This application is the U.S. National Stage of PCT/FR2018/052249, filed Sep. 13, 2018, which in turn claims priority to French patent application number 1758569 filed Sep. 15, 2017. The content of these applications are incorporated herein by reference in their entireties.
Glazing for transport vehicles (aircraft, trains, helicopters, boats, cars, etc.) and, in some cases, glazing for buildings may be provided with heating functions incorporated within the glazing for preventing/removing, as the case may be, condensation on the interior face or frost on the exterior face.
The heating is characterized by its specific power (W/m2), which is suited to the specific needs of each application.
The heating system consists either of wires embedded in the glazing or of transparent conductive layers (doped oxides: tin-doped indium oxide, or indium tin oxide: ITO; AZO (aluminum zinc oxide); SnO2:F; or metals such as silver or gold) allowing heating by Joule effect. In both cases, the heating system is supplied with power via electrodes at a voltage that is available in the vehicle or building. In the simple case of a rectangular glazing with a heating layer having a surface resistivity Rs, heated at the voltage U by two electrodes on two opposite sides separated by a distance D, the resulting specific power Ps is determined by the following equation:
Glasses with a heating layer are obtained either by cutting, and potentially shaping, a glass in which a layer is already present or by depositing the layer on a shaped glass later on (after cutting). The term “glass” is understood here preferably to mean any mineral glass, but a rigid transparent substrate made of polymer material, a typical example of which is poly(methyl methacrylate) (PMMA), is also possible.
Since it is not possible to uniformly heat a non-rectangular shape using a uniform electrically conductive layer, two strategies are implemented:
The use of glass with a pre-deposited conductive layer (deposited before cutting, and potentially before shaping/bending) is industrially and economically much more advantageous because it benefits from the scaling effects of production that is not specific to one glazing.
However, this is not possible in two quite common cases:
In glazing with a high specific power (the threshold being of the order of kW/m2), local overheating effects may lead to the glazing aging badly, or even to deterioration of the optical properties (through local creep of the intercalary adhesive in the laminated glazing) or local bubbling of this intercalary adhesive.
It is possible to overcome these two limitations by depositing the electrically conductive layer in a controlled manner so as:
Lastly, It is also possible to aid in the homogenization of the specific power by channeling the electric current in particular by ablating conductive layer lines using laser-based processes.
The object of the invention is therefore to use glasses with a uniform conductive layer (designed for solar control, low-e performance, motor vehicle heating, etc.) to obtain a desired specific power of heating that is uniform over the entire heating area, regardless of how complex its geometry is.
This object is achieved by the invention, the subject of which is therefore a laminated glazing consisting of a plurality of rigid transparent substrates that are bonded to one another pairwise via an intercalary adhesive layer, at least one of these transparent substrates being coated with an electrically conductive layer that is substantially uniform in nature and thickness, a zone of which has four edges opposing one another in pairs, first and second busbars being arranged along two opposite edges, characterized in that ablation lines of the electrically conductive layer close in on themselves while forming non-conductive strips, each occupying a major portion of the distance between the busbars, the shape of the non-conductive strips being capable of providing a temperature of heating by the electrically conductive layer that is virtually constant over the entire area of the zone.
The non-conductive strips relate of course to the flow of electric current.
The area that is complementary to that of the non-conductive strips defines the conductive strips (or zones), which constitute types of electrically conductive layer wires, the width and spacing of which are suitable for obtaining the desired specific power at the available supply voltage.
The selective ablation of layers allows adaption to the available supply voltage and allows the effects due to shape to be managed. Only a fraction of the area of the layer participates in the circulation of the current, thereby increasing the apparent resistivity. Additionally, this increase in apparent resistivity is accompanied by a channeling of the current, which allows complex shapes to be managed. The apparent conductivity is therefore decreased by allowing the electric current to flow through only a fraction of the layer.
Ablations or ablation lines may generally be designed for any shape.
The width of the non-conductive zones must be small enough (of the order of millimeters, depending on the specific power) not to result in optical haze on heating (the effect of a change in the refractive index of the intercalary adhesive in the laminated glazing with temperature). It is this same issue that governs the permissible spacing for wire-based heated glazing.
According to preferred features of the laminated glazing according to the invention:
The invention also relates to:
These applications are targeted in particular at an air, ground or water vehicle, in particular at an aircraft, and preferably as the front or side glazing of an aircraft cockpit.
The invention will be better understood in the light of the following description of the appended
With reference to
Ablation lines (9) of the electrically conductive layer (2) close in on themselves while forming non-conductive strips (11), each occupying a major portion of the distance between the busbars (7, 8). The area that is complementary to the non-conductive strips (11) in the zone (1) defines conductive strips (10).
Specific power: Ps=7000 W/m2
Surface resistivity: R squared=0.9 Ω/□
Supply voltage: U=40 V
Width: L=0.4 m
Maximum height H1=0.4 m
Minimum height H2=0.2 m
An abscissa x that goes from 0 at the maximum height H1 to 0.4 m at the minimum height H2 is defined. The height H at an abscissa x is
H(x)=H1+x/L·(H2−H1)
The width or pitch of the pattern is defined as the width of one conductive strip (10) and one non-conductive strip (11) that are adjacent to one another; the value of it here is e0=600 μm, i.e. 667 patterns.
The width of the conductive strip (10) depends on the position:
This gives the following numerical application:
busbar with L1=1 m and L2=1.5 m
distance between busbars H=1 m
specific power Ps=1000 W/m2 at U=100 V
layer with R squared=5 Ω/□
n=31 conductive strips:
The width of the pattern as defined above is dependent on the position h between the two busbars x0(h)=(L1+h/H(L2−L1))/n
The center of each conductive strip defines a straight line segment that forms an angle θ relative to the normal to the busbars.
The value of the width of the conductive strip is:
In this specific case, the width of the central conductive strip is 2.52 mm on the side of the short busbar (8) and 1.68 mm on the side of the long busbar (7).
The invention is thus particularly advantageous for vehicle heated glazing for which the electrical power supply is set, since it allows a desired specific power of heating to be established uniformly over the entire heating surface.
Number | Date | Country | Kind |
---|---|---|---|
1758569 | Sep 2017 | FR | national |
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/FR2018/052249 | 9/13/2018 | WO |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2019/053381 | 3/21/2019 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
2878357 | Thomson et al. | Mar 1959 | A |
20050178756 | Degand | Aug 2005 | A1 |
20130186875 | Lisinski | Jul 2013 | A1 |
20180299116 | Kramer | Oct 2018 | A1 |
Number | Date | Country |
---|---|---|
102004029164 | Dec 2005 | DE |
1 897 412 | Dec 2013 | EP |
3487720 | May 2021 | EP |
10-2008-0028890 | Apr 2008 | KR |
WO-2007045786 | Apr 2007 | WO |
WO-2016000927 | Jan 2016 | WO |
Entry |
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International Search Report as issued in International Patent Application No. PCT/FR2018/052249, dated Jan. 2, 2019. |
Notice of Preliminary Rejection as issued in Korean Patent Application No. 10-2020-7008936, dated Dec. 15, 2022. |
Number | Date | Country | |
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20200215797 A1 | Jul 2020 | US |