GRAPHENE-BASED NON-DESTRUCTIVE INSPECTION DEVICE AND RELATED METHOD
20180328895 ยท 2018-11-15
Inventors
- Antonio BRELATI (NOCERA INFERIORE (SA), IT)
- Rosario Del Giudice (Napoli, IT)
- Tommaso ROMANO (ROMA, IT)
Cpc classification
G01N29/2475
PHYSICS
Y02T50/50
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
B64F5/60
PERFORMING OPERATIONS; TRANSPORTING
G01N2291/0258
PHYSICS
G01N29/2431
PHYSICS
B64D2045/0085
PERFORMING OPERATIONS; TRANSPORTING
G01N29/07
PHYSICS
Y02T50/40
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
International classification
Abstract
Non-destructive inspection device, comprising: a first structural layer; a second structural layer coupled to the first structural layer; a chamber sealed between the first and second structural layers, containing a gas; and an active region, housed in the chamber, of a Graphene-based material. In a first operating condition, an AC electric current is fed to the active region and generates by thermoacoustic effect a first acoustic wave propagating away from the chamber. In a second operating condition, a second acoustic wave, generated by a reflection of the first acoustic wave, is received at the chamber and causes a variation in pressure and, consequently, a variation in the temperature of the gas contained in the chamber generating, by means of the thermoelectric effect, an electrical signal in the active region.
Claims
1. A non-destructive inspection device (30) for detecting flaws in a body in composite material (20), comprising: a first structural layer (2), having a first and a second surface (2a, 2b) opposite each other; a second structural layer (10) mechanically coupled to the first surface (2a) of the first structural layer (2); a sealed chamber (14), extending between the first and the second structural layer, containing a gas; and an active region (6), housed in the chamber (14), having a first and a second conduction terminal (7, 4a, 4b), and being made of one of the following materials: partially reduced graphene oxide, reduced graphene oxide, graphene, wherein said first and second conduction terminals (7, 4a, 4b) can be polarized, in a first operating condition, by an AC electric current so as to cause the thermoacoustic generation, by the active region (6), of a first acoustic wave (WE) propagating away from the chamber (14); wherein said chamber (14) is configured to receive, in a second operating condition, a second acoustic wave generated by a reflection of the first acoustic wave; and wherein said active region (6) is configured to generate, in the second operating condition and by thermoelectric effect, an electrical signal between the first and second conduction terminals of the active region (6).
2. The device according to claim 1, wherein the second structural layer (10) is mechanically coupled to said body made of composite material (20), wherein, said chamber (14) and said active region (6) are mutually arranged in such a way that, in the first operating condition, the first acoustic wave propagates towards the body in composite material (20), and wherein, in the second operating condition, the second acoustic wave, generated by the reflection of the first acoustic wave in the presence of a defect in the body in composite material (20), is received by said chamber (14); and wherein said chamber (14) and said active region (6) are mutually arranged in such a way that a pressure variation and, consequently, a temperature variation, in the gas contained in the chamber (14) generates, due to a thermoelectric effect, said electrical signal (i.sub.R) indicative of the presence of said defect.
3. The device according to claim 1, wherein both the first and the second structural layer (2, 10) are made of the same composite material as the body made of composite material (20).
4. The device according to claim 2, wherein said composite material includes carbon fibre in a resin matrix.
5. The device according to claim 1, wherein said active region (6) has a heat capacity per unit area, HCPUA, ranging from 10.sup.1 and 10.sup.2 J m.sup.2 K.sup.1.
6. The device according to claim 1, wherein the gas present in the chamber (14) is air or a noble gas.
7. The device according to claim 1, wherein the first and the second conduction terminals (7, 4a, 4b) are made of partially reduced graphene oxide.
8. The device according to claim 1, wherein the active region (6) and the first and the second conduction terminal (7, 4a, 4b) extend, without interruption, in the same layer of partially reduced graphene oxide, and wherein the electric resistivity value of the active region (6) is lower than the electric resistivity value of the first and the second conduction terminals (7, 4a, 4b).
9. The device according to claim 1, wherein the chamber (14) defines a volume having a base surface ranging from 1 cm.sup.2 to 100 cm.sup.2 and height ranging from 0.1 mm to 10 mm.
10. The device according to claim 1, wherein the chamber (14) is delimited internally by the respective surfaces of the first layer (2) and second layer (10), said active region (6) extending on the surface (2a) of the first layer (2) at a distance from the respective surface of the second layer (10).
11. The device as claimed in claim 1, comprising: a voltage generator (8) coupled to the first and second conduction terminals of the active region (6), operable to generate, in the first operating condition, an AC electric current between the first and second conduction terminals of the active region (6) so as to produce, by means of the thermoacoustic effect, said first acoustic wave (WE; and a current detector (9) coupled to the first and second conduction terminals of the active region (6), configured to detect, in the second operating condition, temporally following the first operating condition, an electrical signal (i.sub.R) between the first and second conduction terminals of the active region (6) and to generate in output a signal indicative of said electrical signal (i.sub.R).
12. An avionic structure provided with a body (20) in composite material, integrating a non-destructive inspection device (30) according to claim 1, wherein the second structural layer (10) of the non-destructive inspection device (30) is mechanically coupled to said body in composite material (20).
13. The avionic structure according to claim 12, wherein the second structural layer (10) and the body (20) extend one on the other without interruptions or regions of discontinuity.
14. The structure according to claim 12, selected from the group comprising: wing structure, fuselage, fin, rudder.
15. A means of transport comprising a structure according to claim 12.
16. The means of transport according to claim 15, selected from the group comprising: an aircraft, a helicopter, an unmanned aerial vehicle or UAV, terrestrial vehicles, naval vessels.
17. A method of manufacturing a non-destructive inspection device (30) for detecting flaws in a body in composite material (20), comprising the steps of: arranging a first structural layer (2), having a first and a second surface (2a, 2b) opposite each other; forming an active region (6) on the first surface (2a) of the first structural layer (2), the active region (6) having a first and a second conduction terminal (7, 4a, 4b), and being made of one of the following materials: partially reduced graphene oxide, reduced graphene oxide, graphene; mechanically coupling a second structural layer (10) to the first surface (2a) of the first layer (2) so as to form a sealed chamber (14), containing a gas, between the first and the second structural layer in the area of said active region (6).
18. The manufacturing method according to claim 17, further comprising the step of mechanically coupling the second structural layer (10) to said body made of composite material (20) to be inspected.
19. The manufacturing method according to claim 18, wherein both the first and the second structural layer (2, 10) are made of the same composite material as the body in composite material (20).
20. The manufacturing method according to claim 19, wherein said composite material includes carbon fibre in a resin matrix.
21. The manufacturing method according to claim 17, wherein said active region (6) has a heat capacity per unit area, HCPUA, ranging from 10.sup.1 to 10.sup.2 J m.sup.2 K.sup.1.
22. The manufacturing method according to claim 17, wherein the gas present in the chamber (14) is air or a noble gas.
23. The manufacturing method according to claim 17, wherein the step of forming the chamber (14) comprises forming locally an evaporating layer between the first and the second structural layer; and carrying out a heat treatment which causes evaporation of the evaporating layer, thus forming a buried region of gas which defines said chamber (14).
24. The manufacturing method according to claim 17, wherein the step of forming the chamber (14) comprises forming a depression in a selective region of the second structural layer (10) prior to the step of coupling the second structural layer (10) to the first surface (2a) of the first layer (2).
25. The manufacturing method according to claim 17, wherein forming the active region (6) includes: carrying out a first operation for reducing a layer of graphene oxide, forming partially reduced graphene oxide in the selective regions of the layer of graphene oxide in which formation of the active region (6) and the first and the second conduction terminal (7, 4a, 4b) is desired; and carrying out a second reduction operation in the selective regions of the layer of graphene oxide in which formation exclusively of the active region (6) is desired, so that the electric resistivity value of the active region (6) is lower than the electric resistivity value of the first and second conduction terminal (7, 4a, 4b).
26. A non-destructive inspection method, comprising the steps of: generating by thermoacoustic effect, in a first operating condition, by means of a non-destructive inspection device (30) according to claim 1, a first acoustic wave propagating away from the non-destructive inspection device (30); receiving, in a second operating condition, by means of the non-destructive inspection device (30) according to claim 1, a second acoustic wave generated by reflection of the first acoustic wave; and generating, by thermoelectric effect, by means of the non-destructive inspection device (30) according to claim 1, an electric signal indicative of the second acoustic wave.
27. The method of operation according to claim 26, wherein the step of generating the first acoustic wave includes supplying an AC electric current between the first and the second conduction terminal of the active region (6) of the non-destructive inspection device (30), and wherein the step of generating an electric signal indicative of the second acoustic wave includes causing a pressure variation and, consequently, a temperature variation, of the gas contained in the chamber (14) of the non-destructive inspection device (30).
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0018] For a better understanding of the present invention, preferred embodiments are described below, purely by way of non-limiting examples, with reference to the attached drawings, in particular:
[0019]
[0020]
[0021]
[0022]
[0023]
DETAILED DESCRIPTION OF THE INVENTION
[0024] According to the present invention, a non-destructive inspection device is provided (shown in its entirety in
[0025] In general, thermoacoustics studies the exchanges of energy in the presence of sound and is based on acoustic and thermodynamic principles. An acoustic wave carries mechanical energy (pressure gradient) and comprises a kinetic component (caused by the oscillatory motion of the propagation medium, for example a gas such as air) and a potential component (caused by local condensation of the propagation medium). Considered a gas for which the known equation PV=nRT is valid (where P is the pressure, V is the volume, n is the quantity of substance, R is the characteristic constant of the type of gas and T is the temperature) inducing a temperature gradient T according to a given function (e.g. sinusoidal law) in the adiabatic system condition, this induces a pressure variation P which will generate a corresponding acoustic wave. The effect is dual in the sense that, starting from an acoustic wave, a temperature gradient can be induced in a gas according to a given function (e.g. sinusoidal law).
[0026] Air (or a noble gas) heats up during condensation and cools down during a rarefaction. In the first case we talk about thermoacoustic engines systems that transform a flow of heat between a hot and a cold body into mechanical energy in the form of a sound wave. In the second case we speak of refrigeration systems that transform the mechanical energy of the sound wave to obtain a flow of heat from a cold to a warm body.
[0027] Thermoacoustic technology has numerous advantages, in particular it does not require moving parts (it is therefore free of problems of wear and friction), it is reliable, it exploits low-cost materials and production technologies, and is modular in the sense that it is possible to modulate the acoustic power emitted by acting on the amplitude of the oscillation of the electric excitation signal.
[0028] The non-destructive inspection device 30 according to the present invention can be integrated into a structural element of a means of transport, in particular parts of an aircraft made of composite material. In one embodiment, the non-destructive inspection device 30 comprises a transducer element, facing a chamber containing gas (e.g., air), which can be polarized to generate, in use, heat by the Joule effect. By thermoacoustic effect, as previously discussed, the temperature variation of the transducer element induces a variation of pressure in the chamber which the transducer element faces towards and, consequently, the generation of an acoustic wave.
[0029] In one embodiment, the transducer element includes a conductive layer of Graphene (ideally, pure Graphene), or partially reduced Graphene oxide (prGO). The conductive layer has a value of HCPUA Heat Capacity per Unit Area) chosen of an extremely low value, ideally close to that of a pure Graphene monolayer. The value C.sub.s of HCPUA of a Graphene monolayer (C.sub.s=dC.sub.p, where d is the thickness, is the density, and C.sub.p is the specific temperature) is about 5.8-10.sup.4 J m.sup.2 K.sup.1 (with d=0.335 nm, 2200 kg m.sup.3, C.sub.p790 kJ kg.sup.1 K.sup.1). The power produced by a thermoacoustic transducer depends on the incoming electrical power and is inversely proportional to the HCPUA value of the material used. Compared to platinum (with a HCPUA equal to about 2 J m.sup.2 K.sup.1), Graphene has a HCPUA value four orders of magnitude lower, thus ensuring a high gain of the device according to the present invention.
[0030] For the purposes of the present invention, the reduced graphene oxide conductive layer of the transducer element is designed to have a HCPUA value which falls within the range of values between 10.sup.1 and 10.sup.2 J m.sup.2 K.sup.1.
[0031] The term reduced graphene oxide, also known as rGO, means a layer of Graphene oxide (which in itself is an insulator and has a resistivity of at least 10.sup.12 m) which has been subjected to a reduction process with the aim of performing a removal of functional groups, such as hydroxyl (OH), carboxyl (COOH) and carbonyl (CO), which give it its high impedance. The reduction of the graphene oxide, or the removal of oxygen atoms from the structure, can be carried out by using reducing agents (hydrazine, dimethylhydrazine, hydroquinone, NaBH4), thermal methods and treatments with UV rays in the presence of TiO.sub.2. Pure Graphene (G) and Graphene Oxide (GO) have complementary physical and electrical properties, the former being an excellent electrical conductor (resistivity 10.sup.8 m) while the second is a perfect insulator (resistivity 10.sup.12 m).
[0032] The reduction process of Graphene oxide makes it possible to obtain a hybrid material (reduced Graphene oxide) with properties that can be modulated by varying the concentration of Oxygen, to obtain controlled intermediate characteristics, i.e. its resistivity can be regulated. A reduced Graphene oxide layer can therefore have a resistivity which is controlled as a function of the duration of the reduction process, reaching resistivity values of metallic conductive materials, or even lower.
[0033] As a result, according to the present description, the term partially reduced graphene oxide, also known as prGO, means a layer of Graphene oxide which, after the reduction process, has a resistivity lower than 10.sup.12 m and greater than 10.sup.8 m, for example between 10.sup.7 m and 10.sup.2 m.
[0034]
[0035] The first structural layer 2 has a first surface 2a and a second surface 2b) opposite each other along the axis Z. On, or at least partially integrated in, the first surface 2a a transducer element 4 extends, including an active layer region 6 of reduced Graphene Oxide having a HCPUA value which tends to the ideal value of a pure Graphene monolayer (in practice, with the currently available technologies, a value of HCPUA between 10.sup.1 and 10.sup.2 J m.sup.2 K.sup.1), and electrical contact regions 7, of reduced graphene oxide, electrically coupled to the active layer region 6. The resistivity value of the electrical contact regions 7 is chosen, for example, in the order of copper resistivity value.
[0036] The resistivity value of the active layer region 6 is lower than that of the electrical contact regions 7 and is obtained by carrying out a reduction process of the Graphene oxide for a longer time than that foreseen for the formation of the electrical contact regions 7.
[0037] The heat generated by feeding the electric current i to the active layer region 6 through the electrical contact regions 7, heats the gas in contact with the active layer region 6, generating a temperature gradient in the gas and, by thermoacoustic effect, sound waves propagating in a direction orthogonal to the first surface 2a (i.e. in the Z direction).
[0038] The transducer element 4 can be functionally coupled, by means of conductive strips 4a, 4b connected to the electrical contact regions 7, to conduction terminals of a voltage generator 8 configured to generate a potential difference V between the electrical contact regions 7 so as to cause, in use, the flow of an electric current i through the transducer element 4. The value of the voltage generated by the generator 8, as well as the current values i, depend on various factors, including the thickness of the active layer region 6, the resistivity value of the active layer region 6 and the thickness of the structure under inspection. The generator 8 can be made integrated in the structural portion 1 and be part of the device 30 according to the present invention, or it can be an element external to the device according to the present invention.
[0039] In an exemplary embodiment, the active layer region 6 has a thickness along Z, for example between 50 m and 150 m, and shape, on the XY plane, quadrangular, for example square. The size of the area (on the XY plane) of the active layer region 6 is chosen according to the specific application. Possible values for the area (on the XY plane) of the active layer region 6 are in the 1 cm.sup.2 to 100 cm.sup.2 range for aerospace applications.
[0040] According to an aspect of the present invention, the transducer element 4 is formed of a thin, Graphene (prGO)-based layer wherein, in one embodiment, the electrical contact regions 7 are made of partially reduced Graphene oxide (prGO) having resistivity of the same order of magnitude as that of the active layer region 6. The reduction process of the Graphene oxide layer, per se known, can be modulated and makes it possible to obtain, by using suitable masks and starting from a layer of Graphene oxide, a resulting layer formed of a plurality of contiguous regions having respective electrical and thermal properties which tend towards those of pure Graphene the further one proceeds with the reduction process in correspondence with non-masked regions.
[0041] One of the main methods for reducing graphene oxide provides, as better illustrated below, for a chemical reduction procedure with hydrazine monohydrate. Alternatively, or together with the use of hydrazine, it is also possible to use hydroquinone, sodium boron hydride and vitamin C.
[0042] The conductive strips 4a, 4b, to which the conduction terminals of the generator 8 are electrically coupled, extend prolonging the electrical contact regions 7 and therefore may also be realized by reducing a layer of Graphene oxide, and having the same conductive characteristics of the electrical contact regions 7.
[0043] It is evident that it is possible to electrically couple together a plurality of transducer elements of the type shown in
[0044] Therefore, on the basis of the foregoing, it is evident that the transducer element 4 does not have structural criticalities due to joints between the active region 6 and the contact regions 7, and can therefore be used in applications requiring a high degree of structural strength, such as aeronautical and avionic applications.
[0045]
[0046] In the chamber 14, a gas (e.g., air) is in thermal contact with the transducer element 4. During use, when the electrical signal is applied to the transducer element 4 by the voltage generator 8, a sound wave WE is generated by thermoelectric effect, whose variation in time is a function of the electric signal applied to the active layer region 6 (i.e., the variation of the electrical signal supplied to the active layer region 6 involves a corresponding variation of the acoustic wave emitted).
[0047] The acoustic wave thus generated propagates along the direction Z away from the active layer region 6.
[0048] In an embodiment of the present invention, the second structural layer 10 is an integral part of a thick, or bulk, structural region 20, formed of a plurality of superposed layers of composite material, bonded together by resin, in the manner in itself known (e.g., a structural region in carbon fibre). In this case, the second structural layer 10 and the thick structural region 20 extend seamlessly on each other, i.e. without interruptions or regions of discontinuity. In a different embodiment, an intermediate acoustic coupling layer may be present.
[0049] As previously discussed, carbon fibre structures may have manufacturing defects such as delamination, inclusions, porosity, voids and internal wrinkles.
[0050] The acoustic wave generated by thermoacoustic effect, propagating along the Z direction away from the active layer region 6 (in the positive direction of the Z axis), can undergo a series of reflections depending on the structural discontinuities present along the Z direction. In other words, the acoustic wave emitted, striking surfaces of regions of discontinuity between materials having different acoustic impedances (due for example to the different density), is reflected with the consequent generation of an acoustic echo wave which is indicative of structural defects in the thick structural region 20 (see
[0051] A reflected acoustic wave W.sub.R propagates along the direction Z towards the transducer element 4 and in particular towards the chamber 14. The reflected acoustic wave, impacting on the gas molecules present in the chamber 14, generates a pressure variation inside the chamber 14 and, consequently, determines, in the gas, a temperature gradient which is a function of the amplitude of the reflected acoustic wave. The temperature variation of the gas in the chamber 14 causes a heating of the active layer region 6. This heat variation of the active layer region 6 causes the generation of an electric current i.sub.R (or, similarly, a voltage) at the ends of the conductive strips 4a, 4b which is proportional to the amplitude of the reflected acoustic wave and whose variation in time is a function of the variation in time of the reflected acoustic wave. In other words, the electric current i.sub.R induced in the active layer region 6 has a temporal variation that reflects the temporal variation of the reflected acoustic wave.
[0052] A current and/or voltage detector 9 (illustrated by way of example in
[0053] A subsequent analysis of the time variation of the electric current i.sub.R thus detected makes it possible to acquire information relative to the reflected acoustic wave and, consequently, relative to the defect that generated the reflected acoustic wave. Such processing of data is not the subject of the present invention.
[0054] The current detector 9 can be made in an integrated form in the structural portion 1 and be part of the device 30 according to the present invention, or it can be an element external to the device according to the present invention.
[0055] The first structural layer 2, the transducer element 4, the second structural layer 10, and the chamber 14 (defined between the first structural layer 2 and the second structural layer 10) form, together, the non-destructive inspection device 30.
[0056] The phases of emission of the acoustic wave transmitted and of reception of the reflected acoustic wave alternate so that the non-destructive inspection device 30 operates alternatively as emitter of an acoustic wave and as receiver of an acoustic wave, in respective time windows of transmission and reception alternating with each other.
[0057] Thus, according to an aspect of the present invention, the transducer element 4, during the emission phase, is supplied with an electric current i of the alternating type (AC current, e.g. sinusoidal or square or pulse wave), and frequency f included in the range of 3.5 MHz to 7 MHz; this way the active layer region 6 is heated and cooled following the same law of variation as the electrical signal i, generating a temperature gradient between the gas molecules in contact (or close) to the active layer region 6 and those further away (along the Z direction) from the active layer region 6. The gas condenses and expands according to the variation defined by the electrical signal i, generating a pressure gradient and thus an acoustic wave in phase with the electrical signal i.
[0058] In the receiving phase, the transducer element 4 is not electrically powered, and the reflected acoustic wave penetrates into the gas present in the chamber 14 giving rise to a pressure gradient and thus to a temperature gradient between the molecules of said gas. The active layer region 6 heats up and cools as a function of the variation of the reflected acoustic wave, to which by thermoelectric effect, the generation of an electric current corresponds, making it possible to determine the presence of a defect in the structure and its position. In fact, the time delay between the emission of the acoustic wave and the reception of the corresponding reflected wave is indicative (proportional) of (to) the distance of the defect from the transducer element 4. The amplitude of the reflected wave can be used to provide a measure of the geometric dimension and an indication of the type of defect, estimated by comparing the amplitude of the signal obtained with that of a known reflector used as a reference.
[0059] It is preferable for the transducer element 4 to operate in resonance conditions. To such purpose, it is recommended that the descent phase of the electric signal i supplied to the active layer region 6 corresponds to the maximum value of the acoustic wave emitted (maximum expansion of the gas in the chamber 14: gas heating phase), and vice versa (i.e. that the ascent phase of the electric signal i corresponds to the maximum compression of the gas in the chamber 14: gas cooling phase).
[0060] With reference to
[0061] With reference to
[0062] Conversely, with reference to
[0063] So, in
[0064] The depth d.sub.def (along the direction of propagation of the acoustic wave, e.g. along Z) of the defect/discontinuity can be obtained using the formula:
d.sub.def=V.Math.t/2
where V is the speed of sound propagation in the material considered and t is the travel time of the acoustic wave (approximable as the time elapsed between the instant t.sub.1 of electrical signal generation I.sub.imp and the instant t.sub.def.sub._.sub.rx of acquisition of the electric signal I.sub.def.sub._.sub.rx).
[0065] The manufacturing steps of the non-destructive inspection device 30 are illustrated here. Explicit reference will be made to a method for the fabrication of a structural component, in particular of an aircraft, without thereby foregoing its generic nature.
[0066] First of all, one or more layers (or sheets) of Graphene oxide are prepared, with a thickness of between 50 m and 150 m, for example. The planar extension of a single layer/sheet varies according to the manufacturer and sheets with dimensions from a few centimetres to several meters are generally available. Solutions in liquid form are also available.
[0067] Then, a step of gluing said sheets of Graphene oxide onto the first structural layer 2 is carried out. For example, the graphene oxide sheets may be made to adhere to respective portions of the first structural layer 2 by means of an interface layer made from an adhesive or glue or resin. A subsequent heat treatment step permits the solidification of the interface layer and optimization of the adhesion.
[0068] Then, a respective mask is formed on the graphene oxide sheets so as to leave bare surface regions of the same at which to reduce the electrical resistivity value, and to generate conductive regions (in particular, the active layer region 6, the electrical contact regions 7, and the conductive strips 4a, 4b, as previously described). The techniques that can be used for the formation of the mask, necessary for the selective processing of surface portions, depend on the size and specific application; for example, known masking processes for chemical milling can be used.
[0069] Then, the first structural layer 2 provided with the graphene oxide layer on which the mask extends is placed in a reaction chamber in which hydrazine is fed. Since the reduction of the graphene oxide is greater the longer the hydrazine reaction lasts, by monitoring the reaction time between the hydrazine and the graphene oxide layers (in the non-masked regions) it is possible to interrupt the reduction process when the desired conductive characteristics have been achieved.
[0070] For example, using a hydrazine solution with a reaction time of 48 hours, the resistivity of a layer of Graphene oxide of about 10 m thickness is reduced by three orders of magnitude, from about 10.sup.12 m to 10.sup.9 m. The Applicant has verified that a reduction process of graphene oxide with hydrazine carried out for a time equal to 48 hours is able to modify the electrical characteristics of the layer which from a perfect insulator (characteristic VI constant with V in the range [5V; +5V], and I<1 pA) becomes an ohmic material (characteristic VI linear with V in the range [5V; +5V], I in the range [6 nA; +6 nA]). This aspect is particularly important for the purposes according to the present invention, since it proves that the reduction of resistivity a Graphene oxide layer is a function of the hydrazine exposure time (increasing the exposure time reduces the resistivity). It is thus possible to first adjust the resistivity value of the electrical contact regions 7 to the desired value.
[0071] Then, a masking step is performed of the newly formed electrical contact regions 7, leaving the reduced graphene oxide portions, in which the active layer region 6 is to be formed, exposed. By performing a new reduction process, it is possible to further reduce the resistivity of the exposed regions, reaching the desired value (depending on the desired HCPUA value).
[0072] Lastly, the first structural layer 2, provided with the reduced graphene oxide sheets, is removed from the reaction chamber and the masks present are removed. The transducer element 4 is thus obtained.
[0073] For the creation of the chamber 14, it is possible to proceed in various ways.
[0074] In a first embodiment, it is possible to generate local depressions of the second structural layer 10 by techniques which provide for the formation of air bubbles by creating cavities between two successive sheets by a pressure shaping between the two successive layers and/or by local insertion of a separating material which prevents the complete adhesion and compacting of the layers. Then, the first structural layer 2 is laid on the second structural layer 10, so that the transducer element 4 (and in particular the active layer region 2) is directly facing the depression made in the second layer structural 10.
[0075] In a second embodiment, a thin layer (film) of highly reflective ultrasonic material (e.g., 1 cm1 cm in size) inside a transparent, semi-permanent epoxy separation material, for composite materials and polyester resins, solvent-based, which polymerises with moisture (also known as Frerotte), and placing the pile thus formed between two successive layers of layers of composite material (e.g., carbon fibre) or, in the context of the present invention, between the structural layer 2 and the structural layer 10.
[0076] During a polymerization phase (e.g. in an autoclave), the structure thus formed undergoing specific pressure (between 1 bar and 6 bar) and temperature conditions (between 0 and 180 C.), the creation of a cushioning layer of gas is facilitated due to the evaporation of the separation material and consequent localised detachment between the structural layer 2 and the structural layer 10. The chamber 14 is thus formed.
[0077] According to an aspect of the present invention, the chamber 14 has a volume approximable to a cylindrical or truncated cone shape defined by lower and upper surfaces of an area comprised between 1 cm.sup.2 and 100 cm.sup.2 and a height between 0.1 mm and 10 mm. These dimensions are functions of the surface and of the thickness of the part or structure to be inspected, in general they are determined considering values of at least 2 orders of magnitude smaller.
[0078] It is evident that it is possible to use other materials which, when subjected to a thermal process, evaporate causing the formation of a pocket of buried gas which forms the chamber 14.
[0079] The structural component considered, provided with one or more non-destructive inspection devices manufactured as described above, can then be subjected to the remaining manufacturing steps, such as for example painting on the second surface 1b of the first structural layer 2.
[0080] As previously mentioned, alternatively to the use of hydrazine, or in addition to it, sodium boron hydride NaBH.sub.4 can be used for the reduction of the graphene oxide. Other reducing agents used are, for example, gaseous hydrogen, hydroquinones and strong alkaline solutions.
[0081] Other known methods for the reduction of Graphene oxide include high temperature heat treatment (typically, about 1000 C.); however, a heat treatment at such high temperatures could compromise the structural solidity of the components which the oxide layer has been glued to, as well as the functionality of the adhesive or glue interface layer.
[0082] According to a different embodiment of the present invention, it is possible to perform a negative process, i.e. a process in which unmasked areas of graphene sheets are oxidized to bring them into an electrical insulating condition. In this case, the process starts from sheets of graphene (an excellent electrical conductor) which are coupled to the avionic structure to form respective layers of Graphene. Then, a partial oxidation of such layers of Graphene is carried out (masking the active layer regions 6) until a desired electrical resistivity value is obtained for the electrical contact regions 7 and for the conductive strips 4a, 4b, forming controlled resistivity regions of partially oxidized Graphene (also known as poG). Oxidation is carried out by bathing in an aqueous solution rich in oxidizing agents.
[0083] Thus, according to an embodiment of the present invention, the first structural layer 2 is the outermost layer (or one of the outermost layers) of a structural component of an aircraft, such as a fuselage portion or a wing portion, or other, made of composite material. The second structural layer 10, together with the thick structural region 20 belong, instead to the remaining part of the structural component of the aircraft, and substantially define the thickness of the structural component considered. In other words, any defects not detectable by visual inspection extend exclusively in the thick structural region 20. By forming a plurality of transducer elements 4, each provided with its own chamber 14, facing towards the thick structural region 20 (i.e., suitable to emit respective acoustic waves towards the thickness of the thick structural region 20), it is possible to verify, both during the phases of testing and assembly and during the entire operating life of the aircraft, the presence of pre-existing or newly generated defects, thus adding considerably to the relative structural safety.
[0084] With reference to
[0085] The transducer elements 4 may extend to form a matrix, or grid, or curvilinear, or spoke patterns, or others yet, as needed.
[0086] Regardless of the number of transducer elements 4 integrated into the structure considered, the voltage generator 8 is configured to polarise each active layer region 6 at working voltages, e.g. between 0.5 V and +0.5 V, generating a power that falls in the range 10 dB and 50 dB to allow the inspection of a structure with a thickness of the order of 1 cm up to 5 cm.
[0087] For example, in the case of avionics applications, the on-board power supply is used, typically of a variable value in the range between 24 V and 48 V in direct current (DC). In this case, it is advisable to have a DC-AC converter of the reduction, or buck type 32, between the voltage generator 8 and the transducer elements 4. The choice of the voltage value supplied to the transducer elements 4 is, specifically, a function of the thickness of the active layer region 6 and of the resistivity of the active layer region 6, as well as, as said, of the thickness of the avionic part or structure to be inspected. As a result, transducer elements 4 arranged at different portions of the same aircraft could be supplied with voltages/currents of different values, according to local conditions.
[0088] From what has been described, it is evident that the present invention represents a significant evolution with respect to what is reported in the literature and known in the prior art.
[0089] The graphene oxide layer, which is selectively reduced at specific portions thereof, has characteristics of lightness, strength, flexibility and reliability, with controlled electrical conductivity. The same advantages are conferred by the use of a dual layer of pure graphene subsequently oxidized. Graphene sheets with a thickness of a few tens of micrometres, as well as its derivatives (prGO, poG), are extremely resistant and have excellent elastic and flexible properties, and do not impact the thickness or structural solidity of the structure which they are integrated in. It is therefore ideal for the construction of non-destructive test instruments in the aeronautic field.
[0090] Moreover, the integration achievable according to the present invention makes it possible to perform non-destructive structural tests during the entire working life of the aircraft which can be performed not only in the laboratory during the manufacture of the parts, but also after the assembly of the aircraft and for parts whose surface is not accessible from the outside since the instrumentation probes are integrated on the surface of the individual parts making up the aircraft. The present invention also offers advantages of reliability (high fidelity probes), compactness and low cost.
[0091] Lastly, it is clear that modifications and variants may be made to the invention described and illustrated herein while remaining within the protective scope of the present invention, as defined by the appended claims.
[0092] The non-destructive inspection device 30 previously described can be formed on a structural element different from a layer of composite material. For example, the layer 2 and layer 10 may be made of metal (e.g. aluminium), or semiconductor material (e.g., silicon).
[0093] Moreover, the non-destructive inspection device 30, having a chamber 14 defined between the two structural layers 2, 10 and housing the transducer element 4, can be used in different fields from those previously discussed in detail. For example, it may not be integrated into a vehicle structure or avionic structure, but be used in ocean probes, in devices for the ultrasound detection of hazardous material (e.g. for the detection of mines), for sonar systems or for the realization of biomedical instrumentation.
[0094] To summarize, the present disclosure describes a manufacturing method of a non-destructive inspection device, and the device itself, for the application of non-destructive ultrasound tests on composite materials used in aeronautics. Important aspects of the device concern, in a non-limiting embodiment, the presence of a network of micro probes integrated in the structure of the composite material to be analysed. A matrix of acoustic micro probes integrated in the material, makes it possible to overcome all the limitations of the prior art, also guaranteeing: better performance in resolution, smaller probes and therefore ability to detect smaller defects; better performance in terms of time and costs, no expert operator is required and the test time does not depend on the surface; the processing of the signals acquired by the micro probes takes place in parallel and not in sequence, as in the case of external probes according to the prior art; it is possible to extend the tests also to post-assembly phases, even if the surface is not accessible from the outside. Furthermore, the weight of the structure to be inspected is not increased significantly.
[0095] As regards the manufacturing process, the proposed solution provides for the manufacturing of the inspection device at the same time as the manufacture (autoclave, bonding, laying of carbon fibres, etc.) of the composite material (carbon ply multilayer) used as raw material for the aeronautical structures. The steps needed for the construction of the inspection device are a certain combination of the processing methods of the Graphene (reduction/oxidation) combined with some aeronautical processes (masking, bonding) and characteristic of the silicon electronics (selective doping of portions of layer of the same material to create conductive, insulating and resistive sections).
[0096] The requirements for use in aeronautical structures are guaranteed, in particular: homogeneity of the structure for safety requirements related to compactness and robustness; the conductive layer, the insulating layer and the sensor layer are all made Graphene hybrids (the limits of the prior art which required the use of non-homogeneous metals and oxides, which cannot be integrated are thus overcome); homogeneity of the structure for detection resolution requirements, limiting the generation of false positives; fabrication contextual to the processing of the composite material of the structure to be inspected (the probe cannot be inserted after the construction of the material).
[0097] As for the non-destructive inspection procedure, it is to be noted that the non-destructive test is not necessarily carried out in the laboratory, but can also be performed on a built aircraft, and is therefore also extendable to the periodic revision and testing of aircraft; the test can also be performed with an aircraft in flight, for an online diagnosis; the test is performed without the aid of a certified operator, so that it is not affected by possible human errors; the test is performed with a significant reduction in time and costs, because the execution is automatic and takes place with a matrix of probes with parallel processing; the test can also be performed on non-flat surfaces without the aid of additional interfaces; the test is more reliable since algorithms for filtering false positives due to second trace echoes can be used.