US20080047545A1
2008-02-28
11/510,471
2006-08-26
A method and an apparatus for the 24 hours a day conversion of the high difference of temperatures between two working mediums accumulating the Sun-radiation-heat gets concentrated by the parabolical mirror, during light-days, and the cosmic cold, during nights, into electro-power & refrigeration-output which are realized and called for service (under the shadow of this mirror or near this shadow), which method and apparatus provide not only to perform (fulfil) this conversion, but also to intensify the semiconductive thermoelectrical transformer as well as the heat-exchange of these heat-accumulating working mediums with the heat-absorbing and heat-transferring components of the absorption-refrigeration machines and heat-mechanical electro-generating machines.
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The invention pertains to the field of conversion of the high difference of temperatures into the electrical or some other power conformably to accumulation of the concentrated Sun-heat, up to its materialization through the hydrogenâfuel, but also may be considered conformably to realization of the high-potential heat of some other origin in those cases when the object with the high temperature may be placed close enough to the object with the lower temperature.
When the author was solving problems of obtaining of the fresh water from the atmospheric air and of the hydrogenâfuel from the fresh water, basing his solutions only on energy of Sun-heat and the cosmic cold, he (me) collided with the necessity to fill up two gaps. The first of them is the gap between the well known and quite developed methods and devices for the electrolytical decomposing of water into hydrogen and oxygen and methods and devices for getting the Sun-radiation-heat and for accumulating this heat by a working medium which changes its state of aggregation at the relatively high temperature. The second gap is the accumulation of the night cosmic cold.
The known transformers of the Sun-radiation into electrical power, despite they are the successful energy-suppliers for many on-Earth and cosmic objects, can not be chosen for filling up the first aforesaid gap in virtue of the very serious negative moments: 1) the huge (thousands of square metres) surface area of perception of the power of the Solar-lightânot of the Sun-heat power, which area makes practically impossible to protect it from as wind affection, as pollutions made by insects, birds and atmospherical precipitations and completely impossible to follow the Sun-movement along the sky-sphere; 2) the practical unfitness for accumulation of the Sun-heat by some working medium because of impossibility of its distribution under such a huge surface area of the Sun-radiation perception.
The known (by books of reference and text-books) conductive transformers of the difference of temperatures into difference of electrical potentialsâthe electric-driving-force (E.D.F.), which transformers are the measuring thermocouples, are unfit for energetic needs because of their too modest coefficient of transformation (only about 0.04+0.07 mV/° C.) that requires to gather many hundreds of thousands of thermocouples and makes engineering and spending difficulties irresistible. But the well known (by books of reference and text-books) semiconductive thermo-electrical transformers are good enough for the energetic needs, having their efficiency about 15% and their coefficient of transformation about 5+10 mV/° C. that is quite acceptable to fill up the first aforesaid gap with this invention which has to add the aforesaid leading invention. They were mailed concurrently with my HZ001 and 002.
And as concerns (to) accumulation of the night cosmic cold, this thing, having been discovered first only in the aforesaid leading invention, is not yet to refer to it.
In its embodiment as a method, the invention provides: 1) to accumulate the Sun-heat, was gotten concentrated at the focus of the parabolical mirror, through the reversible change from solid into liquid state of aggregation of some part of mass of a working medium which medium may be supposed: to be a body of lower thermal stability inside a heat-absorbing or an one-directedly heat-radiation-transparent enclosure of higher thermal stability; to be (with the lowest probability of some practical realization) a heat-radiation-transparent enclosure of lower thermal stability gets warmed from inside by a heat-absorbing body of higher thermal stability located within this enclosure; to be (with the highest probability of the really practical realization) a heat-absorbing body of lower thermal stability located within an enclosing heat-absorbing body of higher thermal stability and of ability to be mechanically loaded which enclosing body, in its turn, located within an enclosing one-directedly heat-radiation-transparent enclosure of high thermal stability; 2) to transform into differences of electrical or thermodynamical potentials the difference between the limitedly (to keep safe the transformer) highest temperature of the meltingâcrystallization of the âhotâ working medium and the relatively low temperature of the âcoldâ working medium; which low temperature gets stabilized through accumulation of the night cosmic cold changes, from liquid into solid state of aggregation, some part of the âcoldâ working medium; which difference of electrical potentials is the electric-driving-force (E.D.F.) between two âp-nâ junctions of the semiconductive thermoelectrical transformer when one of these junctionsâthe âhotâ one absorbs the stable temperature of the âhotâ working medium and other of them absorbs the stable temperature of the âcoldâ working medium; which âhotâ and âcoldâ working mediums never get completely melted or completely crystallized and keep their heat-exchange with those âhotâ and âcoldâ âp-nâ junctions 24 hours a day every day; which semiconductive thermoelectrical transformer completes the circuit of an recipient of its E.D.F.;
which differences of thermodynamical potentials concern the sides of the high and low pressures as of the refrigerant in the heat-exchangers of the absorption refrigeration machine, as of the working medium in the heat-exchangers of the closed heat-contour of heat-mechanical electro-generating machine.
In its embodiment as an apparatus, the invention provides the necessary and adequate combinations of the necessary and adequate components which components are:
{circle around (1)} Getting conjointly or partedly (not in one and the same device),
The semiconductive thermoelectrical transformer with its twoâthe âhotâ and the âcoldâ âp-nâ junctions;
The heat-absorbing partâthe boiler of the absorption refrigeration machine & of heat-mechanical machine that(those) goes(go) instead of or conjointly with the âhotâ junction of the semiconductive thermoelectrical transformer; as well as the heat-losing (the cooled) partâthe condenser with the absorber of the absorption refrigeration machine & the condenser of the heat-mechanical machine those go instead or conjoin the âcoldâ junction of the semiconductive thermoelectrical transformer.
{circle around (2)} The accumulator of the concentrated Sun-heatâthe thermostat for the âhotâ âp-nâ junction & for the boiler of the absorption refrigeration machine & heat-mechanical machine, which accumulator includes the heat-radiation-transparent enclosure and the heat-radiation absorbing body inside this enclosure.
{circle around (3)} The accumulator of coldâthe thermostat for the âcoldâ junction & the absorber with the condenser of the absorption refrigeration machine & the condenser of the heat-mechanical machine, which accumulator includes the receiver of the night cosmic cold possessing the one-directed heat-transfer to cosmos.
{circle around (4)} Electro-conductors to complete the electro-circuit of the semiconductive thermoelectrical transformer and its electro-recipient(s) (for the first aforesaid gap, this recipient is the electrolyzer of the fresh waterâproducer of hydrogen and oxygen), as well as conductors of the working mediumsâtubes to set the heat-absorbing and the heat-losing (cooled) parts into closed heat contour(s) of the refrigeration & heat-mechanical machine(s).
{circle around (5)} Devices to get the components 1+4 supported and reciprocatedly moveable along the focal axis of the parabolical mirror.
The semiconductive thermoelectrical transformer, even if it was gotten from numbers of patterns are manufactured in many countries, may be somehow acceptable to use it in this invention as a component makes get adapted to itself all other components of the invention as an apparatus. But, to design this transformer conjointly with other components and then to manufacture it customerwise would be much better. The same may concern the heat-absorbing part (boiler) and the heat-losing (cooled) parts (absorber, condenser) of the absorption refrigeration machine and of the heat-mechanical machine.
A design of the accumulator of the concentrated Sun-heatâthe thermostat for the âhotâ âp-nâ junction of the semiconductive thermoelectrical transformer & for boilers has to fit the following requirements:
the heat-absorbing body has to possess the same average density (mass/volume) that the material of the heat-radiation-transparent enclosure possesses, being in its melted state,âsuch is the condition of conservation of position of this body inside the partly melted enclosure if the heat-stability of this body is higher than the heat-stability of the material of such an enclosure, despite the nullity of probability of such a situation; if the heat-stability of the enclosure is higher than the heat-stability of the heat-absorbing body, the position of this body inside the enclosure is conserved by conservation of solidity of such an enclosure;
the heat-radiation-transparent enclosure has to prevent from losing any heat through its wall back to environment and to limit the heat-influx to the outside layer of its wall, which layer may be considered (however the probability is null) as the mechanically loaded one when the inside layer of its wall is melted;
the full preference has to be given to a design with two heat-absorbing bodiesâthe internal one which possesses the lower heat-stability, and the outer one which possesses the higher heat-stability and can serve as a mechanically-loaded tank, wherein the heat-radiation-transparent enclosure may be only to prevent from losing the absorbed heat back to environment;
A design of the accumulator of coldâthe thermostat for the âcoldâ âp-nâ junction & condensers and the absorber which accumulator includes the receiver of the night cosmic cold possesses the one-directed heat-transfer only to cosmos, has to suppose the following circumstances:
immersion of the âcoldâ âp-nâ junction in the thermostat has to be from below upwards same as the only direction of the heat-transfer from this accumulator-thermostat to cosmos has to be (to go);
the fresh water and salt-water-solutions change reversibly the state of aggregation from liquid into solid in the interval of temperatures between 0° C. and â50° C. and, possessing the high enough value of the specific melting-heat (about 70+80 Kcal/Kg), can be considered as the ideal working medium for cold-accumulating and thermostatting of the âcoldâ âp-nâ junction; but, possessing the electro-conduction, they are not advisable for immersion in them any objects with opposite electrical potentials, which objects, in such a case, have to be either electro-insulated or immersed through some heat-conductive, but electro-insulating agent (for example, teflon);
the one-directed heat-transfer from the cold-accumulating, thermostatting working medium from below upwards to cosmos may be realized in the best way by the well known deviceâthe super-heat-conductive tube (the John Perkins' tube), possessing the diode-property, if this device is protected from the strange heat-influxes.
A device of electro-conductors, getting completed the electro-circuit of the semiconductive thermoelectrical transformer and its electro-recipient(s), and of tubes set the heat-absorbing and the cooled heat-exchangers into the closed heat-contour(s) of the heat-transforming machines, has to suppose the peculiarities of the generally known semiconductive thermoelectrical transformer and known (must probably, coil-like) heat-exchangers in the new (for them) assemblyâconditions, prompting the choice of their designâsolutions.
No one of the aforenamed components of this invention has to shade the active (except central aperture with radius about 300 mm) part of the parabolical mirror, which mirror may be imagined with radius about 10 m and with its focal axis directed to the centre of the Sun's disk,âso all these components have to be inscribed in the cylindrical room with its radius about 300 mm and with its axis of unlimited length between the focus of this mirror and the centre of the Sun's disk. The real possibility of fulfillment of this requirement gets confirmed by calculation (upon a napkin):
If to suppose that about 300 KW of Sun-heat, which gets concentrated by the aforenamed parabolical mirror (of its 10 m radius) with coefficient of concentrating within 0.5 (let the mirror be a rough one), gets accumulated with coefficient of uncertainty 0.8 and with relative duration of daily accumulation 0.3, gets transformed into electropower with efficiency of the semiconductive thermoelectrical transformer 0.15,âwill turn into the electropower goes to the electrolyzer (300Ă0.5Ă0.8Ă0.3Ă0.15) 5.4 KW, the value of the electrocurrent, according to coefficient of transformation of potentials about 5 mV/° C. and according to the difference of temperatures between the âhotâ and the âcoldâ âp-nâ junctions about 500° C.,âso, according to voltage 2.5V,âwill be (5400 W/2.5V) 2160 A. If to limit the current-density at its value 1 A/mm2 (such as to keep the electro-conductor cold), the section-area of the electrocurrent-conductor has to be 2160 mm2, and this conductor may be imagined as a strip with a section 216 mmĂ10 mm, or 144 mmĂ15 mm, or 432 mmĂ5 mm, or as a combination of strips 2Ă108 mmĂ10 mm, or 3Ă144 mmĂ5 mm, or 4Ă108 mmĂ5 mm, or some else. The power 5.4 KW for electrolyzer during 16 night hours, when this power is not covered by income of the Sun-heat to the focus of the parabolical mirror, has to be replaced (substituted) by the energy (5.4Ă16/0.15) 576 KWhours that is (576Ă860) about 500,000 Kcal, which energy has to be accumulated in the heat-accumulator as the heat of transition between states of aggregation of the âhotâ working medium. If to suppose this âhotâ working medium as an aluminium alloy with its melting temperature about +550° C. and its specific heat of melting about 60 Kcal/Kg and to suppose also that only about 80% of its mass will be melted in the process of the heat-accumulation, this mass has to be (500,000/60Ă0.8) about 10,400 Kg. If the density of the melted alloy is about 5,000 Kg/m3, the volume for the âhotâ working medium- has to be about 2 m3. If to suppose the length of the cylindrical volume 2 m3 about 5 m, its radius will have to be about 360 mm. The same quantity of energy (about 500,000 Kcal) has to be accumulated during 8 night hours in the accumulator of the cosmic cold as the heat of transition between states of aggregation of the âcoldâ working medium. If this âcoldâ working medium is the pure fresh water with its melting temperature 0° C. and its specific heat of melting about 80 Kcal/Kg, and if the radius of the cylindrical volume for this working medium is also 360 mm, the length of this volume will have to be (500,000/80Ă1,000Ă3.14Ă0.362) about 15.5 m. If to determine the specific density of heat-radiation from the condenser of the J. Perkins' tube to cosmos at the temperature 0° C.=+273° K, the value of this density will be (0.95Ă4.9Ă(273/100)4) 258 Kcal/m2Ăhour,âso, to radiate 500,000 Kcal during 8 night hours will require the surface-area of the J. Perkins tube's condenser (500,000/8Ă258) about 242 m2, that will require the length of a smooth-surfaced hollow cylinder with its radius about 300 mm (242/3.14Ă2Ă0.3) about 128 m (what a huge one!), but if to corrugate this hollow cylinder with deep corrugations which make coefficient of corrugation about 30+40, the length of this cylinder may be reduced up to 4+5 m. If to suppose that it will be enough to add to the radius 360 mm more 2 mm for thickness of the wall of the heat-stable part of the heat-absorbing body, more 5 mm for thickness of the internal wall of the heat-radiation-transparent enclosure, more 15 mm for the vacuum heat-insulation, and more 5 mm for thickness of the outer wall of the heat-radiation-transparent enclosure, the increased radius of the cylinder goes alignedly to the focal axis of the parabolical mirror will prove to be (360+27) about 390 mm. If to add more 20 mm for laying electroconductors & tubes along this cylinder, the final radius will be 410 mm. The shade of its radius 0.41 m will damage the heat-concentrating area of the parabolical mirror of its radius 10 m, but the percentage of this damage (100Ă0.412/102) 0.17% is beyond to be unacceptable. The âupon a napkinâ-calculation has shown that components of this invention as an apparatus can be located in the cylindrical room of about 400 mm in radius and of about 25 m in length, being together of about 25 tons in weight,âso they together are beyond to be unacceptable as well. In addition to that, the aforesaid presence of the 5 m in length cylinder of the âhotâ working medium in the accumulator of the Sun-heat prompts the necessity of the reciprocating movement, along the focal axis of the parabolical mirror, of all the 25 m in length cylindrical composition, such as, before the night break, to get melted at least 80% of the mass of the âhotâ working medium. So, devices to realize such a movement are also the quite necessary components of this invention.
In so far as the semiconductive thermoelectrical transformer has to take its place within the cylindrical room along the focal axis of the parabolical mirror between two accumulators, one of whichâthe âhotâ one has to be cylindrical at least because the parabolical mirror, in its outer contour, has, as the simplest, to stay round, the design-arrangement of the semiconductive thermo-electrical transformer, with its âhotâ (heat-absorbing) âp-nâ junction below and with its âcoldâ (cooled) âp-nâ junction upwards, suppose to arrange this transformer either as a battery of some concentric hollow vertical cylindersâtransformers, or as a battery of some radially-packed in the vertical cylindrical room flat vertical transformers, or as one single whole spirally packed in the vertical cylindrical room vertical transformer. The structural advantages as of the electro-current collectors (buses), which, at the same time, will serve as substrates of the (semiconductive) wafers of âpâ and ânâ types and have to come out from the middle zone between the âhotâ and the âcoldâ junctions by the possibly shortest route, as of the heat-conductors, which also will serve as substrates of wafers of âpâ and ânâ types, prompt to prefer the battery from the vertical flat transformers are radially packed in the cylindrical room. The lower (heated) part of the semiconductive thermoelectrical transformer, in order to prevent from the short circuit between substrates of positive and negative wafers, may be immersed in the melted dielectric (for example, glass) with the melting temperature and density some lower than the melting temperature and density of the âhotâ working medium (aluminium alloy) in the thermostat. The upper (cooled) part of the semiconductive thermoelectrical transformer, for the same reason, may be covered by some film of dielectric possesses the high heat-conduction (for example, teflon).
The lower (heated) part of the semiconductive thermoelectrical transformer, in its locality, may be replaced or refilled by the boiler of the absorption refrigeration machine & heat-mechanical machine, and the upper (cooled) part of this transformer, in its locality,âby the absorber and condenser of this refrigeration machine & by condenser of this heat-mechanical machine.
FIG. 1 gives a notion about the general design-arrangement of whole combination of the substantial components of this invention together with the parabolical mirrorâconcentrator of the Sun-heat, which concentrator is refilled by this invention, and, being drawn on some scale according to the aforegiven âupon a napkinâ calculation, gives also a notion about proportions of these components and this parabolical mirror.
FIG. 2 gives a notion about the provided (by this invention) design and arrangement of the semiconductive thermoelectrical transformer and about its interaction with the âhotâ and âcoldâ thermostats.
FIG. 3 gives a notion about the provided (by this invention) design and arrangement of the âhotâ accumulator of the concentrated Sun-heat.
FIG. 4 gives a notion about the provided (by this invention) design and arrangement of the âcoldâ accumulator with its receiver of the night cosmic cold and with its thermostat of the âcoldâ working medium.
FIG. 5 gives some more detailed notion about the provided (by this invention) rigging of the semiconductive thermoelectrical transformer with electro-conductors and electro-current collectors (buses) those complete the electro-circuit of this transformer and its electro-recipient(s).
FIG. 6 gives some more detailed notion about the provided (by this invention) general arrangement of devices to get the whole combination of the heat (cold)-absorbing and transforming components supported and reciprocatedly movable along and alignmently the focal axis of the parabolical mirror.
The semiconductive thermoelectrical transformer 1 (FIG. 1) is installed and fastened, between the âhotâ accumulator 2 of the concentrated Sun-heat and the âcoldâ accumulator 3 of cold, in such a way that the âhotâ âp-nâ junction 4 and the âcoldâ âp-nâ junction 5 of the thermoelectrical transformer 1 are immersed, accordingly, in the âhotâ and the âcoldâ thermostats of these accumulators while this transformer's middle zone, which is embraced by the annular parts of positive and negative electro-collectors (buses) 6 and 7 those, then, go under the mirror (the transformer 1 is installed alignmently with the focal axis of this parabolical mirror that belongs to the leading invention) to get completed the electro-circuit of the transformer 1 and its electro-recipient(s) (is (are) not introduced in the drawings), is just between these two accumulators 2 and 3. The totality of components 1+7 is hung, as the united weight load, by several (not less than three) identical devices 8 such as to be supported and to get reciprocatedly movable along the focal axis of the parabolical mirror, that is quite necessary for the cyclical (within hours of the active receiving of the Sun-heat) attendance in the focus 9 of the parabolical mirror of all sections of the long enough âhotâ accumulator 2. In so far as such reciprocated shaffle has to be realized simultaneously with the altering of azimuth and height of the axis and focus of the parabolical mirror are directed to the moving by the sky-sphere Sun (such altering is provided by the leading invention), all devices 8, in their turn, are rested upon the load-receiving shell 10 of the parabolical mirrorânot upon the set in ground base of this mirror (such way is much simpler). The parabolical mirror and its load-receiving shell 10 are introduced in their axis-section.
The FIG. 2 gets the semiconductive thermoelectrical transformer 1 (FIG. 1) introduced by four sections: three of them are cross-sections and one of them is the longitudinal section (please, look at cross-sections A-A, B-B, and C-C, and the longitudinal section D-D within its part concerns the middle zone of the transformer 1 (FIG. 1)), giving a notion, accordingly, about the design-arrangement in the zone of the âcoldâ âp-nâ junctions, in the middle zone, in the zone of the âhotâ âp-nâ junctions, and about design-arrangement of the electro-collectors (buses) at the middle zone of the transformer 1. In the zone 5 (FIG. 1) of the âcoldâ âp-nâ junctions (section A-A, FIG. 2), pairs of the radially packed in the vertical cylindrical room flat vertical semiconductive wafers II of âpâ-property andâ12 of ânâ-property get formed the âp-nâ transitions being in the ideal electrical (electron-vacancy) contact 13 with each other by the plane of their (bearing) fit (the cold welding) or in their soldered connection. Getting assembled mechanically, thermally and electrically in the united composition by the means of the V-shaped profiles (sections) 14, which are in the ideal contact 15 with planes of wafers 11 of âpâ-property and in the ideal contact 16 with planes of wafers 12 of ânâ-property, and, being placed between the adjacent pairs of the wafers of the one and the same property, perform functions of the mechanical carcass, heat-conductors, and equalizers of âpâ and ânâ electro-potentials along the joint area of two wafers of âpâ or ânâ-property, these pairs of wafers are electro-insulated from any other (strange) electrical contacts by the means of the reliable thickness 17 of the electroinsulating, anticorrosive, and well-heat-conductive material (for example, teflon). At the border between the zone 5 (FIG. 1) of the âcoldâ âp-nâ junctions (section A-A, FIG. 2) and the middle zone (section D-D, FIG. 3), this thickness 17 gets united with the monolithic washer 18 of the casing 19, those are made from the same (teflon) material and embrace hermetically, accordingly, the close to the border part of the zone 51 (FIG. 1) of the âcoldâ âp-nâ junctions and the lower part of the loaded enclosure of the accumulator 3 of cold (FIG. 1). The sectoral gullets of the V-shaped profiles (sections) 14 (section A-A, FIG. 2) are filled with water (as cold as 0° C. and, being a salt-solution,âas up to â50° C.) or with ice, those are restrained by the washer 18 and the casing 19.
In the middle zone (section B-B, FIG. 2), the same, but the gotten prolonged pairs of the radially packed in the vertical room wafers 11 and 12, do not get formed the âp-nâ-transitions. On the contrary, they are electrically insulated from each other by the thickness 17 of some other (no teflon) electroinsulating material of the much lower (the lowest possible) heat-conductivity, which thickness fills the gaps between wafers 11 and 12 in each of their pairs, while the taking turns sectoral gullets, those are bordered by surfaces of wafers either 11 or 12, accordingly, of âpâ or ânâ-property, are filled, with the ideal electrical contact, separatedly at the âhotâ and at the âcoldâ end of this zone, with the metal wedges 20 of high electro-conduction, which wedges do not contact either each other or the V-shaped profiles (sections) 14, but are gathered (monolithically or with the ideal electrical contact with each even-other even (with each odd-other odd,âso, over one) by the means of the annular bandages 21 and 22, accordingly, of the positive or the negative electro-collectors (buses), which collectors are one above other (section D-D, FIG. 2), do not contact each other, are covered by the reliable thickness 17 of some electroinsulating material of the high heat-conductivity, and are (each of them separately) prolonged (being connected monolithically or with the ideal electrical and thermal contact) by a group of several directed downwardsâunder the parabolical mirror collectors (buses), which, in their turn, are covered by the thickness 17 of the same electro-insulating material of the high heat-conductivity (for example, teflon). In the zone 4 (FIG. 1) of the âhotâ âp-nâ junctions (section C-C, FIG. 2), the same prolonged pairs of the radial packed in the vertical cylindrical room wafers 11 of âpâ-property and wafers 12 of ânâ-property do (again) get formed the âp-nâ-transition, being (again) in the ideal electrical (electron-vacancy) contact 13 with each other by the plane of their bearing (the cold welding) or in their soldered connection. They are assembled mechanically, thermally, and electrically in the united composition (again) by the means of the V-shaped profiles (sections) 14, which are (same as in the zone 5 (FIG. 1) of the âcoldâ âp-nâ junctions (section A-A, FIG. 2)) in the ideal contact 15 with planes of wafers 11 of âpâ-property and in the ideal contact 16 with planes of wafers 12 of ânâ-property, and, being (again) placed between the adjacent pairs of the wafers of the one and the same property, perform (again) functions of the mechanical carcass, heat-conductors, and equalizers of âpâ and ânâ electro-potentials along the joint area of two wafers of âpâ or ânâ-property. But, in difference of the zone 5 (FIG. 1) of the âcoldâ âp-nâ junctions (section A-A, FIG. 2), they (âpâ and ânâ-property wafers) are prevented from any strange electro-contacts by the melt of some thermo-stable and electro-insulating material (for example glass at its temperature about 500° C., which temperature keeps the semiconductive materials of wafers 11 and 12 beyond possible thermal damages or changings of their working properties) which material is, indeed, the electro-insulating heat-transmitter 23 from the thermostatting working medium in the âhotâ accumulator 2 (FIG. 1) of the concentrated Sun-heat, into which heat-transmitter 23, the zone 4 (FIG. 1) of the âhotâ âp-nâ junctions of the semiconductive thermoelectrical transformer 1 (FIG. 1) got immersed.
The FIG. 3 gets the accumulator 2 (FIG. 1) of the concentrated Sun-heat introduced by the lower part of the longitudinal axial section D-D (FIG. 1). The embracing the zone 4 (FIG. 1) of the âhotâ âp-nâ junctions of the thermoelectrical transformer 1 (FIG. 1) heat-transmitter 23 (FIGS. 2 and 3), with its temperature about 500° C. and its density quite lower than the density of the keeping it floatable thermostatting working medium 24 (FIG. 3), together with this working medium 24, which is as hot as 550° C.+600° C. and as possessive of density as about 5 g/cm3, both get filled the vessel 25 which (if to keep on following the âupon a napkinâ calculation) is made in its measure about 360 mm (radius) by about 5 m (length) overall from some relatively thin-walled, but mechanically and thermally stable, load and heat-standing heat-conductive material (for example, the stainless steel), allowing the local (by its length) wall's overheating up to 800° C.+900° C. under the weight-loading (by the melts inside this vessel) not less than 10,500 Kg. The outer surface of the vessel 25 is embraced, with a gap (for the vacuum heat-insulation), but hermetically, by the heat-radiation-transparent enclosure 26, made from some thermostable and quite heat-resistant material, for example, quartz glass. In order to limit the radiation-heat-losses through the enclosure 26, the internal surface of this enclosure 26 got treated such as to return the heat-radiation leaves the surface of the vessel 25, because of some inperpendicularity of falling upon this surface, back quite perpendicularily to this surface. In order to limit the convective-heat-losses through enclosure 26, the capacity of the cavity 27 between surfaces of the enclosure 26 and of the vessel 25 got vacuumized.
In addition to that, the wall of the enclosure 26 got prevented from destruction by the atmospheric pressure by the means of juts 28 on its internal surface, which juts 28 are rested on springs 29 serving as the mechanically flexible heat-insulators between the juts 28 and the big with deformation wall of the vessel 25. Vacuum in the cavity 27 and the atmospheric pressure, which affects the outer surface of the enclosure 26 with its radius of the horizontal projection about 300 mm, may result in retaining of the enclosure 26 at the vessel 25 by the atmospheric pressure acting against the weight up to 2500 Kg, that is much more than its possible real weight. To get the reliable sealing of the vacuum cavity 27 at the expense of the atmospheric pressure is attainable as well, for example, by the means of the annular U-shaped seal device 30 made from the relatively heat-standing, but flexible alloy (for example, of aluminium and copper) and by the means of strengthening of the cylindrical verge of the enclosure 26 by the strong shell 31. The summary weight of the vessel 25, plus the filling this vessel bodies 23 and 24, plus the hanging under the vessel 25 enclosure 26, and plus the floating in the melt of the heat-transmitter 23 thermoelectrical transformer 1 (FIGS. 3 and 1), which summary weight is not more than 15,000 Kg (if to keep on following the âupon a napkinâ calculation), is hung-under to the body of the accumulator 3 (FIG. 1) of cold by the means of the pendants 32 (FIG. 3) those get the vessel 25 drawn to this body of the accumulator 3 and by the means of the monolithic washer 33, made alike the washer 18 (FIG. 2, section A-A), but from the heat-standing material (for example, the high-temperature cast ceramics), and the struts 34 those get quite sealed the melt of the heat-transmitter 23 and the zone 4 (FIG. 1) of the âhotâ âp-nâ junctions in the upper part of the vessel 25.
In the FIG. 4, the accumulator 3 (FIG. 1) of cold is introduced by the upper part of the longitudinal axis section D-D (FIG. 1). This accumulator 3 of cold is a hollow cylinder 35 (FIG. 4) which is hermetically closed from below by the casing 19 (FIG. 2, section A-A as well) with its washer 18 (FIG. 3, section D-D as well) those continue the thickness 17 (FIG. 2, section A-A as well) of the heat-conductive electroinsulating and anticorrosive material which covers whole outer surface of all details of the immersed in this cylinder zone 5 (FIG. 1) of the âcoldâ âp-nâ junctions. From above, this cylinder 35 is hermetically closed by the partly immersed in its upper part receiver 36 of the cosmic cold, which receiver is filled, in all its vecant capacity, by the thermostatting working medium 37. This working medium 37 changes reversibly its state of aggregation (solid-liquid) at the temperature about 0° C. (if it is the fresh water) or below 0° C. up to â55° C. (if it is the solution of âCaCl2â with its density about 1,300 Kg/m3). The outer element surface of the cylinder 35 is embraced by heat insulation 38 which may be (same as it made for the âhotâ accumulator 2 (FIG. 1)) the vacuumized cavity between this surface and an embracing enclosure. The element wall of the cylinder 35 is the mechanical load-carrying structure which is joint with and loaded by all other components of the apparatus and interacts with devices 8 (FIG. 1) such as to be supported and reciprocatedly moved, together with those components, along the focal axis of the parabolical mirror.
The receiver 36 of the cosmic cold (look, please, at its mention in the summary of the invention) is the J. Perkins' heat-conductive tube which is filled with the working medium. The boiling-point of this working medium is some lower than the temperature of the liquid-solid transition of the thermostatting the zone 5 (FIG. 1) of the âcoldâ âp-nâ junctions working medium 37 in the accumulator 3 of cold,âso, it is about â5° C.+â55° C. The evaporator 39 of this J. Perkins' tube is fulfiled in the form of lots of thin-walled hollow tentacles, filled with the boiling medium, those pierce the thermostatting working medium 37, approaching and almost touching the zone 5 (FIG. 1) of the âcoldâ âp-nâ junctions immersed in this working medium 37. The condenser 40 of this J. Perkins' tube, with its huge (if, to compare to the evaporator 39) corragated surface of radiation, is prevented from the outer convective and radiant heat-influxes by the means of the one-directedly heat-transparent enclosure 41. The cavity between this enclosure 41 and the outer surface of the condenser 40 is vacuumized while the internal and outer surfaces of this enclosure 41 are treated such as to maximize the absorbing of the heat-radiation from inside (Δâ 0.96+0.98) and to minimize the absorbing of the heat-radiation from outside of the enclosure (Δâ =0.04+0.05). In addition to that, the washer 18 and the casing 19 (FIG. 4), in order to prevent from heat-exchange through them, are additionally heat-insulated at their side looking at the middle zone of the thermoelectrical transformer 1 (FIG. 1), as it is noticed in the FIG. 4.
In the FIG. 5, the electro-conductors 6 and 7 (FIG. 1), with their annular bandages 21 and 22 (FIG. 2, section B-B) completing the electro-circuit of the thermoelectrical transformer 1 (FIG. 1) and its electro-recipient(s), are introduced schemicallyâwithout any scale or proportionality of their sections. The reciprocated shuffle of the totality of components 1+7 (FIG. 1) along the focal axis of the parabolical mirror as well as the altering of azimuth and height of this focal axis itself result in the necessity to have, in each of the electro-conductors 6 and 7, some deformable (for example, wattled) section 42 before their fixed sections 43, connected to the electro-recipient(s), which is(are) not introduced. Each of electro-conductors 6 and 7 (look, please, at the summary and at the âupon a napkinâ calculation of the invention as an apparatus) is represented by the combination of strips 44, for example, 4Ă144 mmĂ5 mm, that makes easier to lay these electro-conductors along the âhotâ accumulator 2 (FIG. 2) without to add significantly the shade gets upon the parabolical mirror. Such a laying, which crosses the zone of irradiation of the accumulator 2 (FIG. 2) by the concentrated Sun-heat, requires to protect each of the strips 44, within this zone, by a heat-standing screen-jacket 45 made from ceramics.
And in addition to that, the shade will be minimized if to lay strips, which are protected by screen-jackets, in the radial order.
In the FIG. 6, devices 8 (FIG. 1) for support and reciprocated shuffle of the totality of components 1+7 (FIG. 1) along the focal axis of the parabolical mirror, are introduced by the structurally-kinematical diagram that corresponds with the FIG. 1. Each of devices 8 (FIGS. 1 and 6) may, for example, be a combination of the driven lever 46 of the first order, which is hingely rested upon the load-receiving shell 10 (FIGS. 1 and 6), and of the crank 47, which is a hanger of the body 35 of the accumulator 3 (FIGS. 1 and 6) of cold (so, of the totality of components 1+7 (FIG. 1)). Load-moments on the lever's 46 arms are balanced by the counterweight 48 off-loading the drive 49. This drive 49 is hingely connected with the end of the lever's 46 arm (loaded by the counterweight 48) as well as with the shell 10 (FIGS. 1 and 6) and, getting altered the interval between axises of its hinges, realizes the swing of ends of the lever 46 and of the crank 47, so, the reciprocated shuffle of the body 35 of the accumulator 3 of cold and, with it together, of the totality 1+7 (FIG. 1) along the focal axis of the parabolical mirror. The totality of the aligned between themselves components 1+7 (FIG. 1) has to be kept aligned with the focal axis of the parabolical mirror in conditions of the permanent altering of azimuth and height of this axis, which axis, only in the equatorial zone of the earth (±23° from equator) and only two times a year takes, for a short moment during the light day, its plumb attitude. The technical solution that allows to keep this alignment may, for example, provide two supporting power-rings 50, located (please, look at the FIG. 1): oneâthe lower one just under the lower position of the hanger of components 1+7 (FIG. 1) at the end of the crank 47, and the secondâthe upper one between the upper position of the hanger of components 1+7 (FIG. 1) and the end of the crank 47 and the lower position of the upper end of the body 35 of the accumulator 3 of cold. The power-ring 50 may be shaped like equilateral triangle, square, pentagon, hexagon and so on. Each of these power rings is connected with other one and rested upon the shell 10 (FIGS. 1 and 6) by the means of sets of the power-scape-connections 53 (FIG. 6). Each of these power-rings 50, at its internal element surface is equipped, for example, by rollers 54, such as to interact with the power-ribs 55, those are an equipment of the body 35 of the accumulator 3 of cold or (in the case of the vacuum-heat-insulation) of the enclosure of the vacuumized capacity embracing the body 35 of this accumulator 3. The quantity of sets of the power-scape-connections 51, 52 and 53, of the power-ribs 55 as well as of the devices 8 (FIG. 1) has to be not less than three and each of them has to be symmetrical to others. Any other technical solution, that keeps the alignment of the components 1+7 with the focal axis of the parabolical mirror, is acceptable as well.
Substitution of the lower (heated) part of the semiconductive thermoelectrical transformer, that may be done by the boiler (for example, by the coil-pipe-made one) and of the upper (cooled) part of this transformer, that may be done by the absorber and condenser or by only condenser (for example, by the coil-pipe-made one(s) as well), doing not change either general structure or details, got introduced in FIGS. 1+6, will be followed only by replacement of the electro-conductors from the middle zone of the thermoelectrical transformer by two pairs of tubes (groups of tubes) from those substituting heat-exchangers.
Addition of those heat-exchangers to the lower (heated) part and to the upper (cooled) part of the semiconductive thermoelectrical transformer will be followed by addition of those pairs of tubes (groups of tubes) to the electro-conductors from the middle zone of this thermoelectrical transformer.
In addition to that: the flattering of tubes and their laying in the radial order will promote in minimization of the shade upon the parabolical mirror; those of tubes which conduct the cooled medium or the medium that has to be cooled, in the zone of crossing the stream of the concentrated Sun-heat, have to be heat-insulated and protected by the heat-proof juckets; each of those tubes, under the parabolical mirror, has to have the deformable section before to be connected to its recipient.
These just aforesaid possible painless substitution & addition reflects the possible very important choice of the possible way of transformation of the âbigâ difference of temperatures of the Sun-Cosmic provenance into the electrical power and into refrigeration-output, which way may be:
the straight direct thermoelectrical transformation into the direct electro-current of the high-ampere and the low-voltage, which current is necessary for the electrolyzer to decompose water into hydrogen-oxygen and may also (for some reason) used for the opposite electro-thermo-transformation with obtaining of the cryogenic cold, but, practically, unacceptable for some powerful electro-drive;
the thermodynamical transformation into the cryogenic cold directly fulfiled by the heat-absorbing refrigeration machine;
the thermodynamical transformation fulfiled in the heat-mechanical machine and then the mechanic-electrical transformation into the electro-current of any frequency, strength and voltage to be used in any electro-drives, among them, for an air-compressor - the main part of the refrigeration machine of the air-cycle that is the one of the best way to obtain the cryogenic cold and, through it, to obtain the fresh water from the atmospheric air.
And here, it's necessary to underline that both just aforesaid thermodynamical transformations keep possibilities to get the heat of absorption and of condensation not only directly to the cosmos as a source of cold, but also to the atmospheric and water cold sources, and among them, to sources those are replenished by the accumulated cosmic cold as it is provided by the leading invention (where the parabolical mirror is not only the huge concentrator of the Sun-heat during the light days, but also the huge radiator of heat from the working medium of the huge J. Perkins' tube includes this mirror as its condenser, having its huge evaporator under the ground such as to cool up the working medium of a huge accumulator of the night cosmic cold).
Having completed the detailed description of the invention, to discuss some concomitant moments will not be unnecessary:
1) Possibilities of fouling of the working surfaces of the parabolical mirror and of the heat-radiation-transparent enclosures, which fouling is contributed by the atmospheric dust, insects and birds, has prompted the reducing coefficients 0.5 and 0.8, those, in the âupon a napkinâ calculation, take into account not only the possible incorrectness of the parabolical mirror's surface and the surely unreachable focusing upon the cylindrical surface. If, beyond this invention, the prophylactic measures to clean up these surfaces get provided by projection and are successful, the final coefficient of transformation of the light-day Sun-heat into all-day-long electro-power for the electrolyzer, which was figured out as 2% (5.4/300) will prove to be much bigger than this âupon a napkinâ one.
2) The concentrated by the parabolical mirror light-day Sun-heat is directed (by the constructive-thermal reasons) onto the cylindrical surface of the vessel 25 (FIG. 3). Such a go assumes to lose some part of Sun-heat on account of some unperpendicularity between some parts of the heat-radiation-stream and the accepting this stream cylindrical surface. The considerable part of the heat-stream, that was reflected (was not accepted) by the cylindrical surface (despite its very roughness), can be returned to this surface, being reflected by the internal surface of the one-directedly transparent for the heat-radiation wall of the enclosure 26 (FIG. 3), which internal surface directs the reflected heat-radiation athwart to the cylindrical surface of the vessel 25 (FIG. 3). If, beyond this invention, the optical projection of the enclosure 26 (FIG. 3) as well as the optical projection of the parabolical mirror get realized the expected results, the final coefficient of transformation of the light-day Sun-heat into 24 hours electro-power for the electrolyzer, so, this electro-power itself, will be bigger than it was figured out by the âupon a napkinâ calculation even more.
3) The arrangemental solution of the semiconductive thermoelectrical transformer, which is remarkable by its huge (more than 2 m2) summary area of its âhotâ or âcoldâ âp-nâ junctions and by its two (not one!) current pick-offs those are separated and belong one to the âhotâ and other to the âcoldâ end of the transformer such as to reduce losses of power for the Joule'sâheat on account of very limitation of the heat-conduction that is limited also by the very length of the middle zone between the âhotâ and the âcoldâ âp-nâ junctions, is truly extraordinary. If this arrangemental solution results in rising, up to 25%+35%, of efficiency of the semiconductive thermoelectrical transformation, as it quite may be expected, the summary coefficient of transformation of the light-day Sun-heat into the 24 hours electro-power for electrolyzer and this electro-power itself, indeed, will be additionally as much as twice bigger than their âupon a napkinâ evaluation.
4) Effectiveness of heat-transfer to the heat-exchangers which may be located in the âhotâ and âcoldâ thermostats either together with or instead of, accordingly, âhotâ and âcoldâ âp-nâ junctions of the semiconductive thermoelectrical transformer, can be expected considerably higher than it is achievable for the known steam-generators, boilers of refrigerants, absorbers and condensers in the known conditions, in so far as, being, in conditions of this invention, set in the medium which counteracts the high pressure of their working medium, these heat-exchangers may be made with their heat-transfer-wall of considerably less thickness and, at the same time, gain the coefficient of the heat-transfer to this wall from the medium they are set in. This advantage, to a full extent, concerns absorbers and condensers those are set in the accumulator of the cosmic cold provided by the leading invention to be located under the ground.
5) The ânapkinlyâ made apparent imposing sizes and weight of the apparatus got proposed by this invention concern not only and not so the accumulation, for all day long, of the light-day Sun-heat concentrated by the parabolical mirror, but, at the same time, the accumulation, for all day long, of the night cosmic cold, in the same amount. These sizes and weight are dictated by the natural factors.
So, if even the progress in the field of creating of new semiconductive, thermostatting, heat-transferring and heat-protecting materials is perspectively able to reduce a little bit the length and the weight of the totality of components are aligned with the focal axis of the parabolical mirror, the dead dependence of the radius of this mirror upon the quantity of the necessary light-day Sun-heat accumulation, upon the density of the Sun-heat-stream is given to our Earth, upon rotations of the light day and night darkness will stay the same for ever. Correlatively, it should be liked to engage one's attention to the ânapkinlyâ made apparent proportions of the parabolical mirror of 20 m in its diameter and of the 25 mâČ length of the totality of the aligned with the focal axis of this mirror components of the apparatus. Any one can see here just proportions, no disproportions,âthings are in harmony.
The Great Russian aircraft-designer of the 20th century A. N. Toopolev and many his famous Russian Contemporaries in aviation, doing not settle, were noticing, in their no confidential writings, that the beauteous machines fly better. Evidently, the French, the English, the American Greats did never doubt about it.
1. A method for conversion of the difference between the high temperature of the heat-accumulating working medium in the limited space at the focus of the parabolical mirror, where the Sun-heat-radiation gets concentrated, during the light-day hours, and the lower temperature of the cold-accumulating working medium beyond this limited space, during the night hours, into the electrical power & the difference of the thermodynamical potentials that(those) gets(get) realized and required (called for service), the clock round (during 24 hours a day), which method provides: the distributed in time receipts of the Sun-heat-radiation to the heat-accumulating working medium through the embracing this working medium one-directedly heat-radiation-transparent enclosure which, at the same time, prevents this working medium from convective heat-losses; the distributed in time heat-transfer of the accumulated heat from this working medium to the directly contacting with it, and almost got its temperature, heat-absorbing part of a heat-transformer(s)âthe âhotâ end of the semiconductive thermoelectrical transformer & a boiler of an absorption-refrigeration machine & a heat-mechanical electro-generating machine; stabilization of the high temperature of the accumulating the Sun-heat-radiation working medium by the reversible changing of the state of aggregation of some part of its mass in processes of heat-absorption and heat-transfer; the distributed in time one-directed to cosmos radiant heat-transfer from the cold-accumulating working medium through the J. Perkins' heat-conductive tube those, together, are embraced by the one-directedly heat-radiation-transparent enclosure which protects them from the convective and radiant heat-influxes; the distributed in time cold-transfer of the accumulated cold from the cold-accumulating working medium to the directly contacting with it, and almost got its temperature, heat-transferring (cooled) part of a heat-transformer(s)âthe âcoldâ end of the semiconductive thermoelectrical transformer & absorber and condenser of the refrigeration machine & condenser of the heat-mechanical electro-generating machine; stabilization of the lower temperature of the cold-accumulating working medium by the reversible changing of the state of aggregation of some part of its mass in process of heat-transfer through the J. Perkins' heat-conductive tube to cosmos and of heat-absorption from the heat-transferring (cooled) part of a heat-transformer; the according with requirements for usage transfer, by the electro-conductors & medium conductors, of the electro-potentials-difference between the âhotâ and the âcoldâ ends of the semiconductive thermoelectrical transformer & thermodynamic-potentials-difference between the heat-absorbing and the heat-transferring parts of the refrigeration & the heat-mechanical machine are realized as the refrigeration-output & as the mechanical power, generating the electrical power, & as the electrical power directly.
2. The method of claim 1, wherein the concentrated Sun-radiation-heat accumulating working medium, which stabilizes its high temperature, in processes of heat-absorption and heat-transfer, by the reversible changing of the state of aggregation of some part of its own mass, may be: either the less heat-stable heat-absorbing body located inside the more heat-stable heat-radiation-transparent enclosure, which lets the concentrated Sun-heat-radiation come in through it; or (with very little probability of some practical realization) the less heat-stable heat-radiation-transparent enclosure which lets the concentrated Sun-heat-radiation come in through it and gets heated from inside by the more heat-stable heat-absorbing body located inside this enclosure; or (with the biggest probability of the practical realization) the less heat-stable heat-absorbing body located inside an embracing more heat-stable and mechanically loadable heat-absorbing body, in its turn, located inside the heat-stable heat-radiation-transparent enclosure which lets the concentrated Sun-heat-radiation come in through it.
3. The method of claim 2, wherein the equal in the whole volume of the heat-accumulating working medium immediate (with the minimal thermoresistance) absorption of the concentrated heat of the Sun-radiation is gotten achieved by the cyclical shuffle of this working medium, together with embracing bodies of its, with regard to the focus of concentration of this radiationâthe focus of the parabolical mirror.
4. An apparatus to realize the method of claim 3, which apparatus includes the following concentric on the focal axis of the parabolical mirror components: the heat-absorbing and heat-transferring part(s) of the thermo-transformer(s)âthe semiconductive thermoelectrical transformer & heat-absorbing absorption-refrigeration machine & heat-mechanical electro-generating machine; an accumulator of the concentrated Sun-radiation-heatâthe thermostat for the heat-absorbing (heated) âhotâ âp-nâ junction(s) of the semiconductive thermoelectrical transformer & for boiler of the absorption-refrigeration machine & of the heat-mechanical electro-generating machine, all of which are immersed in the heat-accumulating thermostatting âhotâ working medium, which working medium is embraced by the enclosure, which, being one-directedly transparent for the receipts of the heat-radiation lets these receipts come only in through its thickness from outside and, at the same time, prevents this working medium from convective heat-losses; an accumulator of coldâthe thermostat for the heat-transferring (cooled) âcoldâ âp-nâ junction(s) of the semiconductive thermoelectrical transformer & for absorber and condenser of the absorption-refrigeration machine & for condenser of the heat-mechanical electro-generating machine, all of which are immersed in the cold-accumulating thermostatting âcoldâ working medium, which is located inside the enclosure, which prevents this working medium from the convective and radiant heat-exchange with the external surroundings, and which working medium gets the heat-receipts from the thermostatted âcoldâ (cooled) part(s) of the thermo-transformer(s) to cosmos through the heat-conductive J. Perkins' tube, which tube is gotten to keep its evaporator immersed in just this âcoldâ working medium and its condenser insulated from any external convective and radiant heat-influxesâso, able to work only as a heat-radiator to the external surroundings; conductors, which are in the form of electro-current collectors (buses) those complete the electro-circuit of the semiconductive thermoelectrical transformer and its electro-recipient(s) & in the form of the working-mediums-conductive tubes those set the heat-absorbing and heat-transferring (cooled) parts of the refrigeration & heat-mechanical electro-generating machine into the closed heat-contour of one & other of these machines; the bearing and driving elements for cyclical reciprocated shuffles of the âhotâ working medium together with its embracing bodies in composition of the accumulator of the concentrated Sun-radiation-heat, with regard to the focus of concentration of this heat at the axis of the parabolical mirror.
5. The apparatus of claim 4, wherein all its components, except the bearing and driving elements, are located in the cylindrical space, the axis of which concurs with the focal axis of the concentrating the Sun-radiation-heat parabolical mirror, so, during the light-day hours, stays directed to the centre of the Sun-disk, and, projecting upon this mirror a shadow with diameter incommensurably smaller than diameter of this mirror, are disposed in the following, from below (from the mirror) order: the cylinder of the accumulator of the concentrated Sun-radiation-heat together with the immersed in it heat-absorbing âhotâ parts of the heat-transformers, among which parts, the âhotâ âp-nâ junction(s) of the semiconductive thermoelectrical transformer takes (take) the top location which closes this accumulator from above; the cylinder of the lengthy middle zone of the semiconductive thermoelectrical transformer, which zone gives the beginning of the electro-current-collectors those are directed downwards (along the cylinder of the heat-accumulator and, after having gotten accompanied with tubes from the heat-absorbing parts (boilers) of the absorption-refrigeration & heat-mechanical machines, through the central hole in the parabolical mirror) to the space under the mirror; the cylinder of the accumulator of cold, together with the immersed in it heat-transferring (cooled) âcoldâ parts of the heat-transformers, among which, the âcoldâ âp-nâ junction(s) of the semiconductive thermoelectrical transformer takes (take) the bottom location which closes this accumulator from below, together with tubes from the cooled in this accumulator parts of the absorption-refrigeration & heat-mechanical electro-generating machines, which tubes are directed also to the space under the parabolical mirrorâ, at first, along this cylinder, and, then, being accompanied by the electro-current-collectors and tubes from the heat-absorbing parts of these machines, together with the immersed in it evaporator of the heat-conductive J. Perkins' tube, together with the cylinder of the condenser of this J. Perkins' tube which closes the accumulator of cold from above; and in this composition, cylinders of accumulators of heat and of cold, having inside themselves the according parts of the semiconductive thermoelectrical transformer and holding the lengthy middle zone of this thermoelectrical transformer fixed between them, are stiffly connected with each other, so, the upper of themâthe cylinder of the accumulator of cold accepts the summary force and the summary reaction of the bearing and driving elements, which, being, in their turn, beared through the load-receiving shell, upon the circular edge of the parabolical mirror, support and shuffle these stiffy connected components as the united dynamical load.
6. The apparatus of claim 5, wherein the semiconductive thermoelectrical transformer is fulfiled from (tens of) the radially packed in the cylindrical room pairs of the most thermo-stable semiconductive wafers of âpâ and ânâ types (properties), which wafers in each of their pairs are in the ideal electrical (electron-vacancy) contact along the surface of their fit, which surface is just the âp-nâ transition along each of the lengthy ends of these wafers' pairs, one of which ends is immersed in the âhotâ and other of themâin the âcoldâ thermostat, accordingly, of the âhotâ accumulator of the Sun-radiation-heat and of the âcoldâ accumulator of the cosmic cold; which wafers, in the same their pairs, but along the lengthy middle (between the âhotâ and âcoldâ âp-nâ transitionsâjunctions) zone of theirs, are completely electro-insulated from each other along the same surface of their fit; which wafers are mechanically, thermally, and electrically integrated into the united composition: at their âhotâ and âcoldâ ends,âby the V-shaped profiles (sections) which are in the ideal electrical and thermal contact, by turns (alternatively), with the pairs of wafers of the same âpâ or the same ânâ type and perform functions of the mechanical carcass, heat-conductors, and equalizers of âpâ and ânâ electro-potentials along the joint lengthy area of two wafers of âpâ or ânâ property; and at their lengthy middle zone, separatedly at the âhotâ and the âcoldâ end of this zone,âby the high electro-conductive metal wedges which are protected from electro-contacts with each other and with the V-shaped profiles (sections), but are united with each other (with the ideal electrical and thermal contact), over one, by the means of the annular bandages of the positive and negative electro-collectors (buses) which bandages are one above other, do not contact with each other, are covered with electro-insulation, and are prolonged separatedly by these collectors, directed downwards, along the âhotâ accumulator, under-to the parabolical mirror.
7. The apparatus of claim 6, wherein the heat-absorbing, heat-standing vessel of the accumulator of the concentrated Sun-radiation-heat, within the upper part of its cylindrical capacity, occupied by the hermetically immersed in it âhotâ âp-nâ junction(s) of the semiconductive thermoelectrical transformer, is filled with the melted dielectric (for example, glass) of its density and temperature some lower than the density and temperature of the heat-accumulating, thermostatting (for example, metallic) working medium, occupying the rest capacity of this vessel, which vessel is embraced by the one-directedly (from outside-to inside) heat-radiation-transparent enclosure (for example, made from the heat-standing glass); the cavity between this enclosure and this vessel is hermetically sealed and vacuumized; the wall of this enclosure is protected (from its internal side) by the heat-insulating flexible juts from destruction by the atmospheric pressure and, at the same time, the surface of this side of this wall is gotten treated such as to return that part of the concentrated Sun-heat-radiation which leaves the surface of this vessel, because of some inperpendicularity of falling upon this surface, back quite perpendicularily to this surface, while the outer side of this wall is kept smoothly cylindricalâso, easy cleanseable from the possible pollutions.
8. The apparatus of claim 7, wherein the insulated from the convective and radiant heat-exchange with surroundings enclosure which comprises the âcoldââcold-accumulating working medium, together with the immersed in this working medium heat-transferring (cooled) part(s) of the heat-transformer(s) and of the heat-absorbing evaporator of the heat-conductive J. Perkins' tube, is just the hollow cylinder, which is hermetically closed from below by the âcoldâ âp-nâ junction(s) of the semiconductive thermoelectrical transformer and by the continuing the anticorrosive, heat-conductive electro-insulation of the surface of this immersed in that working medium transformer washer and casing those, together, are embracing the lower edge of the outer surface of this cylinder, which cylinder closed also from aboveâby the middle section of the J. Perkins' tube, between its evaporator and its condenser, the heat-radiative surface of which condenser is radically developed with the deeply goffered corrugations and protected from pollutions and outer radiant and convective heat-influxes by the means of the smooth, easy-cleansable, one-directedly (from inside to outside) heat-radiation-transparent (for example, the mirror-glassy) enclosure, the cavity between which enclosure and the corrugated surface of this condenser is hermetically sealed, vacuumized, and protected from destruction by the atmospheric pressure.
9. The apparatus of claim 8, herein all electro-collectors (buses) and those of tubes which conduct as the subjected to be cooled as the gotten cooled mediums, at their sections where they intersect the directed from the surface of the parabolical mirror to its focus streams of the concentrated radiation of the Sun-heat, are protected, by the heat-standing jackets, from getting heated in this stream; in the space under the parabolical mirror, each of electro-collectors (buses) and each of tubes, before to be connected to one's moveless expectant, has its deformable sectionâcompensator of its possible cyclical reciprocated shuffles together with other components are above the parabolical mirror; and, in addition to that, each of positive and negative electro-collectors (buses) those take their beginning from one of two thermally separated positive annular bandages, accordingly, at the âcoldâ and âhotâ ends of the middle zone of the semiconductive thermoelectrical transformer, as well as from one of two thermally separated negative annular bandages also at the âcoldâ and âhotâ ends of this middle zone, is thermally separated from the rest of electro-collectors (buses) along all its length until its connection to its (their) expectant.