TURBINE AND METHOD FOR THE ROTATION THEREOF
20210115891 · 2021-04-22
Inventors
Cpc classification
F05B2240/9176
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F05B2210/16
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F05B2240/30
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F03B17/061
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F03D1/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F03D1/0608
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Y02E10/72
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
F05B2240/92
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Y02E10/30
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
F05B2250/15
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F05B2240/93
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F03B3/12
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F03D1/0625
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F05B2240/20
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
F03B17/06
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
The present turbine is intended for use in the field of renewable energy. The turbine comprises a rotor with a guide apparatus disposed thereon, said guide apparatus having inlets for a working fluid which are in the form of ducts that spiral around each other in helices and have nozzles situated along a tangent to the circle of rotation. The guide apparatus is configured in the form of adjacent ducts which are open along their entire length or along at least a significant portion of their length and are situated on second order surfaces of revolution or on portions of such surfaces, and in particular on convex-concave surfaces of the pseudosphere type with a cone in the pole of an axial cowl of the rotor. The result is in simplification of the structure and reduction in the turbine mass, the gyroscopic effect and the starting speed of the working fluid.
Claims
1. A turbine containing the rotor (1) with a guide apparatus holding a working fluid inlet in a form of ducts (K) that spiral around each other in helices or similar way, with nozzles (C) situated along a tangent to a circle of rotation or close to a tangent, that differs in that the guide apparatus is made in the form of adjacent ducts (K) which are open along a whole length or at least a considerable length and are situated on second order surfaces of revolution, or on portions of such surfaces, or on combinations of these portions, in particular on convex-concave surfaces of a pseudosphere type with a cone in a pole of an axial cowl (O) of a rotor (1).
2. The turbine of claim 1 differs in that the ducts (K) of the guide apparatus have a form of smooth function spirals such as a logarithmic spiral with increasing pitch, an Archimedes spiral with constant pitch, a Fermat spiral with pitch reducing in a projection on a plane, or a loxodromic curve.
3. The turbine of claim 1 differs in that the ducts (K) of the guide apparatus have a form of spirals with quasismooth function and arranged along paths gradually approaching nozzle (C) angles or close to it.
4. The turbine of claim 1 differs in that the ducts (K) of the guide apparatus are made on the axial cowl (O) with ribbons (2) or ribbon-like elements parallel to an axis of rotation.
5. The turbine of claim 4 differs in that the ribbons (2) have such elasticity and are connected in the nozzle area (C) with the surface of revolution at such an arc size that, should a specified angular velocity of the turbine be exceeded, the ribbons (2) can be slightly straightened under an influence of centrifugal forces to change a nozzle (C) cross-section.
6. The turbine of claim 1 differs in that the ducts (K) of the guide apparatus are formed with ribbons (2) or ribbon-like elements such as chutes, in a form of helicoidal surface.
7.-9. (canceled)
10. The turbine of claim 1 differs in that the axial cowl (O) is inflatable.
11. The turbine of claim 1 differs in that the axial cowl (O) is designed in a form of a tethered aerostat, mostly drop-shaped and quasispheroidal with a cone in a pole, and the nozzles (C) are located in a diameter zone of a maximum cross-section.
12. The turbine of claim 11 differs in that the tethered aerostat is made with an inflatable shell ring (17) with the ducts (K) inside.
13. The turbine of claim 11 differs in that the tethered aerostat is made with an inflatable shell ring with the ducts (K) both inside and outside.
14. The turbine in of claim 1 differs in that it is designed with a dome in a form of a round parachute with its shrouds (11) connected to a shaft (3), in particular telescopic one, as well as to additional shrouds fixed to the dome in a zone of the nozzles (C) circle and are wrapped with flexible material as the axial cowl (O).
15. The turbine of claim 14 differs in that the axial cowl (O) is designed as a top part of the dome turned out inside, towards the nozzles (C).
16. The turbine of claim 15 differs in that the turned out part of the dome is closed and inflatable.
17. The turbine of claim 14 differs in that the dome, at least before its intersection with the axial cowl, is multi-walled, at least two-walled, and is multi-ducted with inlets in its face part and with bypass holes in its rear part, designed with such parameters that ensure maintaining a specified dome shape with velocity pressure of working fluid at minimal operating speed.
18. The turbine of claim 1 differs in that it is designed with the dome (21) in a form of an umbrella, in particular with a telescopic shaft and guy lines (18) wrapped with flexible material as the axial cowl (O) and spokes (Sh) are connected to the shaft (3) with the shrouds (11) on a periphery.
19. The turbine of claim 18 differs in that the axial cowl (O) is designed in a form of a tethered aerostat penetrating the dome (21).
20. (canceled)
21. The turbine of claim 11 differs in that the tethered aerostat is connected to a kite (14) which is in particular has a structure of a paraplane with a multi-ducted dome or with an airplane wing profile.
22. The turbine of claim 21 differs in that the dome ducts (H), at least part of them, are closed and inflatable.
23.-28. (canceled)
29. A method for turbine rotation, according to which a working fluid is divided into several flows and is directed, along helical or similar paths spiraling each other, into nozzles located along a tangent to a circle of their rotation or close to it, according the invention, differs in that the continuous flow of working fluid is divided into adjacent ducts which are open along a whole length or at least a considerable part.
30.-31. (canceled)
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0054] The concept of the invention is explained with the drawings containing the following:
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[0088] The dotted arrows indicate direction of working fluid, the curved arrow indicates direction of the turbine rotation.
[0089] All the drawings are made as technical sketches.
PREFERRED EMBODIMENT OF THE INVENTION
[0090] The claimed turbine (
[0091] The ducts K of the guide apparatus can be placed in the form of helices with smooth function such as a logarithmic spiral (
[0092] The ducts of the guide apparatus can be formed on the axial cowl with ribbons or ribbon-like elements running parallel to the axis of rotation. These ribbons can have such elasticity and are connected in the nozzle area to the surface of revolution at such an arc size that, should the specified angular velocity of the turbine be exceeded, the ribbons can be slightly straightened under the influence of centrifugal forces to change the nozzle cross-section.
[0093] The ducts of the guide apparatus can be formed with ribbons of ribbon-like elements such as chutes in the shape of helicoidal surfaces that can be bordered with an axial cowl and a shell ring (
[0094] An axial cowl can be inflatable (
[0095] The turbine can be designed with a dome in the form of a round parachute with shrouds (
[0096] In this option, the dome, at least before the intersection with the axial cowl, can be multi-walled, at least two-walled, and is multi-ducted with inlets in its face part and bypass holes in its rear part, made with such parameters that ensure maintaining the specified dome shape with velocity pressure of working fluid at minimal operating speed. Moreover, the ducts can be closed and inflatable.
[0097] The dome can be designed in the form of an umbrella with a shaft, in particular a telescopic one (
[0098] The axial cowl can be designed in the form of a tethered aerostat penetrating the dome. The aerostat can be connected to a kite (
[0099] The duct inlets on the axial cowl (
[0100] The turbine has such a number of nozzles and such parameters that at the rated speed of working fluid the total capacity of the nozzles approaches that of the working fluid inlets.
[0101] The outside turbine surfaces can be coated, at least partially, with photovoltaic elements, particularly thin-film ones.
[0102] The drawings contain several examples of the turbine design.
[0103] The wind turbine (
[0104] The operating principle of the turbine is explained below.
[0105] Flow of working fluid (wind) strikes the operating (swept) surface of the wind turbine, moves inside the open helical ducts K, compresses, accelerates under influence of centrifugal and other forces, while additional masses are joining during ejection process and move towards the nozzles C. In rated mode, layers of working fluid (air) move through the ducts along the corresponding immutable plane running through the point where air layer contacts the turbine and axis of its rotation. The jet reaction force from the nozzles C creates torque on the shaft 3 of the rotor 1. In case of exceeding the rated angular speed, the parts of helical ribbons 2 that are not fixed on the periphery are straighten (pos. B on
[0106] The hydro turbine (
[0107] The hydro turbine works like the wind turbine described above (
[0108] The hydro turbine (
[0109] The hydro turbine works like the hydro turbine described above (
[0110] The wind turbine (
OPERATION OF THE INVENTION
[0111] The operating principle of the turbine is explained below.
[0112] Flow of working fluid (wind) strikes the operating surface of the swept wind turbine (the open ducts K), compresses, accelerates under influence of centrifugal and other forces, and moves towards the nozzles C. Torque is created partly because the working fluid changes its direction and partly thanks to jet forces of the nozzles C.
[0113] The hydro turbine (
[0114] The hydro turbine works like the turbine described above (
[0115] The wind turbine (
[0116] The wind turbine works like the wind turbine described above (
[0117] The wind turbine (
[0118] The wind turbine works like the wind turbine described above (
[0119] The wind turbine (
[0120] The wind turbine works like the wind turbine described above (
[0121] The wind turbine (
[0122] The wind turbine works like the wind turbine described above (
[0123] The wind turbine (
[0124] The wind turbine works like the wind turbine described above (
[0125] The wind turbine-umbrella on the tethered aerostat (
[0126] The wind turbine works like the wind turbine described above (
[0127] The claimed method is to be embodied as follows.
[0128] Working fluid (liquid, gas) is distributed into several flows that are directed along the helical paths spiraling each other into the nozzles situated along a tangent to the circle of rotation thereof or close to a tangent. Continuous flow of working fluid is divided into adjacent flows that are open over their total length or at least over significant part of their length.
[0129] The flows can be directed along paths in the form of a spiral with smooth function such as an Archimedes spiral with constant pitch, a Fermat spiral with pitch decreasing in a projection on a plane, and loxodromic curves, as well as along paths in the form of spirals with quasismooth function, namely paths gradually closing to the nozzle angles.
[0130] An example. In the wind turbine (