equal to approximately 2.45 cm (centimeters).
[0068] Furthermore, the flat top of the fifth step c5 has a width f
5 equal to approximately 2.7 7 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but closer to the reference plane P than the flat top of the
fourth step c4, at a distance h
5 from the flat top of the fourth step c4 equal to approximately 2.45 cm (centimeters).
[0069] The flat top of the sixth step c6 has instead a width f
6 equal to approximately 2.1 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance h
6 from the flat top of the fifth step c5 equal to approximately 4.9 cm (centimeters).
[0070] The flat top of the seventh step c7 has instead a width f
7 equal to approximately 30.9 cm (centimeters) and lays substantially on the reference
plane P of the profile, at a distance h
7 from the flat top of the sixth step c6 equal to approximately 1.23 cm (centimeters).
[0071] The flat top of the eighth step c8 has instead a width f
8 equal to approximately 10.7 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance h
8 from the flat top of the seventh step c7 equal to approximately 1.23 cm (centimeters).
[0072] The flat top of the ninth step c9 has instead a width f
9 equal to approximately 8.6 cm (centimeters) and lays behind (under) the reference
plane P of the profile, at a distance h
9 from the flat top of the eighth step c8 equal to approximately 4.9 cm (centimeters).
[0073] Furthermore, the flat top of the tenth step c10 has a width f
10 equal to approximately 6.9 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but closer to the reference plane P than the flat top of the
ninth step c9, at a distance h
10 from the flat top of the ninth step c9 equal to approximately 2.45 cm (centimeters).
[0074] Instead, the flat top of the eleventh step c11 has a width f
11 equal to approximately 5.4 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but further from the reference plane P than the flat top of
the tenth step c10, at a distance h
11 from the flat top of the tenth step c10 equal to approximately 2.45 cm (centimeters).
[0075] Finally, the flat top of the twelfth step c12 has a width f
12 equal to approximately 4.3 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance h
12 from the flat top of the eleventh step c
11 equal to approximately 4.9 cm (centimeters).
[0076] Figure 6, instead, shows a third elementary diffusion profile optimized to reflect
the incident acoustic waves with reference frequency or "band center" equal to approximately
1000 Hz (Hertz) in "diffused" manner, and with reference frequency or "band center"
equal to approximately 2000 Hz (Hertz). Such a third elementary profile again consists
of 12 steps of mutually different length, and has a total width w
0 preferably, but not necessarily equal to approximately 100.2 cm (centimeters).
[0077] In this third elementary diffusion profile, the flat top of the first step e1 has
a width w
1 equal to approximately 30.9 cm (centimeters) and lays on a reference plane P of the
profile, while the flat top of the second step e2 has a width w
2 equal to approximately 10.7 cm (centimeters) and is positioned in front (over) the
reference plane P, at a distance k
2 from the flat top of the first step e1 equal to approximately 2.45 cm (centimeters).
[0078] The flat top of the third step e3 has instead a width
W3 equal to approximately 8.6 cm (centimeters) and lays behind (under) the reference
plane P of the profile, at a distance k
3 from the flat top of the second step e2 equal to approximately 9.8 cm (centimeters).
[0079] Furthermore, the flat top of the fourth step e4 has a width
W4 equal to approximately 6.9 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but closer to the reference plane P than the flat top of the
third step e3, at a distance k
4 from the flat top of the third step e3 equal to approximately 4.9 cm (centimeters).
[0080] Instead, the flat top of the fifth step e5 has a width w
5 equal to approximately 5.4 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but closer to the reference plane P than the flat top of the
fourth step w
4, at a distance k
5 from the flat top of the fourth step e4 equal to approximately 4.9 cm (centimeters).
[0081] The flat top of the sixth step e6 has instead a width w
6 equal to approximately 4.3 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance k
6 from the flat top of the fifth step e5 equal to approximately 9.8 cm (centimeters).
[0082] Instead, the flat top of the seventh step e7 has a width w
7 equal to approximately 15.5 cm (centimeters) and lays substantially on the reference
plane P of the profile, at a distance k
7 from the flat top of the sixth step e6 equal to approximately 2.45 cm (centimeters).
[0083] The flat top of the eighth step e8 has instead a width w
8 equal to approximately 5.4 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance k
8 from the flat top of the seventh step e7 equal to approximately 1.23 cm (centimeters).
[0084] Instead, the flat top of the ninth step e9 has a width w
9 equal to approximately 4.3 cm (centimeters) and lays behind (under) the reference
plane P of the profile, at a distance k
9 from the flat top of the eighth step e8 equal to approximately 4.9 cm (centimeters).
[0085] Instead, the flat top of the tenth step e10 has a width w
10 equal to approximately 3.4 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but closer to the reference plane P than the flat top of the
ninth step e9, at a distance k
10 from the flat top of the ninth step e9 equal to approximately 2.45 cm (centimeters).
[0086] Instead, the flat top of the eleventh step e
11 has a width w
11 equal to approximately 2.7 cm (centimeters) and lays behind (under) the reference
plane P of the profile, but further from the reference plane P than the flat top of
the tenth step e10, at a distance k
11 from the flat top of the tenth step e10 equal to approximately 2.45 cm (centimeters).
[0087] Finally, the flat top of the twelfth step e12 has a width w
12 equal to approximately 2.1 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance k
12 from the flat top of the eleventh step e11 equal to approximately 4.9 cm (centimeters).
[0088] Finally, figure 7 shows a fourth elementary diffusion profile optimized to reflect
the incident acoustic waves with reference frequency or "band center" equal to approximately
2000 Hz (Hertz) in "diffused" manner, and with reference frequency or "band center"
equal to approximately 4000 Hz (Hertz). Also this fourth elementary diffusion profile
consists of 12 steps which, in this case, have length alternatively equal to approximately
9 cm (centimeters) or approximately 4 cm (centimeters), and has a total length m
0 preferably, but not necessarily equal to approximately 78 cm (centimeters).
[0089] In this fourth elementary diffusion profile, the flat top of the first step b1 has
a width m
1 equal to approximately 9 cm (centimeters) and lays on a reference plane P of the
profile, while the flat top of the second step b2 has a width m
2 equal to approximately 4 cm (centimeters) and is positioned behind (under) the reference
plane P, at a distance g
2 from the top of the first step b1 equal to approximately 1.23 cm (centimeters).
[0090] The flat top of the third step b3 has a width m
3 equal to approximately 9 cm (centimeters) and lays behind (under) the reference plane
P of the profile, but closer to the reference plane P than the flat top of the second
step m2, at a distance g
3 from the flat top of the second step b2 equal to approximately 0.61 cm (centimeters).
[0091] Furthermore, the flat top of the fourth step b4 has a width m
4 equal to approximately 4 cm (centimeters) and lays behind (under) the reference plane
P of the profile, but closer to the reference plane P than the flat top of the third
step b3, at a distance g
4 from the flat top of the third step b3 equal to approximately 4.9 cm (centimeters).
[0092] Instead, the flat top of the fifth step b5 has a width m
5 equal to approximately 9 cm (centimeters) and lays behind (under) the reference plane
P of the profile, but closer to the reference plane P than the flat top of the fourth
step b4, at a distance g
5 from the flat top of the fourth step b4 equal to approximately 2.45 cm (centimeters).
[0093] Instead, the flat top of the sixth step b6 has a width m
6 equal to approximately 4 cm (centimeters) and lays behind (under) the reference plane
P of the profile, but more distant from the reference plane P than the flat top of
the fifth step b5, at a distance g
6 from the flat top of the fifth step b5 equal to approximately 2.45 cm (centimeters).
[0094] The flat top of the seventh step b7 has a width m
7 equal to approximately 9 cm (centimeters) and lays behind (under) the reference plane
P of the profile, but closer to the reference plane P than the flat top of the sixth
step b6, at a distance g
7 from the flat top of the sixth step b6 equal to approximately 1.23 cm (centimeters).
[0095] Instead, the flat top of the eighth step b8 has a width m
8 equal to approximately 4 cm (centimeters) and lays behind (under) the reference plane
P of the profile, but further from the reference plane P than the flat top of the
seventh step b7, at a distance g
8 from the flat top of the seventh step b7 equal to approximately 2.45 cm (centimeters).
[0096] Instead, the flat top of the ninth step b9 has a width m
9 equal to approximately 9 cm (centimeters) and lays behind (under) the reference plane
P of the profile, but further from the reference plane P than the flat top of the
eighth step b8, at a distance g
9 from the flat top of the eighth step g8 equal to approximately 1.23 cm (centimeters).
[0097] Instead, the flat top of the tenth step b10 has a width m
10 equal to approximately 4 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance g
10 from the flat top of the ninth step b9 equal to approximately 4.9 cm (centimeters).
[0098] The flat top of the eleventh step b11 has instead a width m
11 equal to approximately 9 cm (centimeters) and lays behind (under) the reference plane
P of the profile, at a distance g
11 from the flat top of the second step b10 equal to approximately 2.45 cm (centimeters).
[0099] Finally, the flat top of the twelfth step b12 has a width m
12 equal to approximately 4 cm (centimeters) and lays in front of (over) the reference
plane P of the profile, at a distance g
12 from the flat top of the eleventh step b11 equal to approximately 1.23 cm (centimeters).
[0100] The operation of the acoustic panel 1 may be easily inferred from the description
above, and thus does not require further explanations except for specifying that in
order to obstruct the propagation of the incident acoustic wave, the acoustic panel
1 must be arranged so that the stepped-profile surface 6a of the reverberating plate
6 faces the polluting acoustic source.
[0101] The acoustic concepts on which the "Quadratic Residue" or "Schroeder's" mathematical
model are based are extensively described in many scientific papers and publications
and do not therefore require further explanations.
[0103] Instead, with regards to the assembly of the acoustic panel 1, the reverberating
panel or panels 9 forming the reverberating plate 6 are suited to be made directly
on-site, by casting the concrete directly into the containment basins or formworks
10, where provided, after having positioned stiffening armatures inside the containment
basins or formworks 10.
[0104] The bottom of the various containment basins or formworks 10 is obviously shaped
so as to follow at least one part of the stepped-profile surface 6a of the reverberating
plate 6a. In other words, the shape of the bottom of the containment basins or formworks
10 consists of one of the elementary diffusion profiles described above, which is
cyclically repeated substantially along the entire bottom of the containment basins
or formworks 10.
[0105] After the concrete has completely hardened in the containment basins or formworks
10, forming the filling core 11, the construction of the acoustic panel 1 consists
in fixing, if needed, the reverberating panels 9 sideways with respect to one another
so as to form the reverberating plate 6; and then positioning the layer 7 of sound-absorbent
material on the resulting reverberating plate 6 to cover the respective surface with
a stepped-profile surface 6a.
[0106] The construction of the sound-absorbent panel 1 is then concluded by positioning
the protective half-shell 8 on the body of the reverberating plate 6, over the sound-absorbent
material layer 7, and subsequently anchoring the protective half-shell 8 onto the
body of the reverberating plate 6, so as to block and press the sound-absorbent material
layer 7 stably abutting onto the surface of with the stepped-profile surface 6a of
the reverberating plate 6.
[0107] Possibly, the construction of the acoustic panel 1 may also include removing the
containment basins or formworks 10 from the reverberating panel 9 before composing
the reverberating plate 6, or before positioning the sound-absorbent material layer
7 to cover the stepped-profile surface 6a of the reverberating plate 6.
[0108] In this case, the reverberating plate 6 will be formed by one or more filling cores
11 made of concrete, fixed sideways to one another.
[0109] There are many advantages deriving from the particular structure of the acoustic
panel 1.
[0110] Experimental tests have shown that the combined use of a reverberating plate 6 provided
with a stepped-profile surface 6a made according to the "Quadratic Residue" or "Schroeder's"
mathematical model and of a layer of sound-absorbent material 7 to cover the surface
of the stepped-profile surface 6a, allows to make acoustic panels 1 which have a shielding
capacity much higher than that of the acoustic panels of noise barriers currently
in use.
[0111] In other words, the synergetic effect between "diffused reflection with destructive
interference" implemented by the stepped-profile surface 6a and the systematic attenuation
of the sound-absorbent material layer 7 allows to block the propagation of acoustic
waves in a much more effective manner than the acoustic panels for noise barriers
currently in use.
[0112] Furthermore, by appropriately shaping the stepped-profile surface 6a of the reverberating
plate 6 it is possible to optimize the performance of the acoustic panel 1 and of
the noise barrier 2 according to the frequency spectrum of the acoustic waves emitted
by the polluting acoustic source to be shielded.
[0113] It is finally apparent that the construction of the reverberating panel 9 on-site
considerably reduces the installation costs of the noise barrier 2.
[0114] It is finally apparent that changes and variants can be made to the acoustic panel
1 and noise barrier 2 described and shown above without departing from the scope of
protection of the present invention.