WO1992016746A1 - Entrainement centrifuge - Google Patents

Entrainement centrifuge Download PDF

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Publication number
WO1992016746A1
WO1992016746A1 PCT/EP1992/000536 EP9200536W WO9216746A1 WO 1992016746 A1 WO1992016746 A1 WO 1992016746A1 EP 9200536 W EP9200536 W EP 9200536W WO 9216746 A1 WO9216746 A1 WO 9216746A1
Authority
WO
WIPO (PCT)
Prior art keywords
centrifugal
flywheels
drive according
track
loop
Prior art date
Application number
PCT/EP1992/000536
Other languages
German (de)
English (en)
Inventor
Reinhold Will
Original Assignee
Reinhold Will
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Reinhold Will filed Critical Reinhold Will
Publication of WO1992016746A1 publication Critical patent/WO1992016746A1/fr

Links

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

Definitions

  • the invention relates to a centrifugal drive by means of guided flywheels.
  • the object of the invention is to create a centrifugal drive by means of guided centrifugal masses, which generates a continuously acting, directed thrust force, which, moreover, builds up the centrifugal force without support from its center of rotation, even without support on a medium such as earth , Water, air or fire works.
  • a guideway pattern is e.g. can be produced as follows: a paper strip approx. 300 mm long and 15 mm wide is held at one end and rotated by 360 ° at the other end, after which the two ends are joined together, e.g. by gluing.
  • the thrust force released increases with the angular velocity ⁇ or the velocity v squared, so that with a relatively small centrifugal force drive considerable thrust forces can be generated which act without the support media mentioned.
  • the acceleration power does not need to be much greater than is needed to cover the friction losses if the primary drive has enough time to start up the flywheel masses.
  • centrifugal drive is not to be dimensioned according to the force-power principle, but, in comparison with the conventional drives, requires less than 2% of the drive power in order to achieve an equally large thrust force. produce.
  • the centrifugal drive is not to be dimensioned according to the force-power principle, but, in comparison with the conventional drives, requires less than 2% of the drive power in order to achieve an equally large thrust force. produce.
  • not every near-earth vehicle has to carry its own energy generator, which is useful for ships or space vehicles, preferably as an arrangement according to claim 11 and / or as a solar generator.
  • a conventional battery pack which allows an electric car to drive only about 125 km with a charge, is more than sufficient, because, because of the 98% energy saving according to the invention, about 6,000 km can be driven with a charge according to the invention.
  • the centrifugal drive according to the invention only reacts to external accelerations and decelerations, and it behaves at constant speed as if it were not present.
  • a FÜehkiaft drive according to the invention is sufficient for accelerating and braking if it is arranged pivotably in the direction of travel.
  • the thrust is directed downwards when the vehicle is at a standstill and forwards or backwards when driving or braking.
  • the flywheels can rotate at a constant speed.
  • gravity acts as a stabilizing counter pole, and the thrust of the individual centrifugal drives can be directed so that they cancel each other out, add up or act as the resulting thrust.
  • centrifugal drives For space vehicles that need to stabilize without an opposite pole, three or more centrifugal drives according to the invention are required in order to enable all control nanoevers quickly and precisely. Otherwise, the structure is similar to that for suspended traffic near the earth.
  • US -A- 4884465 ZACHYTAL
  • DE -B- 1 476678 DE -B- 1 476678
  • DE -A- 2046865 POHLIG - HECKEL - BLEICHERT ... AG: a "balancing gear" with the same structure and operation as above in US -A- 4 884465 and DE -B- 1 467 678 is intended for upward thrust forces produce.
  • FR -A- 2216461 states that the masses circulating within a circular path produce a directed centrifugal force when the motor driving the masses is displaced from its central position.
  • the masses are flexibly connected to the drive, the drive axle displacement does not even create an imbalance, let alone a directed centrifugal force.
  • the masses continue to follow their given path as if they were circling around a fixed wave.
  • FIG. 1 in two views each an embodiment of the Füehkraft- drive according to the invention, wherein Fig. 2 on the left shows a (greatly enlarged) section A - A of Fig. 1;
  • Flg. 4 shows another exemplary embodiment of the electromagnetic primary drive for smaller centrifugal drives
  • Fig. 5 in two views eight centrifugal drives mounted on two opposite axles to drive four generators via a planetary gear.
  • flywheels 2 On a twisted 8 (eight) similar guideway 1, as many flywheels 2 are arranged as possible, each of which is carried by roller carriages 3 with six rollers 4 each and, if possible, in the neutral point by tension or pressure elements, e.g. . B. a rope 5 are kept at the same mutual (minimum) distance.
  • roller portion can be halved by a different track profile or a direct ball guide can be installed.
  • the guide track 1 causes the flywheel masses 2 to change their center of gravity distance r and thus their track speed v twice during one revolution, so that a directional centrifugal thrust F s arises which can be calculated on the basis of the centrifugal force law:
  • the guide track 1 is suspended via a circumferential rib at three points on the (only schematically indicated) housing, namely at the bottom the led-out rib is connected directly to the housing and indirectly via the pipe 11 via a tube 11 to the housing.
  • the guideway 1 can be left or right-handed, so that undesired side thrusts are neutralized when arranged in pairs.
  • the path twist always runs in the specified direction of rotation, and the twist angle is the same everywhere, even on the straight connecting sections between the path loops.
  • roller carriages 3 are accordingly positioned at an angle ⁇ relative to one another, namely by beveling the roller carriage connecting plates 6 on both sides:
  • Each flywheel 2 is pivotally screwed to the roller carriage 3 with two bolts 7.
  • the movable mass suspension between the springs 8 extends the acceleration or deceleration path and thus reduces the load.
  • the permanent magnet strips 12 are arranged in such a way that their force field holds the flywheels 2 in the central position and enables a wear-free compensation stroke on both sides. With this construction, however, elastic stroke limits (not shown) are expedient.
  • the permanent magnet strips 12 can also be arranged in such a way that the repelling poles interact with one another frontally.
  • An electromagnetic primary drive for the flywheels 2 resembles a cut-open and stretched squirrel-cage motor, cages with anchor rods 9 being fastened to the roller carriages 3, while a field winding 10 is arranged stationary over the straight connecting sections of the guideway 1.
  • Magnetic coils 13 are arranged in pairs above the straight connecting sections of the guideway 1 and act on soft-iron plates 14 on the roller carriage 3 by means of electronic pulse control (not shown) which is known per se.
  • the direction of rotation Z is predetermined by an actuation clock IV.
  • the one soft iron plate 14 was pulled in the clock position I to the middle of the coil, while the previous soft iron plate 14 reached the coil edge in the clock position ⁇ .
  • FIG. 1 shows in two views an arrangement in which eight centrifugal drives 16 according to the invention are mounted on two opposite axles 17 and 18 and drive four generators 20 via a planetary gear.
  • This arrangement shows how the required high output speed can be achieved even with slowly rotating axles 17 and 18.
  • the upper axis cross 17 acts via an internal ring gear 21 and the lower axis cross 18 via a web 22 on a gear 23 and further via
  • a bevel gear 26 is used to distribute the gear to the four generators 20 via a countershaft 27, which enables flexible adaptation to the power required in each case.
  • Two FÜeMcraft drives 16 each generate the torque for one generator 20 and form the smallest unit in this arrangement.

Landscapes

  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Connection Of Motors, Electrical Generators, Mechanical Devices, And The Like (AREA)

Abstract

Entraînement centrifuge au moyen de masses centrifuges entraînées (2), caractérisé par une glissière de guidage sans fin (1), similaire à un huit bouclé sur lui-même, avec deux boucles de glissière reliées par des sections de liaison droites, de telle sorte que lors d'un tour sur la glissière de guidage (1), chaque masse centrifuge (2) glisse une fois sur la face externe de l'une des boucles de glissière et une fois sur la face interne de l'autre boucle de glissière, avec une distance au centre de gravité différente (r1 ou r2) par rapport au centre de boucle de glissière respectif, et par conséquent avec une vitesse de glissière différente (v1 ou v2), de manière à ce que, comme différence des forces centrifuges différentes dans des zones angulaires opposées (alpha) des boucles de glissière, une force de poussée (Fs) agisse vers l'extérieur depuis la boucle de glissière, avec une distance au centre de gravité (r1) plus grande des masses centrifuges (2).
PCT/EP1992/000536 1991-03-14 1992-03-11 Entrainement centrifuge WO1992016746A1 (fr)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
EP91103919 1991-03-14
EP91103919.6 1991-03-14

Publications (1)

Publication Number Publication Date
WO1992016746A1 true WO1992016746A1 (fr) 1992-10-01

Family

ID=8206515

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/EP1992/000536 WO1992016746A1 (fr) 1991-03-14 1992-03-11 Entrainement centrifuge

Country Status (3)

Country Link
AU (1) AU1376492A (fr)
DE (2) DE9203251U1 (fr)
WO (1) WO1992016746A1 (fr)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1996001369A1 (fr) * 1994-07-04 1996-01-18 Arthur Rommel Mecanisme rotatif
WO2011158048A3 (fr) * 2010-06-17 2012-12-27 Grigorios Karamitsos Mécanisme de propulsion de l'impulsion inertielle double
WO2018002555A1 (fr) 2016-06-30 2018-01-04 Pi Co Système de propulsion à inertie comportant un freinage par un fluide de la trajectoire retour de la masse

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19517181A1 (de) * 1995-05-11 1996-11-14 Scherbaum Helmut Dipl Ing Fh Trägheitskraftantrieb mit kontinuierlicher und gerichteter Antriebskraft
DE19613369C2 (de) * 1995-07-25 1998-07-02 Munnecke Gustav Adolf Vorrichtung zur Nutzung der Zentrifugalkraft für die Energiegewinnung
DE19808200A1 (de) * 1998-02-27 1999-09-02 Cherkasky Verfahren zur Fortbewegung eines Objekts durch die Wirkung einer nicht ausgeglichenen Zentrifugalkraft und die möglichen Vorrichtungen für die Verwirklichung dieser Fortbewegung
DE10006716A1 (de) * 2000-02-15 2001-08-16 Lothar Jaeger Impulstriebwerk
DE102021003188A1 (de) 2021-06-21 2022-12-22 Fritz Frederich Antrieb zum elektrischen Schweben, Fliegen, Fahren oder Fortbewegen

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2216461A1 (fr) * 1973-02-02 1974-08-30 Mizrahi Jacques
DE2536469A1 (de) * 1975-08-16 1977-02-24 Grossmann Franz Karl Dipl Ing Fliehkraft-getriebe
US4884465A (en) * 1988-01-11 1989-12-05 Zachystal George J Device for obtaining a directional centrifugal force

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2461014A1 (de) * 1974-12-21 1976-06-24 Gerhard Ruedel Richtkraft-motor

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2216461A1 (fr) * 1973-02-02 1974-08-30 Mizrahi Jacques
DE2536469A1 (de) * 1975-08-16 1977-02-24 Grossmann Franz Karl Dipl Ing Fliehkraft-getriebe
US4884465A (en) * 1988-01-11 1989-12-05 Zachystal George J Device for obtaining a directional centrifugal force

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1996001369A1 (fr) * 1994-07-04 1996-01-18 Arthur Rommel Mecanisme rotatif
WO2011158048A3 (fr) * 2010-06-17 2012-12-27 Grigorios Karamitsos Mécanisme de propulsion de l'impulsion inertielle double
WO2018002555A1 (fr) 2016-06-30 2018-01-04 Pi Co Système de propulsion à inertie comportant un freinage par un fluide de la trajectoire retour de la masse
FR3053411A1 (fr) * 2016-06-30 2018-01-05 Pi Co Systeme de propulsion a inertie comportant un freinage par un fluide de la trajectoire retour de la masse

Also Published As

Publication number Publication date
DE9203251U1 (de) 1993-04-01
AU1376492A (en) 1992-10-21
DE4207637A1 (de) 1992-10-01

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