The invention relates to a sedimentation basin for a two-phase suspension, particularly for sewage sludge, in which the denser and therefore heavier phase settles downwards by gravitational separation, resulting in the formation of a separation level between the heavy phase and the light phase.
Nowadays gravitational sedimentation basins are used worldwide as standard constructions for solid/fluid separation in biological purification stages of sewage treatment works. Despite decades of research work in this field, these constructions do not function in an optimal manner. Their separation performance is unsatisfactory in relation to the space which is available to them for this purpose. Also the discharge values of the lighter phase which is to be clarified are frequently unsatisfactory. This is the case in particular when the inlet lies above the separation level. The separation level is defined as the level from which the concentration in the sedimentation basin rises with a high gradient from the residue of the lighter phase to the heavier phase. The discharge value or discharge quality is defined as the residual quantity of heavy phase to be separated off in the discharge of the light phase to be clarified or vice versa. Because of the known problems with sedimentation basins there are numerous publications which deal with optimization of these constructions. They contain repeated references to the dominant influence of the inlet construction.
According to the laws of physics of dense flows, dense flows suck in fluid from the ambience over their edges. The extent to which this sucking in takes place is directly dependent upon how high the total energy is which the flow has at its entry into the ambient fluid. This sucking in of ambient fluid which increases the transported volume flow and mass flow in the dense flow is called entrainment. A volume flow Q grows by entrainment on its flow path from the inlet volume flow Qi to an increased volume flow Q=Qi+ΔQ. Since sedimentation basins fulfil their function all the more efficiently the smaller Q is, any measure which reduces the energy of the in-flowing suspension at the inlet increases the efficiency of the sedimentation basin.
The entrainment behavior of a dense flow can be influenced technically only over a limited area, the so-called near field of the technical construction; in the far field of the construction the entrainment is produced from the locally prevailing physical parameters of density difference between the local density ρi and the density of the ambience ρa, the local pressure gradient, the thickness hD of the dense flow and consequently its local velocity.
The total energy present at the inlet can be written as the sum of its individual components:
Etot=(Epk)min+Eb+ΔEpk+ΔEU
The inlet area Ai of an inlet construction which is flowed through horizontally can be calculated at Ai=hi·bi in case that the height hi of the inlet cross-section remains constant over the inlet width bi. The volume flow per inlet width is qi=Qi/bi, the average inlet velocity is Ui=qi/hi.
If the local energy Etot=(Epk)min+ΔE is higher by an energy surplus ΔE=Eb+ΔEpk+ΔEU than the minimum necessary energy (Epk)min in order to move a dense flow with a given volume flow Q, this leads to entrainment. According to the physical least-energy principle, for sedimentation basins (Epk)min is established when the densimetric Froude number is FrD=Ui/(g′·hi)1/2=1 with simultaneously the widest possible inlet and the inlet lies at the separation level. The gravitation constant g′ which is actually effective locally results from the difference between the local density ρ1 and the density of the ambience ρa as g′=(ρ1−ρa)/ρa·g.
Eb is the amount by which the energy surplus ΔE at the inlet increases if the inflow does not take place at the height of the separation level.
If a suspension of density ρs is introduced below the separation level situated at the height hs at a vertical distance h0 from the point of equal density of the ambient phase into an ambient phase of higher density, because of its lower density it has a buoyancy energy Eb and is consequently deflected upwards from the horizontal at the angle Φ. The deeper the introduction is below the separation level the greater therefore is the buoyancy energy Eb and consequently the rate of entrainment. From the energy point of view these considerations give rise to the requirement to configure the inlet into a sedimentation basin so that the lifting energy for fluctuating heights hs of the separation level is minimized by adaptation of the relative height h0 of the inlet surface just below the separation level with h0≈0 and thus Eb≈0.
ΔEpk is the amount by which the energy surplus ΔE at the inlet increases if the optimal relationship of kinetic and potential energy with FrD=1 is not present. The inlet height hi which is optimal in energy terms is hi=(q12/g′)1/3 with Frd=1. Thus for variable inlet conditions the Froude number can be controlled by adaptation of the height hi of the inlet.
ΔEU is the amount by which the energy surplus ΔE at the inlet increases if the width bi of the inlet is smaller than the maximum possible width. By geometric consideration the maximum possible width is produced with the technical feature of an inlet disposed around the periphery.
The entrainment can have a positive effect on the discharge values of a sedimentation basin when it ensures at the inlet of the suspension that the incoming suspension is to a limited extent enriched with suspension of a higher density from the sedimentation basin and thus the larger flocks of the ambient suspension can hold back smaller particles of the intake suspension and thus a so-called flock filter effect takes place. This Flock filter effect is a desirable process which is demanded for example in dimensioning rules for secondary sedimentation basins.
Flows in sedimentation basins may be distinguished according to their flow direction as source or sink flows. In source flows the fluid is continuously retarded on the flow path by constantly increasing pressure, and in sink flows the fluid is continuously accelerated by constantly falling pressure. A sink flow travels in a substantially more stable fashion and consequently is markedly less susceptible to disturbances. Disturbances are caused in sedimentation basins by flow rates Ui at the inlet which vary over time. These disturbances impose pulse forces on the stratified fluid body which are proportional to the rate Ui. In the case of a central inlet Ui is very great and the resulting great destabilizing disturbances are superimposed on a flow which is in any case unstable. In the case of a peripheral inlet the rate Ui is markedly less and thus the pulse force is drastically reduced and moreover is superimposed uncritically on a stable flow.
The phenomenon that the entrainment decreases as h0 becomes less and therefore the buoyancy energy Eb becomes less is utilized in the method described in the patent DE 197 58 360 C2 and the corresponding publication EP 0 923 971 A1 in which h0 is minimized in stages at a central inlet construction for round sedimentation basins. A minimization of ΔEpk and ΔEU is not considered here. Thus the entrainment phenomenon can be reduced, but remains present to a significant extent. However, adaptation of the height h0 of the inlet in stages is seen as very critical for a central inlet construction, since when a stage is started and taken out of operation the adaptation imposes very discontinuous flow rates and thus particularly destabilizing pulses on a source flow which is physically unstable in any case. This leads potentially to markedly poorer discharge qualities.
The phenomenon that the entrainment decreases as bi becomes greater and thus the energy ΔEU becomes less is utilized for example in the method described in the publication DE 198 30 311 A1, in which the inlet is disposed peripherally, that is to say at the edge of the sedimentation basin, near the floor. A minimization of ΔEpk is not considered here and Eb is actually maximized by placing the inlet near the floor. Thus the disturbing effect of the entrainment is also retained to a large extent in this case.
Patent Abstracts of Japan Vol. 008 No. 077 (C-218), i.e. JP 59 004 407 A, and Patent Abstracts of Japan Vol. 2000 No. 14, i.e. JP 2000 325706 A, disclose a variable inlet construction for a sedimentation basin which makes it possible that for all layers of the separation level within the sedimentation basin the upper edge of the inlet lies as high as possible but always below the separation level. However, no suitable structural measures are provided which force the incoming volume flow into a horizontal flow direction. Rather, the incoming suspension flows through a vertical cylinder which is adjustable in height in a predominantly vertical flow direction past the height-adjustable lower edge of the inlet cylinder into a greater depth. The actual level of the turning point at which the vertically downwardly directed flow of the suspension becomes a horizontal flow direction, and thus the inlet height which determines the resulting lifting energy, is not controlled technically in these previously known inlet constructions. There is no defined inlet surface for the horizontal inlet flow. In this previously known constructions the actual level of the transition between vertical and horizontal flow direction is produced according to physical laws exclusively as a function of the balance of a downwardly directed pulse force by flow velocity on the one hand, and an upwardly directed buoyancy force which the downwardly flowing inlet jet is subjected to by ever increasing ambient density.
In view of the described disadvantages in the prior art, the technical problem is posed of proposing an optimized sedimentation basin which is distinguished by higher separation performance, better discharge plant, lower internal loading and operation with little disturbance.
The present invention is based on the recognition that not only destabilizing pulses but also the inlet energy
Etot=(Epk)min+Eb+ΔEpk+ΔEU
must be decreased as far as possible at the inlet or must be reduced to the technically possible minimum. Thus the entrainment which is dependent upon the inlet energy is also reduced with the highest possible stability of the flow.
In a sedimentation basin with a centrally disposed inlet construction with at least one suspension supply line and at least one inlet which is adjustable in height and opens into the sedimentation basin in the region of the separation level, this object is achieved according to claim 1 in that the inlet has an inlet cross-section which is flowed through substantially horizontally and of which the relative height h0 can be adapted continuously to the respective height hs of the separation level. By the provision of an inlet surface which is flowed through horizontally with a defined upper and lower edge it is possible to adjust the effective height of the inlet flow for each operational state so that the input of energy at the inlet is minimal.
The object is also achieved by a sedimentation basin in which according to claim 7 the inlet is disposed at the edge of the sedimentation basin and the relative height h0 of the inlet can be adapted to the respective height hs of the separation level.
If in a central inlet construction the adaptation of the relative height h0 of the incoming flow to the respective height hs of the separation level takes place continuously, then the critical destabilizing change of pulse is minimized thereby. If the minimization of the relative height h0 is combined with a peripheral introduction, then because of the maximized inlet width bi with simultaneously optimized inlet height hi, surprisingly no further entrainment into the inlet jet takes place. Thus in this case this results in a reduced volume flow in the main flow, so that the loading of the basin decreases, instead of increasing due to entrainment. Consequently the sedimentation basin can be of smaller construction or, in the case of predetermined size, can be more highly loaded.
Advantageous embodiments of the invention are set out in the subordinate claims.
If not only the relative height h0 of the inlet but also the height hi of the effective inlet cross-section can be varied, then depending upon the volume flow and/or density of the introduced suspension a destabilizing change in pulse in the region of the inlet can be prevented even more effectively.
A particularly advantageous construction of a peripheral inlet which can be adjusted in height is provided if the wall of the basin is broken by slots running all or part of the way around at least two levels and the inlet is controlled by means of closure devices so as to be adjustable in height in stages.
A further advantageous construction of a peripheral inlet which is adjustable in height is produced if at least two pipes which run all or part of the way around are disposed one above the other on the periphery of the basin, and feeding thereof can be distributed completely or partially to individual pipes using control and regulating techniques. The pipes must be capable of being flushed or scraped so that the suspension can be completely discharged in pipes which are temporarily not being supplied. Otherwise, for example in the case of biochemically active suspensions such as those flowing into secondary sedimentation basins, disadvantageous decomposition processes take place if the suspension remains for a long time in the inactive pipe.
The entrainment out of higher-density regions which has a positive effect on the flock filter action can be encouraged by means of a flow deflector above the inlet to ensure that entrainment into the incoming suspension flow can be supplied exclusively from the lower region of the sedimentation basin with suspension of a higher density. By means of an inclination of the flow deflector it is possible to limit the angle Φ at which the dense flow moves upwards. The entrainment is also controlled in this way. If one or more flow deflectors are constructed so that their angle Φ can be varied in operation, it is possible to control the entrainment variably for several static inlet heights and to guide the incoming dense flow in a controlled manner to the separation level.
Since the geometric shape of the surface has no qualitative influence on the physical phenomena which are relevant for the invention, it is possible for the surface of the sedimentation basin to be constructed in a round or rectangular shape. Special shapes of the basin surface are also possible.
Since the form of the extraction of the lighter phase has no qualitative influence on the phenomena which are relevant for the invention, the extraction of the lighter phase can take place in the form of weirs, open or immersed discharge pipes or other means.
Since the form of the extraction of the heavier phase also has no qualitative influence on the phenomena which are relevant for the invention, the extraction of the heavier phase can take place gravitationally with or without assistance from scrapers, with an inclined or horizontal floor of the sedimentation basin, by suction or by other means.
For reasons of construction and geometry it is possible that the separation level falls below the inlet surface at times in the case of very low loading of the sedimentation basin for an inlet height at the lowest adjustable point.
Embodiments of the invention are described in greater detail below with reference to the appended drawings, in which:
a-1c show a round sedimentation basin with a central inlet construction, in its height adjustable inlet pipe and adjustable deflector plate;
d shows a rectangular sedimentation basin with a central inlet construction, a partition which is adjustable in height and adjustable deflector plate;
a-2c show a round sedimentation basin with a central inlet construction, inlet pipe and telescopic pipe ring;
a-3c show a round sedimentation basin with peripherally disposed intake basin, partition and telescopic boundary wall;
d shows a rectangular sedimentation basin with peripherally disposed intake basin, partition and telescopic boundary wall;
a, 4b show a round sedimentation basin with peripherally disposed inlet conduit which is adjustable in height;
c, 4d show a round sedimentation basin with centrally disposed inlet conduit which is adjustable in height;
e shows a rectangular sedimentation basin with inlet conduit which is adjustable in height disposed at the edge;
a-5c show a round sedimentation basin with intake basin disposed at the edge and partition having slots;
d shows a rectangular sedimentation basin with intake basin disposed at the edge and partition having slots;
a-6c show a round sedimentation basin with central inlet construction, telescopic inlet pipe and deflector plate which is adjustable in height;
d shows a rectangular sedimentation basin with intake basin disposed at the edge, telescopic partition and deflector plate;
a, 7b show a round sedimentation basin with two inlet conduits disposed one above the other at its edge;
c shows a rectangular sedimentation basin with two inlet conduits disposed one above the other at its edge.
All the drawings show sedimentation basins in highly simplified vertical sections. Similar elements are in each case denoted by the same reference numerals.
The round sedimentation basin which is shown by way of example in
The relative height h0 of the inlet 3 is defined by the distance from the separation level 6. The cross-section of the inlet 3 has the height hi. The suspension flows through the inlet 3 in a predominantly horizontal direction.
A suspension supply line 8 passes through the base of the sedimentation basin 1 and merges into a vertical intake pipe 9. The upper end of the intake pipe 9 merges constantly into a horizontal inlet surface 10. The intake pipe 9 is of telescopic construction, so that the height h0 of the inlet can be continuously altered relative to the separation level 6. A deflector plate 11 is disposed above the inlet surface 10, parallel thereto and spaced therefrom. The deflector plate 11 can be moved upwards or downwards in the vertical direction by means of lifting rods 12. In this way the height hi of the inlet cross-section can be changed as a function of the volume flow and/or the density of the introduced suspension.
In the rectangular sedimentation basin shown in
In the operational state illustrated in
The round sedimentation basin illustrated in
a to 3c show a construction which is similar in principle for a round sedimentation basin 2 with peripheral introduction. An intake basin 13 extends along the edge of the sedimentation basin 2. A partition 14 is disposed between the intake basin 13 and the sedimentation basin 2. A horizontal inlet plate 18 is disposed so as to be adjustable in height on the partition 14. A boundary wall 19 is provided above the inlet plate 18, spaced from and parallel to the partition 14. The boundary wall 19 is of telescopic construction. The distance between the lower edge of the boundary wall 19 and the upper face of the inlet plate 18 defines the height of the inlet cross-section.
As can be seen from a comparison of
d makes clear how a construction which is in principle the same can be provided in a rectangular sedimentation basin 2. Here the intake basin 13 is disposed on the left-hand edge of the sedimentation basin 2.
In the round sedimentation basin 1 according to
In the constructions according to
If the sedimentation basin 2 is of rectangular construction, as shown in
In the round sedimentation basin according to
In the embodiment according to
In the embodiment according to
According to
In the rectangular sedimentation basin 2 according to
Number | Date | Country | Kind |
---|---|---|---|
102 14 963.1 | Apr 2002 | DE | national |
02022051.3 | Oct 2002 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP03/02839 | 3/19/2003 | WO | 5/16/2005 |