ADAPTIVE OSCILLATION DAMPER HAVING A VERTICAL SPRING MECHANISM

Abstract

An oscillation damper for damping unwanted oscillations in oscillation-sensitive systems, such as tall edifices and towers, especially wind turbines. The oscillation damper has a vertical spring mechanism and the oscillation characteristics, such as the frequency and amplitude, and thus the damping capabilities, can be adjusted across a wide range of values.

Claims

1-21. (canceled)

22. A vibration damper for a tall slim structure or building, essentially comprising a pendulum having a damper mass and a spring device such that the spring device is installed below the damper mass, wherein: (i) the spring device is arranged in such a way that an entire spring force of the spring device substantially acts in a vertical direction, and the spring device has at least two different regions which have an effect that an overall spring characteristic line is non-linear or progressive, and (ii) the damper mass is connected, directly or indirectly, to an attachment point in the structure or building, via the spring device, below the vibration damper.

23. The vibration damper according to claim 22, wherein the spring device has at least two spring regions which have different spring stiffnesses.

24. The vibration damper according to claim 23, wherein the spring device has a first spring region which has a first spring stiffness and a second spring region which has a second spring stiffness.

25. The vibration damper according to claim 24, wherein the first spring region has a spring stiffness of <200 N/mm, and the second spring region has a spring stiffness of >200 N/mm.

26. The vibration damper according to claim 25, wherein the first spring region has a spring stiffness of >3 N/mm to <200 N/mm, and the second spring region as a spring stiffness of >200 N/mm to <3000 N/mm.

27. The vibration damper according to claim 22, wherein the spring device comprises one or more vertical springs, and a plurality of vertical springs are connected to one another by either by a series connection or by a parallel connection.

28. The vibration damper according to claim 27, wherein the spring device comprises at least two vertical springs.

29. The vibration damper according to claim 28, wherein at least two vertical springs have different spring stiffness from one another.

30. The vibration damper according to claim 29, wherein the first vertical spring has a spring stiffness of >3 N/mm to <200 N/mm, and the second vertical spring as a spring stiffness of >200 N/mm to <3000 N/mm.

31. The vibration damper according to claim 27, wherein the spring device comprises at least one vertical spring which has at least two spring regions which have different spring stiffness distributed over its length.

32. The vibration damper according to claim 31, wherein the different spring stiffness of the at least one vertical spring is effected by different coiling of the spring.

33. The vibration damper according to claim 27, wherein the vertical springs are at least one of tension springs or compression springs.

34. The vibration damper according to claim 22, wherein a separation between damper mass and attachment point is 0.5 m to 5.0 m.

35. The vibration damper according to claim 34, wherein the separation between damper mass and attachment point is 1.0 m to 3.0 m.

36. The vibration damper according to claim 22, wherein the damper mass is connected to the attachment point via a cable, a bar or a rod.

37. The vibration damper according to claim 22, wherein a separation between the attachment point and the spring device is shortenable and lengthenable by a movable or fixed stop or an attachment device, so that the frequency of the damper can be varied by subsequent extension or compression of the spring device.

38. The vibration damper according to claim 22, wherein the vibration damper additionally comprises a mechanical or hydraulic, mobile or fixed device for changing and adapting pretension of the spring device.

39. The vibration damper according to claim 22, wherein the pendulum consists of a rod or a tube, on a low end of which a damper mass which has an attachment point for the spring device is mounted, and on an upper end of which a joint is mounted which ensures free movement of the pendulum without any torsional rotation being possible.

40. A wind turbine, wherein the wind turbine has a vibration damper according to claim 22.

41. Use of a vibration damper according to claim 22 for the prevention and reduction of vibration events during the construction and operation of a wind turbine.

42. The use of a vibration damper according to claim 22 for the prevention and reduction of large damper amplitudes in a case of vibration-induced extreme events and of resonance-induced vibrations of the structure or building in a normal state or during normal operation.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0032] In the accompanying Figures:

[0033] FIG. 1 shows a diagrammatic view of variant 1 of a simple pendulum damper.

[0034] FIG. 2 shows diagrammatic views of variants 1, 2.1, and 2.2 of a simple pendulum damper.

[0035] FIG. 3 shows diagrammatic views of variants 1, 2.1, 2.2, and 3 of a simple pendulum damper.

[0036] FIG. 4 shows diagrammatic views of variants 1, 2.1, 2.2, 3, and 4 of a simple pendulum damper.

[0037] FIG. 5 shows diagrammatic views of a simple pendulum damper with variant 3 deflected out and variant 5 with a shorter spring length.

[0038] FIG. 6 shows a graph of spring force plotted against damper amplitude.

[0039] FIG. 7 shows a diagrammatic view of an upper suspension point of a damper designed as a variable joint.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT(S)

[0040] As already explained above, it is desirable to keep the deflection of the pendulum as small as possible over the entire range when vibrations occur in the structure, which is sensible, in particular for space reasons, in the usually very narrow towers of a WT or another tall building. This means that the separation between pendulum mass, to which the spring device is attached on one side directly or via a piece of cable, bar or rod, and the attachment point, which is installed below the pendulum damper and below the spring device in the structure and is in turn connected to the other end of the spring device directly or via a piece of cable, bar or rod, should, in the case of medium-sized to large structures, not be greater than 5 or 6 m, preferably <3 m, in particular <2 m, for example 0.5 m to 5.0 m, preferably 1.0 to 3.0 m.

[0041] In accordance with the invention, the damper frequency is thus influenced by the use of vertical springs instead of horizontal springs. In variant 3 (FIG. 3), these horizontal springs (4) are replaced by one or more vertical springs (7).

[0042] The physical correlation can be described as follows for a point mass:

[00003]$f=\frac{1}{2*\pi }*\sqrt{\frac{m*g+F_p*\left(1+l_1\right)}{m*l_s}}.fwdarw.\mathrm{Equation}.Math..Math.3;\mathrm{Variant}.Math..Math.3+4+5$

[0043] g.fwdarw.gravitation constant [m/ŝ2]

[0044] l1.fwdarw.pendulum length (2) [m]

[0045] l3.fwdarw.length from connection point of cable (5) to damper mass (3) [m]

[0046] F.sub.F.fwdarw.pretension force of vertical spring (7) [N/m]

[0047] m.fwdarw.damper mass (3) [kg]

[0048] It can be seen that the damper frequency can now be adjusted via a number of parameters. In this constellation, the damper frequency can be influenced by the vertical pretension force and not by the spring stiffness of the vertical spring(s) (7). This has the advantage that an entire frequency range can be covered with one vertical spring (7) and the spring does not, as is the case in the prior art, have to be replaced by one having a different spring stiffness. From domestic use, this phenomenon is known from a guitar string. If the pretension force in this is increased, the note/frequency is higher, while the spring stiffness of the string remains constant.

[0049] In addition, the dynamic displacement of the vertical spring (7), in relation to variant 2, is smaller for the same displacement of the damper mass (3). This enables a durable design of the spring. The longer the dimension l3 here, the smaller the dynamic change in length of the vertical spring (7) in relation to the movement of the damper mass (3). The longer the dimension l3 here, the less the influence of the vertical spring (7) on the damper frequency. This effect can be utilised positively in that, as also in the case of a guitar string, the dimension l3 is shortened to the dimension l3* (variant 4, FIG. 4). This causes the damper frequency to increase significantly for the same pretension force of the vertical spring. This shortening can be achieved by a stop ring (6), which can be moved in the vertical direction or alternatively is mounted in a fixed manner at one position. In the latter case, this stop ring (6) represents the fixed point of action of the spring.

[0050] In a further embodiment of the invention, the damper according to the invention has a movable or fixed stop or attachment device between the lower end of the spring device and the attachment point on the structure, enabling the separation between attachment point and spring device to be shortened and lengthened, so that the frequency of the damper can be rendered variable by the consequent lengthening or compression of the spring device. As already described above, a significantly higher damper frequency is required during the erection phase of the VVT. This can be achieved in accordance with variant 4 by the shortening to dimension l3*. When erection of the structure is complete, a significantly lower damper frequency is required. In order to meet this requirement, the stop ring (6) is de-installed or moved downwards. The damper frequency drops, since dimension l3 and not l3* now determines the damper frequency. The fine tuning of the damper frequency can now be carried out by increasing/minimising the pretension force of the vertical spring (7). It must be ensured here that the vertical spring (7) is located above the stop ring (6). If the damper mass (3) moves in this constellation, relative movement between the cable (8) and the stop ring (6) is prevented. Conversely, the damper frequency can be increased by raising or introducing the stop device.

[0051] If a damper of this type or a similar damper is installed in a wind turbine, large amplitudes of the damper mass (3) may result due to external influences (for example emergency shutdown, gusts, switch-off operations). In order to keep the vibration displacement of the damper mass (3) small in these situations (which may be necessary in order to prevent the pendulum from hitting the tower wall), the dimension l3* should be chosen short (e.g. between 0.3 m and 6 m). Variant 5 (FIG. 5) arises as follows:

[0052] if, in combination with the short length of l3*, a vertical spring (7) which has a large spring stiffness is now installed, significantly smaller deflection displacements (Y) of the damper mass (3) result compared with variant 3 (deflected out) with lower spring stiffness and larger l3. The smaller the dimension l3* is selected, the greater the deflection angle (A2) of the vertical spring (7) becomes, with the same deflection displacement (Y) of the damper mass (3). This results in greater angled tension of the spring, which counters the movement of the damper mass (3) and limits the amplitude of the damper mass during operation and extreme events.

[0053] In the case of variant 5, a greater change in length (delta X2) of the vertical spring (7) results compared with variant 3 (deflected out), for the same deflection displacement (Y). The spring force increase which results from this is calculated as follows:

increase in spring force=C*delta X

[0054] C.fwdarw.spring stiffness of spring (7)

[0055] delta X.fwdarw.change in length of the spring (7) during deflection of the damper mass (3)

[0056] It can be seen from the formula that in the case of variant 5 the increase in spring force rises to a greater extent than in the case of variant 3 (deflected out).

[0057] If a vertical spring (7) having a large spring stiffness is now installed in a corresponding pendulum damper, the spring force increases significantly above the target level, even in the case of small damper amplitudes. It can be seen from Equation 3 that the damper frequency is consequently likewise increased significantly, which in turn has an adverse effect on the damper action.

[0058] This problem can be solved by aiming at change in the spring force of the vertical spring (7) with the damper amplitude as shown in FIG. 6. This can be achieved in accordance with the invention by a vertical spring device, which can have a progressive or non-linear spring characteristic line over the damper deflection.

[0059] A distinction is made here between a “resonance stimulation” region and “operation/extreme event” region. A passive damper (as described here) can only act in the case of harmonic force stimulation. This harmonic force stimulation is only present in the case of “resonance stimulation”. In operation or during extreme events, by contrast, a stochastic force stimulation with large damper amplitudes is present. In general, there is no damper action in the case of these structure states with the passive damper described here. Rather, the requirement is to keep the damper amplitudes small in the case of operation/extreme events and only to ensure a damper action in the case of resonance stimulation (small damper amplitudes).

[0060] The spring stiffness C1 of the vertical spring (7) is small in the resonance region. If the damper amplitudes now increase during operation or in the case of extreme events, the damper enters the region of high spring stiffness C2. The restoring forces of the vertical spring (7) thus increase significantly, which significantly reduces the damper amplitudes in these structure states. The whole is to be regarded in combination with the short vertical spring (7) from variant 5, which additionally increases the restoration component.

[0061] In accordance with the invention, the combination of a relatively short (0.3 m-3 m) vertical spring device having a progressive spring characteristic line provides a pendulum damper of variable frequency and amplitude which can be employed in the case of extreme states, normal states and states as arise during the erection, modification or de-installation of a vibration-sensitive structure or building. This enables the pendulum damper to be built larger within the tower without the fear of collisions with the walls of the tower or building or the internal structures located therein. Furthermore, an additional stop can be omitted, since the damper amplitudes generally come out smaller.

[0062] In a further embodiment, the vibration damper according to the invention additionally has a mechanical or hydraulic, mobile or fixed device for changing and adapting the pretension of the spring device by subjecting the spring device or parts thereof to compression or tensile loads.

[0063] The invention thus also relates to a corresponding vibration damper in which the separation between attachment point and spring device can be shortened and lengthened again by means of a movable or fixed stop or attachment device, so that the frequency of the damper can be varied or adapted by the consequent expansion or compression of the spring device. The invention furthermore also relates to a vibration damper which additionally comprises a mechanical or hydraulic, mobile or fixed device for changing and adapting the pretension of the spring device.

[0064] In accordance with the prior art, the pendulum length (2) in a pendulum damper is achieved by cables. The damper is consequently able to rotate torsionally in the cables. The vertical springs (7) and also the dampers would thus have to follow this rotation, which would result technically in malfunctions. In an alternative embodiment according to the invention, the pendulum length (2) can be replaced by a torsionally rigid element (tube). At the same time, the upper suspension point of the damper (1) must be designed as a variable joint, for example a universal joint. This prevents torsional rotation in the case of possible movement of the damper mass (3) through 360° (FIG. 7). The invention thus relates to a corresponding vibration damper in which the pendulum consists of a rod or tube, on the lower end of which the damper mass, which has an attachment point for the spring device, is mounted and on the upper end of which a joint that ensures free movement of the pendulum through 360° is mounted, so that torsional rotations are impossible.

[0065] The upper suspension point of the damper can take place, depending on the nature of the structure, tower or building, at the respective upper end of the tower, structure or building or alternatively at any desired position in the upper half or in the upper third. It is also possible for the damper mass (3) to be suspended on one or more suspension points of damper (1). In addition, it is also conceivable for a universal joint to be installed directly on the damper mass (3) and at the connection point of damper (1) and for a torsionally rigid element to be installed in between.

[0066] As already explained the number of times, the dampers according to the invention are suitable, in particular, for installation in WTs. The invention thus also relates to a wind turbine which has a vibration damper according to the invention.

[0067] The invention relates, in particular, to the use of the damper according to the invention for the prevention and reduction of vibration events during the construction and operation of a wind turbine of this type or other vibration-sensitive buildings, but also for the reduction and prevention of large damper amplitudes in the case of vibration-induced extreme events and of resonance-induced vibrations of the structure or building in the normal state or normal operation.

[0068] In the description, drawings and claims, the following items are referred to:

TABLE-US-00001 1 Damper suspension point 2 Pendulum length 3 Damper mass 4 Horizontal spring 5 Cable connection point 6 Stop ring 7 Vertical spring 8 Cable