Patent Application
20150082792
This invention concerns a process for generating electricity using a turbine driven from renewable and/or waste energy sources.
The generation of super heated steam for steam turbines typically involves two phases: feed water pre-heat/evaporation and superheating.
Evaporation involves heating water under pressure to generate saturated steam. The temperature of saturated steam varies with pressure. For example, for a pressure of 1 barG, saturation temperature is 120° C., and at a pressure of 100 barG, saturation temperature is 312° C. Thereafter, the saturated steam is superheated to a temperature of up to, say, 500° C. to enable the use of higher thermal efficiency steam turbine generators.
The concentrated solar power (CSP) industry has struggled to generate consistent high temperature superheated steam. This is because they use a single pass through a solar heat exchanger to convert cold water to super heated steam. Problems arise after evaporation when the heat exchanger is filled with steam, a vapor rather than liquid, dramatically reducing the ability to transfer heat through the heat exchanger tube to the fluid within. The heat transfer rate between the walls of the heat exchanger tube to steam is very much less than that of heat exchanger tube to water. Compounding this, the solar flux is directed to only one side of the heat exchanger pipe. Consequently the risk of overheating the heat exchanger tubes by solar radiation energy (insolation) is increased and the difficulty of managing the heat exchanger tube temperature is magnified.
Traditionally the CSP industry attempts to manage superheating of steam from insolation using two techniques:
Control of the solar reflector (which may include dumping the available solar energy by not using parts of the solar field); or
By using intermediate heat transfer fluids such as molten salt, which adds complexity and losses in efficiency as additional heat exchange processes are required to convert heat from this fluid to steam. The maximum operating temperature of the intermediate heat transfer fluid may need to be constrained to prevent vaporization of the said fluid.
In a first aspect the invention provides a process for operating a turbine driven from renewable or waste energy sources wherein a working fluid which drives the turbine is passed around a working fluid circuit and heated in a two stage heating process using a first heating apparatus using a renewable or waste energy source and a second heating apparatus comprising a graphite body heated by concentrated solar energy the graphite body containing an embedded heat exchanger comprising at least one heat exchanger tube embedded in and in contact with the graphite body, the process, comprising:
According to a second aspect, a system is provided for heating a working fluid from renewable or waste energy sources for operating a turbine wherein a working fluid which drives the turbine is passed around a working fluid circuit and heated in a two stage heating process, the system comprising:
In various embodiments of the invention the relationship between the outer surface area of the embedded heat exchanger tube and the mass of graphite in the graphite body may be in the range of 0.60 m2 to 2.0 m2, or 1.0 m2 to 4.0 m2, or 2.0 m2 to 5.0 m2, or 2.0 m2 to 2.50 m2, or 2.50 m2 to 5.0 m2, or 4.0 m2 to 6.0 m2, or 5.0 m2 to 8.0 m2, or 6.0 m2 to 10.0 m2, or 8.0 m2 to 12.0 m2, or 10.0 m2 to 14.0 m2 or 12.0 m2 to 16.0 m2, or 14.0 m2 to 18.00 m2, or 16.0 m2 to 20.0 m2 of outer surface area of embedded heat exchanger tube per tonne of graphite in the graphite body. Operation of the heat exchanger in graphite body is particularly efficient if the relationship between the outer surface area of the embedded heat exchanger tube and the mass of graphite in the graphite body is in the range of 0.6 m2 to 2.2 m2, or 1.0 m2 to 4.0 m2, or 1.0 m2 to 5.0 m2, 2.0 m2 to 5.0 m2, or 1.2 m2 to 3.0 m2, or 1.2 m2 to 2.2 m2, or 1.5 m2 to 2.5 m2, or 2.0 m2 to 3.0 m2, or 2.0 m2 to 2.50 m2, or 2.50 m2 to 5.0 m2, depending on the mode of operation. For dual mode operation, a useful range is from 1.2 m2 to 3.0 m2/tonne of graphite in the graphite body, and for operation only as a superheater a useful range is from 0.6 to 2.2 m2/tonne of graphite in the graphite body.
The process and system may employ solar concentrators having a capacity to direct concentrated solar energy to the graphite body with a peak power in the range of 20 to 2000 kilowatts (kW) per tonne of graphite at periods of peak insolation.
In various embodiments of the invention the process and system may employ solar concentrators having a capacity to direct concentrated solar energy to the graphite body with a peak power per tonne of graphite in the range of 20 kW to 80 kW, or 50 kW to 100 kW, or 80 kW to 150 kW, or 100 kW to 200 kW, or 150 kW to 250 kW, or 200 kW to 300 kW, or 250 kW to 450 kW, or 300 kW to 500 kW, or 450 kW to 600 kW, or 500 kW to 800 kW, or 600 kW to 900 kW, or 800 kW to 1200 kW, or 900 kW to 1500 kW, or 1200 kW to 1800 kW, or 1500 kW to 2000 kW, or per tonne of graphite in the graphite body.
The heat transfer medium through the embedded heat exchanger may be controlled such that when the stream of working fluid is heated to a temperature less than the intermediate temperature by the first heating apparatus due to a period of inadequate supply of the renewable or waste energy source, the continuous stream of the working fluid out of the heat exchanger embedded in the graphite body continues to be heated to the working temperature for input to the turbine.
The process according to claim 13, wherein the first heating apparatus is also heated by concentrated solar energy and the period of inadequate supply is a period of interruption to, or reduction of, insolation to the first heating apparatus. The first heating apparatus may also be heated using heat provided from a waste heat recovery origin and the period of inadequate supply may be a period of interruption to, or reduction of, availability of heat from the waste heat recovery origin to the first heating apparatus. Alternatively, the first heating apparatus may be heated by heat provided from a geothermal origin and the period of inadequate supply may be a period of interruption to, or reduction of, heat provided from a geothermal origin to the first heating apparatus.
During periods of peak insolation, when the concentrated solar energy being delivered to the graphite body is greater than a level of energy required to heat the working fluid to the working temperature, the graphite body may absorb and store any additional energy for use later whereby energy dumping is minimized or eliminated and the graphite body regulates heat transfer to the heat exchanger tube to avoid overheating of the heat exchanger tube without regard to the level of insolation.
Also during an interruption to, or reduction of, insolation when the concentrated solar energy being delivered to the graphite body is less than a level of energy required to heat the working fluid to the working temperature, thermal energy stored in the graphite body, due to previous heating by the concentrated solar energy, may be drawn on to sustain the heating of the working fluid to the working temperature.
After an interruption to, or reduction of, insolation when the concentrated solar energy being delivered to the graphite body is less than a level of energy required to heat the working fluid to the working temperature for a period of time results in a reduction of the thermal energy stored in the graphite body to a level which ceases to be adequate for heating the working fluid to the working temperature, residual thermal energy in the graphite body may be used to heat the working fluid to a maintenance temperature and circulated to maintain conditions within the working fluid circuit.
The working fluid may be water/steam and the water/steam may be under sufficient pressure so that when it is heated in the heat exchanger embedded in the graphite body it becomes supercritical.
The working fluid at the intermediate temperature from the first heating apparatus may be saturated steam and when the working fluid is heated to a temperature less than the intermediate temperature it may be hot water.
The working fluid may also be carbon dioxide which when at the working temperature is supercritical.
In a third aspect the present invention provides a process for superheating steam, comprising:
Heating the graphite body using solar radiation energy (insolation),
Embodiments of the present process may ensure consistent delivery of high temperature superheated steam generated from insolation and manages the risk of damage to heat exchanger tubes by using graphite as a medium to intermediate the high solar heat flux and the heat exchanger tubes (Superheater Device) as well as provide thermal storage. In this way the potential for damage to the heat exchanger tubes due to overheating from peak solar flux may be eliminated.
The heat transfer rate between a graphite body heated by solar flux and a heat exchanger tube is controlled to be lower than the heat transfer rate if a heat exchanger tube were directly heated by solar heat flux without graphite intermediation. This is because embedding the tube in the graphite ensures that the temperature on the outer wall of the heat exchanger tube is lower than it would be if the tube were directly heated.
Embodiments of the proposed process incorporate the relationship between the amount of graphite mass and the surface area of heat exchanger as this relationship affects both the rate at which the solar heat flux is transferred to the heat exchanger tube; and the amount of thermal storage. The range of heat exchanger surface area to graphite mass best suited to the Superheater Device is from 0.60 m2 to 20 m2 of surface area of heat exchanger tube per tonne of graphite in the graphite body. This range ensures that under all levels of concentration of solar heat flux that could be directed at the Superheater Device (which can vary depending on the time of day, season and concentration ratio applied by the solar mirror or heliostat field) the heat exchanger tube will always be able to superheat steam without risk of over temperature damage to the heat exchanger tube. If the Superheater Device is designed to perform mainly a superheater role, then the surface area of heat exchanger tube per tonne of graphite will be closer to 20 m2. If the Superheater Device is designed to perform mainly a storage role, then the surface area of heat exchanger tube per tonne of graphite will be closer to 0.60 m2.
The relationship between the solar energy concentrated on the graphite mass and the mass of graphite in the graphite body affects the rate of heat transfer into the graphite body by insolation and thus affects the total heat accumulated for storage or extraction by the heat exchanger. The level of solar energy concentrated on the graphite body, may be in the range of 20 to 2000 kW per tonne of graphite. This range can allow the Superheater Device to be designed to balance solar energy between direct superheating of steam and thermal storage for later use. If the Superheater Device is designed to perform mainly at a low extraction rate with no little or heat storage, then the solar energy concentrated per tonne of graphite will preferably be closer to a lower limit. If the Superheater Device is designed to perform mainly at a high extraction rate with a high level of heat storage, then the solar energy concentrated per tonne of graphite will be closer to a higher limit. The described embodiment enables a method of seamlessly transitioning the Superheater Device from functioning as a solar superheater to a solar once-through boiler when insolation is interrupted, such as caused by cloud cover, then back to a superheater when the cloud cover passes.
When the Superheater Device is functioning as a superheater, it may receive from the Evaporator Device low temperature saturated steam. When it is acting as a once-through boiler it may receive hot water.
The evaporation, that heats water to generate saturated steam prior to superheating, may be performed using any suitable non-graphite based apparatus either solar or non-solar powered.
Preferred embodiments provide a method of using the graphite to absorb and store peak solar fluxes so that energy dumping is minimized or eliminated. This occurs when the heat transfer rate from the high solar flux is greater than the heat transfer rate of the fluid within the heat exchanger tube. Thus the heat transfer rate differential is absorbed within the graphite and stored to minimize or eliminate energy dumping.
Preferred embodiments also provide a method of managing heat transfer to heat exchanger tubes from a solar source without regard to the level of insolation or requirement to regularly manage the solar flux from the solar mirror field as is the case with other direct steam CSP technologies.
An example of the invention will now be described with reference to the accompanying drawing,
Referring to
The first heating apparatus 16 uses renewable or waste energy to heat the working fluid to the intermediate temperature. Several examples of such heating apparatus are shown diagrammatically in
For simplicity the following description is provided using water/steam as the working fluid, however it will be appreciated that other working fluids such as super-critical CO2 may also be used. Referring first to
With a solar powered Evaporator Device 16, the evaporation phase may be conducted by passing the water through a heat exchanger tube 24 (see
The Evaporator Device 16 can be a linear heat exchanger tube 24 laterally arranged and heated by lateral solar reflectors 23, for instance a linear Fresnel or light-weight parabolic trough; or a nest of heat exchanger tubes on top of a tower heated by an array of solar reflectors or heliostats (not illustrated). It could also be a non-solar device such as conventional fossil-fueled boilers, waste heat recovery devices, geothermal or from other renewable or waste energy sources (examples of which are described with reference to
During evaporation, the feed water changes phase into vapor, after which, it is then superheated to generate superheated steam by a Superheater Device 12. This change in state from liquid to vapor dramatically reduces the rate of heat transfer between the heat exchanger tubes and the steam within the heat exchanger tubes. When superheating is performed by insolation of the heat exchanger tubes directly, the risk of over temperature damage to the heat exchanger tubes significantly increases because of the drastically reduced heat transfer rate between the heat exchanger tube and the steam within the tube. When direct insolation of the heat exchanger tubes is not managed effectively during peak insolation periods, overheating of the heat exchanger tubes may result.
To overcome this problem, the heat exchanger tubes 32 of the Superheater Device 12 are embedded in graphite 31, so the solar flux 33 is decoupled from the heat exchanger tube by the graphite body 31. The heat transfer from graphite 31 to heat exchanger tube 32 is uniformly distributed across the whole circumference of the heat exchanger tube and is better matched to the heat transfer from the heat exchanger tube to the steam flowing within the heat exchanger tube 32. The level of solar energy concentrated on the graphite body, may be in the range of 20 to 2000 kW per tonne of graphite.
The embedded heat exchanger tube 32 is surrounded and in contact with the graphite 31. The specification of the graphite body 31 and the design of the interface with the heat exchanger tubes have tailored heat transfer characteristics which ensures a controlled flow of heat to the entire circumference of the heat exchanger tube. This intermediates the high heat flux from the solar mirror field 13 and manages any rapid and peaky variations in heat flux, for instance as a consequence of passing cloud cover.
The output of the Superheater Device 12 is generally fed to a steam turbine generator 11 to produce electrical energy or to an industrial steam application. A steam turbine generator driven with saturated steam typically only produces half the electrical output as a turbine driven with steam superheated beyond the point of saturation by a further 200° C. in temperature.
The temperature of the superheated steam may be in the range from saturation point (for example, 120° C. at 1 barG to 374° C. at 219 barG) to 700° C. In energy contribution terms, the feed water pre-heater/evaporation phase is contributing up to 85% of the enthalpy to the steam but the value of steam (due to lower steam turbine generator efficiency) at low temperature is much lower than superheated steam (due to the higher steam turbine generator efficiency). As a result of superheating steam, the value of the steam is doubled while providing only 15% of the enthalpy contribution.
Therefore the relationship of the energy contributions from the Superheater Device 12 when compared to the feed water pre-heater/evaporation phase (first heating apparatus 16) will range from 10% to 25%.
Steam turbine generator efficiency is not only affected by steam temperature. Steam pressure is also a significant factor, as well as the delivered range of steam temperature and pressure at the inlet. The narrower the range of steam temperature and pressure delivered to the steam turbine generator, the higher the steam turbine generator efficiency.
In the event of solar interruption, for instance due to incoming cloud cover or waning solar energy in late afternoon, the Evaporator Device 16 will not be able to maintain saturated steam output, but will deliver hot water. The Superheater Device 12 will draw from its thermal storage (graphite body 31) and as a result of the ratio of surface area of heat exchanger tube 32 to the graphite mass of the graphite body 31, will seamlessly transition to operate in a once-through boiler mode, which still produces superheated steam for the turbine 11 from hot water rather than saturated steam.
When the solar interruption passes, the Evaporator Device 16 will return from producing hot water to again producing saturated steam, and the Superheater Device 12 then transitions back from functioning as a once-through boiler to a superheater.
The Superheater Device 12 cycles its mode of operation between superheating, and evaporating/superheating. The in-built thermal storage of the superheater ensures it is able to maintain steam conditions to the steam turbine generator throughout the solar interruption within specified steam conditions.
The Superheater Device 12 is then designed to maintain the steam temperature and pressure to specified conditions to the inlet of the relevant steam turbine generator. This contrasts with direct steam CSP plants without thermal storage capacity, where the steam turbine generator will operate at reduced efficiency when insolation is interrupted and subsequently trip as steam conditions fall outside the specified temperature and pressure range, interrupting power generation. Typically the plant will need to go through a lengthy start-up procedure before recommencing electricity generation.
An additional process can begin after the Superheater Device 12 has exhausted sufficient thermal storage such that it can no longer maintain steam turbine quality superheated steam. Low flow low pressure steam can continue to be generated to maintain sufficient temperature in the CSP plant throughout the night to enable faster start-up the following morning and to prevent the system from drying up and taking in air which causes corrosion within the system. In this mode whilst there is not sufficient heat retained in the thermal storage to maintain superheated steam, there is enough stored heat to maintain low quality steam for this additional process.
Although the invention has been exemplified with reference to a particular embodiment, it should be appreciated that it may be embodied in many other forms and variants. For instance, the superheater device may receive saturated or low superheated steam directly or indirectly from the evaporation stage. For example, it may receive steam discharged from a steam turbine and reheat it to be fed back to the intermediate or low pressure stage of the steam turbine.
An embodiment of the invention has been described with reference to superheating steam to a level below the supercritical point, but can be applied to superheating steam that is under sufficient pressure so that when heated it becomes supercritical.
An embodiment of the invention has been described with reference to water/steam as the working fluid. This process can equally apply to the use of other fluids, for example carbon dioxide as the working fluid. In this case, the turbine generator would be powered by high temperature supercritical carbon dioxide heated as described above by the
Superheater Device 12. Carbon dioxide at a pressure of 6 barG becomes supercritical at a temperature of 31° C. As with steam turbine generators, supercritical carbon dioxide turbine generators become more efficient the higher the temperature and pressure, ideally greater than 500° C. and 200 barG, although others are designed to operate at lower temperatures and pressures.
An embodiment of the invention describes a method of integrating the Superheater Device 12 to an Evaporator Device 16 which is powered by a waste heat recovery process or geothermal resources. There are many examples of waste heat recovery steam generators that can produce low to medium temperature steam, steam just above the saturation point for the relevant pressure. With this form of saturated steam sourced from waste heat of another process, the Superheater Device can generate superheated steam and due to the storage capability of the graphite mass, provide this superheating capacity for much longer periods of the day than traditional CSP plants, and potentially for 24 hours per day.
This process is similar when the saturated steam source has a geothermal origin.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2012900930 | Mar 2012 | AU | national |
| 2012901857 | May 2012 | AU | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/AU2013/000223 | 3/7/2013 | WO | 00 |
