The invention relates to a helical gearing with the defining characteristics of the preamble to claim 1.
DE 602 22 101 T2 has disclosed a helical gearing with a spindle and a nut placed thereon. When the spindle is driven to rotate, the nut is slid in the axial direction. To this extent, the known helical gearing corresponds to conventional helical gearings. The nut of the known helical gearing has two opposing shaft stubs protruding radially outward on which rollers are supported in rotary fashion. The rollers engage in slots in a sleeve that coaxially encompasses the nut and the spindle. One section of the slots extends in the longitudinal direction of the helical gearing, i.e. in an axially parallel fashion, and at one end, the slots transition into a curved path that ends with a radial path, i.e. one that is transverse to the helical gearing. The sleeve is situated in stationary fashion and the rollers of the nut roll against flanks of the slots in the sleeve. If the rollers of the nut of the known helical gearing are situated in the axially parallel sections of the slots of the sleeve, then the nut is secured in a rotationally fixed fashion and slides in accordance with the thread pitch when the spindle is rotated. This, too, corresponds to conventional helical gearings. If the rollers of the nut travel into the curved sections of the slots, then the nut rotates, with the rotation of the nut coinciding with the rotation of the spindle so that the sliding motion of the nut decreases or increases depending on whether the slots are curved in the thread direction of the spindle or opposite from it. As a result, the apparent pitch of the screw thread changes; it is possible to produce a higher axial force of the nut with a given torque or conversely, it is possible to produce a higher sliding speed with a given rotation speed of the spindle. An apparent multiplication of the helical gearing changes; the expression “apparent multiplication” is understood to mean the ratio of the sliding speed of the nut relative to the rotation speed of the spindle.
It should be noted that these are movements of the nut relative to the spindle. Instead of driving the spindle to rotate, it is also possible to drive the nut and the sleeve encompassing it to rotate, thus causing a sliding motion of the spindle. It is also possible to slide the spindle or nut in order to produce a rotary motion of the respective other part, i.e. of the nut with the sleeve or of the spindle.
The helical gearing according to the invention, with the defining characteristics of claim 1 has a thread, for example on a threaded spindle. The thread is engaged by a counterpart component instead of a nut. For this purpose, the counterpart component has, for example, a pin, a sliding block, a rolling component such as a roller, or the like, which rests against a thread flank of the thread. A contact with a thread flank is sufficient if an advancing motion is only supposed to occur in one direction, i.e. the helical gearing is always loaded in the same direction. For a bidirectional drive, the engagement of the counterpart component with the thread must occur at two thread flanks facing toward or away from each other. In other words, a convolution can be embodied in the form of a groove, for example, in which a roller of the counterpart component engages. The two grooves flanks are composed of thread flanks facing toward each other; the roller of the counterpart component rolls along one of the two thread flanks depending on the rotation direction of the thread. The counterpart component is driven in two directions. The counterpart component can also have two rollers between which is situated a raised convolution of the thread so that the rollers roll along two thread flanks of the thread facing away from each other. The counterpart component in this case is likewise driven in two directions. The engagement with the thread can also occur by means of sliding instead of rolling, for example by means of a pin or a sliding block of the counterpart component.
According to the invention, the thread of the helical gearing has a changing pitch, thus changing a multiplication of the helical gearing. The multiplication of the helical gearing is the ratio of the sliding motion of the counterpart component to the rotation (angle of rotation) of the thread. As explained in connection with the prior art, the counterpart component can be driven to rotate and the thread can thus be slid or a sliding of the thread or counterpart component can be converted into a rotation of the respective other part.
The pitch of the thread of the helical gearing according to the invention can essentially change in any way; in other words, it can increase and then decrease again, for example. It is also possible for some sections to have a pitch of zero or even for some sections to have a negative pitch which means that the thread pitch reverses, i.e. a right-hand thread has one or more sections embodied in the form of left-hand threads. The sliding motion of the counterpart component with reference to the thread reverses in these sections.
As mentioned above, the advantage of the helical gearing according to the invention is the changing multiplication. It is thus possible in some sections of the thread to achieve a powerful axial force with a given torque and in other sections of the thread, to achieve a high sliding speed with a given rotation speed. It is not absolutely necessary for a spindle to be equipped with the thread; it is also conversely possible for the counterpart component to be embodied, for example, in the form of a sleeve equipped with an internal thread that is engaged by a pin, a sliding block, a roller, or the like belonging to a rod or other component that extends through the sleeve. The function of the helical gearing does not change as a result of this; naturally, the design changes as a result, but the design principle underlying the present invention is retained.
Advantageous embodiments and modifications of the invention disclosed in claim 1 are the subject of the dependent claims.
With a multi-start thread (claim 3), for each convolution, the counterpart component preferably has a pin, a sliding block, a rolling element, or a similar element, which engages the respective convolution (claim 4). With two convolutions, the counterpart component can be driven in a moment-free fashion; a moment is understood here to be an imaginary axis radial to the helical gearing, i.e. a tilting moment around the transverse axis of the counterpart component. With three convolutions, the engagement of the counterpart component with the thread is statically defined.
Claim 5 provides a spring element that is placed under stress when the counterpart component is slid in one direction relative to the thread and is allowed to relax when the counterpart component is slid in the opposite direction. In other words, energy is stored in the spring element with a sliding motion in one direction and (disregarding losses) the spring element then gives back this energy with a sliding motion in the opposite direction. The spring element can be prestressed so that it always exerts a spring force on the counterpart component. Also according to claim 5, the thread pitch increases with the decrease in the spring force or prestressing due to the deforming of the spring element, i.e. due to the sliding motion of the counterpart component relative to the thread. The multiplication of the helical gearing thus increases with the decrease in the spring force of the spring element. The subject of claim 5 intrinsically comprises an actuating device that exerts a force or moment. In the opposite movement direction, stress or more stress is placed on the spring element, i.e. energy is stored in it. The actuating device can also be referred to as an actuator. It permits the use of a comparatively low-powered drive unit since part of the force that the actuating device exerts is exerted by the stressed spring element. To accomplish this, the drive unit must actively reset the actuating device, i.e. must place stress on the spring element again after the actuation in order to once again store the previously output energy. As explained previously, the actuating device can exert a force or moment. Aside from a linearly acting spring element such as a compression or tension spring, the actuating device can also have a spring element that exerts a moment, for example a spiral spring.
An actuating device of the kind explained in the preceding paragraph can also have a thread with a constant pitch (claim 7).
Claim 10 provides a brake with which it is possible to fix the helical gearing in any position. For example, it is possible to use an electromagnetic brake that is actuated, i.e. applied, when without current. It is possible to use brakes or clutches that engage in a nonpositive, frictional way or in a form-locked way.
The helical gearing according to the invention can also be used as a variable damper; this is the subject of claim 12. The damping occurs through braking of the rotation of the thread and/or through braking of the sliding motion of the counterpart component. The braking can be carried out by means of a brake or for example also by means of a motor. For example, an electric motor can be operated as a generator or also in so-called four-quadrant operation, i.e. can be selectively operated as a motor and as a generator in order to produce a desired variable damping. As provided here, the motor or a drive unit in general acts in opposition to a load. It is also possible to use a hydraulic motor, hydraulic cylinder, or other drive unit to execute a variable damping and, as needed, a driving function. The helical gearing according to the invention can also be used as an energy storage device.
The invention will be explained below in conjunction with exemplary embodiments shown in the drawings.
Other defining characteristics of the invention ensue from the following description of embodiments of the invention in connection with the claims, the preceding description, and the drawings. The individual features can each be embodied separately or can be embodied several at a time in any combination in the embodiments of the invention.
The helical gearing 1 according to the invention shown in
Convolutions 5 of the thread 3 are embodied in the form of helical grooves; other cross-sections of the convolutions 4 are also possible; for example, the convolutions can also be raised, as depicted in
The counterpart component 4 has a sleeve 6 that encompasses the spindle 2 concentrically. Shaft stubs 7 protrude inward from the sleeve 6 and support rolling elements embodied in the form of rollers 8 in rotary fashion. The rollers 8 engage in the convolutions 5, which are embodied in the form of grooves; when the spindle 2 rotates, the rollers 8 roll along thread flanks 9 of the convolutions 5, i.e. of the thread 3. For each convolution 5, the counterpart component 4 has one roller 8, which engages in the convolution 5 or in other words, engages with the thread 3.
Through rotation of the spindle 2, the counterpart component 4 is slid axially relative to the spindle 2; in the process of this, as a result of the changing thread pitch, the sliding speed of the counterpart component 4 changes with a constant rotation speed of the spindle 2. Also due to the changing thread pitch, a change occurs in the axial force with which the counterpart component 4 is slid with a constant driving moment of the spindle 2.
Naturally, the kinematic reverse is also possible: the counterpart component 4 can be driven to rotate, thus sliding the spindle 2 relative to the counterpart component 4. It is also possible to slide the spindle 2 or counterpart component 4 axially relative to the respective other part 4, 2, thus setting the respective other part, i.e. the counterpart component 4 or the spindle 2 into rotation. The prerequisite for the conversion of a sliding motion into a rotating motion is a sufficiently high thread pitch that avoids a self-locking. A comparatively low thread pitch is sufficient for this purpose due to the rolling support of the engagement of the counterpart component 4 with its rollers 8 in the thread 3.
The rolling support of the thread engagement is not absolutely required; a sliding support is also possible, for example by having the shaft stubs 7 of the counterpart component 4, embodied in the form of pins, engage in the convolutions 5 (not shown). The changing thread pitch changes a multiplication of the helical gearing 1.
Basically, it is sufficient for there to be a single-start thread 3 that the counterpart component 4 engages at one location, i.e. a thread 3 with one convolution 5, in which the counterpart component 4 engages with a roller 8 (not shown). In the embodiment of the invention shown in
In
The spindle 2 of the helical gearing 1 is rigidly connected to a motor shaft 12 of an electric motor 13; it can be of one piece with the motor shaft 12. In order to reduce the centrifugal mass, the spindle 2 and/or the motor shaft 12 can be hollow (not shown). In addition, the rollers can be situated on the motor shaft or on a shaft extending the motor shaft and can roll along internal convolutions of the counterpart component (not shown). Instead of the spindle 2 being rotationally fixed relative to the motor shaft 12, a (reducing) transmission can be situated between the electric motor 13 and the helical gearing 1. The term “between” does not absolutely refer to the spatial location of such a transmission, but to its location with regard to the transmission of moment. A planetary gear arrangement is suitable for this due to its compact design.
The spindle 2 and the motor shaft 12 are coaxial to each other. The electric motor 13 has a tubular motor housing 14 that is situated coaxially in the tubular actuator housing 15. A diameter of the actuator housing 15 is greater than a diameter of the motor housing 14, leaving an annular gap 16 between the actuator housing 15 and motor housing 14 in which gap the spring element 17 is accommodated. In
When the electric motor 13 drives the spindle 2 to rotate, this causes the counterpart component 4 to move in a sliding fashion. The thread pitch increases as the distance from the electric motor 13 increases, i.e. with a relaxing of the spring element 17. In order to output a torque, the electric motor 13 is supplied with current and the motor shaft 12 is consequently driven to rotate. The rotation and torque can be output from the motor shaft 12. The rotation is assisted by the spring element 17, which presses against the counterpart component 4 and exerts a torque on the spindle 2 via the helical gearing 1. The electric motor 13 consequently exerts only part of the torque that the actuator 10 outputs. The torque output by the actuator 10 can generally be understood to be an external load or a reaction moment to an external load that acts on the motor shaft 12 in the form of a moment external to the actuator housing 15. In order to return to the starting position, the electric motor 13 is operated in the opposite rotation direction. As a result, it exerts stress on the spring element 17 via the helical gearing 1, thereby storing energy in the spring element 17, which is subsequently output once more in a rotary drive mode. The returning motion is carried out actively by the electric motor 13, which as described above, must exert a torque in order to exert stress on the spring element. If the external load is also active in the returning action, then it assists the returning action. In this case, the electric motor 13 exerts only part of the moment that is required to exert stress on the spring element 17. In a stopping of the external load, the spring element 17 assists the electric motor 13 thereby reducing its current consumption and thermal load.
The actuator 10 from
The actuators 10 from
With the sliding motion of the counterpart component 4, the helical compression spring 18 that constitutes the spring element 17 is prestressed to a greater degree, thus storing energy that it subsequently outputs with the next extension of the counterpart component 4. The actuator 10 consequently functions as an energy storage mechanism. The energy storage in the spring element 17 also contributes to the possibility of using a less powerful electric motor 13, hydraulic motor, hydraulic cylinder, or other drive unit.
In the region between the radial sections 29, 30, the convolution 5 has a steadily increasing pitch. This is not absolutely required; the pitch of the convolution 5 can also decrease again; it is even possible for there to be sections with a negative pitch in which the movement direction of the counterpart component 4 would reverse (not shown). As is readily apparent from
The actuator 10 constitutes a subassembly with the helical gearing 1 and the electric motor 13 functioning as the drive motor or in
The actuator 10 has a brake 32 with which the motor shaft 12 and the spindle 2 and therefore the actuator 10 as a whole can be immobilized. It can be a brake 32 that is applied in its position of repose and must be actuated in order to be released. In this case, the brake 32 must be released when the actuator 10 is to be actuated. A magnetic brake 32 is symbolically depicted in
Number | Date | Country | Kind |
---|---|---|---|
102008042299.1 | Sep 2008 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/EP09/59634 | 7/27/2009 | WO | 00 | 3/23/2011 |