The invention relates to a device for circulating a liquid received in a container, in particular for circulating wastewater received in a tank.
A device of this type is known from WO 2006/108538 A1. With the known device it is possible to circulate the wastewater received in the tank with a relatively low consumption of electrical energy. Nevertheless, there is a need to improve the efficiency of such a device further still, so that more energy can be saved.
The object of the invention is to specify a device with which a liquid received in a container can be circulated with improved efficiency.
This object is achieved by the features of Claim 1. Expedient embodiments of the invention will emerge from the features of Claims 2 to 11.
In accordance with the invention it is proposed for the geometric centre of gravity of the aperture area to be disposed in a region between the centerline and one of the two transport ribs. It has surprisingly been found that, as a result of the shifting of the aperture area with respect to the centerline into the vicinity of one of the two transport ribs as proposed in accordance with the invention, the efficiency of the device can be significantly increased.
In the context of the present invention, the term “aperture area” is understood to mean a flat surface resulting from projection on a plane extending perpendicularly to the surface normal to the aperture area, said surface normal extending through the centre of gravity.
The geometric centre of gravity of the aperture area corresponds to the centre of mass of a physical body which corresponds to the aperture area, consists of homogeneous material and has the same thickness everywhere. It can therefore be determined by way of example purely mechanically by balancing. However, the geometric centre of gravity of the aperture area can also be calculated using mathematical methods that are known in general. By way of example, the aperture area can be described approximately by a polygon and a mathematical method for calculating the centre of gravity of a polygon can be used to calculate the geometric centre of gravity. In addition, it is also possible to determine the geometric centre of gravity of the aperture area by integration.
The term “upper side of the stirring body” is understood to mean the side formed approximately convexly or in raised manner. By contrast, an “underside of the stirring body” has an approximately concave form or a form forming a depression.
In accordance with an advantageous embodiment the transport ribs each have a curvature directed towards the shaft in the radial direction. In other words, the transport ribs extend in a slanting manner in the region of a peripheral edge and then bend in the radial direction. The efficiency of the stirring body can be improved as a result.
The aperture area extends substantially in the radial direction. It has a first end in the vicinity of the shaft and a second end in the vicinity of the peripheral edge. The aperture area can have a greater width at the second end than at the first end. In other words, the aperture area, which is elongate in the radial direction, advantageously becomes larger towards the peripheral edge.
In accordance with a further embodiment a height of the transport ribs increases from the peripheral edge to approximately the first end of the adjacent aperture area. The height of the transport ribs then decreases again for example from the first end of the adjacent aperture area in the direction of the shaft. A maximum of the height of the transport ribs can also lie between the first and the second end. In this case it lies preferably closer to the first end than to the second end. It has been found that in particular the embodiment of the transport ribs in combination with the adjacent position of the aperture areas leads to a further efficiency increase.
The aperture area is advantageously delimited on one of its long sides by a transport rib. This one long side of the aperture area is advantageously delimited adjacently to or bordering on the side of the transport rib that is convexly curved as considered from the upper side of the stirring body.
In accordance with a particularly advantageous embodiment the transport rib is inclined towards the aperture area of the adjacent or bordering aperture. The transport rib can form an angle a of approximately 90° with the upper side of the stirring body in the region of the peripheral edge. The angle a advantageously decreases in the direction of the aperture area to a value in the range from 60 to 87°, such that the transport rib is inclined towards the aperture area. This surprisingly results in a further increase in efficiency.
In accordance with a further embodiment of the invention a ratio between a lateral surface of the stirring body and a total aperture area of all apertures lies in the range from 10:1 to 10:2. The term “lateral surface of the stirring body” is understood to mean the surface of the upper side of the stirring body, the surfaces formed by the transport ribs being omitted.
In accordance with an advantageous embodiment of the invention the center of gravity of the aperture areas are distanced from one another approximately at the same angle. A symmetry of the stirring body is advantageously defined by an n-fold axis of rotation, wherein n is an integer from 6 to 12. In other words, the stirring body according to the invention advantageously has six to twelve apertures.
In accordance with a further particularly advantageous embodiment the stirring body is formed from structurally identical segments, which are interconnected along joining zones extending from the peripheral edge to a centrally arranged connector piece. This simplifies the production of the stirring body significantly.
It has proven to be particularly advantageous to form each segment such that the transport rib is arranged in the region of a joining zone and the aperture is delimited in part by the transport rib.
In accordance with a further advantageous embodiment the apertures are arranged in the region of a radially inner half of the stirring body. In other words, the aperture extends via its second end at most over half of the radius of the stirring body.
An exemplary embodiment of the invention will be explained in greater detail hereinafter on the basis of the drawings, in which:
An aperture D1 to D8 is provided between each two transport ribs T1 to T8. An aperture area of each of the apertures D1 to D8 has a geometric centre of gravity S1 to S8. The geometric centers of gravity S1 to S8 lie, in the case of the stirring body 1 according to the prior art, on the corresponding centerline, respectively, of which only M1 and M2 are shown here by way of example.
The centers of gravity S1, S8 advantageously are disposed approximately centrally between the respective centerlines M1, M8 and the adjacent transport ribs T1, T8. The geometric centers of gravity S1, S8 can lie in particular in the central region of a straight path W connecting the centerlines M1, M8 to the adjacent transport rib T1, T8 (see
Each aperture D1 to D8 has a first end E1 in the vicinity of the connector piece 2 or a shaft mounted thereon and a second end E2 in the vicinity of the peripheral edge UR (see
Each transport rib T1 to T8 has, in the region of the peripheral edge UR, a minimum height H1 and in the region of the aperture D1 to D8 a maximum height H2. A ratio H1/H2 lies in the range 1/5 to 1/100, preferably in the range 1/5 to 1/20. The maximum height H2 lies advantageously at the first end E1 of the aperture D1 to D8. It can also lie between the first and the second end E2 of the aperture D1 to D8. A normal of the maximum height to the aperture area D1 to D8 expediently lies at a distance of at most 15 cm from the first end E1. The maximum height H2 decreases again from the apertures D1 to D8 in the direction of the connector piece 2.
The transport ribs T1 to T8 extend at least in the region of the peripheral edge UR substantially perpendicularly from the upper side O, i.e. they form an angle a of approximately 90° with the upper side O. The angle a decreases with increasing distance from the peripheral edge UR, such that the transport rib T1 to T8 is inclined in the direction towards the adjacent aperture D1 to D8. In the region of the aperture D1 to D8, the angle a is expediently less than 90°. It lies there in a range from 60 to 87°. On the whole, the angle a can thus lie in a range from 60 to 90°. The partial overlap of the apertures D1 to D8 by the obliquely inclined transport ribs T1 to T8 is visible in particular from
The stirring body 1 is constructed symmetrically in the present exemplary embodiment. Here, it has an eight-fold axis of rotation. It is of course also possible for the stirring body 1 to have an n-fold axis of rotation, wherein n for example is an integer from 6 to 12.
The stirring body 1 can be produced advantageously from a plurality of structurally identical segments Sg1 to Sg8 (see
The first segment Sg1 has, in the region of the second joining portion Fa2, generally a second joining profile P2 (not shown here in detail), which corresponds to the first joining profile P1. In the present exemplary embodiment the second joining profile P2 corresponds to the cross section of a flat plate. The interconnected joining profiles P1, P2 of adjacent segments Sg1 to Sg8 form the joining zones F1 to F8.
The first segment Sg1 shown in
Although the stirring body 1 has a hyperboloid-like form in the figures, it may also be that the stirring body 1 is formed for example in the manner of a truncated cone.
The device according to the invention can be operated with a significantly improved efficiency. The reason for this is essentially the arrangement of the apertures D1 to D8 in such a way that the geometric centers of gravity S1 to S8 thereof are disposed in the vicinity of an adjacent transport rib T1 to T8. The combination of an aperture D1 to D8 with a transport rib T1 to T8 of which the height increases continuously from the peripheral edge UR to the aperture D1 to D8 causes an additional increase in the efficiency. Lastly, the inclination of the transport ribs T1 to T8 towards the adjacent aperture areas contributes to a further efficiency increase.
Number | Date | Country | Kind |
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10 2013 225 659.0 | Dec 2013 | DE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2014/072937 | 10/27/2014 | WO | 00 |