The invention relates to a sound protection panel for a motor vehicle engine compartment and a method for producing such a panel.
Producing a sound protection panel for a motor vehicle engine compartment is known, for example from the document FR 3 024 675 A1, the panel comprising:
With such an arrangement, the shell therefore participates in the absorption of the sound waves.
However, it is observed that this absorption is not optimised in the medium-frequency domain, in particular between 500 and 1000 Hz.
When it is wished to optimise the medium-frequency absorption properties of a porous element—in this case the aforementioned shell—its known to clad it with a “resistive layer”, having resistance to the passage of air greater than that of the element in order to obtain a “bi-permeable” effect as described by J. F. Allard in the work “Sound propagation in porous media”, Elsevier, 2nd edition 2009, p. 266-271.
However, adding such a “resistive layer” makes producing the panel more complex and gives rise to an associated extra cost.
The aim of the invention is to overcome this drawback.
For this purpose, and according to a first aspect, the invention proposes a sound protection panel for a motor vehicle engine compartment, the panel comprising:
It is specified here that the use of the term “density” is a language shorthand signifying “volumetric mass density”; this is why a unit of measurement (kg/m3) is attached thereto.
It is well known that integral skinned polyurethane foams comprise a foam core of moderate density surrounded by a high-density skin of the same chemical nature, the core and the skin being produced in a single moulding operation.
As stated above, the skin corresponds to the proportion of thickness of foam that has a density greater than that of the core, on the understanding that, in reality, this density of skin increases gradually on moving towards the external surface.
The thickness of the skin is dependent in particular on the type of expansion agent used to form the foam, and also on the temperature and pressure conditions used in the mould.
When overall density of the shell is spoken of, the total volume thereof is considered in order to determine it, on the understanding that the shell comprises:
With the arrangement proposed, the shell has a core of uniform density that will play a conventional role of sound protection by absorption.
Since the shell is provided with a porous skin resulting from moulding, the role usually devolved to the “resistive layer” known from the prior art will be conferred on the skin provided with suitable permeability, on the front face of the shell.
In this way the addition of a “resistive layer” is dispensed with, the layer being formed by the skin that is integrated in the foam, which simplifies the production of the panel and reduces the manufacturing cost thereof.
It will furthermore be noted that the presence of a skin makes it possible to protect the panel against fluids such as water or oil to which it may be exposed, and to prevent—or at least to limit—the penetration of the fluids in the shell, which could then no longer fulfil its absorption role if it were impregnated therewith.
Finally, having a moulded panel makes it possible to very easily confer thereon a geometry making it possible best to match the shape of the engine element to be protected, and thus to limit acoustic leaks.
According to a second aspect, the invention proposes a method for manufacturing such a panel.
Other particularities and advantages of the invention will appear in the following description, made with reference to the accompanying FIGURE, which is a partial schematic view in cross section of a panel according to one embodiment.
With reference to the FIGURE, a sound protection panel 1 for a motor vehicle engine compartment is described, the panel comprising:
To facilitate measurement, a strip 9 is preferably taken in a substantially flat region, having for example dimensions 50×50 mm.
According to one embodiment, the shell 2 has a Young's modulus under compression of between 106 and 108 Pa.
In order to make such a measurement, a sample of shell 2 is taken by separating it from the spring layer 5, for example by water-jet cutting.
To facilitate the measurement, the sample is taken in a substantially flat region with a substantially constant thickness.
A shell 2 provided with such a Young's modulus has sufficient stiffness to avoid the appearance of a high-frequency resonance peak.
According to one embodiment, the core 7 of the shell 2 has relatively low a tortuousness—typically less than 1.8—making it possible to avoid, in the presence of the skin 8, saturation of the absorption in medium and high frequencies.
According to one embodiment, the shell 2 has a thickness—which may be variable—of between 3 and 30 mm, and in particular between 7 and 15 mm.
According to one embodiment, the shell 2 has an overall density of between 150 and 250 kg/m3.
With such a thickness combined with such an overall density, the shell 2 has a sufficient mass per unit surface area to make it effective as a mass in a mass-spring system in insulation.
According to one embodiment, the spring layer 5 has a Young's modulus under compression of between 104 and 2.105 Pa.
To make such a measurement, a sample of spring layer 5 is taken by separating it from the shell 2, for example by water-jet cutting.
According to one embodiment, the spring layer 5 has a density of between 40 and 120 kg/m3, and in particular between 70 and 90 kg/m3.
According to an embodiment that is not shown, the foam of the spring layer 5 is also an integral skinned foam, the external face 10 thereof being provided with a porous skin, in the same way as the front face 3 of the shell 2.
It is then possible to observe a phenomenon of sound absorption produced by the spring layer 5 with amplification of the absorption in medium frequencies related to the presence of the skin, as in the case of the shell 2, which can be very effective when the shell follows complex engine shapes.
According to one embodiment, the spring layer 5 has a thickness of between 10 and 40 mm.
In order to produce the shell 2 and the spring layer 5, the water serves as an expansion agent (the proportion of water in the foam precursor mixture of the shell 2 being one of the factors making it possible to adjust the overall density thereof), as well as the mould temperatures and the density obtained after moulding.
Finally, a method for producing such a sound protection panel 1 is described, the method comprising the following steps:
Number | Date | Country | Kind |
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1858538 | Sep 2018 | FR | national |
This application claims the benefit of International application number PCT/EP2019/075258, filed Sep. 19, 2019 and French application number 1858538, filed Sep. 20, 2018 the entire contents of which are incorporated herein by reference.
Filing Document | Filing Date | Country | Kind |
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PCT/EP2019/075258 | 9/19/2019 | WO | 00 |