The present invention relates to a method for expanding a gas flow, more specifically a gas or gas mixture such as steam or similar.
In an industrial process steam is often used as a driving force or as an inhibitor for all kinds of chemical or other processes.
Steam is generally generated in a boiler whose pressure and temperature are generally fixed.
The industrial process generally requires steam at a lower pressure and temperature than at the output of the boiler, whereby the desired steam conditions can also be variable.
Hence in most steam installations a pressure reducing valve is used between the boiler and the downstream industrial process that allows the steam to expand to the desired pressure required for the industrial process.
Generally saturated steam is used, which by definition does not contain any water in liquid form as all water present in the steam has evaporated into a gas.
It is known that with saturated steam there is an unequivocal link between the pressure and temperature of the steam. In other words, if the temperature of the steam is known, the pressure can also be determined from it and vice versa.
The pressure reducing valve is thereby opened or closed more or less to obtain a pressure that is equal to the pressure required by the downstream process. During expansion, the pressure and temperature of the steam change according to an isenthalpic law known in thermodynamics.
An advantage of such control is that it is very simple.
However, a disadvantage of such control is that the pressure drop is not used for an efficient conversion to another form of energy such as mechanical or electrical energy for example.
Another disadvantage is that it only enables the pressure to be controlled, whereby the isenthalpic expansion in the pressure reducing valve, starting with saturated steam, always supplies superheated steam at a temperature that is generally higher than desired. Superheating of the steam also means an inefficient exchange of heat in the downstream process and consequently must be limited as much as possible.
In order to reduce the temperature of the steam and the level of superheating, traditionally a boiler or ‘desuperheater’ is used that presents the disadvantage of being expensive and is consequently limited in its capacities.
The purpose of the present invention is to provide a solution to one or more of the aforementioned and other disadvantages.
To this end the invention concerns a method for expanding a gas flow of a gas or gas mixture such as steam or similar, between an inlet for the supply of the gas to be expanded at certain inlet conditions of inlet pressure and inlet temperature and an outlet for the delivery of expanded gas at certain desired outlet conditions of outlet pressure and outlet temperature, whereby the method at least comprises the step of at least partly expanding the gas flow between the inlet and the outlet through a pressure reducing valve and at least partly expanding it through a pressure reducing unit with a rotor driven by the gas with an outgoing shaft for converting the energy contained in the gas into mechanical energy on this shaft.
By the application of such a pressure reducing unit at least a proportion of the expansion energy can be efficiently converted into mechanical energy on the shaft of the pressure reducing unit, whereby this mechanical energy can be used for example to drive an electricity generator or another useful application.
In contrast to the isenthalpic expansion of the steam in the pressure reducing valve, an expansion in a pressure reducing unit of the intended type proceeds according to a rather polytropic or approximately isentropic thermodynamic law, whereby, compared to an isenthalpic expansion, a polytropic expansion brings about a greater temperature drop for the same pressure drop.
Due to the expansion between the input and output of the device being partly isenthalpic and partly polytropic for the entire flow or for certain parts of the flow, and due to a suitable distribution between isentropic and polytropic expansions, respectively in the pressure reducing valve and in the pressure reducing unit, and/or by a suitable distribution of the subflows, both the pressure and the temperature at the outlet can be adjusted to the values desired by the downstream process, and this without application of additional cooling or a steam cooler and with the additional advantage of being able to draw mechanical energy from the polytropic expansion.
Preferably a screw expander is used as a pressure reducing unit that offers the advantage that it also enables the steam to expand to temperatures below the saturation temperature, whereby steam will partly condense into liquid and which thus enables a wider area of application than with most types of turbines.
According to a preferred variant of the method according to the invention, the gas flow to be expanded is driven through the pressure reducing valve and through the pressure reducing unit in parallel, with a subflow of the gas flow to be expanded that flows through the pressure reducing valve and a subflow that flows through the pressure reducing unit, whereby both subflows are expanded to the desired outlet pressure, after which both subflows are combined at the same desired outlet pressure for the supply of the expanded gas flow at the desired outlet conditions at the outlet.
According to another preferred variant of the method according to the invention the gas flow to be expanded is driven in two successive expansion stages in series through the pressure reducing valve and through the pressure reducing unit, whereby the pressure reducing valve and the pressure reducing unit are controlled such that an intermediate operating point with an intermediate pressure and temperature are obtained after the first expansion stage that ensures an expansion in the second expansion stage to a pressure and temperature corresponding to the desired outlet pressure and outlet temperature.
The invention also relates to a device for expanding a gas flow of a gas or gas mixture such as steam or similar, whereby this device comprises an inlet for the supply of the gas to be expanded at certain inlet conditions of inlet pressure and inlet temperature, and an outlet for the delivery of expanded gas at certain desired outlet conditions of outlet pressure and outlet temperature, whereby the device enables the method according to the invention described above to be applied and which to this end is provided with a pressure reducing valve and a pressure reducing unit with a rotor driven by the gas with an outgoing shaft for converting the energy contained in the gas into mechanical energy on this shaft and pipes to guide the gas flow to be expanded at least partly through the pressure reducing valve and at least partly through the pressure reducing unit.
The advantages are the same as those described for the method applied according to the invention.
With the intention of better showing the characteristics of the present invention, a few preferred applications of a method according to the invention for expanding a gas flow and a device thereby applied are described hereinafter by way of an example, without any limiting nature, with reference to the accompanying drawings, wherein:
The conventional device 1 shown in
The source 2 is a boiler for example that produces saturated steam at certain inlet conditions, i.e. a certain inlet pressure pA and inlet temperature TA at the input A of the device 1.
The operating point of the steam in the inlet A is shown in the phase diagram as the point A located on the saturation curve 4 of the phase diagram, whereby this saturation curve 4 forms the separation between the zone of the gas phase G on the one hand where the temperature and pressure of the steam are such that the steam only occurs in the gas phase of water, and the zone G+V where the gas phase of water is in equilibrium with the liquid phase of water.
The isobar of constant pressure pA that goes through the operating point A is indicated in the phase diagram as a dashed line and presents all operating points for which the pressure is equal to the inlet pressure pA.
When energy is supplied starting from a point on the isobar pA to the left of the saturation line, then the operating point will move along the horizontal section of the isobar pA towards the right at a constant temperature TA and the water droplets present will gradually evaporate until the operating point A is reached where all the water has evaporated and only gas remains.
With the further supply of energy at constant pressure PA, the operating point will move further to the right along the isobar pA and the temperature will gradually rise. In this zone it is a case of superheated steam corresponding to a gas phase without liquid.
The downstream steam device 3 determines the steam conditions that the steam supplied must satisfy, in other words the steam conditions at the output B of the device 1, in particular the outlet pressure pB, outlet temperature TB and composition of the steam.
Generally slightly superheated steam is desired for the downstream steam device 3. The corresponding operating point is shown in the phase diagram as a point B to the right of the saturation line 4 at a pressure pB that is lower than the pressure pA, and a temperature TB that is lower than TA.
In order to expand the steam from the pressure pA at the inlet A to the lower pressure pB at the outlet B, conventionally use is made of a pressure reducing valve 5 that is incorporated in a pipe 6 that connects the inlet A to the outlet B to expand a flow of steam Q through the pressure reducing valve 5.
For a conventional pressure reducing valve 5, this expansion to the outlet pressure pB proceeds essentially according to an isenthalpic development along the isenthalpic expansion curve 7 up to the point C on the isobar pB.
The temperature TC is generally much higher than the desired outlet temperature TB, and so after the pressure reducing valve 5 a steam cooler 8 or similar is used to reduce the outlet temperature to the desired temperature TB at constant pressure pB. The operating point then moves along the isobar pB from point C to point B.
In the example shown of a conventional device 1, the pressure reducing valve 5 is adjustable and provided with a controller 9 to control the expansion through the pressure reducing valve 5 to a desired pressure value pB set in the controller 9, whereby the controller 9 continuously measures the pressure at the outlet B and opens the pressure reducing valve 5 more or less as the pressure is greater or smaller than the set pressure pB until the pressure is equal to the aforementioned set pressure.
The pressure reducing unit is preferably constructed as a screw expander with two meshed rotors 11 of which one rotor 11 is provided with an outgoing shaft 12 for conversion of the expansion energy of the steam into mechanical energy that is available on the shaft 12.
By way of an example, the outgoing shaft 12 is coupled to an electricity generator 14 for the delivery of electricity to a consumer network (not shown).
The speed of the pressure reducing unit 10 is preferably variably adjustable, to which end the generator 14 is provided with a controller 13 for example.
Other forms of pressure reducing units with at least one driven rotor and outgoing shaft are not excluded, for example one or another type of turbine.
The device 1 according to the invention is provided with means 15 and 16, respectively for measuring or determining the temperature and pressure at the outlet B.
Furthermore the device of
The controller 9 is connected via the connections 17 to the aforementioned means 15 and 16 for determining the pressure and temperature at the outlet B and has a control algorithm 18 to split the flow Q into the two aforementioned subflows Q1 and Q2 that both undergo an expansion separately to the desired outlet pressure pB.
The expansion of the subflow Q2 in the screw expander taken as an example typically proceeds according to an approximately isentropic or polytropic law, as illustrated in
The flow thereby changes from the operating point A at the inlet A to the operating point B″ at the outlet B″ of the pressure reducing unit 10, whereby this operating point B″ is located on the isobar pB.
It can be derived from the phase diagram that the temperature TB″ at the outlet B″ is lower than the desired temperature TB.
The expansion of the subflow Q1 in the pressure reducing valve 5 typically proceeds according to an isenthalpic law that proceeds in an analogous way to
The temperature TB′ at the outlet B′ of the pressure reducing valve 5 is thereby higher than the desired set temperature TB.
After expansion both subflows Q1 and Q2 are combined with a pressure pB, whereby a combined flow Q occurs at the outlet B with a pressure pB and a temperature that is between the temperatures TB′ and TB″ and which depends on the mutual mixing ratios of both subflows Q1 and Q2. The control algorithm 18 of the controller 9 is such that the mutual mixing ratio between Q1 and Q2 can be controlled such that the temperature of the combined flow Q corresponds to the desired temperature TB.
To this end the controller 9, is connected on the one hand to the controller 13 via a connection 20 to be able to adjust the speed and thereby also the flow Q2 of the pressure reducing unit 10 and, on the other hand, is connected to the controllable pressure reducing valve 5 via a connection 21 in order to open or close this pressure reducing valve 5 more or less in order to let more or less flow Q1 through.
The control algorithm 18 can be designed as follows for example.
When starting the device 1 the flow Q is distributed equally for example into a flow Q1 through the pressure reducing valve 5 and a flow Q2 through the pressure reducing unit 10, whereby Q1=Q2=Q/2.
In the first instance the combined flow Q is controlled on the basis of the pressure measured at the outlet B. When the measured pressure is lower than the set value of the desired outlet pressure pB this means that the flow Q is too low and the subflows Q1 and Q2 are increased to an equal extent until the measured pressure is equal to the set pressure pB. Analogously, when the measured pressure is higher than the set value pB, the subflows Q1 and Q2 are reduced to an equal extent until the measured pressure is equal to the set pressure pB.
The steam through the pressure reducing valve 5 follows curve 7 up to point B′, while the steam through the pressure reducing unit 10 follows the curve 19 up to point B″. The combination of both flows leads to a point B′″ that differs from the demanded temperature TB.
If the temperature B′″ is lower than temperature TB, as is the case of
As the total combined flow Q is not affected by this initial control, with constant inlet conditions, the outlet pressure will be maintained at pB.
If, on the other hand, the temperature B′″ is higher than the desired temperature TB, then this means that too much steam is expanded via curve 7. That is why in this case the algorithm 18 will ensure that the flow Q1 decreases and the flow Q2 increases to the same extent until temperature TB is reached.
If for example the downstream consumers in the steam device 3 now require less flow Q, then the outlet pressure pB will increase if the device 1 still supplies the flow Q. Then the controller 18 will change the flow Q, upon detection of a change in the outlet pressure, so that the ratio of the flows Q1/Q2 applicable at the time is maintained.
As soon as the correct outlet pressure pB is reached the algorithm 18 will then check whether the ratio of the flows Q1/Q2 must be changed to realise the desired temperature TB at the outlet B.
Upon a change of other conditions such as inlet pressure or inlet temperature the algorithm 18 will also proceed in the same way, i.e.:
Of course there can be additional branches and tap-offs in the device that further divide the flow Q or subflows Q1 and/or Q2 to again be entirely or partially combined afterwards in proportions determined by the controller in order to get the desired outlet conditions.
It is clear that the conditions at the inlet A do not need to be limited to points on the saturation curve 4, but in the inlet it can also start with slightly superheated steam with an operating point to the right of the curve 4 or a slight two-phase mixture of steam and water droplets with an operating point to the left of the curve 4, to nonetheless still be able to make use of the advantages of the invention.
As shown in
A suitable controller 9 makes it possible to control both expansion stages such that the pressure and temperature at the outlet B is equal to a set value pB and TB in the controller 9.
The controller 9 comprises a computation and control algorithm 22 that determines the course of the expansion curves 7 and 19 as a function of the known inlet conditions pA and/or TA and as a function of the desired outlet conditions pB and/or TB, and then determines the operating point C as a section of both expansion curves 7 and 19. This operating point C corresponds to the intermediate operating point that is desired to be reached between both expansion stages to reach the desired pressure pB and temperature TB at the outlet for the given inlet conditions pA and TB.
The control algorithm 22 provides the following control for example.
During a first control step the flow Q is adjusted until the desired pressure pB is reached in the outlet B.
To this end when starting up the device 1 the pressure reducing unit 10 is controlled at a minimum speed by adjusting the load of the generator 14 via the controller 13 and the pressure reducing valve 5 is thereby systematically opened.
When the opening proceeds slowly in the beginning a very large pressure drop will occur across the pressure reducing valve 5, such that the intermediate pressure at the intermediate operating point C′ will be much lower than the desired interim pressure pC. The flow Q will generally be expanded via the expansion curve 7 and to a lesser extent via the expansion curve 19.
The control algorithm 22 will gradually further open the expansion valve 5 at constant speed of the pressure reducing unit 10 until the demanded outlet pressure pB is reached as shown in
The operating point B′ is characterised by an outlet temperature that is higher than the desired outlet temperature TB.
During a second control step the interim pressure of the intermediate operating pressure C is adjusted while preserving the flow rate, and this in the following way for example.
When the interim pressure is lower than the desired interim pressure pC, then the algorithm will increase the speed of the pressure reducing unit 10 until the desired interim pressure pC is reached.
However, when the interim pressure is higher than the desired interim pressure pC, the algorithm will close the pressure reducing valve 5 more until the desired interim pressure pC is reached.
If the downstream consumers now demand less flow Q for example, the outlet pressure in the outlet B will increase if the device still supplies a flow Q. That is why the controller 9, when detecting a change in the outlet pressure in the outlet B, will change the flow Q such that the interim pressure pC is preserved. This can be done in the case of a lower required flow by simultaneously closing the pressure reducing valve 5 and reducing the speed of the pressure reducing unit 10 according to a certain ratio.
As soon as the desired outlet pressure PB is reached the algorithm will then check whether the state of the pressure reducing valve 5 and/or the speed of the pressure reducing unit 10 must be changed to realise the calculated desired interim pressure pC.
It is not excluded that the algorithm comprises a step that refines the calculated interim pressure pC on the basis of the difference between the measured outlet temperature and the desired outlet temperature TB for the case when an inaccuracy in the algorithm or ageing of the machine occurs.
Upon a change of other conditions such as inlet pressure or inlet temperature the algorithm will always proceed in the same way, i.e.:
It is clear that the order of the pressure reducing valve 5 when the pressure reducing unit 10 in series can also be swapped over and that more than two stages can also be provided.
Depending on the complexity of the industrial process it is not excluded that a combination of one or more parallel connections such as that of
Although a screw expander is used in each of the examples described above, it is not excluded using other types of expanders. An advantage of a screw expander it is less sensible to the formation of water droplets during the expansion, such as in the case of
Instead of steam other gases or gas mixtures can also be used.
The present invention is by no means limited to the variants of a method and device for expanding a gas flow described as an example and shown in the drawings, but a method and a device according to the invention can be realised in all kinds of variants without departing from the scope of the invention.
Number | Date | Country | Kind |
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2014/0375 | May 2014 | BE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/BE2015/000024 | 5/11/2015 | WO | 00 |