Due to environmental considerations, great efforts are being made to eliminate sources of noise in motor vehicles to the greatest extent possible. In addition to tires and internal combustion engines, other acoustic sources are add-on components of the internal combustion engine, e.g., engine cooling fans. With acoustic sources of this nature, a general distinction is made between airborne noise vibrations and the occurrence of structure-borne noise. The occurrence of structure-borne noise can be perceived in the form of inertial force-excited vertical vibrations in the steering wheel of a motor vehicle.
With engine cooling fans that are common today, a compensation of the static imbalance is usually carried out so that the permissible limit values can be met. In the case of fans, which often have a flat design, a compensation of the dynamic imbalance (couple imbalance) is not possible at all or only at great expense, since the measurement itself causes problems due to the low flat clearance, and it would not be possible to securely attach the correction masses required to compensate the couple imbalance to the labile fan blades. As a result, it is accepted practice for engine cooling fans to be delivered with non-defined dynamic imbalance. Depending on the respective installation situation in the vehicle, the structure-borne noise produced by the dynamic imbalance can result in complaints about vibrations perceived in the passenger compartment. The remaining remedies, such as installing damping elements in the transmission path, or reworking plastic fans in order to reduce their imbalance present upon delivery, are costly and they do not necessarily result in a satisfactory reduction of vibrations.
The inertial forces—static and dynamic imbalances—are caused by inhomogeneous distributions of mass of the rotating rotor/armature assemblies and fans, and by tolerances of form and position relative to the rotation axis of the drive. Tolerances of form and position cause the rotation axis and main axis of inertia to no longer coincide. A parallel displacement between rotation axis and main axis of inertia, e.g., of a cooling fan having a fan wheel mounted on the armature or rotor shaft results in a static imbalance, while a main axis of inertia tilted relative to the rotation axis can produce a centrifugal moment, the effects of which are comparable to a couple imbalance or dynamic imbalance.
The advantages of the means for attaining the object of the invention proposed according to the invention are seen mainly in the fact that a soft connection of the axial fan to the armature or rotor of an electrical drive permits the axial fan to orient itself in the direction of the rotation axis as rotational speed increases. As a result, the disturbance variable, i.e., the imbalance moment, is automatically reduced by the rotation of the axial fan as the rotational speed increases. The influence of tolerances of form of the axial fan wheel drops off substantially with regard to the dynamic centrifugal moment, since a self-orientation of the axial fan wheel with regard to the rotation axis takes place. As a result, tolerances of form and position of the axial fan wheel are automatically compensated as well with regard to the dynamic imbalance.
Since the dynamic imbalance of an axial fan is clearly dominated by the dynamic imbalance of the axial fan wheel, a two-plane imbalance compensation with the armature and rotor of the electrical drive can be foregone. This, in turn, presents an opportunity for substantial savings, since the processing steps required to obtain two-plan imbalance compensation can now be eliminated entirely. The armature balancing can be foregone entirely, if necessary, by limiting the imbalance compensation to a purely static balancing of an axial fan on the axial fan wheel.
Due to the soft embodiment of the hub of the axial fan wheel, and/or the connection point of the axial fan wheel with the armature or the rotor shaft, the installation of additional damping systems that take up precious space can be foregone. The modifications of the hub of the axial fan wheel with regard to increasing flexural softness can also be carried out in simple fashion and very cost-effectively within the framework of reworking of engine cooling fans that have already been delivered.
The invention will be described hereinbelow with reference to drawings.
An axial fan wheel 1 comprises fan blades 2 and 3 essentially situated on its outer circumferential region, which said fan blades are mounted on the circumference of a hub region 4. An axial fan wheel 1 according to the depiction in
A rotation axis coordinate system 8, characterized by the rotation axis ξ—ξ and the axis η—η extending at a right angle thereto, is displaced relative to the aforementioned axes of inertia x—x and y—y. The rotation axis coordinate system 8 is tilted slightly compared to the coordinate system formed by the axes of inertia. The rotation axis ξ—ξ is turnably supported in bearings, one of which is designed as a fixed bearing 5 that absorbs axial and radial forces, and the other bearing 6 of which is designed as a movable bearing capable only of absorbing radial forces and permitting an axial displacement of the rotation axis ξ—ξ of the axial fan wheel 1.
The center of gravity, in which the axes of inertia x—x and y—y of the axial fan wheel 1 intersect, is labelled with reference numeral 7. ω represents the angular velocity at which the axial fan wheel—driven by an electrical drive not shown here—rotates around the rotation axis ξ—ξ.
According to the depiction shown as a model in
According to the depiction in
The axial force FAx (11) acts on the fixed bearing 5 in the axial direction, and the radial force FAy (12) acts on the fixed bearing 5 in the radial direction. In contrast, the movable bearing 6 only absorbs forces in the radial direction, characterized by FBy (13). The angle between the main axis of inertia x—x of the axial fan wheel 1 and its rotation axis ξ—ξ is labelled with δ.
The inclination δ of the axial fan wheel at rotational speed ω=0 is shown in the depiction according to FIG. 3.
In the case of an axial fan wheel, centrifugal moments produce considerable forces and moments depending on the rotational speed. With a maximum centrifugal moment of 45000 gmm2, for example, the imbalance moment characterized as follows acts on the axial fan wheel 1 at a speed of 2500 rpm:
According to the depiction shown in
The forces 15 labelled with Fc act on the hub region 4 of the axial fan wheel 1 modelled as a rigid disk. Said forces act on the rotation axis ξ—ξ of the axial fan wheel 1 around the lever arm a—also labelled with reference numeral 14—and counteract the moment produced by the centrifugal moment Jξη·ω2. As rotational speed increases, the axial fan wheel 1 is pushed in the direction of the rotation axis ξ—ξ as a result of the centrifugal moment Jξη·ω2. It follows from this that, when the hub region is designed to be as flexurally soft as possible, that is, with a flexurally soft connection of the hub region 4, 27 of the axial fan wheel 1 with its rotation axis ξ—ξ, the imbalance moment that occurs and that decreases with the rotational speed can be utilized to re-align the main axis of inertia x—x of the axial fan wheel 1 in the rotation axis ξ—ξ of said axial fan wheel with tilting at ω=0.
The inclination of the axial fan wheel 1 modelled as a rigid disk 1 that occurs at a given speed ω≠0 is characterized by δ minus α. To obtain re-alignment, that is, to make the main axis of inertia x—x coincide with the rotation axis ξ—ξ, the centrifugal moment Jξη·ω2 is utilized by the soft connection of the hub region 5 to the rotation axis ξ—ξ as rotational speed increases. In order to obtain a return of the axial fan wheel 1 modelled as a rigid disk in the depiction according to
The moment relationship for the axial fan wheel 1 that occurs as far as the axial fan wheel 1 is concerned is:
ΣM=0, that is, Jξη·ω2·ω2=Fc·a.
If this relationship is fulfilled, the axial fan wheel 1 rights itself in its rotation around the rotation axis ξ—ξ in such a manner that the rotation axis ξ—ξ and the main axis of inertia x—x of the axial fan wheel 1 coincide. The axial and radial forces acting on the bearings 5 and 6 of the rotation axis ξ—ξ through the axial fan wheel 1 are characterized with the reference numerals 11, 12 and 13 in the depiction according to FIG. 4.
The depiction according to
According to the side view in
Retaining devices are labelled with reference numeral 25; they can be used to fasten the housing 22 of the electrical drive 21 to a radiator assembly in the engine compartment of a motor vehicle.
A balancing weight is labelled with reference numeral 26; it is accommodated on a fan blade 3 on the circumference of the hub region 4 of the axial fan wheel 1 according to the depiction in
Hub and disk bores 28 are formed in the hub and disk at the connection of the hub plate 27—turned inward in the manner of a well—in the hub region 4 of the axial fan wheel 1 and the elastic disk 23, which said bores accommodate the fastening screws 24 with optional spring elements 30 accommodated on them. The hub bores 28 are arranged on a divided circle of hub bores 29, which is shown in
The depiction according to
The pot-shaped hub region 4 of the axial fan wheel according to the depiction in
A further possibility for obtaining a flexurally soft connection of the hub region 4 with the driven shaft 20 of an electrical drive 21 is to reduce the material strength in the hub region 4 in the region of the hub plate 27 turned inwardly in the manner of a well. Furthermore, a flexurally softer connection of the hub region 4 to the driven shaft 20 of the electrical drive 21 can be obtained by forming spring elements on the spring elements 24 that interconnect the elastic disk 23 and the hub plate 27—turned inwardly in the manner of a well—of the hub region 4, which said spring elements produce spring moments Fc·a depending on the displacement that counteract the centrifugal moment Jξη that increases as rotational speed increases. If the two moments mentioned hereinabove are in equilibrium, the axial fan wheel 1 is aligned in such a manner that its main axis of inertia x—x coincides with the rotation axis ξ—ξ, and no vibrations can be transmitted by means of structure-borne noise to other components in the engine compartment of a motor vehicle, or to the passenger compartment of a motor vehicle.
According to the depiction in
The depiction according to
The axial fan wheel 1 according to the depiction in
In the depiction according to
The armature shaft 20 of the electrical drive 21 comprises a bearing area 46 on which the support 44 of the bush element 42 rests. The support 44 represents a tilting point of the bush element 42 tiltable in the radial direction and secured on the armature shaft 20 in the axial direction. Due to the fact that the bush element 42 can move relative to the bearing area 46 of the armature shaft 20, an inclination of the hub plate 27—and, therefore, the axial fan wheel 1—mounted on the tiltably supported bush element 42 can take place within the range of the permitted tilting play. Dynamic imbalances that occur are automatically compensated by means of this seating of the bush element 42, acted upon by a tensioning element 43 when the armature shaft 20 of the electrical drive 21 rotates.
The required tilt angle can be calculated from the expected dynamic imbalance of the fan. This explained briefly with reference to an example calculation. In the case of a fan with 25000 gmm2 expected dynamic imbalance, the soft tilt angle required can be calculated using the equation
with a fan diameter of 390 mm and a fan weight of 463 g:
The calculated angle of 0.32° corresponds to a soft displacement of s=50·sin 0.32°=0.28 mm, assuming a divided circle of screw connections 29 of 50 mm.
Based on this example calculation for the given example and assuming the stated data, the displacement path “s” labelled with reference numeral 38 is approximately 3/10 mm.
Number | Date | Country | Kind |
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101 53 412 | Oct 2001 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/DE02/02881 | 8/6/2002 | WO | 00 | 5/13/2003 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO03/04057 | 5/15/2003 | WO | A |
Number | Name | Date | Kind |
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1760619 | Woolson | May 1930 | A |
2702087 | Beier | Feb 1955 | A |
3302867 | Roffy | Feb 1967 | A |
3368835 | Hackforth | Feb 1968 | A |
4917573 | Sikula, Jr. | Apr 1990 | A |
Number | Date | Country |
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91 02 865 | Jul 1992 | DE |
41 43 383 | Feb 1994 | DE |
100 58 935 | Jun 2001 | DE |
199 58 261 | Jul 2001 | DE |
2 756 021 | May 1990 | FR |
2756021 | May 1998 | FR |
1 376 710 | Dec 1974 | GB |
Number | Date | Country | |
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20040013517 A1 | Jan 2004 | US |