Reboiler/condenser heat exchanger of the bath type

Abstract
A reboiler/condenser bath heat exchanger for heat exchange between a first fluid to be vaporized and a second fluid to be condensed includes a number of passages for heat exchange between the two fluids in order to make the second fluid flow, which fluid has a temperature of T2-2 at the outlet of the passages; a vessel containing the passages for making the first fluid flow between the passages by thermosiphon effect from the bottom upwards over a height h, the first fluid having an entry temperature T1-1 where T1-1
Description




FIELD OF THE INVENTION




The subject of the present invention is a reboiler/condenser heat exchanger of the bath type and a heat exchange process in a heat exchanger of the bath type.




More specifically, the invention relates to a reboiler/condenser heat exchanger of the bath type for heat exchange between a first fluid to be vaporized and a second fluid to be condensed, and to the use of this type of heat exchanger. The term “vaporization” is understood to mean partial or complete vaporization and the term “condensation” is understood to mean partial or complete condensation.




BACKGROUND OF THE INVENTION




This arrangement is used especially, but not exclusively, in air distillation plants of the double-column type in which, for example, liquid oxygen at the bottom of the low-pressure column is vaporized in a bath reboiler by heat exchange with gaseous nitrogen taken from the top of the medium-pressure column.




The operation of bath heat exchangers, because of their intrinsic characteristics, imposes limitations as regards the height for exchange between the first and second fluids or as regards the temperature difference between the primary fluid and the secondary fluid.




This problem will be more clearly understood with reference to the appended

FIGS. 1 and 2

which show, on the one hand, an example of a functional diagram showing the operation of a bath heat exchanger and, on the other hand, an example of a functional diagram showing the heat exchange between the primary fluid and the secondary fluid.





FIG. 1

shows, in a simplified manner, the external vessel


10


of the bath heat exchanger, inside which vessel a number of passages


12


for the “warm” second fluid F


2


are contained, the said second fluid entering the vessel in the upper part of these passages at


14


and leaving it in the lower part at


16


. With regard to the “cold” first fluid F


1


to be vaporized, this is contained in the external vessel


10


and flows by thermosiphon effect from the lower end


12




a


of the passages for the second fluid F


2


to its upper end


12




b


, the height of this heat exchange region being equal to h.




As the diagram in

FIG. 2

shows more clearly, the first fluid F


1


at the inlet of the exchange region is at a temperature T


1-1


and at a pressure P


1-1


. This Temperature T


1-1


and this pressure P


1-1


correspond to a subcooling state, that is to say correspond to a temperature below the bubble temperature T


b1


of the fluid F


1


at the pressure P


1-1


because of the hydrostatic pressure due to the head of liquid fluid F


1


. This will be shown in the above diagram in which T


b


denotes the temperature (the bubble temperature) at which the first gas bubble appears in the fluid F


1


during the heat exchange (at an intermediate pressure between P


1-1


and P


1-1


). It will be understood that the energy used to bring the primary fluid to the bubble temperature T


b


is “lost” energy, in order to vaporize the first fluid. Also shown in this

FIG. 2

is the second fluid F


2


with its entry temperature T


2-1


at which it enters the exchange region


12


and its exit temperature T


2-2


. It can be seen that the subcooling phenomenon results in a “pinching effect” in the heat exchange between the two fluids.




Furthermore, the thermosiphon effect, which allows the first fluid F


1


to flow, is made possible by the formation of bubbles in the first fluid. If the head in the heat exchanger corresponding to the “desubcooling” phase is too great, the thermosiphon effect will be insufficient.




It will be understood that the greater the height h of the heat exchange region the greater the hydrostatic pressure on the first fluid at the inlet of the exchange region and therefore the greater the subcooling region must be too. To sustain the thermosiphon effect which ensures flow of the first fluid, the “pinching” phenomenon must therefore be limited. In heat exchange plants of the bath type, this height is therefore limited to 2.5 meters.




Another drawback present in this type of bath heat exchanger is that the “pinching phenomenon” described above requires there to be a temperature difference between the entry temperature T


1-1


of the cold fluid F


1


to be vaporized and the temperature T


2-2


of the warm fluid F


2


of more than about 1.2° C. in order to allow the heat exchanger to operate by thermosiphon effect because of the “pinching effect”. However, it will be understood that increasing this temperature difference increases the thermodynamic irreversibilities and, consequently, reduces the energy efficiency of the entire plant. For example, in the case of the distillation of the gases contained in the air using a double column, the pressure in the column called the medium-pressure column and, consequently, the pressure in the feed air compressor, must be increased, thereby increasing the energy consumption of the entire plant.




There is therefore a real need for reboiling/condenser heat exchangers of the bath type or for heat exchange processes in a plant of the bath type which make it possible either to increase the vertical heat exchange height, in order to reduce the floor space of the plant, or to reduce the temperature difference between the first fluid and the second fluid, or else to allow a combination of these two characteristics of the reboiler/condenser heat exchanger.




SUMMARY OF THE INVENTION




According to the invention, to achieve this objective the reboiler/condenser heat exchanger of the bath type, for heat exchange between a first fluid (F


1


) to be vaporized and a second fluid (F


2


) to be condensed, the said heat exchanger, having a minimum exit pressure P


m,ex


of the said first fluid in order to allow the plant in which the said heat exchanger is mounted to operate, comprises:




means for defining a number of passages for heat exchange between the two fluids in order to make the said second fluid flow, the said second fluid having a temperature T


2-2


at the outlet of the said passages;




vessel-forming means containing the passage-forming means for making the said first fluid flow by thermosiphon effect between the said passages from the bottom upwards over a height h, the said first fluid having an entry temperature T


1-1


where T


1-1


<T


2-2


and the said vaporized first fluid having an exit pressure P


1-2


;




means for giving the entry pressure P


1-1


of the said first fluid a value such that the pressure P


1-2


is greater than the said minimum pressure P


m,ex


and means for ensuring that at least one of the two following conditions is fulfilled:




the height h of the heat exchange passages is at least equal to 2.5 m; and




the temperature T


2-2


of the said second fluid is less than T


1-1


+1.2° C.




It has in fact been demonstrated that if the exit pressure of the first fluid is increased, the pinching effect is modified, thereby allowing either the heat exchange height h to be increased or the temperature difference between the two fluids to be decreased.




According to another aspect of the invention, the process for vaporizing a first fluid (F


1


) using a reboiler/condenser bath heat exchanger comprises the following steps:




a second fluid (F


2


) is made to flow through vertical exchange passages, the said second fluid having an exit temperature T


2-2


;




the said first fluid is made to flow from the bottom up over a height h by thermosiphon effect between the said heat exchange passages, the said first fluid having an entry temperature T


1-1


(where T


1-1


<T


2-2


) and the vaporized fraction of the said first fluid having an exit pressure P


1-2


;




the said pressure P


1-2


is given a value greater than the minimum exit pressure of the vaporized fraction of the first fluid needed to allow the plant in which the said heat exchanger is mounted to operate; and




the height h of the heat exchange passages and the temperature T


2-2


of the said second fluid are chosen in such a way that at least one of the two following conditions is fulfilled:




the height h of the said heat exchange passages is at least equal to 2.5 m; and




the temperature T


2-2


of the said second fluid is less than T


1-1


+1.2°C.




It will be understood that this process makes it possible to improve the characteristics of the bath heat exchanger as was already explained in connection with the above definition of the bath heat exchanger according to the invention.




According to a preferred embodiment, the exit pressure of the first fluid P


1-2


is about 4 bar absolute, or higher.




According to another characteristic, the height of the passages for heat exchange between the two fluids is preferably at least equal to 3 m.




Preferably, the passages for heat exchange between the two fluids are bounded by parallel plates these possibly being of the type with brazed fins.




According to a variant embodiment, the passages may consist of tubes.




According to a first embodiment, the vessel-forming means comprise a single vessel which contains the said heat exchange passages and through which the first fluid flows by thermosiphon effect.




According to a second embodiment, the vessel-forming means comprise a first vessel defining a lower volume for the entry of the first fluid and an upper volume for the exit of the first fluid and a second vessel connected to the upper and lower volumes respectively, this second vessel possibly being reduced to a pipe.











BRIEF DESCRIPTION OF THE DRAWINGS




Further features and advantages of the invention will become more apparent on reading the description which follows of several embodiments of the invention, given by way of non-limiting examples. The description refers to the appended figures in which:





FIG. 1

, already described, is a simplified view of a known bath heat exchanger;





FIG. 2

, already described, shows the heat exchange diagram for the bath heat exchanger of

FIG. 1

;





FIG. 3

shows a first embodiment of a bath heat exchanger according to the invention, used in the distillation of air;





FIG. 4

is a heat exchange diagram showing the operation of the bath heat exchanger of

FIG. 3

;





FIG. 5

shows a variant embodiment of the bath heat exchanger according to the invention; and





FIG. 6

shows curves of the variation in subcooling as a function of the pressure of the liquid for a net positive suction head of 1 meter.











DETAILED DESCRIPTION OF THE INVENTION




A first embodiment of the bath heat exchanger according to the invention will be described first of all with reference to

FIGS. 3 and 4

. In the description which follows, the case in which the cold fluid to be vaporized is liquid oxygen and the warm fluid is gaseous nitrogen will more particularly be considered, this being the case, for example, in the cryogenic distillation of the gases in air, with an arrangement of the double-column type. However, it goes without saying that the present invention may be applied to heat exchange between two other fluids, for example to the cryogenic separation of synthesis gases, such as methane, carbon monoxide, hydrogen, etc.




A first embodiment of the bath heat exchanger will be described firstly with reference to

FIGS. 3 and 4

. The external vessel


20


containing the first fluid F


1


which, in the example in question, is pure oxygen, has been depicted. In the upper part of the vessel


20


is the interface


22


between the first fluid F


1


in liquid form and the fluid F


1


in vapour form, recovered from the upper part of the vessel. Inside this vessel is a heat exchange module


24


which defines, in a manner known per se, passages


26


for the “warm” second fluid F


2


which, in the example in question, is pure nitrogen, these passages lying between an inlet box


28


connected to the inlet pipe


30


and an outlet box


32


connected to the outlet pipe


34


. These passages, as is known, may consist of tubes or of parallel plates defining the circuit for the second fluid. These passages may be vertical, as shown in

FIG. 3

, horizontal or oblique. The heat exchange module


24


also defines vertical passages for the flow of the first fluid F


1


, that is to say of the oxygen.




As already indicated, in this type of bath heat exchanger the fluid F


1


to be vaporized flows by thermosiphon effect through the vertical heat exchange passages. The fluid F


1


has, at its inlet, that is to say at the lower end


24




a


of the exchange module, a temperature T


1-1


and a pressure P


1-1


, and a temperature T


1-2


and a pressure P


1-2


at the upper end


24




b


of the exchange module. The total height of the exchange module, that is to say the flow length of the first fluid between the inlet end


24




a


and the outlet end


24




b


, is called h.




The second fluid, which is gaseous nitrogen in the example in question, enters at the temperature T


2-1


via the pipe


30


and leaves the exchange module in liquid form at the temperature T


2-2


.





FIG. 4

shows the heat exchange between the fluid F


1


(pure oxygen) and the fluid F


2


(pure nitrogen). Curve A, which is approximately vertical because the fluid F


2


is pure nitrogen, shows the change in this fluid between its entry into the exchange module and its exit therefrom. Curve B shows the change in the first fluid (pure oxygen). It has a first part B


1


corresponding to the “desubcooling” of the oxygen and a part B


2


for partial vaporization of the oxygen above the oxygen bubble temperature T


b


.




As already explained, by increasing the exit pressure P


1-2


of the first fluid it is possible to reduce the “pinching effect”, thereby making it possible to increase the exchange height h and/or to reduce the temperature difference T


2-2


−T


1-1


.




In the case of the cryogenic distillation of the gases in air with an arrangement of the double-column type, the exit pressure P


1-2


of the first fluid (oxygen) depends on the exit pressure of the complete plant containing the bath heat exchanger, taking into account the head loss due to the apparatus between the outlet of the heat exchanger and the outlet of the complete plant. If the outlet of the plant is at atmospheric pressure, the pressure at the outlet of the bath heat exchanger is about 1.3 bar absolute.




It goes without saying that, in order to increase the exit pressure P


1-2


of the first fluid, it is necessary to increase the pressure of the warm fluid F


2


and consequently the pressure of the gas (for example air) at the inlet of the plant.




If a pressure P


1-2


of 4 bar absolute is allowed, it is possible to construct a bath heat exchanger in which the height h of the exchange module is equal to 3 or 4 meters, keeping a temperature difference of about 1.2° C.




With the same exit pressure of 4 bar absolute and keeping a height h of 2 meters, it is possible to reduce the temperature difference to 0.4 or 0.5° C.





FIG. 5

shows one alternative embodiment of the bath heat exchanger.




The heat exchanger comprises a main vessel


40


in which the exchange module


42


is mounted. The vessel


40


also defines a lower chamber


44


for the entry of the first fluid and an upper chamber


46


for the exit of the first fluid with a take-off


48


for the vaporized first fluid. The heat exchanger also includes a vessel


50


for recirculating the first fluid essentially in the liquid state, which vessel


50


is connected to the upper and lower chambers via pipes


52


and


54


. This vessel could simply amount to a pipe.





FIG. 6

shows the variations ΔT


b


of the subcooling caused by a net positive suction head of 1 m as a function of the pressure P for pure oxygen (curve I) and for pure methane (curve II). It may be seen that the higher the pressure (P), the lower the subcooling effect. These curves make it possible to more clearly understand the favourable effect of the increase in pressure of the first fluid on the “pinching effect”. This is because the higher the exit pressure P


1-2


, the more the exchange height h, that is to say the hydrostatic pressure (P


1-2


−P


1-1


), can be increased while keeping the same variation in the subcooling ΔT


b


.



Claims
  • 1. A reboiler/condenser bath heat exchanger, for heat exchange between a first fluid to be vaporized and a second fluid to be condensed, said heat exchanger having a minimum exit pressure Pm,ex of the first fluid in order to allow the plant in which the heat exchanger is mounted to operate, the heat exchanger comprising:means for defining a number of passages for heat exchange between the first fluid and the second fluid in order to make the second fluid flow, the second fluid having an outlet temperature T2-2 at the outlet of the passages; vessel-forming means containing the heat exchange passage-defining means for making the first fluid flow by a thermosiphon effect between the passages from the bottom upwards over a height h, the first fluid having an entry temperature T1-1 where T1-1<T2-2 and the vaporized first fluid having an exit pressure P1-2; means for pressurizing the first fluid having an entry pressure P1-1 to a value such that the exit pressure P1-2 of the first fluid is greater than the minimum pressure Pm,ex, and means for ensuring that at least both of the two following conditions are fulfilled: the height h of the heat exchange passages is at least equal to 2.5 m; and the outlet temperature T2-2 of the second fluid is less than T1-1+1.2° C.
  • 2. The reboiler/condenser bath heat exchanger according to claim 1, wherein the minimum pressure Pm,ex is about 1.3 bar absolute, and the exit pressure P1-2 of the first fluid to be vaporized is about 4 bar absolute, or higher.
  • 3. The reboiler/condenser bath heat exchanger according to claim 1, wherein the height of the heat exchange passages is at least equal to 3 meters.
  • 4. The reboiler/condenser bath heat exchanger according to claim 1, wherein the outlet temperature T2-2 of the second fluid is between T1-1+1.2° C. and T1-1+0.4° C.
  • 5. The reboiler/condenser bath heat exchanger according to claim 1, wherein the heat exchange passages are bounded by parallel plates.
  • 6. The reboiler/condenser bath heat exchanger according to claim 5, wherein the parallel plates include brazed fins.
  • 7. The reboiler/condenser bath heat exchanger according to claim 1, wherein the heat exchange passages are tubes.
  • 8. The reboiler/condenser bath heat exchanger according to claim 1, wherein the vessel-forming means comprise a single vessel, which contains said heat exchange passages and through which said first fluid flows by the thermosiphon effect.
  • 9. The reboiler/condenser bath heat exchanger according to claim 1, wherein the vessel-forming means comprise a first vessel defining a lower volume for entry of the first fluid and an upper volume for exit of the first fluid, and a second vessel connected to the upper and lower volumes, respectively.
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Number Name Date Kind
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5775412 Montestruc, III et al. Jul 1998 A