This invention relates to the field of transport of cryogenic fluids by ships and more particularly to the field of the transfer of cryogenic fluids from a floating vessel into a pipeline submerged in the sea
Liquified Natural Gas (LNG) is a hydrocarbon mixture comprised primarily of methane, but may also contain some lower hydrocarbons typically c2 through c4. This liquid, in the existing technology, is transported at sea by special tanker vessels at near atmospheric pressure and a temperature of approximately −161 degrees C.
These tanker vessels typically discharge their cargo at in-harbor ordinary piers into storage tanks. The gas is then typically dispatched from the storage tanks via pipeline to consumers at ambient temperature and moderately high pressure. The distribution pipeline pressure is usually in the range of 5 MPa to 12 MPa Before being dispatched, the gas must be heated.
The heating is ordinarily done in heat exchangers using sea water if this is available at a suitable temperature or by using some of the gas to heat the fluid used in the heat exchangers. If the latter method is the only method used to heat the gas, then the consumption of gas for this purpose is ordinarily around 1.25% of the throughput.
Taking a throughput of 20,000 tonnes/day and assuming that the value of the delivered gas is US$200 per tonne, this method of heating the gas consumes 250 tonnes gas per day at a cost of US$50,000 per day.
To heat the LNG from −161 degrees C. to ambient at the pipeline pressure requires about 600 kJ/kg of gas. It can be assumed that seawater is used for heating the gas. This water may be cooled in the equipment to no less than 2 degrees C. The heat capacity of water is approximately 4 Kj/kg/deg C. Taking an inlet water temperature of 8 degrees C., then each kg of water may deliver (8−2)*4=24 kJ of heating. Thus in this example, 600/24=25 kg of water is required to heat one kg of LNG. In the example of delivering 20,000 tonnes LNG per day 500,000 tonnes/day of seawater is required for purposes of heating the LNG. This requires a supply of approximately 6 m3/second. This is a major quantity which would typically require large intake works and discharge works.
Note, that if the sea water temperature is to be lower at some part of the year, for example 4 degrees C., the amount of water required would be 3 times as large or 18 m3/second. The capital and operating costs of a system heated by sea water depend strongly on local conditions and could exceed, by a considerable margin, the corresponding costs of using the gas itself to provide the energy for heating.
An alternative method for discharging gas from a cryogenic tanker consists of using equipment aboard the tanker to raise the pressure of the liquid to the pressure of the subsea pipeline and then heat the gas to a temperature of at least −40 deg C. or more typically to a range between −10 deg C. and 0 deg C. In this case the tanker may in some cases be able to deliver the gas to an existing infrastructure of submarine gas pipelines, such as for example exists in the Gulf of Mexico or the North Sea.
In the alternative method, the cryogenic tanker acts as the storage in the system and delivers gas as demanded at any one time.
Each tanker must in the alternative method have the equipment to raise the pressure of the liquid to pipeline pressure and the equipment to heat the gas to near ambient temperature. A typical discharge rate is 0.5 m3/sec of LNG and a typical pipeline pressure is 10 MPa The theoretical pumping power is thus 5 MW. Allowing for all losses, a practical power supply would need a capacity of around 7 MW. Thus each tanker must be equipped with a pumping plant with a power on the order of 5 to 10 MW. Consequently it is very costly to equip each vessel with this capability.
The alternative method is particularly suited for use with single point moorings such as for example featured in U.S. Pat. Nos. 5,305,703 and 5,380,229. This method also alleviates present concerns about the security and danger of fires and explosions originating from a burning and disintegrating cryogenic tanker, because the discharge facilities may be placed far from the shore distant from population centers.
The present invention is directed to the alternative method of discharging cryogenic fluids such as LNG into subsea pipelines for delivery to a pipeline network operated at near ambient temperature.
Very large cost savings are achieved by not equipping the tankers with the high pressure pumps and the heating equipment for heating the cryogenic fluid to near ambient temperature. This invention teaches the placement of this equipment on the seabed and to use the ambient heat capacity of the seawater to heat the cryogenic fluid.
The present invention relates to the discharge of LNG at relatively low pressure within the typical capability of currently existing cryogenic tankers into a subsea system for direct delivery at near ambient temperature to a gas pipeline system operated at normal operating pressures.
The normal operating pressures of the gas pipelines may be in the range of 5 to 20 MPa.
The discharge pressure of the cryogenic tanker may be in the range of 0.5 to 1 MPa. Pumps provided at the discharge point on the seabed or at a nearby platform remote from the tanker boost the pressure of the LNG to the pipeline pressure. These pumps feed the LNG into a subsea heat exchanger of special design that interacts directly with the ocean and thereby efficiently and inexpensively heats the LNG to near ambient temperature.
The LNG may be maintained at all times above the critical pressure during the heating process such that it is converted to pressurized gas at near ambient temperature without changing into two phases at any time during the heating process.
The cryogenic fluid that is discharged from tanker 10 is stored in tank 20. The cryogenic fluid is delivered from tank 20 to the customer delivery gas pipeline 25 via suction pipe 21, booster pump 22, pipe 23, and heater 24. The gas leaving heater 24 would be delivered at the back pressure of pipeline 25, typically 5 to 12 MPa and at a temperature near ambient, typically −10 to 0 deg C. A main advantage of the system illustrated by
The application of any specific mooring may be determined by capital and operating costs at the specific site. Regardless of the type of mooring used, the function is the same. In this case the pumps 22 pressurizing the discharged fluid and the heater 24 are located on the tanker 10. For the sake of clarity the pumps 22 are shown on top of the cargo tanks, although the pumps may be located within the hull of vessel 10 or on deck. The LNG is sent through a booster pump 22 boosting the pressure of the LNG to a pressure above the pressure in the delivery pipeline 25. The pump 22 delivers the LNG to the heater 24 where the gas is heated to near ambient temperature.
A special problem may exist at the time of start up of the process. LNG ordinarily has a boiling temperature of −161 deg C. at atmospheric pressure. At 500 kPa the boiling temperature is approximately −140 deg C. It may be anticipated that the riser 40 is at ambient temperature before commencing delivery of LNG to pump 42 on the seabed. Prior to start-up of the pumping, riser 40 may contain natural gas under pressure. The first step in the start-up is to bleed off the pressure in riser 40 through back flow in pipe 27 to a vent on vessel 10. The riser 40 is now filled with ambient temperature gas at near atmospheric pressure. The riser 42 may, for example, be a metal pipe with a diameter of 500 mm. The gas at atmospheric pressure and ambient temperature has an approximate weight of 0.8 kg/m3. The pipe between the delivery pump in vessel 10 and the booster pump 42 may comprise a lineal length of 300 m. Thus the volumetric capacity of the pipe is n/4*0.5ˆ2*300=120 m3, thus containing approximately 0.8*120=100 kg of gas in vapor form. The heat of vaporization of LNG is approximately 550 kJ/kg and cp is approximately 3 kJ/kg. Assuming a cool down of approximately 175 degrees and liquefaction the energy required is 550+3*175=1075 kJ/kg or 108,000 kJ for the 100 kg vapor content of the riser 42. The specific heat of the LNG is approximately 3 kJ/kg/deg C. Assume that the LNG is heated 10 deg C. then 108,000/10/3=3600 kg is required to entrain the content of riser 40 into the LNG. The density of the LNG is approximately 400 kg/m3. Consequently 3600/400=9 m3 of LNG being heated 10 degrees is needed to entrain the gas in riser 40 into the LNG. The cross sectional area of the pipe in riser 40 in this example is approximately 0.19 m2. Therefore the content of approximately 9/0.19=50 m of pipe is needed to provide the energy for entrainment of the gas in the riser 40 into the initial delivery of LNG to pump 42. This is unlikely to work because the heat cannot be evenly distributed in the initial slug of LNG. If it does work it would subject pump 42 to thermal shock and to extreme pressure fluctuations on the suction side during start-up.
An alternative arrangement for starting the delivery of LNG from vessel 10 to the delivery pipeline 25 may be to equip riser 40 with two parallel fluid paths and manifold these fluid paths into the piping of vessel 10 such that during startup LNG can be circulated by vessel 10 through the two fluid paths in riser 40. This would solve the problem of extreme pressure transients being experienced in the suction 44 of pump 42 during startup, however, the pump 42 would still experience thermal shock being cooled from ambient to approximately −160 deg C. during each start-up. Conventional pumps would need frequent replacement and would be unreliable if subjected to the service conditions described above.
Pump 42 is contained within a cryogenic insulated pressure vessel 50. Pump 42 is not connected directly to suction pipe 44 but rather takes suction at 56 through suction pipe 51 within the cryogenic pressure vessel 50. Suction 51 is placed at a low point in cryogenic vessel 50. During normal operations of discharging the ship 10, the cryogenic vessel 50 may be completely filled with liquid, because the capacity of the pumps aboard the vessel 10 may exceed the combined capacities of pumps 42 and 55 removing fluids from cryogenic vessel 50. In addition, the vapor pressure of the LNG transferred may be only slightly above atmospheric about 110 kPa absolute and the discharge pressure of the pumps aboard ship 10 maybe on the order of 500 kPa to 1000 kPa. Cryogenic vessel 50 may be located on the seabed as shown in
Cryogenic vessel 50 is also fitted with a pump 55 taking suction 57 through pipe 58 approximately in the center of cryogenic vessel 50. Pump 55 is of much lower capacity than pump 42, however it is of a type that can pump both liquid phase and vapor phases of the contents of cryogenic vessel 50 and deliver these to the discharge pipe 45. This pump 55 is running whenever the pressure is above 300 kPa or the temperature in cryogenic vessel 50 is above −145 deg C. The starting and stopping is automatically controlled by conventional equipment inside cryogenic vessel 50.
When cargo is discharged from ship 10, pump 55 assists in delivering the cargo to discharge pipe 45. When the pumping from ship 10 stops, the cryogenic vessel 50 and the riser 40 (
Suppose the system is designed to deliver 1,000 tonnes per hours of LNG. This corresponds to 1000/0.44=2300 m3/H=0.63 m3/sec. Suppose the delivery pressure in pipe 45 is 11 Mpa then the theoretical power of pump 52 is 0.63*11=7 Mw. To account for all losses this pump is likely to need a driver with a power of 10 Mw. The cryogenic vessel 50 may be cylindrical with an internal diameter of 5 meters and a length of 30 meters. The volume of this tank 50 is 585 m3. Deducting the volume occupied by the equipment inside the cryogenic tank 50 it may have an effective volume of 550 m3.
Pump 55 may be designed to deliver 0.01 m3/sec. This pump would need a driver with about 150 kW power. The volumetric capacity of the riser system is in the prior example 120 m3. Pump 55 would remove this volume in about 120/0.01=12000 sec=3.33 Hours. In addition pump 55 would remove approximately 50%=0.5*550=275 m3 of the liquid in cryogenic vessel 50 in an additional time of 275/0.01=27500 seconds=7.6 hours. Consequently approximately 11 hours after ship 10 stops delivery will pump 55 take suction within the gas filled volume above the interface 59 of cryogenic vessel 50.
Cryogenic tank 50 has an exterior surface of approximately 600 m2. Suppose that the insulation layer is 100 mm thick and comprised of a material with a heat conductivity of 0.04 w/m/deg C. Thus the heat influx in the tanks is 10*0.04*600=240 w/deg C. Assume a temperature differential of 170 deg C. then the heat influx into tank 50 is 240*170=40,000 w or 40 kW. The heat of evaporation of methane is approximately 550 kJ/kg thus 40/550=0.072 kg/sec evaporates. The density of LNG vapor at −160 deg C. and atmospheric pressure is approximately 120 kg/m3 requiring removal of approximately 0.072/120=0.6 liters per second. This is negligible compared to the capacity of pump 55. When the content of cryogenic vessel 50 is reduced to 50% 11 hours following the discharge of ship 10 the cryogenic vessel 50 contains approximately 275*440=121,000 kg of LNG. The evaporation per hour is 0.072*3600=260 kg/H. To completely evacuate cryogenic vessel 50 due to heat influx from the environment would require 121,000/260=465 hours=19 days.
Cryogenic vessel 50 is fitted with check valves 49 preventing backflow into pipe 44 and check valves 53 preventing backflow from high pressure pipe 45 into the cryogenic vessel 50. Cryogenic vessel 50 would normally also be fitted with a range of items such as, penetrations for electric cables, instrumentation and relief valves, needed for safe operation of the facility.
Start-up is particularly simple and safe with the, arrangement shown in
A note is required on the materials used in the pipe of riser 40. This is subjected to sudden cooling from ambient to −160 deg C. at start-up. Completely restrained structures made from metals such as titanium with a low modulus of elasticity and low coefficient of thermal expansion may withstand temperature changes of 180 deg C. without becoming over stressed, and may consequently be used for this service. Another candidate material is INVAR which has a very low coefficient of thermal expansion.
Vessel 10 would typically have a length around 300 m. Thus the weathervaning circle of vessel 10 may have a diameter close to 700 m. The parallel pipes 60 in heat exchanger 43 may, for example, be deployed in a circle with a diameter of approximately 1000 m, maling each pipe 60 approximately 3000 m long. An approximate calculation of the number of parallel pipes required to heat the LNG e.g. −10 deg C. from the inlet temperature of −161 deg C. may be made considering the heat influx into the pipe from the sea water. The prior example of delivering 1000 tonnes/H is used. It is assumed that the seawater surrounding heater 43 has a temperature of 8 deg C. It may be further assumed that the pipe 60 is of nominal diameter of 250 mm. It will later be shown that the heat influx through the pipe in these circumstances may be on the average 4 kW/m. Thus each pipe can provide 12000 kW of heating. Each kg of LNG requires heating of approximately 600 kJ. The mass flow in each pipe 60 is then 12000/600=20 kg/second=72,000 kg/H. The heating of 1000 tonnes/H thus requires 1000/72=14 pipes 60 in parallel. Each pipe is in this example 3000 m long. With the pipe, thus dimensioned, the resulting diameter of the circular heat exchanger 43 approximately 1000 m. As a result, the heat exchanger 43 is placed close to tanker 10 yet at a safe distance such that objects dropped from tanker 10 cannot impact the heat exchanger. Yet the heat exchanger 43 is close to tanker 10 making it a simple matter to maintain a security zone around the mooring and the heat exchanger.
The heat exchanger pipe 60 may be insulated by ice 66 forming on the outside of pipe 60 for almost the entire length between manifolds 61 and 62 shown on
Seawater flowing past the ice having a temperature of 8 deg C. and flowing with a velocity of 0.1 m/sec will transfer 3.7 kW/m2 through the exterior surface of ice 66. It may be assumed that pipe 60 is filled with LNG at a temperature of −160 deg C. It may further be assumed that pipe 60 is nominally a 250 mm pipe with outside diameter of 273 mm, then ice 66 of a thickness of 106 mm will form limiting the heat transfer to the fluid inside pipe 60 to 5.58 kW/m. It may also be assumed that the prior example of a mass flow of 20 kg/sec and a heat capacity of 4 kJ/kg/deg C., then the increase in temperature in each meter of pipe 60 is 5.58/20/4=0.07 deg C. Thus the temperature rises 1 deg C. in the interior of pipe 60 as one moves 14 meters downstream near the upstream end. At the downstream end of pipe 60 the content may have reached a temperature of −20 deg C. In this case ice 66 of thickness 9 mm will form. The heat transfer rate is 3.46 kW. The content has a heat capacity of 5 kl/kg/deg C. at this temperature. The increase in temperature per m of pipe 60 is at this end 3.46/20/5=0.035 deg C. Thus, at the downstream end, a temperature increase of one deg C. may require a length of 29 m of pipe 60 at the conditions cited in the above example in this paragraph.
The heat exchanger pipes 60 may be deployed in numerous patterns. Assume that the pipes 60 on
Pipe 80 serves in this case the dual role of heat exchanger pipe and delivery pipe to shore. Pipe 80 is shown on
In the first embodiment of the invention, vessels trying to anchor above the heat exchanger 43 as shown in
In
The entrainment of this gas in the LNG contained within pumping assembly 96 requires cooling at approximately 1075 kJ/kg or 400*1075=430,000 kJ. The LNG contained within pumping assembly 96 has a heat capacity of approximately 3 kJ/kg/deg C. Suppose that the allowable rise in temperature of the LNG contained within pumping assembly 96 is arbitrarily limited to 3 deg C. then pumping assembly 96 must contain 430,000/(3*3)=47,000 kg of LNG at the initiation of pumping by tanker 10. Assuming that the pumping assembly 96 is similar to the vessel 50 in
Pumping assembly 96 may be fitted with a refrigeration plant that re-liquefies any evaporated natural gas and returns this liquid to assembly 96. In this event there is no limit to the time between departure of one vessel 10 and the arrival of the next vessel 10. At initial start-up and in the event that insufficient LNG is present in assembly 96 to permit immediate initiation of liquid transfer, cool down will be performed by pumping cold vapor from vessel 10 to pumping assembly 96 through riser 40 and pipe 100. This vapor will be vented at assembly 96. Once a steady state temperature in the system is achieved, final cool down will be performed by slowly adding liquid LNG to the cold vapor being pumped from vessel 10 to pumping assembly 96. Once a small amount of LNG is present in vessel 96 pumping may commence as described above.
The pumping assembly 96 delivers LNG to pipe 97 at a pressure that is higher than both the critical pressure of the LNG gas mixture and the pressure in delivery pipeline 99. Pipe 97 is in fluid connection with manifold 105, which in turn is in fluid connection with each of the heat exchanger pipes 98. Manifold 105 may include control valves that permit regulation of the distribution of flow between the heat exchanger pipes 98 and indeed to selectively take heat exchanger pipes 98 out of service by isolating them from manifold 105. Heat exchanger pipes 98 are in
Pipes 98 are usually of dimensions that they are buoyant in seawater. The pipes 98 are supported within enclosure by an arrangement that permits thermal contraction and expansion and which restrain the pipes 98 sufficiently to resist current, wave, and buoyancy forces and which prevent the pipes 98 impacting each other.
Valve 141 is remotely operated by conventional systems. When an LNG tanker is present and transfers LNG valve 141 is closed and the liquid surface 130 is at the top if tank 114. In this condition tank 114 would normally be pressurized with a pressure close to the discharge pressure of pumps in the LNG tanker. This pressure would ordinarily be on the order of 300 to 1000 kPa. Pump 120 removes LNG via inlet 121 from tank 114 and discharges into pipe 97 via check valve 123.
When the flow in pipe 100 stops following the discharge of the LNG tanker, pump 120 may be operated for a short while until liquid surface 130 is drawn down below inlet 140 to the flare 142. When pump 120 is then stopped, valve 141 is opened and flare 142 lit.
The heat exchanger pipes 98 are anchored to anchors 151 at the seabed 104. The anchors 151 are shown as heavy spheres partly embedded in the seabed 104. However, virtually, all types of anchors 151 may be used, including stake piles. The lower level 160 of pipes 98 are tied by nearly vertical chains 150 to the anchor 151. The next level 161 of pipes 98 is tied to level 160 by nearly vertical chains 154 and level 162 is tied to level 161 by nearly vertical chains 155.
For most practical cases, the pipes 98 are buoyant and would tension the chains 150, 154, and 155. However, additional buoyancy may be provided by vertical chains 156 and buoys 152. The chains 150, 154, 155, and 156 are structurally connected to the pipes 98 by collars 153. The collars 153 may provide electrical insulation between chains 150, 154, 155, and 156 and the pipes 98 to avoid galvanic corrosion by conventional designs. The chains 150, 154, 155, and 156 and collars 153 may be made from materials such as titanium, stainless steel or aluminum that can tolerate the extremely low temperature in pipe 98 without becoming brittle. Alternatively, the collars 153 may be designed to provide both thermal and electrical insulation by many possible designs between the pipes 98 and chains 150, 154, 155, and 156. Ropes from synthetic or natural materials may also be used in lieu of chain for chains 150, 154, 155, and 156.
The heat exchanger 90 is acting like an inverted pendulum supported by the anchors 151 and chains 150, 154, and 155. It will therefore move when subjected to horizontal forces from current and wave action. It is important that the protective structure 92 be removed sufficiently from pipes 98 that impacts due to the motion of pipes 98 do not occur. In most ordinary cases, a distance of a few meters is sufficient. Buoys 152 and pipes 98 are placed sufficiently below the water surface 103 to prevent or hinder the buoys 152 or the pipe 98 from piercing the surface 103 even in the event of extreme wave action. If the surface 103 is pierced, one or more of the chains 156, 155, 154, and 150 may momentarily become slack and then break when tensioned in an impact following the rise of water surface 103.
Combinations of the second embodiment and either the first or third embodiments may also be made in which the offshore heat exchanger only partly heats the gas and the delivery pipe to shore also partly heats the gas. This may be supplemented with a conventional heater on shore. In this arrangement the offshore heat exchanger then does not need to be sized for the peak delivery rate. An optimal balance would ordinarily exist in which the onshore heater is only used when the seawater is cold and when the demand for gas is high. It should also be noted that the construction of the offshore heaters shown in
In the foregoing specification, the invention has been described with reference to specific exemplary embodiments thereof. It will, however, be evident that various modifications and changes may be made thereunto without departing from the broader spirit of the invention as set forth in the appended claims. The specification and drawings are accordingly to be regarded in an illustrative rather than a restrictive sense.
This application claims priority of U.S. Provisional Patent Application No. 60/453,094, filed Mar. 6, 2003 and U.S. Provisional Patent Application No. 60/507,174, filed Sep. 30, 2003, both of which are incorporated herein by reference.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/US04/06944 | 3/5/2004 | WO | 12/21/2006 |
Number | Date | Country | |
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60453094 | Mar 2003 | US | |
60507174 | Sep 2003 | US |