ROOM TEMPERATURE METHOD FOR THE PRODUCTION OF ELECTROTECHNICAL THIN LAYERS, AND A THIN LAYER SEQUENCE OBTAINED FOLLOWING SAID METHOD

Abstract

A method of forming PV layers in which, during the curing process, an additional reaction accelerates and improves curing. In a particularly advantageous embodiment, a double layer sequence having a plastic matrix in which continuous metal particles and, in the upper layer, alkaline-solubilised siloxane portions and metal particles are provided, allows, by means of combined definitive curing during the alkaline-solubilisation, the production of a PV layer sequence with which industrial waste heat/long-wave IR radiation can be utilised photovoltaically. The active exploitation of industrial waste heat/heat/body heat offers clear, financially-viable advantages in a great number of fields.

Claims

1. A room temperature process for producing electrotechnical thin layers, wherein electrically conducting and/or semiconducting inorganic agglomerates are areally provided in a dispersion and hardened to afford a layer, wherein the hardening is performed at room temperature and the hardening is accelerated by exposure to at least one reagent.

2. The process as claimed in in claim 1, wherein a PV layer sequence is formed.

3. The process as claimed in in claim 1, wherein as at least one base layer a layer is applied which comprises at least one metal or a metal compound, wherein the at least one metal or its compound is selected from the group consisting of steel, zinc, tin, silver, copper, aluminum, nickel, lead, iron.

4. The process as claimed in in that in claim 1, wherein as a conductive base layer at least one metallic conductive and/or semiconducting layer is applied and at least partially hardened.

5. The process as claimed in in claim 1, wherein as a carrier an areally extending material web is used, the material web consisting of at least one material selected from the material group consisting of glass, plastic, polycarbonate, plastics film, metal alloy, motor block alloy, heat exchanger tube alloy, heat exchanger alloy, heat exchanger soldering alloy, ceramic, industrial ceramic, natural stone, marble, clay ceramic, roof tile ceramic, laminate wood material, floorboard material, aluminum, stairway aluminum alloy, platinum composites, integrated circuit housing material, processor housing compounds.

6. The process as claimed in claim 1, wherein the inorganic agglomerates of a first layer are metals or metal compounds distributed in a plastics matrix, the metal type of the metals or metal compounds selected from the group consisting of beryllium, boron, aluminum, gallium, indium, silicon, germanium, tin, lead, arsenic, antimony, selenium, tellurium, copper, silver, gold, zinc, iron, chromium, manganese, titanium, zirconium.

7. The process as claimed in claim 1, wherein the inorganic agglomerates of a second layer are metals or metal compounds, which are arranged distributed in an at least partially inorganic matrix, wherein the metal type of the metals or metal compounds is selected from the group consisting of beryllium, boron, aluminum, gallium, indium, silicon, germanium, tin, lead, arsenic, antimony, selenium, tellurium, copper, silver, gold, zinc, iron, chromium, manganese, titanium, zirconium.

8. The process as claimed in claim 1, wherein a layer, as an inorganic matrix, a matrix is used which comprises as the glasslike oxidic matrix at least one chain forming or modifying element, the element selected from the group consisting of boron, phosphorous, silicon, arsenic, sulfur, selenium, tellurium, carbon in amorphous form, carbon in the graphite modification, carbon in the form of carbon nanotubes, carbon in the form of multiwalled carbon nanotubes, carbon in the form of Buckminster fullerenes, calcium, sodium, aluminum, lead, magnesium, barium, potassium, manganese, zinc, tin, antimony, cerium, zirconium, titanium, strontium, lanthanum, thorium, yttrium, fluorine, chlorine, bromine, iodine.

9. The process as claimed in claim 1, wherein an electrically conductive electrode layer is applied atop a carrier, metals or metal compounds distributed in a plastics matrix are applied atop the electrode layer as inorganic agglomerates in a first layer, a second layer of inorganic metallic agglomerates in an at least partially strongly basic or strongly acidic oxidic matrix are applied atop the first layer, wherein during application and hardening the metallic agglomerates react with the strongly acidic or basic matrix, wherein in turn the matrix also reacts with metallic agglomerates of the first layer, during hardening and reacting a photovoltaically active junction is formed, the second layer is provided with a transparent covering electrode and/or a contact electrode and the photovoltaically active layer sequence is suitably contacted and weld-wrapped as a PV layer sequence.

10. An electrotechnical thin layer sequence obtained as a PV layer sequence as claimed in claim 1, wherein the thin layer sequence comprises: a glass carrier, an electrode layer applied atop the glass carrier, comprising silver, a first layer applied atop the electrode layer which comprises aluminum particles in a plastics matrix, a second layer applied atop the first layer which comprises as an at least partially basic, glasslike layer at least silicon-oxygen bridges in a glasslike network and further comprises at least partially base-solubilized aluminum particles as inorganic agglomerates, and a transparent covering electrode applied atop the second layer and having contact electrodes, wherein in turn the thus prepared PV layer sequence exhibits a photovoltaic effect in the long wave and extreme long wave infrared range.

Description

BRIEF DESCRIPTION OF THE FIGURES

[0027] The figures elucidate with reference to in-principle sketches . . . .

[0028] FIG. 1 SEM plan view of a PV double layer comprising on the top side a plastics matrix comprising a siloxane fraction and Al flakes carried and partially solubilized therein applied and hardened atop a pure pre-hardened plastics matrix comprising the same Al flakes;

[0029] FIG. 2 magnified section of the SEM image according to FIG. 1;

[0030] FIG. 3 SEM image of the bottom side of a PV double layer according to FIGS. 1 and 2;

[0031] FIG. 4a measurement of the photovoltaic tappable potential from a PV double layer which could be generated merely by hot water placed to surround a PV double layer as a function of the temperature of the water/the cell falling from 46 C. to 31 C. with illustration of start value, variation and respective end value.

[0032] FIG. 4b light absorption maxima of H2O in the air as a function of the wavelength according to the prior art provided for elucidation of the behavior illustrated in FIG. 4.

DETAILED ELUCIDATION OF THE INVENTION BY REFERENCE TO EXEMPLARY EMBODIMENTS

[0033] In an advantageous embodiment an electrotechnical thin layer sequence obtained as a PV layer sequence by the process according to the invention, is characterized in that the thin layer sequence [0034] comprises a glass carrier, [0035] comprises an electrode layer applied atop the glass carrier comprising silver, [0036] comprises a first layer applied atop the electrode layer which comprises aluminum particles in a plastics matrix, [0037] comprises a second layer applied atop the first layer which comprises as an at least partially basic, glasslike layer at least silicon-oxygen bridges in a glasslike network and further comprises at least partially base-solubilized aluminum particles as inorganic agglomerates, [0038] comprises a transparent covering electrode applied atop the second layer and having contact electrodes, wherein in turn [0039] the thus prepared PV layer sequence exhibits a photovoltaic effect in the long wave and extreme long wave infrared range.

[0040] In a further advantageous embodiment an acrylate-based paint for the outer region is admixed with aluminum flakes (pigment addition of the paint industry for paints having a silver appearance), homogenized and a first layer is deposited on a glass carrier having an area of around 10 cm10 cm which was previously preparatively coated with a semi-transparent, electrically conductive metal layer. The acrylate-based layer comprising aluminum flakes is prehardened in the air at room temperature for 5 minutes. Subsequently a second mixture of the same acrylate-based paint is made up with aluminum flakes, admixed with silica sol and in a cooled stirrer adjusted to basic pH with aqueous sodium hydroxide solution and homogenized. The still-reacting mixture is applied as a second layer atop the first prehardened layer and uniformly and coveringly distributed. The parallel reaction where the aluminum is at least partially solubilized accelerates the final hardening of both layers. The thus obtained layer composite is provided on its top side with a finger electrode made of room temperature conducting silver from Busch. As shown by FIG. 1 in a scanning electron microscope image (SEM) the thus obtained layer on its top side is characterized by a plastics matrix in which the base-dissolved water glass provides a siloxane fraction. The Al flakes carried in the matrix are solubilized and securely integrated into the plastics matrix. As taught by FIG. 2 the Al flakes pass through the plastics layer to the surface and allow a direct electrical contacting of a scaffolding made of Al flakes conductingly interconnected via contact points and short electrolyte bridges. Detachment of a flexible segment of the plastics double layer using a scalpel showed that the double layer is present as a flexible, solid, removable composite; the removed segment was tested on its bottom side by SEM. As is shown by FIG. 3 in an SEM image, on the bottom side too Al flakes are present and in areal contact with the phase interface of the semitransparent electrode and allow electrical contact.

[0041] The top side of the double layer was provided with a finger electrode made of room temperature conducting silver from Busch and supplementally areally contacted with a transparent adhesively bondable ITO film. Subsequently the covering electrode and the bottom side electrode were contacted and the cell was investigated for PV activity. The double layer was initially investigated for PV activity by means of a cold light LED light source with visible light. Photovoltaic currents were weak to non-existent. Upon irradiation with a halogen lamp after a short warm-up phase of 1 to 4 seconds, clear photovoltaic potential differences beyond 100 mV were measured. It was possible to tap a constant load to operate an LED bicycle lamp. The question arises whether this is attributable to a Peltier effect. In order to test this the entire contacted cell was provided with thermocouples on the top side and bottom side, weld-wrapped in a watertight vacuum bag having implemented contact lines and completely submerged in 10 liters of hot water. After a heating time of about 5 minutes the temperature of all thermocouples was identical. The photovoltaic potential difference between the covering electrode and the bottom side electrode was significant and proportionally dependent on the cell temperature now falling slowly with the temperature of the water. The start value, end value and measured value variations occurring in between were digitally recorded and are reproduced in the graphic of FIG. 4. As is shown by FIG. 4a the measurement of the photovoltaic tappable potential from the PV double layer shows a proportional dependence on the temperature of the water falling from 46 C. to 31 C.: the lower the temperature the lower the tappable potential. However, the surrounding water ensures that no temperature gradient is measured here which in a Peltier element would be required for the then-measurable Seebeck effect. The temperature of the cell completely surrounded by uniformly heated water shows no gradients.

[0042] Verification of the removed and unpacked cell in a pizza oven showed, surprisingly, that up to 50 C. at a distance of the cell from the hot wall of the pizza oven no sufficient heat radiation reaches the cell. As shown by FIG. 4b the known light absorption maxima of H2O in air as a function of wavelength are significant in the wavelength range 5 to 10 micrometers.

[0043] The inventors believe that specifically hot water accordingly emits in this wavelength range and thus provides photons of appropriate energy with the highest efficiency in the chosen experimental set up. The measured results clearly indicate a utilizable band gap in the long wave to far IR range beyond 5 micrometers. However, this also means, conversely, that at high thermal incident radiation sufficient heat radiation would need to penetrate a thin air layer around the cell and be able to generate current. This was confirmed: in a pizza oven at 80 C. with a 2 cm air gap between the hot oven stone and the double layer the double layer produced and contacted as described hereinabove delivers clearly and distinctly measurable current which falls again proportionally to the temperature during cooling and gives way at about 60 C. The presently produced double layer sequence makes it possible to achieve advantageous photovoltaic utilization of long wave to extreme long wave light fractions right up to far IR radiation which in the prior art is a disadvantageously ignored and uninvestigated wavelength range. When the above-described cell is connected to a voltmeter and heated with a flat hand placed thereupon a potential difference is established which is proportional to the respective measurable surface temperature. Industrial waste heat and/or body heat in particular may be usefully and effectively utilized with the presently produced PV layer sequences.

INDUSTRIAL APPLICABILITY

[0044] It is a problem of processes according to the prior art that these always require a sintering step at elevated temperature. A further problem is that flexible thin layers, in particular PV layers, often do not tolerate such temperatures and additionally do not allow utilization of industrial waste heat and/or long wave photons.

[0045] The solution to these problems may be provided with a process where during hardening an additional reaction accelerates and improves hardening. This particularly advantageously allows a double layer sequence comprising a plastics matrix in which throughout metal particles are present and in a top layer base-solubilized siloxane fractions and metal particles are present, wherein through mutual final hardening during the base-solubilization it is made possible to produce a PV layer sequence with which industrial waste heat/long wave IR radiation becomes utilizable by photovoltaic means. The effective utilization of industrial waste heat/heat/body heat provides clear economic advantages in a great many fields.