WO1986004647A1 - Device using the force of gravity and transforming it into energy by means of solid and elastic bodies - Google Patents
Device using the force of gravity and transforming it into energy by means of solid and elastic bodies Download PDFInfo
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- WO1986004647A1 WO1986004647A1 PCT/IT1985/000033 IT8500033W WO8604647A1 WO 1986004647 A1 WO1986004647 A1 WO 1986004647A1 IT 8500033 W IT8500033 W IT 8500033W WO 8604647 A1 WO8604647 A1 WO 8604647A1
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- propellant
- pendulum
- gravity
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- ergopendolo
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- 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
- F03G7/00—Mechanical-power-producing mechanisms, not otherwise provided for or using energy sources not otherwise provided for
- F03G7/10—Alleged perpetua mobilia
- F03G7/104—Alleged perpetua mobilia continuously converting gravity into usable power
Definitions
- the ergopendolo brings together many of the properties of the classic pendulum, the inclined plane and the lever of the second kind.
- the classic pendulum has a fixed lens; the ergopendolo has a heavy movable lens which takes the name of propellant. fixed, on short parallel levers ayaht their pivots on the pendulum.
- a special machine blocks the propellant in inclined position with respect to the longitudinal axis of the pendulum during the oscillation of this one. At the end of the osci llation the machine is released and the thruster is triggered and passes to a opposite oblique homologous position by giving a thrust to the pendulum by means of the pivots of its levers.
- the thrust has the direction opposite to the displacement of the thruster; that is to say the direction of the new successive oscillation of the pendulum which will start.
- the propellant by changing position displaces the center of gravity of the ergopendolo thus increasing the amplitude of each oscillation.
- the movement of the propellant is produced by gravity , by the inertia accumulated during the oscillation of the pendulum, by the resonance and by the action of the sensor, action which will be specified later.
- the movements of the propellant are illustrated by the grav.
- 5 is the ergopendolo at the beginning of the oscillation; 6 the same at the end; 7 is the propellant; 1 the direction of the oacillation to the ergopendolo; 2 the trajectory of the propellant movement; 3 the direction of the thrust that the propellant, when triggered, gives to the ergopendolo, by its action on the pivots of its levers; 4 is the vertical. It is essential that the triggering of the propellant comes to the exact end of each oscillation; otherwise the resonance, instead of a positive action, produces a negative action all the greater as the triggering takes place before or after the arrival of the 'ergopendolo at the maximum of its anticipated or delayed oscillation until quickly stopping the oscillations.
- the catch is a heavy solid body weighing about 1/4 to 1/10 the weight of the propellant; it is free to slide on slides along the longitudinal axis of the pendulum; it weighs on an elastic body.
- ergopendolo oscillates, it takes an alternating movement perfectly synchronized with the oscillations of.
- ergopendolo it goes down when the oscillation goes down; it goes back up - as soon as the pendulum has crossed the vertical - when the oscillation goes back up; it begins to descend again when the pendulum starts again: it follows that the starting point of its course is always equal, while the descent takes place when passing the vertical; therefore its stroke is always proportional to the amplitude of the oscillation.
- the maximum length of the stroke is also determined by the degree of flexibility of the elastic body on which it rests.
- the captive flexes the elastic body to a measure several times greater than it does when the ergopendolo stops; that is, when the ergopendolo is in motion, the captor flexes the elastic body to a greater extent than its weight.
- the movement of the captor is also influenced by the laws of the inclined plane; indeed the ergopendolo constitutes an oscillating inclined plane; it is also influenced by the laws of the lever of the second kind because the ascent of the captor constitutes the resistance, the axis of oscillation of the ergopendolo the fulcrum, the reaction of the elastic body the power; it derives from this the need to start the descent of the catch as close as possible to the axis of oscillation of the ergopendolo, not forgetting that the center of gravity of the catch, in the ascent of its reciprocating movement, must never exceed the axis of oscillation (the start of the descent coincides with the end of the ascent) to avoid negative effects; these are caused in smaller quantities, also by the portion of the trap which, possibly, goes beyond the axis of oscillation while remaining below the center of gravity.
- the most precious property of the captor is constituted - as indicated above - by the synchronism which makes the end of its ascent coincide with the height of the oscillation and which - because of this - allows the propellant to unlock at the exact moment.
- the pendulum is constituted by the chassis 1, which can oscillate on the fixed axis 2; 3 these are the two slides on which the catcher performs its reciprocating movement; 5 is the connecting rod which unites the sensor to its lever 6;
- the disc 19 secured to the connecting rod of the sensor so as to unlock the ratchet wheel 16, which is returned to the start position by the spring 18.
- the disc 19 On one of the two levers 9 is fixed the disc 19, on the same pivot as the lever which extends and carries the small pulley 20 at the head.
- the two homologous and flexible tie rods 21 ending in two equal elastic bodies, connected to the ratchet wheel with ratchet 23 in the same place.
- the ratchet wheel with click 16 actuated by lever 6 by means of the tie rod 22, rotates the ratchet wheel with ratchet 23 which thus alternately holds one of the two elastic bodies connected to the disc 19; the position of the thruster being always oblique, a flexible tie is tensioned alternately; the other is loose; the one that is stretched also stretches its elastic body and it will positively influence the movement of the propellant which has a circumferential arc trajectory; the thrust of the terminal elastic body of the tensioned tie must be exhausted at the half of the trajectory so as not to become negative.
- the small pulley 20 lifts the lever 25 which by means of the bar 26 lifts the pawl 24 and unlocks the toothed disc 22 by canceling any remaining tension of the stretched elastic body.
- 32 these are two homologous levers which have their pivot if killed on the longitudinal axis of the pendulum. These are joined by means of two homologous flexible tie rods 33 and two small pulleys 34 with the two hooks 11; at the height of the oscillation, they determine the release of the hook propellant.
- the disc 27 is located on the same axis as the two levers 32; three bars
- the central bar 29 is connected to the spring 35, which has the other end fixed on the longitudinal axis of the same bar; so that this bar cannot remain vertical, if it is barely moved of its axis.
- the triggering can be carried out by printing from the outside the oscillatory movement necessary to set in movement the catching -this normally arrives between the 35 ° and the 50 ° with respect to the vertical -; or lifting the ergopendolo to around 50 ° and abandoning it to itself.
- any brake automatic or controlled outside, which acts on the axis of oscillation l.
- the ergopendolo being set in motion with the propellant in an oblique position in one of the two hooks, from the start of the oscillation of the ergo pendolo to the vertical, the catch 4 descends and tightens the elastic body 7; the click 42 slides on the toothed disc 16; crossing the vertical, the cap as long as 4 begins to rise; the click 42 engages in the toothed disc 16; by rotating it, it loads the stretched elastic body 21 by means of the lever 22; this stretched elastic body will increase the thrust of the propellant by means of the rotation of the ratchet wheel with ratchet 23; this wheel engages in the pawl 24 which will then be released by the complex 20 25 26, when the thruster passes through the center of its trajectory; as explained above.
- the disc 27 prints the push to the ergopendolo by means of its pivots; furthermore it displaces the center of gravity by increasing the amplitude of the oscillation while keeping the ergopen dolo in motion.
- the weight of the propellant the weight ratio between the pendulum and the propellant hang from the length of the pendulum, from the power that we want to obtain; from the specific weight of the material with which the pendulum was built. It is suitable (but it is not essential) to use equipment of low specific weight coupled to the resistance necessary for the effort.
- the weight of the trap can vary from about 1/4 to about 1/10 of the weight of the propellant. All the mechanisms described here and implemented in the working model are mechanical; those which block and unblock the propellant can be replaced by electromagnets.
- the technique offers several means for transforming the oscillatory movement into a rotary movement. For the model realized we used the machine from the engra.
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Abstract
Description
TITRE DE L'INVENTION.TITLE OF THE INVENTION.
Dispositif qui capte la force de gravité et la transforme en énergie au moyen de corps solides et de corps élastiques.Device which captures the force of gravity and transforms it into energy by means of solid bodies and elastic bodies.
DESCRIPTION. Jusqu'à présent on a obtenu de l'énergie de la gravité au moyen des chutes d'eau. Ce dispositif obtient le même résultat au moyen de corps élastiques et de corps solides lourds qui se meuvent par eux-mêmes par action de la gravité, de l'inertie et de la résonance sur un châssis oscillant sur un pivot fixe.Dans cette description,dore navant,j'appellerai pendule le châssis oscillant et "er gopendolo (ergpendule ) l'appareil complet de tous ses engins:châssis,corps élastiques,corps solides lourds, mécanismes d'engagement et de dégagement ;engin por le mouvement de rotation. L'ergopendolo rassemble un grand nombre des propriété du pendule classique, du plan incliné et du levier du second genre. Le pendule classique a une lentille fixe;l'ergopendolo a une lentille lourde mobile qui prend le nom de propulseur. La lentille est. fixée, sur de courts leviers paralliles ayaht leurs pivots sur le pendule.Un engin spécial bloque le propulseur en position inclinée à l'égard de l'axe longitudinal du pen'dule pendant l'oscillation de celui-ci.Au terme de l'oscillation l'engin se débloque et le propulseur se declen che et passe à una position oblique opposée homologue en donnant une poussée au pendule au moyen des pivots de ses leviers .La poussée a la direction opposée au déplacement du propulseur ;c'est à dire la direction de la nouvelle oscillation successive du pendule qui va commencer.En outre le propulseur en changeant de posi tion déplace le centre de gravité de l'ergopendolo en augmentant ainsi l'amplitude de chaque oscillation.Le mouvement du propulseur est produit par la gravité,par l'inertie accumulée pendant l'oscillation du pendule,par la résonance et par l'action du captant,action que sera précisée par la suite .Les mouvements du propulseur sont illustrés par les grav. 2 et 3: 5 est l'ergopendolo au commencement de l'oscillation; 6 le même à la fin; 7 est le propulseur; 1 la direction de l'oacillation ae l'ergopendolo; 2 la trajectoire du mouvement du propulseur; 3 la direction de la poussée que le propulseur en se déclenchant donne à l'ergopendolo,par son action aur les pivots de ses leviers; 4 est la verticale. Il est indispensable que le declancement du propulseur arrive au terme exact de chaque oscillation ;autrement la résonance,au lieu d'une action positive , produit une action négative d'autant plus grande que le déclenchement a lieu avant ou après l'arrivée de l'ergopendolo au maximum de son oscillation anticipée ou retardée jusq'à arrêter rapidement les oscillations. Le captant est un corps solide lourd ayant un poids à peu près de 1/4 à 1/10 du poids du propulseur; il est libre de glisser sur des glissières le long de l'axe longitudinal du pendule ; il pèse sur un corps élastique .Lorsque l'ergopendolo oscille,il prend un mouvement alternatif parfaitement syncrone aux oscillations de. l'ergopendolo: il descend lorsque l'oscillation descend; il remonte -des que le pendule a traversé la verticale - loesque l'oscillation remonte;il recommence ιa descente lorsque le pendule la recommence: il s'ensuit que le point de départ de sa course est toujours égal,tandis que la descente se teraine au passage de la verticale; par conséquent sa course est toujours proportionnelle à l'amplitude de l'oscillation.La longueur maximum de la course est déterminée aussi par le degré de flexibilité du corps élastique sur lequel il s'appuie. Lorsque l'ergopendolo oscille le captant fléchit le corps élastique dans une mesure plusieurs fois plus grande de ce qu'il ne le fléchit à ergopendolo arrêté; c'est à dire que ,lorsque l'ergopendolo est en mouvement, le captant fléchit le corps élastique dans une mesure plus grande que son poids .Le mouvement du captant est aussi influencé par les lois du plan incliné ;en effet l'ergopendolo constitue un plan incliné oscillant ; il est aussi influencé par les lois du levier de second genre car la remontée du captant constitue la résistance,l'axe d'oscillation de l'ergopendolo le point d'appui,la réation du corps élastique la puissance; il en dérive la nécessité de faire commencer la descente du captant le plus près possible de l'axe d'oscillation de l'ergopendolo n'oubliant pas que le centre de gravité du captant, dans la remontée de son mouvement alternatif,ne doit jamais dépasser l'axe d'oscillation (le début de la descente coincide avec la fin de la remontée) pour éviter des effets négatifs ; ceux-ci sont causés en plus petite quantité,aussi par la portion du captant qui,éventuellement,va au delà de l'axe d'oscillation tout en restant au dessous du centre de gravité.De là,la nécessité d'employer dans la construction du captant un matériel de poids spécifique le plus grande ptoistseible et de lui donner une forme de hauteur la plus pe possible . Il est nécessaire en outre de considérer tandis que toutes les autres parties de l'ergopendolo,en oscillant, décrivent des arcs de circonférence ,le captant oscille pendant son mouvement alternatif, en décrivant une ligne trajectoire anomale,qui exerce une action freinante sur les oscillations de l'ergopendolo,toutefois moindre que l'effet positif de l'énergie captée qui est utilisée soit par l'action des différentes mécanismes soit par le mouvement du propulseur. L'expérience conseille de limiter la course du captant d'environ 1/8 à environ 1/5 de la longuer du pendule suivant les nécessités de la construction.La propriété la plus précieuse du captant est constituée -comme indiqué ci-dessus - par le synchronisme qui fait coincider le terme de sa remontée avec le comble de l'oscillation et qui - à cause de cela - permet au propulseur de se débloquer à l'instant exact.Je vais décrire le dispositif qui est illustré à la graveure 1 . Le pendule est constiué par le chassis 1 ,qui peut osciller sur l'axe fixe 2 ; 3 ce sont les deux glissières sur lesquelles le captant accomplit son mouvement alternatif; 5 est la bielle qui unit le captant à son levier 6 ;DESCRIPTION. Up to now, energy from gravity has been obtained by means of waterfalls. This device achieves the same result by means of elastic bodies and heavy solid bodies which move by themselves by the action of gravity, inertia and resonance on an oscillating chassis on a fixed pivot. dore navant, I will call pendulum the oscillating chassis and "er gopendolo (ergpendule) the complete apparatus of all its machines: chassis, elastic bodies, heavy solid bodies, mechanisms of engagement and release; machine por the movement of rotation. The ergopendolo brings together many of the properties of the classic pendulum, the inclined plane and the lever of the second kind.The classic pendulum has a fixed lens; the ergopendolo has a heavy movable lens which takes the name of propellant. fixed, on short parallel levers ayaht their pivots on the pendulum. A special machine blocks the propellant in inclined position with respect to the longitudinal axis of the pendulum during the oscillation of this one. At the end of the osci llation the machine is released and the thruster is triggered and passes to a opposite oblique homologous position by giving a thrust to the pendulum by means of the pivots of its levers. The thrust has the direction opposite to the displacement of the thruster; that is to say the direction of the new successive oscillation of the pendulum which will start. In addition the propellant by changing position displaces the center of gravity of the ergopendolo thus increasing the amplitude of each oscillation. The movement of the propellant is produced by gravity , by the inertia accumulated during the oscillation of the pendulum, by the resonance and by the action of the sensor, action which will be specified later. The movements of the propellant are illustrated by the grav. 2 and 3: 5 is the ergopendolo at the beginning of the oscillation; 6 the same at the end; 7 is the propellant; 1 the direction of the oacillation to the ergopendolo; 2 the trajectory of the propellant movement; 3 the direction of the thrust that the propellant, when triggered, gives to the ergopendolo, by its action on the pivots of its levers; 4 is the vertical. It is essential that the triggering of the propellant comes to the exact end of each oscillation; otherwise the resonance, instead of a positive action, produces a negative action all the greater as the triggering takes place before or after the arrival of the 'ergopendolo at the maximum of its anticipated or delayed oscillation until quickly stopping the oscillations. The catch is a heavy solid body weighing about 1/4 to 1/10 the weight of the propellant; it is free to slide on slides along the longitudinal axis of the pendulum; it weighs on an elastic body. When the ergopendolo oscillates, it takes an alternating movement perfectly synchronized with the oscillations of. ergopendolo: it goes down when the oscillation goes down; it goes back up - as soon as the pendulum has crossed the vertical - when the oscillation goes back up; it begins to descend again when the pendulum starts again: it follows that the starting point of its course is always equal, while the descent takes place when passing the vertical; therefore its stroke is always proportional to the amplitude of the oscillation. The maximum length of the stroke is also determined by the degree of flexibility of the elastic body on which it rests. When the ergopendolo oscillates, the captive flexes the elastic body to a measure several times greater than it does when the ergopendolo stops; that is, when the ergopendolo is in motion, the captor flexes the elastic body to a greater extent than its weight. The movement of the captor is also influenced by the laws of the inclined plane; indeed the ergopendolo constitutes an oscillating inclined plane; it is also influenced by the laws of the lever of the second kind because the ascent of the captor constitutes the resistance, the axis of oscillation of the ergopendolo the fulcrum, the reaction of the elastic body the power; it derives from this the need to start the descent of the catch as close as possible to the axis of oscillation of the ergopendolo, not forgetting that the center of gravity of the catch, in the ascent of its reciprocating movement, must never exceed the axis of oscillation (the start of the descent coincides with the end of the ascent) to avoid negative effects; these are caused in smaller quantities, also by the portion of the trap which, possibly, goes beyond the axis of oscillation while remaining below the center of gravity. Hence the need to use in the construction of a picking the greater specific weight p equipment t i o s t s e ible and give it a form of more pe height possible. It is also necessary to consider while all the other parts of the ergopendolo, while oscillating, describe arcs of circumference, the catch oscillates during its reciprocating movement, by describing an anomalous trajectory line, which exerts a braking action on the oscillations ergopendolo, however less than the positive effect of the captured energy which is used either by the action of the different mechanisms or by the movement of the propellant. Experience advises to limit the stroke of the captor from about 1/8 to about 1/5 of the pendulum length depending on the needs of the construction. The most precious property of the captor is constituted - as indicated above - by the synchronism which makes the end of its ascent coincide with the height of the oscillation and which - because of this - allows the propellant to unlock at the exact moment. I will describe the device which is illustrated in engraver 1. The pendulum is constituted by the chassis 1, which can oscillate on the fixed axis 2; 3 these are the two slides on which the catcher performs its reciprocating movement; 5 is the connecting rod which unites the sensor to its lever 6;
7 c'est le corps élastique symbolisé par un ressort fixé au châssis et au levier 6 ;le corps élastique est fléchi par le captant en descente,au moyen de la bielle et du levier ; sa réaction produit la remontée du captant;7 is the elastic body symbolized by a spring fixed to the chassis and to the lever 6; the elastic body is bent by the collector in descent, by means of the connecting rod and the lever; its reaction produces the rise of the captor;
8 c'est le propulseur fixé aux deux leviers courts parallèles 9 ,oscillant sur leur pivots,fixés sur le pendule; 10 ce sant les deux crochets homologues danx lesquel le propulseur s'engage au moyen de la traverse 14 ,qui unit les deux leviers 9 ; 11 ce sont deux petits leviers homologues qui empêchent les déclenchements du propulseur à contre temps,causes par l'inertie de sa masse; au contraire ils les permettent en se déplaçant au moment juste; 12 c'est le disque qui,par l'action du captant,au moyen des deux tirants homologues 13 déplace les deux petits leviers 11 et soulève le cliquet 36 qui provoque le déclenchement du propulseur décroché par le ressort 35 ; 15 c'est l'axe sur lequel oscille le levier ; sur le même axe est assemblée une roue à rochet 16 avec le déclic 42 (en italien: "arpionismo" débloqué au terme de toutes les oscillations par la barre8 is the propellant fixed to the two short parallel levers 9, oscillating on their pivots, fixed on the pendulum; 10 being the two homologous hooks danx which the propeller engages by means of the cross member 14, which unites the two levers 9; 11 these are two small homologous levers which prevent the propellant from triggering against the clock, caused by the inertia of its mass; on the contrary, they allow them by moving at the right moment; 12 it is the disc which, by the action of the catch, by means of the two homologous tie rods 13 displaces the two small levers 11 and lifts the pawl 36 which causes the triggering of the propellant released by the spring 35; 15 is the axis on which the lever oscillates; on the same axis is assembled a ratchet wheel 16 with the click 42 (in Italian: "arpionismo" released at the end of all the oscillations by the bar
43 solidaire avec la bielle du captant de façon à débloquer la roue à rochet 16 ,qui est reportée à la position de début par le ressort 18. Sur un des deux leviers 9 est fixé le disque 19 ,sur le meme pivot que le levier qui se prolonge et porte en tête la petite poulie 20 . Aux deux extrémités du diamètre du disque 19 -diamètre perpendiculaire à l'axe longitudinal du levier - sont fixés les deux tirants homologues et flexibles 21 se terminant par deux corps élastiques égaux,reliés à la roue à rochet avec cliquet 23 au même endroit. La roue à rochet avec déclic 16 ,actionnée par le levier 6 au moyen du tirant 22 ,fait tourner la roue à rochet avec cliquet 23 qui ten ainsi alternativement un des deux corps élastiques reliés au disque 19 ; la position du propulseur étant toujours oblique,un tirant flexible est tendu alternativement;l'autre est lâche;celui qui est tendu tend aussi son corps élastique et il influera positivement sur le mouvement du propulseur qui a une trajectoire à arc de circonférence ;la poussée du corps élastique terminal du tirant tendu doit s'épuiser à la moitié de la trajectoire pour ne pas devenir négative .A' la moitié de la trajectoire la petite poulie 20 soulève le levier 25 qui au moyen de la barre 26 soulève le cliquet 24 et débloque le disque denté 22 en annullant la tension éventuellement restante du corps élastique tendu. 32 ce sont deux leviers homologues qui ont leur pivot si tué sur l'axe longitudinal du pendule. Celles-ci sont unies au moyen de deux tirants flexibles homologues 33 et de deux petites poulies 34 aux deux crochets 11 ; au comble de l'oscillation,ils déterminent le dessngage ment du propulseur du crochet.le disque 27 est situé sur le même axe que les deux leviers 32 ;trois barres43 secured to the connecting rod of the sensor so as to unlock the ratchet wheel 16, which is returned to the start position by the spring 18. On one of the two levers 9 is fixed the disc 19, on the same pivot as the lever which extends and carries the small pulley 20 at the head. At the two ends of the diameter of the disc 19 - diameter perpendicular to the longitudinal axis of the lever - are fixed the two homologous and flexible tie rods 21 ending in two equal elastic bodies, connected to the ratchet wheel with ratchet 23 in the same place. The ratchet wheel with click 16, actuated by lever 6 by means of the tie rod 22, rotates the ratchet wheel with ratchet 23 which thus alternately holds one of the two elastic bodies connected to the disc 19; the position of the thruster being always oblique, a flexible tie is tensioned alternately; the other is loose; the one that is stretched also stretches its elastic body and it will positively influence the movement of the propellant which has a circumferential arc trajectory; the thrust of the terminal elastic body of the tensioned tie must be exhausted at the half of the trajectory so as not to become negative. At the half of the trajectory the small pulley 20 lifts the lever 25 which by means of the bar 26 lifts the pawl 24 and unlocks the toothed disc 22 by canceling any remaining tension of the stretched elastic body. 32 these are two homologous levers which have their pivot if killed on the longitudinal axis of the pendulum. These are joined by means of two homologous flexible tie rods 33 and two small pulleys 34 with the two hooks 11; at the height of the oscillation, they determine the release of the hook propellant. the disc 27 is located on the same axis as the two levers 32; three bars
28 , 29 , 30 , émergent du disque 27 ,solidaires avec lui. Plus courte que les autres deux, la barre centraie 29 est reliée au ressort 35 ,qui a l'autre extrémité fixée sur l'axe longitudinal de la même barre;de sort que cette barre ne peut rester verticale,si elle est à peine déplacée de son axe.Les deux barres plus longues28, 29, 30, emerge from the disc 27, integral with it. Shorter than the other two, the central bar 29 is connected to the spring 35, which has the other end fixed on the longitudinal axis of the same bar; so that this bar cannot remain vertical, if it is barely moved of its axis. The two longer bars
29 et 30 déterminent alternativement son déplacement. Pendant les oscillations ces deux barres heurtent contre le pointe fixe 31 qui est extérieur à l'ergopendolo et fixé sur le support de celui-ci (le support n'a pas été dessiné:treillage,mur,mθule etc ). La barre 28 déplacée, le ressort 35 se tend et reste tendu parce que le disque 27 est muni de deux dents d'orientation opposée. Ces deux denta s'engagent alternativement dans le cli quet 36 . La charge de ce ressort 35 servira à dé bloquer alternativement les crochets qui retiennent le propulseur; lorsque le cliquet 36 est soulevé,le ressort 35 tirera alternativement les barres 29 et 30 ; ces barres s'y appuyant soulèveront alternativement les leviers 32 et débloqueront alternativement les crochets 10 en provoquant le déclenchement du propulseur. Pour que le propulseur se débloque exactement au comble de cha que oscillation de l'ergopendolo,il est nécessaire que le soulèvement du cliquet 36 arrive immédiatement après le déplacement des deux petits leviers 11 ; ce déplacement permet que les crochets, se débloquent .Au déplacement des petits leviers pourvoit le disque 12 avec les deux ti rants 13 que l'unissent aux deux petits leviers 11 et avec les leviera 39 et 38 . Celui-ci est actionné par le levier 6.Comme le captant,le levier 6 termine toujours sa course vers le haut,au terme de l'oscillation de l'ergo pendolo quelle que soit l'amplitude de l'oscillation. Les deux ressorts 40 ont la seule fonction d'ammortisseurs de choc. Lorsque la construction d'un ergopendolo est terminée,il faut vérifier si l'axe longitudinal du pendule coincide avec la verticale ;ce qui peut être empê ché par le poids et par l'emplacement des différents engins montés sur l'ergopendolo;s'il est nécessaire,on doit appliquer un poids à équilibrer ;poids à appliquer esclusivement dans ce but.Le fonctionnement de l'ergo pendolo est le suivant:le déclenchement peut s'effectuer on en imprimant de l'extérieur le mouvement oscillatoire nécessaire à mettre en mouvement le captant -cela nor malement arrive entre les 35° et les 50° à l'égard de la verticale - ; ou bien soulevant l'ergopendolo à environ 50° et l'abandonnant à lui même. Pour l'ar rêter,il est suffisant un frein quelconque,automatic ou commandé à l' extérieur , qui agit sur l ' axe d' osscil lation 2 .Soit le support de l'ergopendolo (treillagφ, mur,mule,etc ) que le frein n'on pas été dessinés; 41 ce sont deux coussinets du support dans lesquels tourne l'axe d'oscillation.Il n'est pas mal aviser que pour de considérables puissances,il faut monter plusieurs ergopendoli en série,pour éviter les inconvé nients de masses très lourdes . L'ergopendolo,étant mis en mouvement avec le propulseur en position oblique dans un des deux crochets,du début de l'oscillation de l'ergo pendolo jusqu'à la verticale,le captant 4 descend et tend le corps élastique 7 ;le déclic 42 glisse sur le disque denté 16 ;en traversant la verticale,le cap tant 4 commence laremontée; le déclic 42 s'engage dans le disque denté 16 ;en le faisant tourner, il charge le corps élastique tendu 21 au moyen du levier 22 ; ce corps élastique tendu augmentera la poussée du propulseur au moyen de la rotation de la roue à rochet avec cliquet 23 ; cette roue s'engage dans le cliquet 24 qui sera ensuite débloqué par le complexe 20 25 26 , lorsque le propulseur traversera le centre de sa trajec toire ; de la manière expliquée ci-dessus. En traversant la verticale,l'ergopendolo heurte par les barres 29 et 30 contre le point extérieur 31 fixé sur le support;le disque 27 tourne en chargeant le ressort 35 qui se bloque au moyen du cliquet 36 dans une des deux dents opposées du disque 27 ; cependant le levier 6 a commencé sa remontée; ayant atteint son point d'arrivée,il a pressé sur le levier 38 qui fait tourner le disque 12 au moyen de la bielle 39 ; de la manie re dejà expliquée ,le disque 12 déplace les petits leviers 11 ; il agit au moyen du tirant 37 contre le cliquet 36 ,débloquant le disque 27 . Le disque 27 , tiré par le ressort,débloque le propulseur qui se déclanche et se déplace sur le crochet homologue opposé. Comme nous avons déjà expliqué,le disque 27 imprime la poussée à l'ergopendolo au moyen de ses pivots ; en outre il déplace le centre de gravité en augmentant l'amplitude de l'oscillation tout en gardant l'ergopen dolo en mouvement. En prélevant l'énergie excédente celle qui est nécessaire à garder en mouvement l'ergo pendolo,selon une amplitude d'oscillation prédéterminée, on obtient le travail utile. Le poids du propulseur, le rapport de poids entre le pendule et le propulseur de pendent de la longueur du pendule,de la puissance qu'on veut obtenir ;du poids spécifique du matériel avec lequel le pendule a été construit. Il est convenable (mais il n'est pas indispensable ) d'employer du matériel de faible poids spécifique accouplé à la résistance nécessaire à l'effort. Le poids du captant peut varier d'en viron 1/4 à environ 1/10 du poids du propulseur. Tous les mécanismes ici décrits et réalisés dans le modèle qui fonctionne,sont mécaniques; ceux qui bloquent et débloquent le propulseur peuvent être substitués par des électroaimants. La technique offre plusieurs moyens pour transformer le mouvement oscillatoire en mouvement rotatoire. Pour le modèle réalisé on a employé l'engin de la grav. 4 ; il permet n'importe quelle variation dans l'amplitude des oscillations; 7 c'est le volant monté sur la roue libre; sur le même axe,le disque denté 6 est monté solidaire avec la roue libre; les deux déclics 9 agissent en même temps sur le disque denté; ils sont montés sur le même axe du disque denté, et sont reliés aux bielles homologues 5 ; celles-ci ont leur pivot sur la barre 4 glissant dans la glissière 3 dont l'axe coincide avec la verticale ; la barre 4 est ac tionnée par la bielle 2 qui a son pivot sur le pendule 1; cette barre entreprend un mouvement alternatif et, au moyen de la roue à rochet avec cliquet, elle fait tourner le volant . 10 c'est la verticale ; le support n'a pas été dessiné. 29 and 30 alternately determine its displacement. During the oscillations these two bars strike against the fixed point 31 which is outside the ergopendolo and fixed on the support of the latter (the support has not been drawn: trellis, wall, mule etc.). The bar 28 moved, the spring 35 tightens and remains taut because the disc 27 is provided with two teeth of opposite orientation. These two teeth engage alternately in the click 36. The load of this spring 35 will serve to alternately unlock the hooks which retain the propellant; when the pawl 36 is raised, the spring 35 will alternately pull the bars 29 and 30; these bars leaning on them will alternately raise the levers 32 and alternately unlock the hooks 10 causing the propellant to fire. For the propellant to be unlocked exactly at the height of each swing of the ergopendolo, it is necessary that the lifting of the pawl 36 occurs immediately after the displacement of the two small levers 11; this movement allows the hooks to be unlocked. When the small levers are moved, the disc 12 is provided with the two tie rods 13 which join it to the two small levers 11 and with the levers 39 and 38. This is actuated by lever 6. Like the catch, lever 6 always ends its upward stroke, at the end of the oscillation of the ergo pendolo whatever the amplitude of the oscillation. The two springs 40 have the sole function of shock absorbers. When the construction of an ergopendolo is finished, it must be checked whether the longitudinal axis of the pendulum coincides with the vertical; this can be prevented by the weight and by the location of the various devices mounted on the ergopendolo; it is necessary, we must apply a weight to be balanced; weight to be applied exclusively for this purpose. The functioning of the ergo pendolo is as follows: the triggering can be carried out by printing from the outside the oscillatory movement necessary to set in movement the catching -this normally arrives between the 35 ° and the 50 ° with respect to the vertical -; or lifting the ergopendolo to around 50 ° and abandoning it to itself. To stop it, it is sufficient any brake, automatic or controlled outside, which acts on the axis of oscillation l. Either the ergopendolo support (trellis, wall, mule, etc) that the brake has not been designed; 41 these are two bearings of the support in which the axis of oscillation rotates. It is not a bad idea that for considerable powers, several ergopendoli must be mounted in series, to avoid the disadvantages of very heavy masses. The ergopendolo, being set in motion with the propellant in an oblique position in one of the two hooks, from the start of the oscillation of the ergo pendolo to the vertical, the catch 4 descends and tightens the elastic body 7; the click 42 slides on the toothed disc 16; crossing the vertical, the cap as long as 4 begins to rise; the click 42 engages in the toothed disc 16; by rotating it, it loads the stretched elastic body 21 by means of the lever 22; this stretched elastic body will increase the thrust of the propellant by means of the rotation of the ratchet wheel with ratchet 23; this wheel engages in the pawl 24 which will then be released by the complex 20 25 26, when the thruster passes through the center of its trajectory; as explained above. Crossing the vertical, the ergopendolo strikes the bars 29 and 30 against the external point 31 fixed on the support; the disc 27 rotates by loading the spring 35 which is blocked by means of the ratchet 36 in one of the two opposite teeth of the disc 27; however, lever 6 has started to rise; having reached its point of arrival, he pressed the lever 38 which rotates the disc 12 by means of the connecting rod 39; in the manner already explained, the disc 12 moves the small levers 11; it acts by means of the tie rod 37 against the pawl 36, unlocking the disc 27. The disc 27, pulled by the spring, unlocks the propellant which is released and moves on the opposite homologous hook. As we have already explained, the disc 27 prints the push to the ergopendolo by means of its pivots; furthermore it displaces the center of gravity by increasing the amplitude of the oscillation while keeping the ergopen dolo in motion. By taking the energy exceeding that which is necessary to keep the ergo pendolo in motion, according to a predetermined amplitude of oscillation, we obtain the useful work. The weight of the propellant, the weight ratio between the pendulum and the propellant hang from the length of the pendulum, from the power that we want to obtain; from the specific weight of the material with which the pendulum was built. It is suitable (but it is not essential) to use equipment of low specific weight coupled to the resistance necessary for the effort. The weight of the trap can vary from about 1/4 to about 1/10 of the weight of the propellant. All the mechanisms described here and implemented in the working model are mechanical; those which block and unblock the propellant can be replaced by electromagnets. The technique offers several means for transforming the oscillatory movement into a rotary movement. For the model realized we used the machine from the engra. 4; it allows any variation in the amplitude of the oscillations; 7 is the steering wheel mounted on the freewheel; on the same axis, the toothed disc 6 is mounted integral with the freewheel; the two clicks 9 act at the same time on the toothed disc; they are mounted on the same axis of the toothed disc, and are connected to the homologous connecting rods 5; these have their pivot on the bar 4 sliding in the slide 3 whose axis coincides with the vertical; the bar 4 is actuated by the connecting rod 2 which has its pivot on the pendulum 1; this bar makes an alternative movement and, by means of the ratchet wheel with ratchet, it turns the steering wheel. 10 is vertical; the support was not drawn.
Claims
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE1985904486 DE213140T1 (en) | 1985-02-08 | 1985-09-05 | DEVICE FOR UTILIZING GRAVITY AND FORMING THEM BY MEANS OF SOLID AND ELASTIC BODIES. |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| IT45201A/8550 | 1985-02-08 | ||
| IT8545201A IT8545201A0 (en) | 1985-02-08 | 1985-02-08 | ON AN OSCILLATING FRAME ON PIVOT DEVICE ABLE TO CAPTURE THE FIXED FORCE OF GRAVITY TO PRODUCE ENERGY, MOTION AND WORK BY MEANS OF ELASTIC AND HEAVY SOLID MEANS SELF-PROPELLED BY THE ACTION OF GRAVITY, INERTIA AND RESONANCE |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO1986004647A1 true WO1986004647A1 (en) | 1986-08-14 |
Family
ID=11256628
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/IT1985/000033 Ceased WO1986004647A1 (en) | 1985-02-08 | 1985-09-05 | Device using the force of gravity and transforming it into energy by means of solid and elastic bodies |
Country Status (4)
| Country | Link |
|---|---|
| EP (1) | EP0213140A1 (en) |
| AU (1) | AU4861685A (en) |
| IT (1) | IT8545201A0 (en) |
| WO (1) | WO1986004647A1 (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2002061277A1 (en) * | 2001-01-29 | 2002-08-08 | Jauregui Carro Francisco J | Pendulum generator |
| ES2231041A1 (en) * | 2002-01-29 | 2005-05-01 | Fco. Javier Jauregui Carro | PENDULAR GENERATOR. |
| WO2005075824A1 (en) * | 2004-01-18 | 2005-08-18 | Chin-Ho Chiu | A method and device for generating power mechanically |
| WO2005100787A1 (en) * | 2004-04-16 | 2005-10-27 | James David Willis | Electric pulse pendulum power generator |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1298994C (en) * | 2004-08-09 | 2007-02-07 | 李念君 | Kinetic potential energy generator power device |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| BE521698A (en) * | ||||
| FR402619A (en) * | 1909-05-01 | 1909-10-13 | Alain De Coatgoureden | Device applicable to all pistons and used to transform reciprocating rectilinear motion into continuous circular motion |
| FR739548A (en) * | 1931-06-08 | 1933-01-13 | Force multiplier | |
| FR1194199A (en) * | 1959-11-06 | |||
| FR2398898A1 (en) * | 1977-04-29 | 1979-02-23 | Fernez Francis | DEVICE ALLOWING TO UNBALANCE FOLLOWING A DETERMINED ORIENTATION THE CENTRIFUGAL FORCE AND THE FORCES APPLIED TO A BODY ANIMATED BY A CIRCULAR MOVEMENT AROUND AN AXIS |
-
1985
- 1985-02-08 IT IT8545201A patent/IT8545201A0/en unknown
- 1985-09-05 WO PCT/IT1985/000033 patent/WO1986004647A1/en not_active Ceased
- 1985-09-05 AU AU48616/85A patent/AU4861685A/en not_active Abandoned
- 1985-09-05 EP EP85904486A patent/EP0213140A1/en not_active Withdrawn
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| BE521698A (en) * | ||||
| FR1194199A (en) * | 1959-11-06 | |||
| FR402619A (en) * | 1909-05-01 | 1909-10-13 | Alain De Coatgoureden | Device applicable to all pistons and used to transform reciprocating rectilinear motion into continuous circular motion |
| FR739548A (en) * | 1931-06-08 | 1933-01-13 | Force multiplier | |
| FR2398898A1 (en) * | 1977-04-29 | 1979-02-23 | Fernez Francis | DEVICE ALLOWING TO UNBALANCE FOLLOWING A DETERMINED ORIENTATION THE CENTRIFUGAL FORCE AND THE FORCES APPLIED TO A BODY ANIMATED BY A CIRCULAR MOVEMENT AROUND AN AXIS |
Non-Patent Citations (2)
| Title |
|---|
| Jahrbuch der Deutschen Gesellschaft fur Chronometrie, Vol. 34, 1983, Stuttgart, (DE) G. Glaser: 'Doppelpendel und sonstige Koppelschwingungen in der Uhrentechnik', pages 77-85, see page 79, fig. 2b * |
| PATENTS ABSTRACTS OF JAPAN, Vol. 5, No 76 (M-69)(748), 20 May 1981 & JP, A, 5627081 (Kazvo Fujii) 16 March 1981, see Abstract * |
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2002061277A1 (en) * | 2001-01-29 | 2002-08-08 | Jauregui Carro Francisco J | Pendulum generator |
| ES2200618A1 (en) * | 2001-01-29 | 2004-03-01 | Carro Francisco J Jauregui | Pendulum generator |
| ES2231041A1 (en) * | 2002-01-29 | 2005-05-01 | Fco. Javier Jauregui Carro | PENDULAR GENERATOR. |
| ES2231041B1 (en) * | 2002-01-29 | 2007-02-16 | Fco. Javier Jauregui Carro | PENDULAR GENERATOR. |
| WO2005075824A1 (en) * | 2004-01-18 | 2005-08-18 | Chin-Ho Chiu | A method and device for generating power mechanically |
| WO2005100787A1 (en) * | 2004-04-16 | 2005-10-27 | James David Willis | Electric pulse pendulum power generator |
Also Published As
| Publication number | Publication date |
|---|---|
| IT8545201A0 (en) | 1985-02-08 |
| EP0213140A1 (en) | 1987-03-11 |
| AU4861685A (en) | 1986-08-26 |
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