WO2009074123A1 - Fliehkraft-richtantrieb - Google Patents
Fliehkraft-richtantrieb Download PDFInfo
- Publication number
- WO2009074123A1 WO2009074123A1 PCT/DE2007/002241 DE2007002241W WO2009074123A1 WO 2009074123 A1 WO2009074123 A1 WO 2009074123A1 DE 2007002241 W DE2007002241 W DE 2007002241W WO 2009074123 A1 WO2009074123 A1 WO 2009074123A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- flywheels
- force
- rotation
- center
- centrifugal force
- Prior art date
Links
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims abstract description 4
- 230000005484 gravity Effects 0.000 claims description 6
- 230000000694 effects Effects 0.000 claims description 5
- 238000010276 construction Methods 0.000 claims description 2
- 230000003993 interaction Effects 0.000 claims 1
- 230000002146 bilateral effect Effects 0.000 description 1
- 239000002775 capsule Substances 0.000 description 1
- 238000002485 combustion reaction Methods 0.000 description 1
- 230000001066 destructive effect Effects 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 238000005461 lubrication Methods 0.000 description 1
- 238000010248 power generation Methods 0.000 description 1
- 230000000284 resting effect Effects 0.000 description 1
- 230000000087 stabilizing effect Effects 0.000 description 1
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F03—MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
- F03G—SPRING, WEIGHT, INERTIA OR LIKE MOTORS; MECHANICAL-POWER PRODUCING DEVICES OR MECHANISMS, NOT OTHERWISE PROVIDED FOR OR USING ENERGY SOURCES NOT OTHERWISE PROVIDED FOR
- F03G3/00—Other motors, e.g. gravity or inertia motors
- F03G3/08—Other motors, e.g. gravity or inertia motors using flywheels
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B64—AIRCRAFT; AVIATION; COSMONAUTICS
- B64G—COSMONAUTICS; VEHICLES OR EQUIPMENT THEREFOR
- B64G1/00—Cosmonautic vehicles
- B64G1/22—Parts of, or equipment specially adapted for fitting in or to, cosmonautic vehicles
- B64G1/40—Arrangements or adaptations of propulsion systems
- B64G1/409—Unconventional spacecraft propulsion systems
Definitions
- the centrifugal force formula F mv 2 / r contains the solution of all energy, traffic and many environmental problems if it is possible to use the force that increases with the velocity of revolution v squared.
- This invention shows the solution to this problem by arranging rotating flywheels in a circle and moving them so as to produce a directed centrifugal force which is adjustable over 360 ° in any desired direction and without supporting media such as earth, water, air or recoil combustion acts. It can also be directed against Earth's gravity so that it can serve as a propulsion for all aircraft and spacecraft.
- the respective achieved speed is always zero, so that any desired speed can be eneichi.
- the force is set to brake against the direction of travel, so it increases according to the driving or airspeed and can be destructive in careless handling.
- the self-contained leveling drives are always in pairs and against each other rotatable and directional to arrange. Thus, without changing the rotational speed of the rotating flywheels, it is possible to instantaneously set any force effect from zero to maximum only by adjusting the direction of the force.
- centrifugal drive Like all current vehicle engines, the centrifugal drive also requires a resting energy in the form of a battery to start.
- Two battery-powered direct current motors use their centrifugal clutches with V-belt pulleys to lift the centrifugal drives. Then only the frictional losses are covered, so that a drive motor can be switched off.
- the directed centrifugal force now acts from its center of rotation in the respective predetermined direction. With each increase in speed, the speed increases to the square, so four times and causes the quadrupling of the force F, without requiring four times the drive power. Of course, no directed centrifugal force to produce without counter forces occur.
- the ratio is 1: 1, 68, z. B. 1000 N down and 1680 N upwards, free centrifugal force 680 N. The calculation according to Figure 10 proves this.
- Raising the leveling drives requires the greatest amount of energy that the dormant energy has to supply. Wherever space is possible, a small, adapted home power plant should be placed in front of you to always be on the safe side. In the following alternative possibilities of energy supply will be shown.
- the power is supplied by a home power plant, but over 2 opposing discs, on which small straightening drives are installed. The opposite rotation is transmitted via a countershaft on 2 generators. The opposing discs are required anyway because of their stabilizing gyro effect.
- the astronauts no longer need to start helplessly strapped to a "fire chair" and on their return fear to burn up in the air.
- the flexibility and speed of the space capsule is unlimited and the braking capability gives extra security.
- the lighter traffic can be laid almost accident-free on light-marked, wide one-way streets, at any speed the same height is assigned. If these streets spiral in the cities, every point of the city can be reached.
- the energy supply is also provided by lateral wind turbines and the foreigners start is also possible.
- a control shaft 12 is mounted, which controls the centrifugal force via a worm gear with stepper motor 13. This does not apply to energy generation, because centrifugal force only acts in the direction of rotation and can therefore be permanently adjusted.
- a blind hole with thread for screwing a threaded rod located at the end of the control shaft 12 is a blind hole with thread for screwing a threaded rod.
- the lateral bearing discs l ⁇ a + b are connected to each other via threaded rods and the outer casing 33 as a housing and freely rotatably mounted on the S85welle 12.
- 2 control motors 17 carry centrifugal clutches with V-belt pulleys and drive via the V-belt pulley 18 of the right side wall 16b to the machine.
- closed forks 19 with bilateral shaft ends 20a + b flywheels 21 are arranged, which revolve on a countershaft 22 driven high speed.
- the sprocket 23 and the gear 24 are connected together and mounted on the shaft end 20a of the geared side 22, freely rotatable so that the gear 24 engages the gear of the countershaft 22.
- the other shaft side 20b is fixedly connected to the sprocket 25 and both shaft ends 20a + b are freely rotatably mounted in the lateral bearing discs l ⁇ a + b.
- the planet gear 26 engages the gear 15 and is fixedly connected to the sprocket 27. From the side wall 16a protrudes a self-supporting shaft end 28 on which the pennet 26 and the sprocket 27 are freely rotatably mounted.
- flywheels 21 are arranged at the same angular distance. See Fig. 9 and 10. The structure of Fig.
- the flywheels are constructed in a trapezoidal shape, so that their weight mass and thus the center of gravity y is displaced outwards.
- the flywheels are clamped axially fixed by a clamping sleeve.
- a clamping sleeve Between the forks 19 preloaded axial cylindrical roller bearings stabilize the flywheels in addition. All chains, sprockets, gears, shaft bearings of the countershaft, etc., are not burdened by the centrifugal force generated. This guarantees a long service life with the intended splash lubrication, during which only the oil must be changed and the chains must be re-tensioned.
- the sprocket 14 and all 7 or 8 Kettenmann- 25 on the fork shaft 20b are connected to each other via a timing chain 29.
- the ratio between the sprocket 14 and the sprockets 25 is always 1: 2, so that the forks 19 rotate with the flywheels 21 by 180 °, while the side bearing discs 16a + b, with everything that is stored in them, by 360 ° Perform full rotation.
- the center of gravity Y of the flywheel 21 has the same rotational speed v as the side windows l ⁇ a + b (as a housing) in the radius R. From the views A and B can be seen: when a flywheel half 21 a rotates with the housing, the other must Turn the flywheel half 21 b to the opposite direction.
Landscapes
- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Remote Sensing (AREA)
- Aviation & Aerospace Engineering (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Connection Of Motors, Electrical Generators, Mechanical Devices, And The Like (AREA)
Abstract
Description
Claims
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
PCT/DE2007/002241 WO2009074123A1 (de) | 2007-12-12 | 2007-12-12 | Fliehkraft-richtantrieb |
DE112007003757T DE112007003757A5 (de) | 2007-12-12 | 2007-12-12 | Fliehkraft-Richtantrieb |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
PCT/DE2007/002241 WO2009074123A1 (de) | 2007-12-12 | 2007-12-12 | Fliehkraft-richtantrieb |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2009074123A1 true WO2009074123A1 (de) | 2009-06-18 |
Family
ID=40433839
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/DE2007/002241 WO2009074123A1 (de) | 2007-12-12 | 2007-12-12 | Fliehkraft-richtantrieb |
Country Status (2)
Country | Link |
---|---|
DE (1) | DE112007003757A5 (de) |
WO (1) | WO2009074123A1 (de) |
Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR1308410A (fr) * | 1961-12-21 | 1962-11-03 | Dispositif pour le déplacement omnidirectionnel d'un véhicule | |
US3653269A (en) * | 1970-05-15 | 1972-04-04 | Richard E Foster | Converting rotary motion into unidirectional motion |
US3691853A (en) * | 1970-07-27 | 1972-09-19 | North American Rockwell | Torque generator |
FR2293608A1 (fr) * | 1974-12-03 | 1976-07-02 | Siritzky Alain | Moteur gyroscopique |
WO1988004364A1 (en) * | 1986-12-09 | 1988-06-16 | University Of Dundee | Gyroscopic thrust apparatus |
WO1991002155A1 (en) * | 1989-08-09 | 1991-02-21 | Delroy Mortimer S | Gyrostat propulsion system |
US5167163A (en) * | 1982-09-29 | 1992-12-01 | Mcmahon John C | Energy transfer device |
US20010032522A1 (en) * | 2000-01-24 | 2001-10-25 | Ulysses Davis | Vectored inertia drive wobble drive |
WO2007084090A1 (en) * | 2006-01-20 | 2007-07-26 | Lykhovyd Yuriy M | Method of generating coriolis's levitation forces and a gyroscopic system ('gyro-turbine') |
-
2007
- 2007-12-12 WO PCT/DE2007/002241 patent/WO2009074123A1/de active Application Filing
- 2007-12-12 DE DE112007003757T patent/DE112007003757A5/de not_active Withdrawn
Patent Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR1308410A (fr) * | 1961-12-21 | 1962-11-03 | Dispositif pour le déplacement omnidirectionnel d'un véhicule | |
US3653269A (en) * | 1970-05-15 | 1972-04-04 | Richard E Foster | Converting rotary motion into unidirectional motion |
US3691853A (en) * | 1970-07-27 | 1972-09-19 | North American Rockwell | Torque generator |
FR2293608A1 (fr) * | 1974-12-03 | 1976-07-02 | Siritzky Alain | Moteur gyroscopique |
US5167163A (en) * | 1982-09-29 | 1992-12-01 | Mcmahon John C | Energy transfer device |
WO1988004364A1 (en) * | 1986-12-09 | 1988-06-16 | University Of Dundee | Gyroscopic thrust apparatus |
WO1991002155A1 (en) * | 1989-08-09 | 1991-02-21 | Delroy Mortimer S | Gyrostat propulsion system |
US20010032522A1 (en) * | 2000-01-24 | 2001-10-25 | Ulysses Davis | Vectored inertia drive wobble drive |
WO2007084090A1 (en) * | 2006-01-20 | 2007-07-26 | Lykhovyd Yuriy M | Method of generating coriolis's levitation forces and a gyroscopic system ('gyro-turbine') |
Also Published As
Publication number | Publication date |
---|---|
DE112007003757A5 (de) | 2010-11-11 |
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