阅读说明：本技术 在没有头部的随后流出的情况下对于扁平的轧件的冷却 (Cooling of flat rolling stock without subsequent discharge of head ) 是由 K·温泽尔 E·奥皮茨 L·皮赫莱尔 F·波什尔 A·塞林格 于 2020-03-13 设计创作，主要内容包括：由金属构成的扁平的轧件(1)在输送段上沿着运送方向(x)被输送。用于用液态的冷却剂(5)对所述扁平的轧件(1)进行冷却的装置具有至少一个布置在所述输送段的上方的冷却梁(3),所述液态的冷却剂(5)通过供给管路(4)被输送给所述冷却梁。所述冷却梁(3)基本上横向于所述运送方向(x)来延伸并且具有多根出口小管(6),所述出口小管本身分别具有流入口(7)和流出口(8)。所述液态的冷却剂(5)从所述冷却梁(3)经由相应的流入口(7)进入到相应的出口小管(6)中并且经由相应的流出口(8)从相应的出口小管(6)中出来。所述相应的出口小管(6)沿着液态的冷却剂(5)的流动方向看具有以所述流入口(7)为出发点的向上伸展的起始区段(9)、与该起始区段毗连的中间区段(10)以及与该中间区段毗连的向下伸展的并且一直延伸到所述流出口(8)的末端区段(11)。所述中间区段(10)由此包括顶点(12),在该顶点处贯穿流过所述相应的出口小管(6)的冷却剂(5)到达最高点。所述流出口(8)处于所述冷却梁(3)的上方。所述流入口(7)与顶点(12)的高度间距(h1)是所述流出口(8)与顶点(12)的高度间距(h2)的至少双倍大、尤其是至少三倍大。(A flat rolled product (1) made of metal is transported in a transport direction (x) on a transport section. The device for cooling the flat rolled stock (1) with a liquid coolant (5) has at least one cooling beam (3) arranged above the conveying section, to which the liquid coolant (5) is supplied via a supply line (4). The cooling beam (3) extends substantially transversely to the transport direction (x) and has a plurality of outlet tubes (6) which themselves each have an inflow (7) and an outflow (8). The liquid coolant (5) enters the respective outlet pipe (6) from the cooling beam (3) via a respective inflow opening (7) and exits the respective outlet pipe (6) via a respective outflow opening (8). The respective outlet pipe (6) has, as seen in the flow direction of the liquid coolant (5), an upwardly extending starting section (9) starting from the inflow opening (7), an intermediate section (10) adjoining the starting section, and a downwardly extending end section (11) adjoining the intermediate section and extending as far as the outflow opening (8). The intermediate section (10) thus comprises an apex (12) at which the coolant (5) flowing through the respective outlet tubule (6) reaches a maximum. The outflow opening (8) is located above the cooling beam (3). The height distance (h 1) between the inflow opening (7) and the apex (12) is at least twice as large, in particular at least three times as large, as the height distance (h 2) between the outflow opening (8) and the apex (12).)

1. A device for cooling a flat rolled stock (1) made of metal with a liquid coolant (5),

-wherein the flat products (1) are conveyed in a conveying direction (x) on a conveying section,

-wherein the device has at least one chilled beam (3) arranged above the conveying section, to which the liquid coolant (5) is conveyed by means of a feed line (4),

-wherein the chilled beam (3) extends substantially transversely to the transport direction (x) and has a plurality of outlet small tubes (6),

-wherein the outlet canaliculus (6) has an inflow opening (7) and an outflow opening (8), respectively,

-wherein the liquid coolant (5) enters from the chilled beam (3) into the respective outlet stub (6) via a respective inflow opening (7) and exits from the respective outlet stub (6) via a respective outflow opening (8),

-wherein the respective outlet pipe (6), viewed in the flow direction of the liquid coolant (5), has an upwardly extending starting section (9) starting from the inflow opening (7), an intermediate section (10) adjoining the starting section, and a terminal section (11) adjoining the intermediate section, which extends downwardly and extends up to the outflow opening (8), such that the intermediate section (10) comprises an apex (12) at which the coolant (5) flowing through the respective outlet pipe (6) reaches an apex,

it is characterized in that the preparation method is characterized in that,

the outflow opening (8) is located above the cooling beam (3), and the height distance (h 1) of the inflow opening (7) from the apex (12) is at least twice as large, in particular at least three times as large, as the height distance (h 2) of the outflow opening (8) from the apex (12).

2. The apparatus of claim 1, wherein the first and second electrodes are disposed on opposite sides of the housing,

it is characterized in that the preparation method is characterized in that,

the outlet pipe (6) is arranged on the upper side of the cooling beam (3).

3. The apparatus of claim 1 or 2,

it is characterized in that the preparation method is characterized in that,

the initial section (9) of the outlet pipe (6) projects at least partially into the cooling beam (3).

4. The apparatus of claim 1, 2 or 3,

it is characterized in that the preparation method is characterized in that,

the starting section (9) extends vertically.

5. The device according to any one of the preceding claims,

it is characterized in that the preparation method is characterized in that,

the intermediate section (10) is curved and extends over a respective bending angle (a) of 150 DEG to 180 deg.

6. The device according to any one of the preceding claims,

it is characterized in that the preparation method is characterized in that,

the end section (11) has a length of 0.

7. The device according to any one of the preceding claims,

it is characterized in that the preparation method is characterized in that,

the outlet small tubes (6) each have a flow resistance element (13), in particular in the region of their inflow opening (7).

8. The apparatus of claim 7, wherein the first and second electrodes are disposed on opposite sides of the substrate,

it is characterized in that the preparation method is characterized in that,

the respective flow resistance element (13) is releasably connected to the respective outlet pipe (6).

9. The device according to any one of the preceding claims,

it is characterized in that the preparation method is characterized in that,

the outlet pipe (6) has a venting opening (15), in particular in the middle section (10) thereof.

Technical Field

The invention relates to a device for cooling flat rolling stock made of metal with a liquid coolant,

-wherein the flat products are conveyed in the conveying direction on a conveying section,

-wherein the device has at least one chilled beam arranged above the conveying section, to which the liquid coolant is conveyed by means of a supply line,

-wherein the cooling beam extends substantially transversely to the transport direction and has a plurality of outlet small tubes,

-wherein the outlet tubules have an inflow and an outflow, respectively,

-wherein the liquid coolant enters from the chilled beam via a respective inflow opening into a respective outlet tubule and exits from a respective outlet tubule via a respective outflow opening,

-wherein the respective outlet tubule has, seen in the flow direction of the liquid coolant, an upwardly extending starting section starting from the inflow opening, an intermediate section adjoining the starting section and a terminal section adjoining the intermediate section and extending downwardly and up to the outflow opening, such that the intermediate section comprises an apex at which the coolant flowing through the respective outlet tubule reaches an apex.

Background

Such a device is known, for example, from DE 19934557 a1 and also from DE 102010049020 a 1.

In the cooling section of the rolling mill, the metallic, flat rolling stock is cooled after rolling. The flat rolling stock can be made of steel or aluminum, for example. It can be a strip or a slab, as desired. It is common to have precise temperature control in the cooling section for setting and constantly maintaining desired material properties with low dispersion. In particular, for the cooling section arranged downstream of the rolling train, cooling beams are installed along the cooling section for this purpose, by means of which liquid coolant, usually water, is applied to the flat rolling stock at least from above, often from above and from below for cooling the hot rolling stock.

As explained correctly in DE 1020100490201, the following effects occur with the cooling beam of DE 19934557 a1 when the coolant supply is switched off, namely: the chilled beam is evacuated through the outlet tubules according to the principle of a siphon. During this time, the coolant flows out of the outlet tube in an uncontrolled manner and thus leads to uncontrolled cooling of the flat rolling stock and the associated adverse effects.

In other words, this effect is avoided in DE 102010049020 a 1. This is achieved in DE 102010049020 a1 by: each individual outlet pipe is assigned its own valve which is used to open and close the respective outlet pipe. This solution therefore prevents evacuation of the chilled beam, but is very expensive. Furthermore, the outlet tubule can only be simply switched (fully open or fully closed), but no continuous adjustment is possible.

Another solution consists in configuring the outlet small tube as a straight small tube which projects from below into the cooling beam and reaches a considerable height there, so that it ends in the region of the upper part of the cooling beam. In this solution, however, a considerable subsequent outflow of coolant (Nachlaufen) takes place when the cooling beam is switched off. This solution only gives good results when the intensive cooling of the work is carried out with high pressure.

Disclosure of Invention

The object of the present invention is to provide a possibility by means of which the subsequent outflow of coolant can be limited to an unavoidable minimum with simple measures.

This object is achieved by a device having the features of claim 1. Advantageous embodiments of the device are the subject matter of the dependent claims 2 to 9.

According to the invention, a device of the type mentioned at the outset is designed in such a way that: the outflow opening is located above the cooling beam and the height distance of the inflow opening from the apex is at least twice as large, in particular at least three times as large, as the height distance of the outflow opening from the apex.

The invention is based on the recognition that: although there is an equilibrium state immediately after the supply of the coolant to the chilled beam is stopped, the equilibrium state is unstable. When there is minimal disturbance of this equilibrium state, which practically always occurs, liquid coolant flows out of a part of the outlet tubules when air is sucked in through the other outlet tubules. The quantity of the liquid coolant which thus moves in the outlet pipe is first accelerated. The acceleration increases until the air sucked in through the other outlet tubules reaches the apex of the respective outlet tubule. Thereafter, the amount of movement of the liquid coolant is further accelerated. However, the degree of acceleration is reduced. When the sucked-in air reaches the same height in the initial section as the outflow opening of the respective outlet tube, the acceleration reaches the value zero. This level represents another equilibrium state, which is however more stable than the first mentioned equilibrium state.

However, since the coolant quantity in the outlet small tube already moves at a certain speed at this point in time, the movement of the coolant continues beyond this stable equilibrium state. However, the amount of liquid coolant that now moves in the outlet pipe is slowed down. If the height, by which the apex of the respective outlet small tube lies above the outflow opening of the respective outlet small tube, is denoted by h, the height position, in which the amount of movement of the liquid coolant in the outlet small tube (temporarily) comes to rest, lies approximately 1.5h below the outflow opening of the respective outlet small tube, but at most 2h below the outflow opening of the respective outlet small tube. Thereafter, a return oscillation is performed due to exceeding of a stable equilibrium state.

Air can thus flow into the cooling beam if the inflow opening of the outlet small tube is located above the mentioned level of approximately 1.5h or 2h below the outflow opening of the respective outlet small tube. This results in a weighted subsequent outflow of the coolant. Whereas if the inflow opening of the outlet tubule is at or below the mentioned level of about 1.5h or 2h below the outflow opening of the respective outlet tubule, the oscillation remains limited to the amount of coolant in the outlet tubule. Only these very small quantities may subsequently flow out.

The above description of about 1.5h and a maximum of 2h applies to the following assumptions, namely: the movement of the coolant in the outlet tubule takes place without appreciable frictional losses. However, such a friction loss is actually present. They reduce the extent to which the coolant is accelerated in the outlet tubule and enlarge the extent to which the coolant is decelerated in the outlet tubule. In practice, it may therefore often be sufficient for the height distance of the inflow opening from the apex to be (only) twice as great as the height distance of the outflow opening from the apex.

Preferably, the outlet small pipe is arranged on the upper side of the cooling beam. This condition of the outflow opening being above the cooling beam can thereby be achieved in a particularly simple manner and in particular with a comparatively small overall structural height of the cooling beam, including the outlet tubules.

Preferably, the initial section of the outlet pipe projects at least partially into the cooling beam. The overall structural height of the cooling beam, including the outlet small tubes, can thereby be kept as small as possible.

Preferably, the initiation section extends vertically. This results in a particularly simple construction.

Preferably, the intermediate section is curved and extends over a respective bending angle of 150 ° to 180 °. In this way, a laminar, virtually swirl-free flow can be maintained in a simple manner despite the direction of movement of the coolant in the outlet pipe being reversed.

Preferably the length of the end segment is 0. The overall structural height of the cooling beam, including the outlet small tubes, can thereby be kept as small as possible.

Preferably, the outlet small tubes each have a flow resistance, in particular in the region of their inflow opening. In particular, the vertical length of the start section can thereby be kept small.

Preferably, the respective flow resistance element is releasably connected to the respective outlet tube. This makes it possible, on the one hand, to adjust the flow resistance later, if necessary. Furthermore, the flow resistance element can also be replaced if it is calcified or otherwise exhausted, for example after a longer period of operation.

It is possible for the outlet tube to have a venting opening, in particular in its middle section. However, this is generally not required.

Drawings

The above-described features, characteristics and advantages of the present invention and how to implement them will become more apparent in conjunction with the following description of embodiments, which is to be read in connection with the accompanying drawings. The figures here show the following in schematic form:

FIG. 1 shows a section of the cooling section from above;

FIG. 2 illustrates the chilled beam of FIG. 1 from the front;

FIG. 3 shows a cross-section of the chilled beam of FIG. 1 along line III-III in FIG. 1;

FIG. 4 shows a cross section of a single outlet vial;

FIG. 5 shows in section the initial section of the outlet tubule; and is

Fig. 6 shows the middle section of the outlet tubule.

Detailed Description

According to fig. 1 to 3, the flat rolling stock 1 is to be cooled in a cooling section. The flat rolling stock 1 consists of metal, wherein the term "metal" is also intended to include common, widely used alloys in the sense of the present invention. For example, the flat rolling stock 1 can be made of steel or aluminum. The flat rolling stock 1 can be, for example, a strip or a slab. The cooling line can be arranged, for example, on the discharge side of a multi-stand finishing train.

The flat rolled stock 1 is conveyed through the cooling section in the conveying direction x. For this purpose, the cooling line has a conveying line, on which the flat products 1 are conveyed. For reasons of clarity, only one of the transport rollers 2 of the conveying section is shown and this is also only shown in fig. 2.

For cooling the flat rolled stock 1, at least one cooling beam 3 is present. The chilled beam 3 is arranged above the conveyor section. A liquid coolant 5 is supplied to the cooling beam 3 via a supply line 4, with which the flat rolling stock 1 is to be cooled. For good regulation, it is mentioned that a cooling beam can also be arranged below the cooling section, by means of which cooling medium 5 in liquid form is to be applied to the flat rolling stock 1 from below. However, these cooling beams are not the subject of the invention, as far as the mechanical design of the cooling beam 3 is concerned. The following explanations regarding the mechanical design of the cooling beam 3 therefore always relate to the cooling beam 3 above the conveyor section.

The chilled beams 3 extend substantially transversely to the transport direction x, i.e. along the transverse direction y. The width b of the chilled beam 3 in the transverse direction y is typically between 1m and 2 m. However, it can also be above or below this value. For example, there are cooling sections located after the so-called medium-wide strip mill train or in the mill train for aluminum. In such cases, the width b can in some cases be only 30cm or slightly higher. There are also thick-plate rolling trains, for example, for which the width b of the cooling section can be up to 4 m. The liquid coolant 5 is usually water or at least substantially consists of water (fraction of at least 98%). The pressure used to feed the coolant 5 to the chilled beam 3 is typically between 0 and 2 bar, typically about 0.8 bar. The chilled beam 3 is in this case a laminar chilled beam.

The chilled beam 3 has a plurality of outlet small tubes 6. The outlet tubules 6 have an inflow 7 and an outflow 8, respectively. The outflow opening 8 is located above the chilled beam 3, i.e. above the highest point of the chilled beam 3. The height distance h0 between the outflow opening 8 and the upper side of the cooling beam 3 should be at least 5 cm.

Typically the outlet tubules 6 form two rows, wherein the two rows extend in the transverse direction y. However, in some cases, there is only a single row or there are more than two rows. As long as there are a plurality of rows, the rows are spaced from each other along the transport direction x. There are always a plurality of outlet small tubes 6 inside each row. In many cases, there are at least 10, sometimes even 20 and more outlet tubules 6. The spacing a of the outlet tubules 6 (measured from the center of the outlet opening 8 to the center of the outlet opening 8 of the next outlet tubule 6) is typically between about 4cm and 5 cm. The inner diameter d of the outlet tubule 6, see in particular fig. 5, is typically between about 10mm and about 20 mm.

The outlet tubules 6 are generally constructed of the same type. Therefore, only one single of the outlet small tubes 6 will be explained in detail below with reference to fig. 4. For the other outlet tubules 6, a similar explanation applies due to the same type of construction.

According to fig. 4, the outlet tubes 6 are designed such that the liquid coolant 5 passes from the cooling bar 3 via the inlet opening 7 of the outlet tube 6 into the respective outlet tube 6. In the simplest case, the entry is directly from below. The coolant 5 flows upward in the starting section 9 starting from the inflow opening 7. The start section 9 can extend in particular vertically.

The intermediate section 10 adjoins the start section 9. In the intermediate section 10, the liquid coolant 5 is diverted such that it flows completely or at least substantially downward. In particular, the intermediate portion 10 can be bent with a uniform bending radius r, wherein the bending angle α covered by the intermediate portion 10 is typically at least 150 ° and at most 180 °.

The end section 11 adjoins the middle section 10. The end section 11 extends as far as the outflow opening 8. In the end section 11, the liquid coolant 5 flows downwards, in the ideal case vertically downwards. The coolant 5 then flows out of the outlet small pipe 6 and falls from above onto the flat rolling stock 1.

The end section 11 can be longer or shorter. The shorter the end section 11 can be kept, the better. In the extreme case, the length of the end section 11 can be 0, so that the end section 11 is cancelled in the result. In the result, this means that the outflow opening 8 can directly adjoin the intermediate section 10. This is less critical in this respect, since the coolant 5 already flows from top to bottom in the region of the intermediate section 10 facing away from the starting section 9.

Due to the designed design of the outlet small tube 6, the intermediate section 10 comprises an apex 12, at which the coolant 5 flowing through the outlet small tube 6 reaches its highest point. The coolant 5 flows horizontally at the apex 12. The apex 12 can correspond, for example, to the lowermost point of the internal cross section of the outlet small tube 6 at this location, the uppermost point of the internal cross section of the outlet small tube 6 at this location or a point between them, in particular in the center.

Both the inflow opening 7 and the outflow opening 8 are located below the apex 12. The height distance h1 between the inflow opening 7 and the vertex 12 is greater than the height distance h2 between the outflow opening 8 and the vertex 12. In particular, the height distance h1 is at least twice as large, for example 2.5 times as large, as the height distance h 2. Preferably it is at least three times as large.

The outlet small tubes 6 are not only of the same type, but are also arranged uniformly. The expression "uniformly arranged" should in this respect mean that the vertices 12 are at a uniform height level, the height spacings h1 are equal to one another and the height spacings h2 are equal to one another. The inflow opening 7 is thus also at a uniform height level. The same applies to the outflow opening 8. For example, the apex 12 can be located approximately 15cm above the upper edge of the cooling beam 3, the outflow 8 can be located approximately 7.5cm above the upper edge of the cooling beam 3, and the inflow 7 can be located approximately 15cm below the upper edge of the cooling beam 3. The numerical values mentioned should, however, be understood purely exemplary. If the mentioned values are realized, the height distances h1, h2 are furthermore in a ratio of 4:1 relative to one another.

The outlet small pipe 6 is arranged on the upper side of the cooling beam 3 according to the illustrations in fig. 1 to 3. The expression "arranged on the upper side" is intended to mean that the outlet pipe 6 is inserted into the cooling beam 3 from above. This does not mean that the outlet small tubes 6 end at the upper side of the cooling beam 3. Although this is possible, it is preferred according to the illustration in fig. 3 that the initial section 9 of the outlet tubule 6 at least partially protrudes into the chilled beam 3. In particular, the outlet small tube 6 should protrude into the cooling beam 3 to the greatest possible extent. This is particularly true, since the ratio of the height spacings h1, h2 relative to one another can thereby be maximized without enlarging the overall structural height of the cooling beam 3, including the outlet small tubes 6.

It is possible for the outlet small tube 6 to have a uniform cross section over its entire extent, i.e. from the starting section 9 to the end section 11. As an alternative, it is possible for the outlet small tubes 6 to each have a flow resistance 13 according to the illustration in fig. 5. The flow resistance 13 acts in particular for the respective outlet small tube 6. It reduces the available cross section of the respective outlet tubule 6. For example, the available cross section of the respective outlet small tube 6 in the region of the flow resistance 13 may be between 20% and 80% of the cross section of the respective outlet small tube 6 in the remaining region. In general, the cross-section left in the region of the flow resistance 13 is between 40% and 60% of the cross-section in the remaining region of the respective outlet tube 6. The flow resistance element can be arranged, in particular, according to the illustration in fig. 5 in the region of the inflow opening 7 of the outlet tube 6.

The respective flow resistance 13 is preferably releasably connected to the respective outlet pipe 6. For example, the respective flow resistance 13 can be connected to the respective outlet pipe 6, in particular can be screwed into the respective outlet pipe 6, by means of a screw connection 14, as shown in fig. 5.

The outlet tubules 6 are usually closed except for a respective inflow 7 and a respective outflow 8. However, it is possible for the outlet small tube 6 to have a vent opening 15, preferably in its middle section 10, according to the illustration in fig. 6. The exhaust openings 15, if present, are arranged on the upper side of the middle section 10 and preferably in the vicinity of the respective vertex 12. However, in general, said venting holes 15 are not required.

According to the illustration in fig. 1 and 2, a regulating valve 16 is arranged in the supply line 4. By means of the regulating valve 16, the quantity of liquid coolant 5 supplied to the cooling beam 3 can be regulated. According to the illustration in fig. 1, an actuating element 17 is assigned to the control valve 16. By means of the actuating element 17, the control valve 16 can be moved from the fully open position into the fully closed position and back.

The present invention has many advantages. It is achieved in particular that, after the supply of coolant 5 to the cooling beam 3 has ceased, only that amount of coolant 5 which is already present in the outlet small pipe 6 can flow out of the outlet small pipe 6. This quantity is in practice usually a maximum of 1 l and is therefore a complete order of magnitude smaller than in the prior art (i.e. a factor of 10). Furthermore, no air can reach the chilled beam 3 from the environment. The amount of coolant 5 that is transported to the chilled beam 3 can be very accurately adjusted.

Although the invention has been illustrated and described in detail with respect to a preferred embodiment, the invention is not limited by the disclosed example and other variants can be derived therefrom by the person skilled in the art without departing from the scope of protection of the invention.

List of reference numerals:

1 rolled stock

2 transfer roll

3 chilled beam

4 supply line

5 Coolant

6 outlet small tube

7 flow inlet

8 outflow opening

9 initial section

10 middle section

11 end segment

12 vertex

13 flow resistance element

14 screw connection

15 air vent

16 regulating valve

17 operating mechanism

a distance between

b width of

h0, h1 and h2 height spacing

radius of curvature r

x direction of conveyance

y transverse direction

The angle of bending alpha.