专利摘要:
The sprocket with radius in broken lever radius, is a wheel (3) that forms a perimeter with teeth, which is joined to its central axis by broken axes (4-6), which protrude from both sides of the wheel (3) forming broken sayings. This arrangement forms a broken lever radius that increases the force that a crown can transmit, towards a pinion, with respect to the force that this wheel (3) would have, in the case that its spokes were rectilinear, and, did not protrude, - escaping from the plane of the wheel (3) -, and, they had the same rectilinear and virtual distance that this wheel (3) has, between its central axis, and, its perimeter. (Machine-translation by Google Translate, not legally binding)
公开号:ES2632133A1
申请号:ES201600199
申请日:2016-03-09
公开日:2017-09-11
发明作者:Fº JAVIER PORRAS VILA
申请人:Fº JAVIER PORRAS VILA;
IPC主号:
专利说明:

WHEEL DENTED WITH RADIOS IN BROKEN LEVER RADIO OBJECT OF THE INVENTION
The main objective of the present invention is to increase the radius of a wheel, so that it behaves as if it had a much longer radius, which implies that the force it can transmit will be much greater than that transmitted when its radii they are normal and remain in the plane of the Wheel (3), without escaping from said plane, as it happens on this occasion, which are seen to protrude from the plane of the Wheel (3), forming broken axes (4-6) beyond of its two faces.
In this sense, this Wheel with Broken Lever Radii, will be optimal to increase the Force that transmits a Crown to a Pinion, without having to increase the size of the Wheel, or ca, without having to increase its Virtual Rectilinear Radio that can be Measure on the existing Distance, on the Wheel (3), from its center, to its Perimeter. BACKGROUND OF THE INVENTION
The main antecedent of the present invention can be found in the Radius Principle of Archimedes Lever, and, also, in my Principle of Broken Lever Radio, which comes to be the same as the Archimedes Principle, though, for those cases in which the Radio is not rectilinear, but it forms broken lines. Another background of the present invention can be find in my Utility Model, presented in the year (2003), whose final number was: U200502069, entitled: Rectangular axle for the pedals and the bicycle plate. Another variant of the previous device is also presented in another of my Patents. This is Patent P200502543, entitled: Bent axle pedal (180 "). We find another immediate precedent in my Patent na P20110J344, entitled: Rigid spiral gear, and also in my Patent P20120093, entitled: Gear -with a spiral lever arm cl / adrada, which featured a Gear-Cone whose rods, which remotely join the two Cogwheels, -Pylon and Crown-, were bending at angles of (90 ") forming different sections.
The Principle of the Broken Lever Radius, in the Gear-Cone of the aforementioned Patent, had some rods that formed this type of Broken Radii (4-6) to increase the Force that could transmit the Pipion, to its Crown, without having that increase the Length of the Rods, between said Crown and Dieho Piñón. As we will see later, there is an express difference between this device, the Gear-Cone, and, a Pinion-Crown transmission, because the sense of the Force is different too. In the Gear-Cone with Rods in Broken Lever Radio, there is also a Perpendicular Lever Radius, which does not exist in the device presented today, which implies that, in the Gear-Cone, the Force that will transmit the Pinion, will increase its value, depending on the value of the Broken Shafts, while, in the Cogwheel (3) of the invention today, the exact opposite would occur, and, the Force of the Pinion, would be reduced, by instead of increasing
DESCRlPCJ6N OF THE INVENTION The toothed Rl / eda with radii in broken lever radius, is a metal wheel (3), whose Radii (4-6) form a Broken Lever Radius (RPQ) when they escape from the plane of the Wheel.

The usual thing is that the Radios pennanezcan in the same plane of the Wheel (3), but, on this occasion, it is about Fleeting Radio (4-6), which come and go from one side of the Cogwheel (3), To the other side. In figure na 1, -y, in the upper half of the Wheel (3) -, it is observed that these Radii (4-6) start from the center of the Wheel (3), and, protrude outward from the plane of the Wheel (3), connecting three Broken Axes (4-6). The third Axis (6) is the one that joins the Perimeter, and, it is fixed, -by the inner face of the Wheel (3) -, to the center of it. The Axis (5) extends, then, from the end of the Axis (4), to the end of the Axis (6), crossing the inner plane of the Wheel (3). In the lower half of the same Wheel (3), there are also three other Broken Shafts (4-6), same as the previous ones, although, on this occasion, and, as it could not be otherwise, the External Axis (6), is the one that is fixed to the Perimeter, on the other side of the Cogwheel (3).
In Figure I I have only represented three Broken Axes (4-6) in each half of the Wheel (3), but, four, five or six Broken Axes can be placed as described. Date of the invention: (08.03.16). DESCRiPTION OF THE FIGURES
Figllra # 1: Front view of a Cogwheel (3) whose Radii form a Broken Lever Radius (RPQ) because they are Radii (4-6) that break when they escape the plane of the Wheel, to return, later, on that same plane, to which they cross later, and, they return to find another broken one in the other face of the Wheel (3).
Figure # 1:
1) Electric motor 2) Shaft
3) Cogwheel 4) First broken radio
5) Second broken radius 6) Third broken radius
DESCRiPTION OF A PREFERRED EMBODIMENT
The serrated RlIeda with radii in crowded lever radius, is characterized by being a component for mechanical devices that has the quality of increasing the Force that a Crown can transmit, towards a Pinion, without having to increase the Crown Radius, or, rather, without having to increase the existing virtual distance between the perimeter of the wheel (3) and its central axis. On this occasion, it is about putting some Broken Radii (4-6) that will transmit a Flierty in crowded lever radius, which can be measured, approximately, with the following
equation: (FRPQ = Fo. Rn. cos (n-l) a), in which the relationship between the Ftlerza of
Origin that sends, towards the Perimeter of a Pinion, the Force of a Crown .., the Length of each Broken Axis (4, 5a, 5b, 6) raised to the Power (n) of the Number of Radii that has the Radius of Broken Lever, -which should all be equal, for which, we will have to consider that the Axis (5) must be divided into two sections (5a, 5b) that will have the same Length-, and, the Cosine of Alpha, raised to ( nl), which will be the Angle that forms each Broken Axis (4, 5a, 5b, 6), with the line of the previous immediate section, always counting in the direction and direction in which the Force is transmitted, which means that it is necessary to count, from the Axis (6), to the Axis (4), which is connected to the center of the Wheel (3). It must be taken into account that, when the sense of the Force that is transmitted, starts from the center of the Wheel (3), and, is directed towards its Perimeter, Force L. 3 will be reduced by the same amount as it increases , when transmitted in the reverse direction, that is, when it circulates from the Perimeter of the Wheel (3), to its center. Hence, this Wheel with Broken Lever Radius, is optimal for increasing the Force that a Crown will transmit, towards a Pinion, but, it will also be optimal, to reduce it, when it is the Axis centered, the Axis (2) of a motor (1), which transmits it to the perimeter of its wheel. With the previous equation we can study what happens when we give values other than (R), starting with the smallest values. If we imagine that, instead of a Cogwheel (3), it is a Balance that has one of its Radii, Broken in three equal sections, we will observe that, when the measure of its three sections is equal to that of the other Radius that does not is Broken, the resulting Force is almost the same that, if this Broken Radio in three sections, it was a single rectilinear section, whose Length was equal to the sum of the three sections. There is a small loss of value caused by the Angles that form the three sections together. If we increase, then, the value of the Length of the three broken sections of this Balance, we will observe that the Force that is transmitted is increasing considerably, and, in direct proportion to said increase. All this indicates that the Wheel (RPQ) that is presented, is very useful for aWDentantar much the Force that can transmit, tIDa Corona, to a Pinion, without having to put another Wheel, in which we would have to greatly increase the Length of its rectilinear radii. I mean by this, that the Force, in the Wheel (RPQ) is not put in direct proportion, now, with the ratio between the respective Crown Radii and the Pinion, since, in the Broken Lever Spoke Wheel ( 3), the Force that is transmitted can be much greater than the Virtual and rectilinear Radio that forms the distance between the center of the Wheel (3) and its Perimeter.
权利要求:
Claims (1)
[1]
1) Cogwheel with spokes in broken lever radius, characterized by being a Wheel
metal (3), whose Radii (4-6) form a Broken Lever Radius when they escape the plane of
the wheel. These are elusive Radios (4-6), which come and go from one side of the Cogwheel (3),
5 to the other side. In the upper half of the Wheel (3), it is observed that these Radii (4-6) start from its center, - where they join the Axis (2) of the Motor (l) -, and, protrude outward from the plane of the Wheel (3), forming three Broken Axes (4-6). The third Axis (6) is the one that joins the Perimeter, and, it is fixed, -by the inner face of the Wheel (3) -, to the center of it. The Axis (5) then extends from the end of the Axis (4), to the end of the Axis (6), crossing the inner plane of the Wheel
10 (3). In the lower half of the same Wheel (3), there are also three other Broken Shafts (4 6), the same as the previous ones, although, on this occasion, the outer Axis (6), is the one that is fixed to the Perimeter, on the other side of the Cogwheel (3).
4 3 2 1



Figure 1
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引用文献:
公开号 | 申请日 | 公开日 | 申请人 | 专利标题
WO1996035606A1|1995-05-13|1996-11-14|Christian Seibert|Crankshaft for transforming a linear motion into a rotational one or vice versa|
ES2277539A1|2005-10-18|2007-07-01|Fco. Javier Porras Vila|Pedal for mechanical traction of bicycle is placed on major plate whose diameter is crossed by double axis|
ES2409091A2|2011-12-14|2013-06-24|F. Javier Porras Vila|Gear with rigid spiral |
ES2454365A2|2012-09-17|2014-04-10|Fº JAVIER PORRAS VILA|Gear-cone with line-shaped rods with successive folds |
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优先权:
申请号 | 申请日 | 专利标题
ES201600199A|ES2632133B1|2016-03-09|2016-03-09|Cogwheel with spokes in broken lever radius|ES201600199A| ES2632133B1|2016-03-09|2016-03-09|Cogwheel with spokes in broken lever radius|
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