ITMC990065A1 - MUTUAL SUPPORT OF TIE RODS BETWEEN TWO CONCENTRIC CIRCLES FOR SINGLE SELF-ROTATING. - Google Patents

Description

EXPLANATION of the Industrial Invention entitled MUTUAL TIE RODS BETWEEN TWO CONCENTRIC CIRCLES FOR SINGLE SELF-ROTATING =

SUMMARY

Unlimited energy for MACHINES and pumps alternators.

TEXT of the Description

The perpetual motion of WHEEL two is done with two circles (fig. N.

3.408) and two tie rods, the winding of which, leaning on the median rim, raises close to the attachment of the main wheel, the; whose hook is the fibnal part (tail) of the other tie, whose R R is absorbed (canceled) by the Action (A-A ') and unified with the opposite and opposite Action which becomes active. so the two circles become a spinning wheel (mysteriously... mystery more mysterious less, the Italian universities are teeming with mysteries ...), able to develop any strength, especially with half-weight weight, in function both centrifugal and Newton's (circular pendulum). Figures 3.404 and 3.405 have a 1st type lever, angled In function aR (anti-reactive) against the reaction (oblique radius) of the bicycle - 1st type lever with teeth against the median wheel. a quadrangular figure in function aR for the purpose of thrusting the tie rod from bicycle to radius of the second bicycle. Fig. 3.410 crosses the tie rods twice for two supports on the arm (long-but too short) to balance it.

Claims (1)

3.423) As the previous 3.422 with open quadrangular fig (other fig. Geom.) With eccentric support or rope on the rim side of the single wheel, and two bicycles on the opposite side for the tie rod (with or without weight) with or without hooks towards the center and the two ends of the tie rod from the short arm (side of the quadrangle almost halfway) to the long side (arm). 3.424) Single tie rod crisscrossed on central ring and resting on the rim of the single wheel (more called central ring or small concentric central wheel), on two bicycles, and the two ca = pi attached to the double 11th type lever rod in lateral thrust double of the (true) middle concentric wheel. And drag radii from the middle to the largest rim. With the two bicycles supplied or not (one or the other or both) of weight. 3.425) As above from n.0001 to n.3.424 and to this he constructs a self-rotating system between two concentric wheels, of which the rim of the r. Maggiore cancels in the center with one (and levers, levers) or two bicycles the two thrusts (Attiva and Reactiva: A-R) of the tie rod that goes from the long arm of the lever pivoted on; wheel median to the radius of the lever (or of the other bicycle) which folds at 90 ° (or in any case) on the oblique radius of the median wheel which with the radius pushes the said larger wheel rim; thrust added to that of the short arm of said lever of I) ° with = tro the other lever. With a without weight in the position (between tie rod and middle wheel) of N.-C. (Newton-Centrifugation).-With or without drag ratio (synchrony) for F = A A 'A "-3.426) As above in nos. 3.425 and 3.426 also this author takes energy from the eccentric tie rod (spring stretched with or without weight between tie rod and median wheel), with a fulcrum resting on said median wheel or on a central axis ring, smaller than it, with 1st type lever, with active long arm and short arm partially braked by the other end of the tie rod, lowered, and extended to push (A) the rim of the larger wheel, and use the uniform Reaction (R) to the motion. 3.4271) As the previous 3.426, but with two levers (one of which is a mixed type: i ° and 11 °) superimposed on the long arm of the underlying pivoted towards the center with an adjustable bicycle and two thrusts against the rim of the two levers of I ° t. With or without drag hooks (spokes or rope). 3.428} As the previous one, also this fig. 3.428 proposes a self-rotating one made with a rim and / or wheel, with an external rope pulled by the short arm of the only I ° type lever pivoted on the rim or rim of the single wheel, which uses also the Reaction (R) uniform to the motion. 3.429) As above from n.0001 to n.3.428 and to this 3.429, which makes the motor wheel with the strongest tie rod on the right for the long arm pivoted on a radius of a central ring, different from that of the wheel (or rim) pushed by it spoke, and pulled by the short arm inclined and lowered to pull the rope on the lateral eccentric spoke 3,430) As above from n.0001 to n.3.429 to this n.3.450 which wants to make the WHEEL-MOTOR with 1st type lever pivoted on the ring of the center or one of the two (or only) concentric wheels to the greater external thrust from the short angled arm of the aforesaid lever on which the tie rod ends and on the other side pulls the long arm. 3.431) As above in n.3.430 each self-rotating with traction and c = centric tie rod with or without weight, which starts from the long arm, to the left (in the hypothesis) of a 1st type lever, pivoted on a median wheel (with or weightless) and the short arm, which pushes the angled shaft against the inner bicycle of the larger rim, pushing the oblique radius of the median wheel, with or without spokes (rope hooks) for driving between the wheel rims 2.432) As above in n.3.430 each motor wheel made with two concentric wheels, of which the median for support of the tie. the two ends of which grasp the long arm of the I "type lever, pivoted on the rim of the r.magg. with a bicycle or other fulcrum, and the short arm in traction (with rope) or in thrust with hook of the wheel ned; with or without weight. 3. 433) As the previous 3.432, but without weight, with or without spokes or hooks (or rope) of drag or synchrony. 3,434) As above from n.l to n. length of the lever on the vertical lever and eccentric rope on the other side. 3.435) As above in 3.434, with the central lever not vertical, but oblique, in order to have a greater grip of the tie rod. 3,436) As above from 3,423 to no. Instructs a self-rotating made with two concentric wheels, of which the smallest central ring) serves to support the fulcrum rod of the first lever which, equipped with a tie rod (with or without weight), has a short arm with rope traction and a long arm. = go of a second type I lever, which with its short arm (even much longer than its long arm) with an eccentric cord pulls the rim of the larger wheel, which has its bearing ring on the central axis. 3. 437) As above from n.0001 to n. 3,436 and to this 3. 437, which like the previous one has two type I and II levers, as it also uses the fulcrum as eccentric pressure, of the first with an oblique radius (or angled see above n. 3. 436, or no spokes) as in this case, which also has the weight between the two pieces of the rant and the eccentric final hook against the larger wheel, and provides a summary formula of the force: F = A + A 'A' 1 A '' ' 3.438) As above at 3.437) we claim each self-rotating with eccentric traction, with tie rod (with or without weight) between a I ° type lever rod, planted on the central central wheel, by its long arm (even if shorter than the other) and another I ° type lever rod pivoted on the angled radius of the said med wheel. with the short arm against the rim of the larger wheel, and the long arm pulled both by the tie rod and by the rope of the short arm of the first lever (type I). "Radius angled both outward as in fig.) And inward (towards the center) with respect to the tie rod.