Further advantages and embodiments of the present invention can be appreciated from the accompanying drawings, in which:
The two-row gas cooler 110 in accordance with this embodiment exhibits a tube interconnection from 29/31-31/29 and overall dimensions of a heat exchanger matrix in the order of approximately B×H=462.0×660 mm2. A block depth of the two-row gas cooler 110 is in the order of approximately 16 mm.
In
The flat tube 100 exhibits a tube length in the order of approximately 670 mm and a flat tubular cross section 101 with a long side, a flat tube depth of 5.8 mm, and a significantly shorter side, a flat tube width, of 1.5 mm in relation to this long side.
Moreover, the flat tube 100 exhibits a linear course for the tubes over the entire length of the tube along a longitudinal axis of the tube.
In the two-row gas cooler in accordance with the embodiment, the tubes 100 are arranged on two mutually parallel levels 102, 103.
Within each level 102, 103, the flat tubes 100 are also arranged parallel with one another at a distance of approximately 2 mm to 10 mm, preferably between 4 mm and 8 mm, and in particular approximately 6 mm.
Between two flat tubes 100 arranged in each case adjacent to and parallel with one another on a level 102, 103, corrugated ribs 106, in each case with a rib height in the order of approximately 6 mm, are arranged along the length of the tube and in the longitudinal direction 104 of the tubes 100.
The two-row gas cooler 110 in accordance with the embodiment exhibits an overall rib density of 75 ribs/dm. A preferred range for the density of the ribs is in the order of 65 to 85 ribs/dm.
A cooling medium under high pressure flows through the flat tubes 100 in the longitudinal direction 104, for which purpose in the flat tube 100 a plurality of flow channels 105 run essentially parallel with the longitudinal direction 104 and the longitudinal axis of the flat tube 100.
A couple of collection tanks 120 exhibiting two collection tubes 123, 124 are connected to each flat tube end 121 at a connection point provided for the purpose, in order to extend in a direction, a principal direction of extension, perpendicular to the longitudinal direction 104 of each tube 100. A cooling medium under high pressure also flows through these.
Consequently, the flat tubular cross section 101 and the long side of the flat tubular cross section 101 of the tube 100 exhibit, at each connection point, a predetermined angle in the order of approximately 90° in relation to the principal direction of extension of the collection tank 120.
A recess for the connection of the flat tube 100 is provided at the connection point on the side of the collection tank 120. A cross section through the recess is adapted in this case to the cross section 101 of the flat tube 100. In addition, the recess exhibits a supplementary formed area, in the form of a guide taper for the flat tubes 100.
The expression connection to one another is used to denote a connection of a kind such that a fluid in liquid and/or gaseous form, such as the cooling medium in this case, is able to flow through this connection in a liquid-tight and/or gas-tight manner.
Corresponding methods for producing a tight connection of this kind, such as soldering, welding and/or adhesive bonding, or combinations thereof, are familiar from the prior art.
The collection tanks 120 and the collection tubes 123, 1124 in each case exhibit a tubular cross section 122, in conjunction with which an internal diameter 200 of the tubular cross section 122 is approximately equal to the tube depth of the flat tube 100. A collection tube wall thickness 201 is dependent on a stipulated bursting pressure.
The block depth T(Ges) is determined from:
T(Ges)=2*T(F1)+2×d(wall, collection tube)+b(gap),
where T(Fl) is the flat tube depth, d(wall, collection tube) is a wall thickness of a collection tube, and d(gap) is a gap between the two collection tubes.
The graphical relation depicted here is based on the fact that b(gap)=0.8 mm, and d(wall, collection tube) is determined by
d(wall, collection tube)=0.1×p(burst)*T(F1)/(2*s),
where p(burst) designates the bursting pressure, and s is a limit of elasticity of a collection tube material. s is assumed in the present case to have a value of 50 N/mm2 (AA 3003 mod).
It can be appreciated from
The flat tube depth T(Fl)<6 mm is thus adequate for a bursting pressure of 270 bar for linear flat tubes in the case of two-row high-pressure gas coolers with a block depth of 16 mm.
Consideration must also be given here to the circumstance that, with decreasing flat tube depths T(Fl), a contact surface between a corrugated rib and the flat tube is reduced at a constant block depth. For this reason, at a block depth of 16 mm, the individual flat tube depth should also not be less than approximately 5 mm. Corresponding consideration must also be given to other total block depths.
It can also be appreciated from
It can be appreciated from
In
Gas cooler 1 exhibits conventional flat tubes with twisted flat tube ends and with a flat tube depth of 7 mm. The dimensions of the heat exchanger matrix of this gas cooler 1 are B×H=462.0×650.0 mm2 for an end face F(St)=30.0 dm2.
Gas cooler 2 exhibits the flat tubes in accordance with the invention with a linear course for the tubes and with a flat tube depth of 5.8 mm. The dimensions of the heat exchanger matrix of the gas cooler 2 are B×H=462.0×664.0 mm2 for an end face F(St)=30.7 dm2.
The larger end face of the gas cooler 2 means that the disadvantage of the smaller flat tube depth and the associated reduced contact surface between the corrugated rib and the flat tube can be more or less equalized. The gas cooler 2 exhibits a greater pressure drop on the cooling medium side for an identical mass flow rate.
Gas cooler 1 exhibits conventional flat tubes with twisted flat tube ends and with a flat tube depth of 7 mm. The dimensions of the heat exchanger matrix of this gas cooler 1 are B×H=458.8×650.0 mm2 for an end face F(St)=29.8 dm2.
Gas cooler 2 exhibits the flat tubes in accordance with the invention with a linear course for the tubes and with a flat tube depth of 5.8 mm. The dimensions of the heat exchanger matrix of the gas cooler 2 are B×H=458.0×664.0 mm2 for an end face F(St)=30.5 dm2.
The larger end face of the gas cooler 2 means that the disadvantage of the smaller flat tube depth and the associated reduced contact surface between the corrugated rib and the flat tube can be more or less equalized. The gas cooler 2 exhibits a higher pressure drop on the cooling medium side for an identical mass flow rate.
The relationships for a flat tube in accordance with the invention having a flat tube depth of T(Fl)<6 mm and for a conventional flat tube having a larger flat tube depth, namely T(Fl)=7 mm are depicted in
The relationships are depicted in each case for flat tube widths of 1.4 mm and 1.6 mm and for two corrugated rib heights of 4.5 mm and 6 mm for a rib density of 75 ribs/dm. The thickness of a single corrugated rib is 0.1 mm.
It can be appreciated from
The gas cooler output depicted here relates to the gas cooler already dealt with in
It can be appreciated from
The present invention is particularly suitable for application to the coolers or auxiliary heaters of a high-pressure cooling circuit. A design of the heat exchanger matrix in each case is not restricted to the geometries described above. It can be selected freely in the context of the flat tube geometry in accordance with the invention and the bursting pressure requirements.
Although the present invention has been explained fully in conjunction with preferred embodiments with reference to the accompanying drawings, numerous variations and modifications will be obvious to a person skilled in the art, all of which come within the scope of the present invention, as laid down in the accompanying patent claims.
Number | Date | Country | Kind |
---|---|---|---|
10 2004 005 621.8 | Feb 2004 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/EP05/01032 | 2/2/2005 | WO | 00 | 5/11/2007 |