• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The pedal car with gear trains-double-cone, is a mobile formed by a chassis with four rubber wheels (1, 12). Those of the anterior axis are independent of the thrust mechanism that begins in the pedals (3) that have, at the ends of their axis, two crowns (4) that mesh with the pinions (5) of two gear-double brakes- cone (5-9) and (5'-9 '), formed, in turn, by a pinion (5, 5') and a crown (9, 9 '), connected at a distance by metal rods (6, 6). ') that intersect in a bearing (8, 8') that is fixed in the chassis and that acts as a balance fulcrum. This bearing (8, 8 ') is located closer to the crowns (9, 9') than to the pinions (5, 5 '). The crowns (9, 9 ') engage the pinions (10) of the axle (11) of the rear wheels (12) of rubber. (Machine-translation by Google Translate, not legally binding)
    公开号:ES2676604A1
    申请号:ES201700084
    申请日:2017-01-23
    公开日:2018-07-23
    发明作者:Fco. Javier Porras Vila
    申请人:Fco. Javier Porras Vila；
    IPC主号:
    专利说明:

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    DESCRIPTION
    CAR PEDALS WITH GEAR-DOUBLE-CONE TRAINS
    The main objective of the present invention is to form a pushing mechanism, which can multiply the force that the pilot applies to the pedals (3) of his toy car, -or, to his racing car in a larger version dimensions-, so you can reach enough speed that, not only allows you to move, but also to be able to go faster than the other drivers. BACKGROUND OF THE INVENTION
    The main antecedent of my invention of the day (21.01.17) is in the Archimedes lever, while the double-cone gear (4-8) is based on it. The second main antecedent can be found in my cone-gears, formed by a pifion and a crown that are remotely joined by metal rods, which join the sides of their perimeters. These cone-gears can be found, for example, in my patent No. P201200374, entitled: reciprocating toy with spirals, where, in addition, they multiply to form gear-cone trains. DESCRIPTION OF THE INVENTION
    The pedal car with double-cone gear trains, is an object of displacement, both toy and racing, formed by the two rubber wheels (1) located at the ends of the previous axle (2), which are independent of the mechanism described below, in which some pedals (3), similar to the crankshaft arches of a combustion engine, have, at both ends of their axis, a system that doubles and extends on each side of the pilot, which is formed by the toothed crown (4) of the ends of the pedal axle (3), which are engaged with the pinion (5) of a double-cone gear (5-9), which is formed by that pifion (5) and a crown (9), which are joined at a distance by metal rods (6, 8), which intersect in a bearing (7) located one fifth of the distance that the it separates, closer to the crown (9) than the pipion (5). This crown (9) is engaged with the pinion (5 ') of a second double-cone gear (5'-9'), whose crown (9 ') is engaged with the pinion (10) of the shaft (11) of the rear wheels (12).
    DESCRIPTION OF THE FIGURES
    Figure No. T. Plan view of the motion system presented, in which the previous rubber wheels (1) are in the upper area, and, below them, the two systems formed by the two are duplicated double-cone gears (5-9) and (5'9 '), which are engaged with the pifions (10) of the axle (11) of the rear rubber wheels (12).
    Figure n ° I:
    1) Rubber front wheels
    2) Axis
    3) Pedals
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    4) Crown
    5) Pipion
    6) Long Pifion rods
    7) Bearing or fulcrum
    8) Short crown rods
    9) Crown
    5 ’) Pipion of the second double-cone gear
    6 ’) Long rods of the second gear-double-cone plunger
    7 ’) Bearing or fulcrum of the second double-cone gear
    8 ’) Short crown rods of the second gear-double-cone
    9 ’) Second gear-double-cone crown
    10) Rear wheel axle pinion
    11) Rear wheel axle
    12) Rubber rear wheels
    DESCRIPTION OF A PREFERRED EMBODIMENT
    The pedal car with double-cone gear trains, is characterized by being an object for the game, or, to make races, according to the dimensions in which it is presented. It uses two gears - double-cone (5-9) and (5'-9 ') that form a train, so that the crown (9) of the first, will engage with the pipion (5') of the second, and, the crown (9 ') of the second, would be engaged with the pipion (5 ”) of the third, and so on. In each of these gears-double-cone (5-9) and (5'-9 ') of the train, a pifion (5, 5') and a crown (9, 9 '), are joined at a distance by means of metal rods (6, 8) that intersect in a bearing (7), one fifth of the distance that separates them, this bearing being (7) closer to the crowns (9, 9 ') than to the pifions ( 5, 5 '). If you look closely, this double-cone gear (5-9) is the same as an Archimedes lever. If, from figure 1, we eliminate one of the rods, the top one for example, and, we make the rod (6, 8) that remains, instead of going up and down supported by the bearing (7), - which functions as the fulcrum of the lever of Archimedes-, turn, because we have previously joined the ends of the rod (6, 8) in the pivot of the side of the perimeter of the pifion (5) and the crown (9), we will observe that the force of the pifion (5) that is transmitted, will increase with the length of its own radius, - be the rod (6) -, so that, the further this pipion (5) moves away, from the bearing (7), -o, fulcrum-, its strength will increase proportionally, as the principle of the Archimedes lever says. If we come back now
    to put the other upper rod to re-form the double-cone gear (5-9), the effect will be exactly the same, and, the pifion (5) and the crown (9) will be better fixed to the structure of the
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    double-cone gear (5-9). In this way, we can increase the strength of the pilot's pedaling, which will increase even more if we double the thrust system, - that is, the double-cone gear (5-9) -, on each side of the pedals ( 3). Archimedes' strength can be measured with the
    following equation, in which the force of origin is conjugated, -which, in this case would be the force applied by the pilot's legs, and, in other cases, could be the force of any motor-, with the radius
    of the own rod: (FArq = Fo R). The advantage of using in this way a part of the
    Archimedes' equation, is that it allows us to better understand the difference between the weight and strength of Archimedes, which are different concepts, while the weight, -the weights we put on a scale's plates-, even though , in themselves they are a force, they always remain identical to themselves, although we progressively separate them from the fulcrum. However, Archimedes' strength is what increases with the increase in the radius of each weight, even though the value of the weight remains constant. Hence, a small difference between this is established
    Archimedes force equation, and, Archimedes balance equation (
    W¡ R] = fV2 R2), whereas, with this equation we can determine the balance situation of the balance, -or, that of a lever-, while, with the previous one, we measure what increases the force of Archimedes in each of the balance plates, and, separately, what it means is that, what it measures, is not the equilibrium situation of the balance, but, precisely, quite the opposite, that is, what unbalances it , or, that can unbalance it. The most immediate consequence of
    This equation of the Archimedes force affects the concept of the energy that the Archimedes force of each plate of the scale would have. If we consider that the height (y) is the distance that goes up and down each of its plates, the energy of this movement of the scales plates can be measured
    by this equation: (FAly = F0 ■ R), and, (Balance_plate = FArq y = (F0 • R) ■ y), | 0 that would be very different from what the classical energy equation would measure, which would be this other equation: (
    ^ Plato-Balanza-I = w ■ jKi), or so: (£ Waf0_a] ¡anza.2 = W2 ■ y2), which would be written in this way based on the idea that all weight is, in itself same, a force that, as it travels through a space, can be measured as energy, according to the classical equation of energy that we all know:
    (E = F ■ X). Now, as, in today's invention, it is a turntable, -the pinions (5, 5 ') and the crowns (9, 9') -, the height (and) will be replaced by the perimeter of its rotation circular, which will lead us to modify the previous equation, in this other way: (
    Enao-Balance = EArq ‘Fet = (E'0 ■ R) '(27t R)). With my equations, what is reflected
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    Archimedes' strength increases as a function of the radius increase, which is what cannot be done with the classical energy equation. And, these equations better justify the operation of the invention that I present here today. Moreover, we can also study the advantage of these double-cone gears, compared to the previous cone gears. Let's assume that
    we have the figure of that toy that was called a discologen at the time, which is formed by two exactly equal cones, joined by their respective vertices, and, which is rolled with a rope that runs through the union of the two vertices. In this figure, the force of Archimedes that could transmit the wheel of one of the bases of one of the cones, towards the other wheel, would be (00%) of the force of Archimedes received from the wheel of an engine, or , from the pedaling of a pilot. Now,
    we increase the length of the radius, -or, of the height-, of one of the two cones, and, as it happens in a balance, the force of Archimedes of the wheel of the base of that cone that lengthens, will also increase in proportion to the increase of that height, and, it will increase in each centimeter more than it moves away from the fulcrum, or, of the bearing (7) that we put in the union of the two vertices of the two cones, the short and the long. In this sense, in the double-cone gear (5-9), the force will increase in the percentage of Archimedes force that is transmitted, from the pipion (5) to the crown (9), from (100 %), while, in a gear-cone, the force that was increasing as we increased the length of the metal rods that join the pinion and the crown, only increased from (50%), because we know that, in A piece of gear, with two cogwheels attached, the pinion can only transmit (50%) of the force it receives, towards its crown. And, when we progressively increase the length of the rods that join that pinion and that crown to form a gear-cone, the force will gradually increase, but, as I say, it can only do so from that (50%), and , not from (100%), as I have just pointed out what happens in today's double-cone gear (5-9). We should only modify one element of the previous equations, while the crown (9) can have a larger diameter than the pipion (5), even though it could have the same diameter, and, it would work the same. In the event that the diameter of the crown (9) is double, or, triple that of the pipion (5), the rods (8) of the crown (9), would form a greater angle with respect to the line that it will be formed in the case that the pifion (5) and the crown (9) had the same diameter. As this angle grows, the force of Archimedes that is transmitted from the pipion (5) to the crown (9) will be less, so the above equations should accuse such variation. In this sense, the force of Archimedes who would receive the crown (9), has to
    multiply by the cosine of that angle, what we will do like this: (FÁrq- = (^ o-i / ,) ■ COS «), and,
    (Fjrq-i * (^ 0-2 ^ 2) cos a)> 1st flue will therefore affect the equations derived from them:
    (Erirto-Boi ™ = Fa „, ■ y = ((F0 ■ R) ■ eos a) y)
    (Epiao-Botan * = FÁrq ‘Per = ((F0 'R)' eos a) ■ (2n R)).
    权利要求:
    Claims (1)
    [1]
    I) Pedal car with double-cone gear trains, characterized by being an object of displacement, both toy and racing, formed by the two wheels (I) of the previous axle (2), which are independent of the mechanism described below, in which about 5 pedals (3), similar to the crankshaft arches of a combustion engine, have, in both
    ends of its axis, a system that duplicates forming a train, and, which extends to each side of the pilot, which is formed by the toothed crown (4) of the end of the pedal axis (3), which engages with the pifion (5) of a double-cone gear (5-9), which is formed by that pifion (5) and a crown (9), which are joined at a distance by metal rods (6, 8), which they cross in a bearing 10 (7) located one fifth of the distance that separates them, closer to the crown (9) than to the pipion
    (5); this crown (9) meshes with the pipion (5 ’) of a second double-cone gear (5’-9’) that forms a train with the previous one; its crown (9 ’) engages with the pinion (10) of the axle (11) of the rear wheels (12).
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    同族专利:
    公开号 | 公开日
    ES2676604B1|2019-05-14|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    GB446428A|1934-10-31|1936-04-30|Stewart St George|Mechanically propelled conveyance of the tank or endless track type for amusement purposes|
    US4084836A|1976-11-16|1978-04-18|Lohr Raymond J|Pedal car|
    US4479327A|1982-07-10|1984-10-30|Mitsuwa Kogyo Co., Ltd.|Electric car with winch having automatic shutoff|
    ES2461567A2|2012-04-02|2014-05-20|Fº JAVIER PORRAS VILA|Push-pull toy with spirals |
    法律状态:
    2018-07-23| BA2A| Patent application published|Ref document number: 2676604 Country of ref document: ES Kind code of ref document: A1 Effective date: 20180723 |
    2019-05-14| FG2A| Definitive protection|Ref document number: 2676604 Country of ref document: ES Kind code of ref document: B1 Effective date: 20190514 |
    优先权:
    申请号 | 申请日 | 专利标题
    ES201700084A|ES2676604B1|2017-01-23|2017-01-23|Pedal car with gear trains-double-cone|ES201700084A| ES2676604B1|2017-01-23|2017-01-23|Pedal car with gear trains-double-cone|
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