Ceramic-to-metal turbine shaft attachment

Information

  • Patent Grant
  • 9051873
  • Patent Number
    9,051,873
  • Date Filed
    Monday, May 21, 2012
    12 years ago
  • Date Issued
    Tuesday, June 9, 2015
    9 years ago
Abstract
A metallic-ceramic joint for a turbo-compressor spool is disclosed. A temperature-limited joint is moved from outside the bearings to between the bearings and near the center of the shaft joining the turbine and compressor. This placement can lower the temperature at and around the joint and reduces the sharp gradient (and associated thermal stress) naturally occurring between the turbine rotor and the cooler joint. The bearing closest to the compressor can be an oil bearing and the bearing closest to the turbine an air bearing. The bearing closest to the compressor and the bearing closest to the turbine can both be an oil bearing. The bearing closest to the compressor and the bearing closest to the turbine can both be an air bearing. Moving the metallic-ceramic joint between the bearings can provide sufficient isolation to enable the all-air bearing solution.
Description
FIELD

This disclosure relates generally to the field of vehicle propulsion and power generation and more specifically to an apparatus attaching a ceramic turbine rotor to a metal shaft.


BACKGROUND

There is a growing requirement for alternate fuels for vehicle propulsion and power generation. These include fuels such as natural gas, bio-diesel, ethanol, butanol, hydrogen and the like. Means of utilizing fuels needs to be accomplished more efficiently and with substantially lower carbon dioxide emissions and other air pollutants such as NOxs.


The gas turbine or Brayton cycle power plant has demonstrated many attractive features which make it a candidate for advanced vehicular propulsion and power generation. Gas turbine engines have the advantage of being highly fuel flexible and fuel tolerant. Additionally, these engines burn fuel at a lower temperature than reciprocating engines so produce substantially less NOx per mass of fuel burned.


The efficiency of gas turbine engines can be improved and engine size can be further reduced by increasing the pressure and temperature developed in the combustor while still remaining well below the temperature threshold of significant NOx production. This can be done using a conventional metallic combustor or a thermal reactor to extract energy from the fuel. As combustor temperature and pressure are raised, new requirements are generated in other components, such as the recuperator and compressor-turbine spools.


In a high efficiency gas turbine engine, the turbine adjacent to the combustor may have a ceramic rotor or it may be an all-ceramic turbine (volute, rotor, rotor shroud). The ceramic rotor is typically attached to a shaft which in turn is usually attached to a compressor which is comprised of a metallic rotor because the compressor blades see much lower temperatures than the turbine blades. The ceramic-to-metal attachment joint represents one of an important feature that, if not designed correctly, can limit the allowable operating temperature of the turbine rotor especially in small turbo-compressor spools such as used in turbo-chargers and microturbines. Most prior art joints are limited to operating temperatures below 800° K. The objective of achieving increased efficiency is pushing the rotor temperatures to levels approaching 1,400° K and, in the future, higher. In the prior art, this joint is typically located close to the turbine rotor, thereby requiring aggressive cooling to maintain the allowable temperature at and around the joint. The steep thermal gradient also creates an area of elevated thermal stress at and around the joint.


There remains a need for a joint design that will allow increased combustor temperatures which, in turn, can improve overall engine efficiency and reduce engine size while maintaining very low levels of NOx production.


SUMMARY

These and other needs are addressed by the various embodiments and configurations of the present disclosure which are directed generally to gas turbine engine systems and specifically to moving the temperature-limited joint to a location between the bearings near the center of the shaft joining the turbine and compressor. This placement lowers the temperature at and around the joint and reduces the sharp gradient (and associated thermal stress) which naturally occurs between the turbine rotor and the cooler joint. This requires a large outside diameter bearing on the turbine side so that it can be assembled. It is also anticipated that the ceramic turbine stub shaft needs to be relatively large in diameter relative to the steel shaft to have the proper stiffness.


In a first configuration the bearing closest to the compressor is an oil bearing and the bearing closest to the turbine is an air bearing.


In another configuration the bearing closest to the compressor is an oil bearing and the bearing closest to the turbine is also an oil bearing.


In yet another configuration the bearing closest to the compressor is an air bearing and the bearing closest to the turbine is also an air bearing. This all-air bearing configuration for the ceramic turbine may be difficult, since air is not as good as oil for cooling. Moving the metallic-ceramic joint between the bearings may provide sufficient isolation to enable the all-air bearing solution.


In various configurations, one or more of the following elements are employed:


1. Relocation of the metallic-ceramic joint substantially further away from the hot turbine gases to substantially reduce the thermal gradient and the thermal stress on the joint.


2. Relocating the joint on the other side of the bearing closest to the turbine.


3. Increasing the diameter of the ceramic shaft coming off the ceramic rotor and using a short, smooth transition down to the diameter of the metallic shaft.


4. In place of the ceramic shaft being inserted into a counterbore in the metallic shaft, the diameter of the ceramic and metallic shaft are the same. Brazing and the use of a connecting sleeve are used to form a strong joint with the required stiffness.


5. Relocating the joint so that either an all-oil bearing; an all-air-bearing; or a combination air and oil bearing system can be used.


In one embodiment, an engine is comprised of a plurality of turbo-compressor spool assemblies, each turbo-compressor spool assembly comprising a compressor and a turbine attached by a common shaft and a first of the turbo-compressor spool assemblies is in fluid communication with a second of the turbo-compressor spool assemblies, at least one of the common shafts of a selected turbo-compressor spool assembly comprising a metallic compressor rotor and a ceramic turbine rotor connected by a metallic-to-ceramic attachment joint and a first bearing being positioned adjacent to the metallic compressor rotor and a second bearing adjacent to the ceramic turbine rotor; a free power turbine driven by a gas flow output by at least one of the turbo-compressor assemblies; and a combustor operable to combust a fuel and a gas output by one of the plurality of turbo-compressor spool assemblies, wherein: when the engine is in operation, the ceramic turbine rotor of the selected turbo-compressor spool assembly operates in a no-failure regime of the ceramic material; the ceramic-to-metallic attachment joint is located on the common shaft of the selected turbo-compressor spool assembly to be in a no-failure regime of the ceramic material, the location of the metallic-to-ceramic attachment joint being positioned between the first and second bearings on the common shaft, and when the engine is in operation, the metallic-to-ceramic attachment joint operates at a temperature of no more than about 800° K.


In another embodiment, an engine is comprised of a plurality of turbo-compressor spool assemblies, each turbo-compressor spool assembly comprising a compressor and a turbine attached by a common shaft and a first of the turbo-compressor spool assemblies is in fluid communication with a second of the turbo-compressor spool assemblies; a free power turbine driven by a gas flow output by at least one of the turbo-compressor assemblies; and a combustor operable to combust a fuel and a gas output by one of the plurality of turbo-compressor spool assemblies, wherein a selected turbo-compressor spool assembly comprises a metallic compressor rotor and a ceramic turbine rotor connected by a metallic-to-ceramic attachment joint, wherein a first and second bearings are located along a common shaft of the selected turbo-compressor spool assembly, and wherein at least one of the following is true: (i) a turbine rotor of a selected turbo-compressor spool assembly operates in a no-failure regime of the ceramic material and the metallic-to-ceramic attachment joint is located to be in a no-failure regime of the ceramic material; (ii) the metallic-to-ceramic attachment joint is located between the first and second bearings; (iii) a ceramic portion of the common shaft has a length of at least about 40% of a length of the shaft; and (iv) respective diameters of the ceramic portion and a metallic portion of the common shaft are substantially the same in the vicinity of the metallic-to-ceramic attachment joint.


A method is disclosed, comprising providing a gas turbine engine, the gas turbine engine comprising a turbo-compressor spool assembly, the turbo-compressor spool assembly comprising a compressor and a turbine attached by a common shaft, a free power turbine driven by a gas flow output by the turbo-compressor assembly, and a combustor operable to combust a fuel and a gas output by the turbo-compressor spool assembly, the compressor comprising a metallic compressor rotor and the turbine comprising a ceramic turbine rotor connected by a metallic-to-ceramic attachment joint; and when the gas turbine engine is in operation, maintaining the turbine rotor and the metallic-to-ceramic attachment joint in a no-failure regime of the ceramic material.


The following definitions are used herein:


As used herein, “at least one”, “one or more”, and “and/or” are open-ended expressions that are both conjunctive and disjunctive in operation. For example, each of the expressions “at least one of A, B and C”, “at least one of A, B, or C”, “one or more of A, B, and C”, “one or more of A, B, or C” and “A, B, and/or C” means A alone, B alone, C alone, A and B together, A and C together, B and C together, or A, B and C together.


A bellows is a flexible or deformable, expandable and/or contractable, container or enclosure. A bellows is typically a container which is deformable in such a way as to alter its volume. A bellows can refer to a device for delivering pressurized air in a controlled quantity to a controlled location.


A ceramic is an inorganic, nonmetallic solid prepared by the action of heating and cooling. Ceramic materials may have a crystalline or partly crystalline structure, or may be amorphous (e.g., a glass).


An engine is a prime mover and refers to any device that uses energy to develop mechanical power, such as motion in some other machine. Examples are diesel engines, gas turbine engines, microturbines, Stirling engines and spark ignition engines.


A free power turbine as used herein is a turbine which is driven by a gas flow and whose rotary power is the principal mechanical output power shaft. A free power turbine is not connected to a compressor in the gasifier section, although the free power turbine may be in the gasifier section of the gas turbine engine. A power turbine may also be connected to a compressor in the gasifier section in addition to providing rotary power to an output power shaft.


A gas turbine engine as used herein may also be referred to as a turbine engine or microturbine engine. A microturbine is commonly a sub category under the class of prime movers called gas turbines and is typically a gas turbine with an output power in the approximate range of about a few kilowatts to about 700 kilowatts. A turbine or gas turbine engine is commonly used to describe engines with output power in the range above about 700 kilowatts. As can be appreciated, a gas turbine engine can be a microturbine since the engines may be similar in architecture but differing in output power level. The power level at which a microturbine becomes a turbine engine is arbitrary and the distinction has no meaning as used herein.


A gasifier is a turbine-driven compressor in a gas turbine engine dedicated to compressing air that, once heated, is expanded through a free power turbine to produce


A prime power source refers to any device that uses energy to develop mechanical or electrical power, such as motion in some other machine. Examples are diesel engines, gas turbine engines, microturbines, Stirling engines, spark ignition engines and fuel cells.


A heat exchanger is a device that allows heat energy from a hotter fluid to be transferred to a cooler fluid without the hotter fluid and cooler fluid coming in contact. The two fluids are typically separated from each other by a solid material, such as a metal, that has a high thermal conductivity.


The term means shall be given its broadest possible interpretation in accordance with 35 U.S.C., Section 112, Paragraph 6. Accordingly, a claim incorporating the term “means” shall cover all structures, materials, or acts set forth herein, and all of the equivalents thereof. Further, the structures, materials or acts and the equivalents thereof shall include all those described in the summary of the invention, brief description of the drawings, detailed description, abstract, and claims themselves.


A metallic material is a material containing a metal or a metallic compound. A metal refers commonly to alkali metals, alkaline-earth metals, radioactive and nonradioactive rare earth metals, transition metals, and other metals.


The no-failure regime of a ceramic material, as used herein, refers to the region of a flexural strength versus temperature graph for ceramic materials wherein both the flexural stress and temperature are low enough that the ceramic material has a very low probability of failure and has a lifetime of a very large number of flexural and/or thermal cycles. Operation of the ceramic material in the no-failure regime means that the combination of maximum flexural stress and maximum temperature do not approach a failure limit such as the Weibull strength variability regime, the fast fracture regime, the slow crack growth regime or the creep fracture regime as illustrated in FIG. 3. When the ceramic material approaches or enters any of these failure regimes, then the probability of failure is increased precipitously and the lifetime to failure of the component is reduced precipitously. This applies to ceramic components that are manufactured within their design specifications from ceramic materials that are also within their design specifications. Typically, the no-failure regime of the ceramics used herein exists at operating temperatures of no more than about 1,550° K, more typically of no more than about 1,500° K, and even more typically of no more than about 1,400° K. Common maximum flexural strengths for the no-failure regime of the ceramics used herein are about 250 MPa and more commonly about 175 MPa.


Power density as used herein is power per unit volume (watts per cubic meter).


A recuperator is a heat exchanger dedicated to returning exhaust heat energy from a process back into the process to increase process efficiency. In a gas turbine thermodynamic cycle, heat energy is transferred from the turbine discharge to the combustor inlet gas stream, thereby reducing heating required by fuel to achieve a requisite firing temperature.


Regenerative braking is the same as dynamic braking except the electrical energy generated is captured in an energy storage system for future use.


Specific power as used herein is power per unit mass (watts per kilogram).


Spool refers to a group of turbo machinery components on a common shaft.


A thermal energy storage module is a device that includes either a metallic heat storage element or a ceramic heat storage element with embedded electrically conductive wires. A thermal energy storage module is similar to a heat storage block but is typically smaller in size and energy storage capacity.


A thermal oxidizer is a type of combustor comprised of a matrix material which is typically a ceramic and a large number of channels which are typically circular in cross section. When a fuel-air mixture is passed through the thermal oxidizer, it begins to react as it flows along the channels until it is fully reacted when it exits the thermal oxidizer. A thermal oxidizer is characterized by a smooth combustion process as the flow down the channels is effectively one-dimensional fully developed flow with a marked absence of hot spots.


A thermal reactor, as used herein, is another name for a thermal oxidizer.


A turbine is a rotary machine in which mechanical work is continuously extracted from a moving fluid by expanding the fluid from a higher pressure to a lower pressure. The simplest turbines have one moving part, a rotor assembly, which is a shaft or drum with blades attached. Moving fluid acts on the blades, or the blades react to the flow, so that they move and impart rotational energy to the rotor.


Turbine Inlet Temperature (TIT) as used herein refers to the gas temperature at the outlet of the combustor which is closely connected to the inlet of the high pressure turbine and these are generally taken to be the same temperature.


A turbo-compressor spool assembly as used herein refers to an assembly typically comprised of an outer case, a radial compressor, a radial turbine wherein the radial compressor and radial turbine are attached to a common shaft. The assembly also includes inlet ducting for the compressor, a compressor rotor, a diffuser for the compressor outlet, a volute for incoming flow to the turbine, a turbine rotor and an outlet diffuser for the turbine. The shaft connecting the compressor and turbine includes a bearing system.


A volute is a scroll transition duct which looks like a tuba or a snail shell. Volutes may be used to channel flow gases from one component of a gas turbine to the next. Gases flow through the helical body of the scroll and are redirected into the next component. A key advantage of the scroll is that the device inherently provides a constant flow angle at the inlet and outlet. To date, this type of transition duct has only been successfully used on small engines or turbochargers where the geometrical fabrication issues are less involved.


Weibull statistics are used in characterizing the strength of brittle materials such as most ceramics and relate a series of bending strength measurements to the probability of failure. Weibull statistics include a strength modulus called Weibull modulus.





BRIEF DESCRIPTION OF THE DRAWINGS

The disclosure may take form in various components and arrangements of components, and in various steps and arrangements of steps. The drawings are only for purposes of illustrating the preferred embodiments and are not to be construed as limiting the disclosure. In the drawings, like reference numerals refer to like or analogous components throughout the several views.



FIG. 1 is prior art schematic of the component architecture of a multi-spool gas turbine engine.



FIG. 2 is a line drawing of a gas turbine suitable for long haul trucks. This is prior art.



FIG. 3 is a stress-temperature map showing ceramic failure regimes.



FIG. 4 is a schematic of a prior art turbo-compressor spool showing a metallic compressor rotor and a ceramic turbine rotor.



FIG. 5 is a schematic of a prior art gas turbine compressor/turbine spool comprising a ceramic rotor, volute and shroud.



FIG. 6 shows a general configuration of an air and oil hybrid bearing system with a ceramic-to-metal attachment joint of the present disclosure.



FIG. 7 shows a general configuration of an all-oil bearing system with a ceramic-to-metal attachment joint of the present disclosure.



FIG. 8 shows a general configuration of an all-air bearing system with a ceramic-to-metal attachment joint of the present disclosure.





DETAILED DESCRIPTION

Exemplary Gas Turbine Engine


An exemplary engine is a high efficiency gas turbine engine. It typically has lower NOx emissions, is more fuel flexible and has lower maintenance costs than comparable reciprocating engines. For example, an intercooled recuperated gas turbine engine in the range of about 10 kW to about 750 kW is available with thermal efficiencies above 40%. A schematic of an intercooled, recuperated gas turbine engine is shown in FIG. 1.



FIG. 1 is prior art schematic of the component architecture of a multi-spool gas turbine engine. Gas is ingested into a low pressure compressor 1. The outlet of the low pressure compressor 1 passes through an intercooler 2 which removes a portion of heat from the gas stream at approximately constant pressure. The gas then enters a high pressure compressor 3. The outlet of high pressure compressor 3 passes through a recuperator 4 where some heat from the exhaust gas is transferred, at approximately constant pressure, to the gas flow from the high pressure compressor 3. The further heated gas from recuperator 4 is then directed to a combustor 5 where a fuel is burned, adding heat energy to the gas flow at approximately constant pressure. The gas emerging from the combustor 5 then enters a high pressure turbine 6 where work is done by the turbine to operate the high pressure compressor 3. The gas exiting from the high pressure turbine 6 then enters a low pressure turbine 7 where work is done by the turbine to operate the low pressure compressor 1. The gas exiting from the low pressure turbine 7 then enters a free power turbine 8. The shaft of the free power turbine, in turn, drives a transmission 11 which may be an electrical, mechanical or hybrid transmission for a vehicle. Alternately, the shaft of the free power turbine can drive an electrical generator or alternator. This engine design is described, for example, in U.S. patent application Ser. No. 12/115,134 filed May 5, 2008, entitled “Multi-Spool Intercooled Recuperated Gas Turbine”, which is incorporated herein by this reference.


As can be appreciated, the engine illustrated in FIG. 1 can have additional components (such as for example a re-heater between the high pressure and low pressure turbines) or can have fewer components (such as for example a single compressor-turbine spool, or no free power turbine but shaft power coming off the low pressure turbine spool).


A gas turbine engine is an enabling engine for efficient multi-fuel use and, in particular, this engine can be configured to switch between fuels while the engine is running and the vehicle is in motion (on the fly). In addition, a gas turbine engine can be configured to switch on the fly between liquid and gaseous fuels or operate on combinations of these fuels. This is possible because combustion in a gas turbine engine is continuous (as opposed to episodic such as in a reciprocating piston engine) and the important fuel parameter is the specific energy content of the fuel (that is, energy per unit mass) not its cetane number or octane rating. The cetane number (typically for diesel fuels and compression ignition) or octane rating (typically for gasoline fuels and spark ignition) are important parameters in piston engines for specifying fuel ignition properties.


The gas turbine engine such as shown schematically in FIG. 2 enables a multi-fuel strategy. This engine is prior art although even more efficient multi-fuel configurations will require innovative modifications to components and sub-components. This is an example of a 375 kW engine that uses intercooling and recuperation to achieve high operating efficiencies (40% or more) over a substantial range of vehicle operating speeds. This compact engine is suitable for light to heavy trucks. Variations of this engine design are suitable for smaller vehicles as well as applications such as, for example, marine, rail, agricultural and power-generation. One of the principal features of this engine is its fuel flexibility and fuel tolerance. This engine can operate on any number of liquid fuels (gasoline, diesel, ethanol, methanol, butanol, alcohol, bio diesel and the like) and on any number of gaseous fuels (compressed or liquid natural gas, propane, hydrogen and the like). This engine may also be operated on a combination of fuels such as mixtures of gasoline and diesel or mixtures of diesel and natural gas. Switching between these fuels is generally a matter of switching fuel injection systems and/or fuel mixtures.


This engine operates on the Brayton cycle and, because combustion is continuous, the peak operating temperatures are substantially lower than comparably sized piston engines operating on either an Otto cycle or Diesel cycle. This lower peak operating temperature results in substantially less NOx emissions generated by the gas turbine engine shown in FIG. 2. This figure shows a load device 209, such as for example a high speed alternator, attached via a reducing gearbox 217 to the output shaft of a free power turbine 208. A cylindrical duct 284 delivers the exhaust from free power turbine 208 to a plenum 214 which channels exhaust through the hot side of recuperator 204. Low pressure compressor 201 receives its inlet air via a duct (not shown) and sends compressed inlet flow to an intercooler (also not shown). The flow from the intercooler is sent to high pressure compressor 203 which is partially visible underneath free power turbine 208. As described previously, the compressed flow from high pressure compressor 203 is sent to the cold side of recuperator 204 and then to a combustor which is contained inside recuperator 204. The flow from combustor 215 (whose outlet end is just visible) is delivered to high pressure turbine 206 via cylindrical duct 256. The flow from high pressure turbine 206 is directed through low pressure turbine 207. The expanded flow from low pressure turbine 207 is then delivered to free power turbine 208 via a cylindrical elbow 278.


This engine has a relatively flat efficiency curve over wide operating range (from about 20% of full power to about 85% of full power). It also has a multi-fuel capability with the ability to change fuels on the fly as described in U.S. patent application Ser. No. 13/090,104 filed Apr. 19, 2011 entitled “Multi-Fuel Vehicle Strategy” which is incorporated herein by reference.


Ceramics Used in Gas Turbines



FIG. 3 is a stress-temperature map illustrating failure regimes for typical ceramic materials. This graphic shows that when flexure stress and temperature experienced by a ceramic component are high, the component operates in the fast fracture regime and the ceramic component lifetime would be expected to be unpredictable and typically short. This graphic also shows that when flexure stress and temperature experienced by a ceramic component are low, then the component operates in the no-failure regime and the ceramic component lifetime would be expected to be predictable and typically long. When the flexure stress is high but the temperature is low, then the component operates in a regime characterized by Weibull strength variability. When the flexure stress is low but the temperature is high, then the component operates in a regime characterized by slow crack growth or creep and the ceramic component lifetime would be expected to be somewhat unpredictable and variable.


Some gas turbine engines, especially microturbines, have used ceramic components in prototype situations. These have been used for relatively high temperatures and operated in the slow crack growth region. These engines have experienced failure of the ceramic components. One of the design goals used in the present disclosure is to maintain ceramic component operation well inside the no-failure regime so that incidences of component failure are substantially minimized and component lifetime is substantially maximized. A number of turbochargers have used ceramic components operating in the no-failure region, most notably ceramic rotors.


The following table shows some important properties of ceramics that are typically used for gas turbine components.















TABLE 1









Silicon
Silicon




Alumina
Cordierite
Carbide
Nitride
Mullite





















Density
3,700-3,970
2,600
3,210
3,310
2,800


(kg/m3)


Specific
670
1,465
628
712
963


Heat


(J/kg/K)


Thermal
24
3
41
27
3.5


Conductivity


(W/m/K)


Coefficient
8.39
1.7
5.12
3.14
5.3


Thermal


Expansion


(μm/m/K)


Thermal
200-250
500
350-500
750
300


Shock


Resistance


(ΔT (K))


Maximum
3,925
1,645
1,675
1,775
1,975


Use


Temperature


(K)










FIG. 4 is a schematic of a prior art turbo-compressor spool showing a metallic compressor rotor and a ceramic turbine rotor. This figure illustrates a compressor/turbine spool typical of use in a high-efficiency gas turbine operating in the output power range of about 300 to about 750 kW. A metallic compressor rotor 402 and a ceramic turbine rotor 403 are shown attached to the opposite ends of a metal shaft 401. The ceramic rotor shown here is a 95-mm diameter rotor fabricated from silicon nitride and was originally designed for use in turbocharger applications. As can be seen, the joint 404 between the ceramic rotor and metallic shaft is close to the ceramic rotor and is therefor exposed to high temperatures of the combustion products passing through the turbine. As can be seen, the joint 404 between the ceramic rotor and metallic shaft is close to the ceramic rotor and would typically be between the leftmost oil bearing and the ceramic rotor. The joint 404 is formed by inserting the ceramic shaft stub into a counterbore in the metallic shaft. The joint 404 is about 20 to about 25 mm from the ceramic rotor and is therefore exposed to high temperatures of the gas products passing through the turbine. Typical turbine inlet temperatures for this design are in the range of about 1,250° K to about 1,400° K.



FIG. 5 is schematic of a prior art gas turbine compressor/turbine spool assembly with ceramic and metallic components. This figure was taken from U.S. patent application Ser. No. 13/180,275 entitled “Metallic Ceramic Spool for a Gas Turbine Engine” filed Jul. 11, 2011 which is incorporated herein by reference. FIG. 5 illustrates a turbo-compressor spool with an all-ceramic high pressure turbine section. A ceramic turbine rotor 503 is shown separated by a small clearance gap from a ceramic shroud 502 which is integral with a ceramic volute 501. The volute, shroud and rotor are housed inside a metal case 504. The ceramic shroud 502 is also attached to a compliant metallic bellows 506 which is attached to an outer metal case 505. This configuration is capable of operating safely at turbine inlet temperatures in the approximate range from about 850° K to about 1,400° K. The ceramic rotor may be fabricated from rotor fabricated from silicon nitride. The ceramic shroud and volute can be fabricated from silicon carbide, for example, which has a coefficient of thermal expansion similar to that of silicon nitride used for the rotor. The use of a rotor and volute/shroud fabricated from the same or similar ceramics adequately thus controls radial and axial shroud clearances between the rotor 503 and shroud 502 and maintains high rotor efficiency by controlling the clearance and minimizing parasitic flow leakages between the rotor blade tips and the shroud. This design of a single piece or two piece ceramic volute and shroud for use with a ceramic turbine rotor is preferred if the ceramic material used can be operated well within the no-failure region as shown in FIG. 3. U.S. patent application Ser. No. 13/180,275 also describes a turbo-compressor spool comprised of ceramic and metallic components and with an active clearance control system.


Present Disclosure


The ceramic-to-metal attachment joint represents an important feature that, if not designed properly, limits the allowable operating temperature of the turbine rotor. Most joints of this type are limited to operating temperatures below 800° K. The drive for increased efficiency is pushing the rotor temperatures to levels approaching 1,400° K and higher. In the prior art, this ceramic-to-metal attachment is typically located close to the turbine rotor (see FIG. 4 for example), thus aggressive cooling is required to maintain the allowable temperature. The steep thermal gradient creates an area of elevated thermal stress.


Moving the temperature-limited joint between the bearings lowers its temperature and reduces the sharp gradient (and associated thermal stress) which naturally occurs between the turbine rotor and the cooler joint. A large outside diameter bearing is required on the turbine side so that it can be assembled. It is also anticipated that the ceramic turbine stub shaft needs to be relatively large in diameter relative to the metallic portion of the shaft to have the proper stiffness.


In the embodiments described herein, one or more of the following configurations are employed:

  • 1. Relocation of the ceramic-metallic joint substantially further away from the hot turbine gases to substantially reduce the thermal gradient and the thermal stress on the joint.
  • 2. Relocating the joint on the other side of the bearing closest to the turbine.
  • 3. Increasing the length and diameter of the ceramic shaft that is an integral part of the ceramic rotor and using a short, smooth transition down to the diameter of the metallic shaft.
  • 4. In place of the ceramic shaft being inserted into a counterbore in the metallic shaft, the diameter of the ceramic and metallic shaft is made the same. Brazing and the use of a connecting sleeve are used to form a strong joint with the required stiffness and ability to transmit the required torque.
  • 5. Relocating the joint so that either an all-oil bearing; an all-air bearing; or a combination air and oil bearing system can be used.


Consider the joint re-design in terms of the stress-temperature map of FIG. 3 which illustrates ceramic failure regimes. In the prior art joint, flexure stress and temperature experienced by the ceramic material in the vicinity of the joint are relatively high and the ceramic material operates near the creep fracture regime where ceramic component lifetime would tend to be somewhat unpredictable and variable. By moving the joint away from the turbine rotor thereby lowering the temperature at the joint, flexure stress would increase and the net result is that the ceramic material near the joint would remain near the creep fracture region and begin to approach the region characterized by Weibull strength variability. By increasing the ceramic shaft diameter and utilizing a sleeve to stiffen the joint, the flexure stress is reduced while temperature is maintained at its lower value. This places the ceramic joint material well within the no-failure regime and the lifetime of the ceramic material around the joint would be expected to be predictable and typically long.


As the turbine inlet temperature is increased over time as part of continued product improvement, the ceramic material in the vicinity of the joint should remain well within the no-failure zone of flexure stress versus temperature. Therefore the present disclosure not only solves a near term problem but is robust enough to maintain a long lifetime for the ceramic material in the vicinity of the metallic-ceramic joint.



FIG. 6 shows a general configuration of an air and oil hybrid bearing system with a ceramic-to-metal attachment joint 600 of the present disclosure. The ceramic-to-metal joint 600 is shown positioned approximately mid-way between the compressor rotor (not shown) and turbine rotor 603 and between an oil bearing 608 on the compressor side and an air bearing 606 on the turbine side. A coupler sleeve 601 is shown around joint 600 between the ceramic and the metallic shaft 602. The ceramic shaft is also part of the ceramic rotor 603 and is typically made from silicon nitride, silicon carbide, alumina or the like. The metallic shaft is typically fabricated from a high strength, high temperature steel such as for example a stainless steel or an Inconel steel. The metallic portion of the shaft may also be made from other metals such as titanium and even a high strength-high temperature aluminum. The metallic shaft 602 is the same diameter as the end of the ceramic shaft and the ceramic shaft transitions smoothly o a larger diameter to improve shaft stiffness. The ceramic and metallic shafts are typically brazed together to form a strong joint 600. The coupler sleeve 601 may also be brazed to the outer surface of the metallic and ceramic shafts. The coupler sleeve 601 is typically made from a high strength, high temperature steel such as for example a stainless or an Inconel steel. In the configuration of FIG. 6, the compressor-side bearing 608 is an oil bearing where oil is forced between the oil bearing and the metallic shaft during operation. Region 609 is filled with an oil mist. The turbine-side bearing 606 is an air bearing where air, typically bled from the compressor air flow, is directed between two labyrinth seals 604 and forced between the air bearing and the ceramic shaft during operation. The compressor bleed 605 is approximately about 2% of the total air flow through its corresponding compressor. The air and oil are separated by a discourager 607. In FIG. 6, the ceramic/metallic joint 600 is about 75 mm from the 95-mm diameter turbine rotor and is about 3 to about 4 times as far away from the turbine rotor as the prior art joint shown in FIG. 4.



FIG. 7 shows a general configuration of an all-oil bearing system with a ceramic-to-metal attachment joint 700 of the present invention. The ceramic-to-metal joint 700 is shown positioned approximately mid-way between the compressor rotor (not shown) and turbine rotor 703 and between an oil bearing 708 on the compressor side and a larger split oil bearing 706 on the turbine side. This latter bearing may be split for assembly. A coupler sleeve 701 is shown around joint 700 between the ceramic and the metallic shafts. The metallic shaft 702 is the same diameter as the end of the ceramic shaft and the ceramic shaft transitions to a larger diameter to improve shaft stiffness. In the configuration of FIG. 7, the compressor-side bearing 708 is an oil bearing where oil is forced between the oil bearing 708 and the metallic shaft 702 during operation. Region 709 is filled with an oil mist. The turbine-side bearing 706 is also an oil bearing where oil is forced between the oil bearing and the ceramic shaft during operation. Air is typically bled from the compressor air flow and directed between two labyrinth seals 704 and helps prevent oil from leaking into the turbine rotor air flow. In FIG. 7, the ceramic/metallic joint 700 is about 75 mm from the 95-mm diameter turbine rotor and is about 3 to about 4 times as far away from the turbine rotor as the prior art joint shown in FIG. 4.



FIG. 8 shows a general configuration of an all-air bearing system with a ceramic-to-metal attachment joint 800 of the present disclosure. The ceramic-to-metal joint 800 is shown positioned approximately mid-way between the compressor rotor (not shown) and turbine rotor 803 and between an air bearing 808 on the compressor side and a similar sized air bearing 806 on the turbine side. One or both bearings may be split for assembly. As shown in FIG. 8, the metallic shaft 802 has a large diameter section so that the two air bearings can be the same component. A coupler sleeve 801 is shown around the joint 800 between the ceramic and the metallic shafts. The metallic shaft 802 is the same diameter as the end of the ceramic shaft and the ceramic shaft transitions to a larger diameter to improve shaft stiffness. In the configuration of FIG. 8, the compressor-side bearing 808 is an air bearing where air is forced between the air bearing and the metallic shaft 802 during operation. The turbine-side bearing 806 is also an air bearing where air is forced between the air bearing and the ceramic shaft during operation. Air is typically bled from the compressor air flow and directed between a labyrinth seal 804 and a discourager 807. In FIG. 8, the ceramic/metallic joint 800 is about 75 mm from the 95-mm diameter turbine rotor and is about 3 to about 4 times as far away from the turbine rotor as the prior art joint shown in FIG. 4. Moving the joint to about halfway between the air bearings 806 and 808 is anticipated to provide sufficient isolation to enable this all-air bearing solution.


The disclosure has been described with reference to the preferred embodiments. Modifications and alterations will occur to others upon a reading and understanding of the preceding detailed description. It is intended that the disclosure be construed as including all such modifications and alterations insofar as they come within the scope of the appended claims or the equivalents thereof.


A number of variations and modifications of the disclosures can be used. As will be appreciated, it would be possible to provide for some features of the disclosures without providing others.


The present disclosure, in various embodiments, includes components, methods, processes, systems and/or apparatus substantially as depicted and described herein, including various embodiments, sub-combinations, and subsets thereof. Those of skill in the art will understand how to make and use the present disclosure after understanding the present disclosure. The present disclosure, in various embodiments, includes providing devices and processes in the absence of items not depicted and/or described herein or in various embodiments hereof, including in the absence of such items as may have been used in previous devices or processes, for example for improving performance, achieving ease and\or reducing cost of implementation.


The foregoing discussion of the disclosure has been presented for purposes of illustration and description. The foregoing is not intended to limit the disclosure to the form or forms disclosed herein. In the foregoing Detailed Description for example, various features of the disclosure are grouped together in one or more embodiments for the purpose of streamlining the disclosure. This method of disclosure is not to be interpreted as reflecting an intention that the claimed disclosure requires more features than are expressly recited in each claim. Rather, as the following claims reflect, inventive aspects lie in less than all features of a single foregoing disclosed embodiment. Thus, the following claims are hereby incorporated into this Detailed Description, with each claim standing on its own as a separate preferred embodiment of the disclosure.


Moreover though the description of the disclosure has included description of one or more embodiments and certain variations and modifications, other variations and modifications are within the scope of the disclosure, e.g., as may be within the skill and knowledge of those in the art, after understanding the present disclosure. It is intended to obtain rights which include alternative embodiments to the extent permitted, including alternate, interchangeable and/or equivalent structures, functions, ranges or steps to those claimed, whether or not such alternate, interchangeable and/or equivalent structures, functions, ranges or steps are disclosed herein, and without intending to publicly dedicate any patentable subject matter.

Claims
  • 1. An engine, comprising: a plurality of turbo-compressor spool assemblies, each turbo-compressor spool assembly comprising a compressor and a turbine attached by a common shaft and a first of the turbo-compressor spool assemblies is in fluid communication with a second of the turbo-compressor spool assemblies, at least one of the common shafts of a selected turbo-compressor spool assembly comprising a metallic compressor rotor and a ceramic turbine rotor connected by a metallic-to-ceramic attachment joint and a first bearing being positioned adjacent to the metallic compressor rotor and a second bearing adjacent to the ceramic turbine rotor;a free power turbine driven by a gas flow output by at least one of the turbo-compressor assemblies; anda combustor operable to combust a fuel and a gas output by one of the plurality of turbo-compressor spool assemblies, wherein:when the engine is in operation, the ceramic turbine rotor of the selected turbo-compressor spool assembly operates in a no-failure regime of the ceramic material;the ceramic-to-metallic attachment joint is located on the common shaft of the selected turbo-compressor spool assembly to be in a no-failure regime of the ceramic material, the location of the metallic-to-ceramic attachment joint being positioned between the first and second bearings on the common shaft, andwhen the engine is in operation, the metallic-to-ceramic attachment joint operates at a temperature of no more than about 800° K.
  • 2. The engine of claim 1, wherein the turbine rotor of the selected turbo-compressor spool assembly operates at a temperature of at least about 1,200° K.
  • 3. The engine of claim 1, wherein the first bearing is an oil bearing and the second bearing is an air bearing, and wherein at least one of the following is true: (i) the air and oil are substantially separated by a discourager; and(ii) the air bearing has a larger inside diameter than the oil bearing.
  • 4. The engine of claim 1, wherein the first bearing is an air bearing and the second bearing is an oil bearing.
  • 5. The engine of claim 1, wherein the first and second bearings are air bearings and wherein at least a portion of the air in the air bearing is removed from a gas flow of the compressor of the selected turbo-compressor spool assembly.
  • 6. The engine of claim 5, wherein the air is directed between a labyrinth seal and a discourager and the common shaft.
  • 7. The engine of claim 1, wherein the first and second bearings are oil bearings.
  • 8. The engine of claim 7, wherein air is bled from a compressor air flow and is directed between two labyrinth seals and the common shaft to inhibit oil from leaking into a turbine rotor air flow.
  • 9. The engine of claim 1, wherein a ceramic portion of the common shaft of the selected turbo-compressor spool assembly is at least about 40% of a length of the corresponding common shaft.
  • 10. The engine of claim 1, wherein an outer diameter of a ceramic portion of the common shaft of the selected turbo-compressor spool assembly is substantially the same as an outer diameter of a metallic portion of the common shaft at the joint and wherein the metallic-to-ceramic attachment joint is brazed and comprises a connecting sleeve.
  • 11. The engine of claim 1, wherein an outer diameter of the ceramic portion increases by at least about 20% in proximity to the ceramic turbine rotor while the metallic portion remains substantially constant between the metallic-to-ceramic joint and the metallic compressor rotor.
  • 12. An engine, comprising: a plurality of turbo-compressor spool assemblies, each turbo-compressor spool assembly comprising a compressor and a turbine attached by a common shaft and a first of the turbo-compressor spool assemblies is in fluid communication with a second of the turbo-compressor spool assemblies;a free power turbine driven by a gas flow output by at least one of the turbo-compressor assemblies; anda combustor operable to combust a fuel and a gas output by one of the plurality of turbo-compressor spool assemblies, wherein a selected turbo-compressor spool assembly comprises a metallic compressor rotor and a ceramic turbine rotor connected by a metallic-to-ceramic attachment joint, wherein a first and second bearings are located along a common shaft of the selected turbo-compressor spool assembly, and wherein at least one of the following is true:(i) a turbine rotor of a selected turbo-compressor spool assembly operates in a no-failure regime of the ceramic material and the metallic-to-ceramic attachment joint is located to be in a no-failure regime of the ceramic material;(ii) the metallic-to-ceramic attachment joint is located between the first and second bearings;(iii) a ceramic portion of the common shaft has a length of at least about 40% of a length of the shaft; and(iv) respective diameters of the ceramic portion and a metallic portion of the common shaft are substantially the same in the vicinity of the metallic-to-ceramic attachment joint.
  • 13. The engine of claim 12, wherein (i) is true.
  • 14. The engine of claim 12, wherein (ii) is true.
  • 15. The engine of claim 12, wherein (iii) is true and wherein an outer diameter of a ceramic portion of the common shaft of the selected turbo-compressor spool assembly is substantially the same as an outer diameter of a metallic portion of the common shaft at the joint.
  • 16. The engine of claim 12, wherein (iv) is true.
  • 17. A method, comprising: providing a gas turbine engine, the gas turbine engine comprising a turbo-compressor spool assembly, the turbo-compressor spool assembly comprising a compressor and a turbine attached by a common shaft, a free power turbine driven by a gas flow output by the turbo-compressor assembly, and a combustor operable to combust a fuel and a gas output by the turbo-compressor spool assembly, the compressor comprising a metallic compressor rotor and the turbine comprising a ceramic turbine rotor connected by a metallic-to-ceramic attachment joint; andwhen the gas turbine engine is in operation, maintaining the turbine rotor and the metallic-to-ceramic attachment joint in a no-failure regime of the ceramic material.
  • 18. The method of claim 17, wherein the turbine of the turbo-compressor spool assembly operates at a temperature of at least about 1,200° K and wherein the metallic-to-ceramic attachment joint operates at a temperature of no more than about 800° K.
  • 19. The method of claim 17, wherein a first bearing is positioned adjacent to the metallic compressor rotor and a second bearing is positioned adjacent to the ceramic turbine rotor and wherein the ceramic-to-metallic attachment joint is positioned between first and second bearings on the common shaft of the turbo-compressor spool assembly.
  • 20. The method of claim 19, wherein the first bearing is an oil bearing and the second bearing is an air bearing and wherein the air and oil are substantially separated by a discourager.
  • 21. The method of claim 19, wherein the first bearing is an air bearing and the second bearing is an oil bearing.
  • 22. The method of claim 19, wherein the first and second bearings are air bearings and wherein at least a portion of the air in the air bearing is removed from a gas flow of the compressor of the turbo-compressor spool assembly.
  • 23. The method of claim 22, wherein the air is directed between a labyrinth seal and a discourager and the common shaft.
  • 24. The method of claim 19, wherein the first and second bearings are oil bearings.
  • 25. The method of claim 24, wherein air is bled from a compressor air flow and is directed between two labyrinth seals and the common shaft to inhibit oil from leaking into a turbine rotor air flow.
  • 26. The method of claim 17, wherein a ceramic portion of the common shaft of the turbo-compressor spool assembly is at least about 40% of a length of the common shaft.
  • 27. The method of claim 17, wherein an outer diameter of a ceramic portion of the common shaft of the selected turbo-compressor spool assembly is substantially the same as an outer diameter of a metallic portion of the common shaft at the joint and wherein the metallic-to-ceramic attachment joint is brazed and comprises a connecting sleeve.
  • 28. The method of claim 26, wherein an outer diameter of the ceramic portion increases by at least about 25% in proximity to the ceramic turbine rotor while the metallic portion remains substantially constant between the metallic-to-ceramic joint and the metallic compressor rotor.
CROSS REFERENCE TO RELATED APPLICATION

The present application claims the benefits, under 35 U.S.C. §119(e), of U.S. Provisional Application Ser. No. 61/488,575 entitled “Ceramic-to-Metal Turbine Shaft Attachment” filed on May 20, 2011, which is incorporated herein by reference.

US Referenced Citations (462)
Number Name Date Kind
2463964 Graf Mar 1949 A
2543677 Traupel Feb 1951 A
2696711 Marchant et al. Dec 1954 A
2711071 Frankel Jun 1955 A
3032987 Taylor May 1962 A
3091933 Wagner et al. Jun 1963 A
3166902 Maljanian et al. Jan 1965 A
3204406 Howes et al. Sep 1965 A
3209536 Howes et al. Oct 1965 A
3237404 Flanigan et al. Mar 1966 A
3283497 Kaplan Nov 1966 A
3319931 Bell, III May 1967 A
3518472 O'Callaghan Jun 1970 A
3623318 Shank Nov 1971 A
3639076 Rowen Feb 1972 A
3646753 Stearns et al. Mar 1972 A
3660977 Reynolds May 1972 A
3706203 Goldberg et al. Dec 1972 A
3729928 Rowen May 1973 A
3748491 Barrigher et al. Jul 1973 A
3764814 Griffith Oct 1973 A
3766732 Woodcock Oct 1973 A
3817343 Albrecht Jun 1974 A
3831374 Nicita Aug 1974 A
3848636 McCombs Nov 1974 A
3866108 Yannone et al. Feb 1975 A
3888337 Worthen et al. Jun 1975 A
3893293 Moore Jul 1975 A
3937588 Kisslan Feb 1976 A
3939653 Schirmer Feb 1976 A
3945199 Bradley et al. Mar 1976 A
3953967 Smith May 1976 A
3964253 Paduch et al. Jun 1976 A
3977183 Stearns Aug 1976 A
3986364 Cronin et al. Oct 1976 A
3986575 Eggmann Oct 1976 A
3999373 Bell et al. Dec 1976 A
3999375 Smith et al. Dec 1976 A
4002058 Wolfinger Jan 1977 A
4005946 Brown et al. Feb 1977 A
4027472 Stearns Jun 1977 A
4027473 Baker Jun 1977 A
4056019 Ahlen Nov 1977 A
4059770 Mackay Nov 1977 A
4067189 Earnest Jan 1978 A
4082115 Gibb et al. Apr 1978 A
4122668 Chou et al. Oct 1978 A
4242042 Schwarz Dec 1980 A
4242871 Breton Jan 1981 A
4248040 Kast Feb 1981 A
4270357 Rossi et al. Jun 1981 A
4276744 Pisano Jul 1981 A
4277938 Belke et al. Jul 1981 A
4280327 Mackay Jul 1981 A
4282948 Jerome Aug 1981 A
4312191 Biagini Jan 1982 A
4336856 Gamell Jun 1982 A
4399651 Geary et al. Aug 1983 A
4411595 Pisano Oct 1983 A
4449359 Cole et al. May 1984 A
4467607 Rydquist et al. Aug 1984 A
4470261 Kronogard et al. Sep 1984 A
4474007 Kronogard et al. Oct 1984 A
4492874 Near Jan 1985 A
4494372 Cronin Jan 1985 A
4499756 Medeiros et al. Feb 1985 A
4509333 Nussdorfer et al. Apr 1985 A
4529887 Johnson Jul 1985 A
4586337 Fox May 1986 A
4754607 Mackay Jul 1988 A
4783957 Harris Nov 1988 A
4815278 White Mar 1989 A
4819436 Ahner et al. Apr 1989 A
4858428 Paul Aug 1989 A
4864811 Pfefferle Sep 1989 A
5010729 Adamson et al. Apr 1991 A
5036267 Markunas et al. Jul 1991 A
5069032 White Dec 1991 A
5081832 Mowill Jan 1992 A
5083039 Richardson et al. Jan 1992 A
5090193 Schwarz et al. Feb 1992 A
5097658 Klaass et al. Mar 1992 A
5113669 Coffinberry May 1992 A
5129222 Lampe et al. Jul 1992 A
5144299 Smith Sep 1992 A
5181827 Pellow et al. Jan 1993 A
5214910 Adair Jun 1993 A
5231822 Shekleton Aug 1993 A
5253470 Newton Oct 1993 A
5276353 Kobayashi et al. Jan 1994 A
5301500 Hines Apr 1994 A
5329757 Faulkner et al. Jul 1994 A
5333989 Missana et al. Aug 1994 A
5343692 Thomson et al. Sep 1994 A
5349814 Ciokajlo et al. Sep 1994 A
5386688 Nakhamkin Feb 1995 A
5427455 Bosley Jun 1995 A
5448889 Bronicki Sep 1995 A
5450724 Kesseli et al. Sep 1995 A
5488823 Faulkner et al. Feb 1996 A
5497615 Noe et al. Mar 1996 A
5529398 Bosley Jun 1996 A
5549174 Reis Aug 1996 A
5555719 Rowen et al. Sep 1996 A
5564270 Kesseli et al. Oct 1996 A
5586429 Kesseli et al. Dec 1996 A
5609655 Kesseli et al. Mar 1997 A
5610962 Solorzano et al. Mar 1997 A
5625243 Lindgren et al. Apr 1997 A
5667358 Gaul Sep 1997 A
5685156 Willis et al. Nov 1997 A
5697848 Bosley Dec 1997 A
5722259 Sorensen et al. Mar 1998 A
5742515 Runkle et al. Apr 1998 A
5752380 Bosley et al. May 1998 A
5784268 Steffek et al. Jul 1998 A
5791868 Bosley et al. Aug 1998 A
5819524 Bosley et al. Oct 1998 A
5820074 Trommer et al. Oct 1998 A
5827040 Bosley et al. Oct 1998 A
5850732 Willis et al. Dec 1998 A
5850733 Bosley et al. Dec 1998 A
5855112 Bannai et al. Jan 1999 A
5873235 Bosley et al. Feb 1999 A
5894720 Willis et al. Apr 1999 A
5899673 Bosley et al. May 1999 A
5903116 Geis et al. May 1999 A
5915841 Weissert Jun 1999 A
5918985 Bosley Jul 1999 A
5928301 Soga et al. Jul 1999 A
5929538 O'Sullivan et al. Jul 1999 A
5954174 Costin Sep 1999 A
5964663 Stewart et al. Oct 1999 A
5966926 Shekleton et al. Oct 1999 A
5983986 Macintyre et al. Nov 1999 A
5983992 Child et al. Nov 1999 A
5992139 Kesseli Nov 1999 A
6002603 Carver Dec 1999 A
6011377 Heglund et al. Jan 2000 A
6016658 Willis et al. Jan 2000 A
6020713 Geis et al. Feb 2000 A
6023135 Gilbreth et al. Feb 2000 A
6031294 Geis et al. Feb 2000 A
6037687 Stewart et al. Mar 2000 A
6049195 Geis et al. Apr 2000 A
6062016 Edelman May 2000 A
6065281 Shekleton et al. May 2000 A
6070404 Bosley et al. Jun 2000 A
6082112 Shekleton Jul 2000 A
6085524 Persson Jul 2000 A
6093975 Peticolas Jul 2000 A
6094799 Stewart et al. Aug 2000 A
6098397 Glezer et al. Aug 2000 A
6107693 Mongia et al. Aug 2000 A
6138781 Hakala Oct 2000 A
D433997 Laituri et al. Nov 2000 S
6141953 Mongia et al. Nov 2000 A
6155076 Cullen et al. Dec 2000 A
6155780 Rouse Dec 2000 A
6158892 Stewart et al. Dec 2000 A
6169334 Edelman Jan 2001 B1
6170251 Skowronski et al. Jan 2001 B1
6178751 Shekleton et al. Jan 2001 B1
6190048 Weissert Feb 2001 B1
6192668 Mackay Feb 2001 B1
6194794 Lampe et al. Feb 2001 B1
6205765 Iasillo et al. Mar 2001 B1
6205768 Dibble et al. Mar 2001 B1
6213234 Rosen et al. Apr 2001 B1
6239520 Stahl et al. May 2001 B1
6265786 Bosley et al. Jul 2001 B1
6274945 Gilbreth et al. Aug 2001 B1
6281596 Gilbreth et al. Aug 2001 B1
6281601 Edelman et al. Aug 2001 B1
6305079 Child et al. Oct 2001 B1
6314717 Teets et al. Nov 2001 B1
6316841 Weber Nov 2001 B1
6324828 Willis et al. Dec 2001 B1
6324846 Clarke Dec 2001 B1
6325142 Bosley et al. Dec 2001 B1
6349787 Dakhil Feb 2002 B1
6355987 Bixel Mar 2002 B1
6361271 Bosley Mar 2002 B1
6381944 Mackay May 2002 B2
6405522 Pont et al. Jun 2002 B1
6410992 Wall et al. Jun 2002 B1
6425732 Rouse et al. Jul 2002 B1
6437468 Stahl et al. Aug 2002 B2
6438936 Ryan Aug 2002 B1
6438937 Pont et al. Aug 2002 B1
6453658 Willis et al. Sep 2002 B1
6468051 Lampe et al. Oct 2002 B2
6487096 Gilbreth et al. Nov 2002 B1
6489692 Gilbreth et al. Dec 2002 B1
6495929 Bosley et al. Dec 2002 B2
6499949 Schafrik et al. Dec 2002 B2
6522030 Wall et al. Feb 2003 B1
6526757 MacKay Mar 2003 B2
6539720 Rouse et al. Apr 2003 B2
6542791 Perez Apr 2003 B1
6543232 Anderson et al. Apr 2003 B1
6552440 Gilbreth et al. Apr 2003 B2
6574950 Nash Jun 2003 B2
6598400 Nash et al. Jul 2003 B2
6601392 Child Aug 2003 B2
6605928 Gupta et al. Aug 2003 B2
6606864 Mackay Aug 2003 B2
6612112 Gilbreth et al. Sep 2003 B2
6629064 Wall Sep 2003 B1
6634176 Rouse et al. Oct 2003 B2
6638007 Bartholomä et al. Oct 2003 B2
6639328 Wacknov Oct 2003 B2
6644916 Beacom Nov 2003 B1
RE38373 Bosley Dec 2003 E
6657332 Balas Dec 2003 B2
6657348 Qin et al. Dec 2003 B2
6663044 Munoz et al. Dec 2003 B1
6664653 Edelman Dec 2003 B1
6664654 Wall et al. Dec 2003 B2
6670721 Lof et al. Dec 2003 B2
6675583 Willis et al. Jan 2004 B2
6683389 Geis Jan 2004 B2
6684642 Willis et al. Feb 2004 B2
6698208 Teets Mar 2004 B2
6698554 Desta et al. Mar 2004 B2
6702463 Brockett et al. Mar 2004 B1
6709243 Tan et al. Mar 2004 B1
6713892 Gilbreth et al. Mar 2004 B2
6720685 Balas Apr 2004 B2
6729141 Ingram May 2004 B2
6732531 Dickey May 2004 B2
6735951 Thompson May 2004 B2
6745574 Dettmer Jun 2004 B1
6747372 Gilbreth et al. Jun 2004 B2
6748742 Rouse et al. Jun 2004 B2
6751941 Edelman et al. Jun 2004 B2
6766647 Hartzheim Jul 2004 B2
6784565 Wall et al. Aug 2004 B2
6787933 Claude et al. Sep 2004 B2
6794766 Wickert et al. Sep 2004 B2
6796527 Munoz et al. Sep 2004 B1
6804946 Willis et al. Oct 2004 B2
6810677 Dewis Nov 2004 B2
6812586 Wacknov et al. Nov 2004 B2
6812587 Gilbreth et al. Nov 2004 B2
6815932 Wall Nov 2004 B2
6817575 Munoz et al. Nov 2004 B1
6819999 Hartzheim Nov 2004 B2
6823675 Brunell et al. Nov 2004 B2
6829899 Benham, Jr. et al. Dec 2004 B2
6832470 Dewis Dec 2004 B2
6834226 Hartzheim Dec 2004 B2
6836720 Hartzheim Dec 2004 B2
6837419 Ryan Jan 2005 B2
6845558 Beacom Jan 2005 B2
6845621 Teets Jan 2005 B2
6847129 McKelvey et al. Jan 2005 B2
6847194 Sarlioglu et al. Jan 2005 B2
6848249 Coleman et al. Feb 2005 B2
6863509 Dewis Mar 2005 B2
6864595 Wall Mar 2005 B2
6870279 Gilbreth et al. Mar 2005 B2
6877323 Dewis Apr 2005 B2
6883331 Jonsson et al. Apr 2005 B2
6888263 Satoh et al. May 2005 B2
6891282 Gupta et al. May 2005 B2
6895760 Kesseli May 2005 B2
6897578 Olsen et al. May 2005 B1
6909199 Gupta et al. Jun 2005 B2
6911742 Gupta et al. Jun 2005 B2
6931856 Belokon et al. Aug 2005 B2
6951110 Kang Oct 2005 B2
6956301 Gupta et al. Oct 2005 B2
6958550 Gilbreth et al. Oct 2005 B2
6960840 Willis et al. Nov 2005 B2
6964168 Pierson et al. Nov 2005 B1
6966173 Dewis Nov 2005 B2
6968702 Child et al. Nov 2005 B2
6973880 Kumar Dec 2005 B2
6977446 Mackay Dec 2005 B2
6979914 McKelvey et al. Dec 2005 B2
6983787 Schoenenborn Jan 2006 B2
6989610 Gupta et al. Jan 2006 B2
6998728 Gupta et al. Feb 2006 B2
7019626 Funk Mar 2006 B1
7053590 Wang May 2006 B2
7059385 Moilala Jun 2006 B2
7065873 Kang et al. Jun 2006 B2
RE39190 Weissert Jul 2006 E
7092262 Ryan et al. Aug 2006 B2
7093443 McKelvey et al. Aug 2006 B2
7093448 Nguyen et al. Aug 2006 B2
7112036 Lubell et al. Sep 2006 B2
7117683 Thompson Oct 2006 B2
7147050 Kang et al. Dec 2006 B2
7166928 Larsen Jan 2007 B2
7181337 Kosaka Feb 2007 B2
7185496 Herlihy Mar 2007 B2
7186200 Hauser Mar 2007 B1
7211906 Teets et al. May 2007 B2
7224081 Larsen May 2007 B2
7244524 McCluskey et al. Jul 2007 B2
7266429 Travaly et al. Sep 2007 B2
7285871 Derouineau Oct 2007 B2
7299638 Mackay Nov 2007 B2
7304445 Donnelly Dec 2007 B2
7309929 Donnelly et al. Dec 2007 B2
7318154 Tehee Jan 2008 B2
7325401 Kesseli et al. Feb 2008 B1
7343744 Abelson et al. Mar 2008 B2
7393179 Kesseli et al. Jul 2008 B1
7398642 McQuiggan Jul 2008 B2
7404294 Sundin Jul 2008 B2
7415764 Kang et al. Aug 2008 B2
7423412 Weng et al. Sep 2008 B2
7464533 Wollenweber Dec 2008 B2
7513120 Kupratis Apr 2009 B2
7514807 Donnelly et al. Apr 2009 B2
7518254 Donnelly et al. Apr 2009 B2
RE40713 Geis et al. May 2009 E
7554278 Wegner-Donnelly et al. Jun 2009 B2
7565867 Donnelly et al. Jul 2009 B2
7572531 Forte Aug 2009 B2
7574853 Teets et al. Aug 2009 B2
7574867 Teets et al. Aug 2009 B2
7595124 Varatharajan et al. Sep 2009 B2
7605487 Barton et al. Oct 2009 B2
7605498 Ledenev et al. Oct 2009 B2
7607318 Lui et al. Oct 2009 B2
7608937 Altenschulte Oct 2009 B1
7614792 Wade et al. Nov 2009 B2
7615881 Halsey et al. Nov 2009 B2
7617687 West et al. Nov 2009 B2
7656135 Schram et al. Feb 2010 B2
7667347 Donnelly et al. Feb 2010 B2
7671481 Miller et al. Mar 2010 B2
7766790 Stevenson et al. Aug 2010 B2
7770376 Brostmeyer Aug 2010 B1
7777358 Halsey et al. Aug 2010 B2
7804184 Yuan et al. Sep 2010 B2
7841185 Richards et al. Nov 2010 B2
7861696 Lund Jan 2011 B2
7866532 Potter et al. Jan 2011 B1
7906862 Donnelly et al. Mar 2011 B2
7921944 Russell et al. Apr 2011 B2
7926274 Farkaly Apr 2011 B2
7944081 Donnelly et al. May 2011 B2
7957846 Hakim et al. Jun 2011 B2
7966868 Sonnichsen et al. Jun 2011 B1
7977845 Heitmann Jul 2011 B1
8008808 Seeker et al. Aug 2011 B2
8015812 Kesseli et al. Sep 2011 B1
8046990 Bollinger et al. Nov 2011 B2
8055526 Blagg et al. Nov 2011 B2
8188693 Wei et al. May 2012 B2
8244419 Wegner-Donnelly et al. Aug 2012 B2
20010030425 Gilbreth et al. Oct 2001 A1
20010052704 Bosley et al. Dec 2001 A1
20020054718 Weissert May 2002 A1
20020063479 Mitchell et al. May 2002 A1
20020067872 Weissert Jun 2002 A1
20020073688 Bosley et al. Jun 2002 A1
20020073713 Mackay Jun 2002 A1
20020079760 Vessa Jun 2002 A1
20020083714 Bakholdin Jul 2002 A1
20020096393 Rouse Jul 2002 A1
20020096959 Qin et al. Jul 2002 A1
20020097928 Swinton et al. Jul 2002 A1
20020099476 Hamrin et al. Jul 2002 A1
20020103745 Lof et al. Aug 2002 A1
20020104316 Dickey et al. Aug 2002 A1
20020110450 Swinton Aug 2002 A1
20020119040 Bosley Aug 2002 A1
20020120368 Edelman et al. Aug 2002 A1
20020124569 Treece et al. Sep 2002 A1
20020128076 Lubell Sep 2002 A1
20020148229 Pont et al. Oct 2002 A1
20020149205 Gilbreth et al. Oct 2002 A1
20020149206 Gilbreth et al. Oct 2002 A1
20020157881 Bakholdin et al. Oct 2002 A1
20020158517 Rouse et al. Oct 2002 A1
20020166324 Willis et al. Nov 2002 A1
20030110773 Rouse et al. Jun 2003 A1
20040008010 Ebrahim et al. Jan 2004 A1
20040011038 Stinger et al. Jan 2004 A1
20040035656 Anwar et al. Feb 2004 A1
20040065293 Goto Apr 2004 A1
20040080165 Geis et al. Apr 2004 A1
20040090204 McGinley May 2004 A1
20040103669 Willis et al. Jun 2004 A1
20040106486 Jonsson Jun 2004 A1
20040119291 Hamrin et al. Jun 2004 A1
20040148942 Pont et al. Aug 2004 A1
20040160061 Rouse et al. Aug 2004 A1
20050000224 Jonsson Jan 2005 A1
20050103931 Morris et al. May 2005 A1
20050206331 Donnelly Sep 2005 A1
20050228553 Tryon Oct 2005 A1
20050229586 Whurr Oct 2005 A1
20060076171 Donnelly et al. Apr 2006 A1
20060090109 Bonnet Apr 2006 A1
20070012129 Maty et al. Jan 2007 A1
20070068712 Carnahan Mar 2007 A1
20070178340 Eickhoff Aug 2007 A1
20070181294 Soldner et al. Aug 2007 A1
20070239325 Regunath Oct 2007 A1
20070290039 Pfleging et al. Dec 2007 A1
20080034759 Bulman et al. Feb 2008 A1
20080080682 Ogunwale et al. Apr 2008 A1
20080148708 Chou et al. Jun 2008 A1
20080197705 Dewis et al. Aug 2008 A1
20080208393 Schricker Aug 2008 A1
20080243352 Healy Oct 2008 A1
20080271703 Armstrong et al. Nov 2008 A1
20080278000 Capp et al. Nov 2008 A1
20090045292 Maddali et al. Feb 2009 A1
20090071478 Kalfon Mar 2009 A1
20090090109 Mills et al. Apr 2009 A1
20090106978 Wollenweber Apr 2009 A1
20090109022 Gangopadhyay et al. Apr 2009 A1
20090158739 Messmer Jun 2009 A1
20090193809 Schroder et al. Aug 2009 A1
20090204316 Klampfl et al. Aug 2009 A1
20090211260 Kesseli et al. Aug 2009 A1
20090211739 Nash et al. Aug 2009 A1
20090211740 Kesseli et al. Aug 2009 A1
20090249786 Garrett et al. Oct 2009 A1
20090271086 Morris et al. Oct 2009 A1
20090292436 D'Amato et al. Nov 2009 A1
20090313990 Mustafa Dec 2009 A1
20090326753 Chen et al. Dec 2009 A1
20100021284 Watson et al. Jan 2010 A1
20100052425 Moore et al. Mar 2010 A1
20100127570 Hadar et al. May 2010 A1
20100154380 Tangirala et al. Jun 2010 A1
20100229525 Mackay et al. Sep 2010 A1
20100288571 Dewis et al. Nov 2010 A1
20100293946 Vick Nov 2010 A1
20100301062 Litwin et al. Dec 2010 A1
20100319355 Prabhu Dec 2010 A1
20110020108 Axelsson et al. Jan 2011 A1
20110100777 Wilton et al. May 2011 A1
20110215640 Donnelly Sep 2011 A1
20110288738 Donnelly et al. Nov 2011 A1
20110295453 Betz et al. Dec 2011 A1
20120000204 Kesseli et al. Jan 2012 A1
20120017598 Kesseli et al. Jan 2012 A1
20120042656 Donnelly et al. Feb 2012 A1
20120096869 Kesseli et al. Apr 2012 A1
20120102911 Dewis et al. May 2012 A1
20120175886 Donnelly et al. Jul 2012 A1
20120201657 Donnelly et al. Aug 2012 A1
20120260662 Nash et al. Oct 2012 A1
20120324903 Dewis et al. Dec 2012 A1
20130111923 Donnelly et al. May 2013 A1
20130133480 Donnelly May 2013 A1
20130139519 Kesseli et al. Jun 2013 A1
20130294892 Dewis et al. Nov 2013 A1
20130305730 Donnelly et al. Nov 2013 A1
20140000275 Kesseli et al. Jan 2014 A1
20140026585 Baldwin Jan 2014 A1
20140306460 Donnelly Oct 2014 A1
Foreign Referenced Citations (291)
Number Date Country
311027 Dec 2005 AT
582981 Apr 1989 AU
587266 Aug 1989 AU
8517301 Mar 2002 AU
2025002 May 2002 AU
2589802 May 2002 AU
2004203836 Mar 2005 AU
2004208656 Feb 2009 AU
2004318142 Jun 2009 AU
1050637 Mar 1979 CA
1068492 Dec 1979 CA
1098997 Apr 1981 CA
1099373 Apr 1981 CA
1133263 Oct 1982 CA
1171671 Jul 1984 CA
1190050 Jul 1985 CA
1202099 Mar 1986 CA
1244661 Nov 1988 CA
1275719 Oct 1990 CA
2066258 Mar 1991 CA
1286882 Jul 1991 CA
2220172 May 1998 CA
2234318 Oct 1998 CA
2238356 Mar 1999 CA
2242947 Mar 1999 CA
2246769 Mar 1999 CA
2279320 Apr 2000 CA
2677758 Apr 2000 CA
2317855 May 2001 CA
2254034 Jun 2007 CA
2638648 Feb 2009 CA
2689188 Jul 2010 CA
595552 Feb 1978 CH
679235 Jan 1992 CH
1052170 Jun 1991 CN
1060270 Apr 1992 CN
1306603 Aug 2001 CN
1317634 Oct 2001 CN
1902389 Jan 2007 CN
101098079 Jan 2008 CN
100564811 Dec 2009 CN
101635449 Jan 2010 CN
101672252 Mar 2010 CN
9101996 Jan 1992 CS
20014556 Apr 2003 CZ
1272306 Jul 1968 DE
2753673 Jun 1978 DE
2853919 Jun 1979 DE
3140694 Jul 1982 DE
3736984 May 1988 DE
69519684 Aug 2001 DE
10305352 Sep 2004 DE
69828916 Mar 2006 DE
60125441 Feb 2007 DE
60125583 Feb 2007 DE
331889 Jul 1989 DK
0092551 Nov 1983 EP
0093118 Nov 1983 EP
0104921 Apr 1984 EP
0157794 Oct 1985 EP
0377292 Jul 1990 EP
0319246 Oct 1990 EP
0432753 Jun 1991 EP
0455640 Nov 1991 EP
0472294 Feb 1992 EP
0478713 Apr 1992 EP
0493481 Jul 1992 EP
0522832 Jan 1993 EP
0620906 Oct 1994 EP
0691511 Jan 1996 EP
0754142 Jan 1997 EP
0784156 Dec 1997 EP
0837224 Apr 1998 EP
0837231 Apr 1998 EP
0901218 Mar 1999 EP
0698178 Jun 1999 EP
0963035 Dec 1999 EP
1055809 Nov 2000 EP
1075724 Feb 2001 EP
1046786 Jan 2002 EP
1071185 Jan 2002 EP
1215393 Jun 2002 EP
0739087 Aug 2002 EP
1240713 Sep 2002 EP
1277267 Jan 2003 EP
1283166 Feb 2003 EP
1305210 May 2003 EP
1340301 Sep 2003 EP
1340304 Sep 2003 EP
1341990 Sep 2003 EP
1342044 Sep 2003 EP
1346139 Sep 2003 EP
1436504 Jul 2004 EP
1203866 Aug 2004 EP
0800616 Dec 2004 EP
1519011 Mar 2005 EP
1132614 Jan 2007 EP
1790568 May 2007 EP
1813807 Aug 2007 EP
1825115 Aug 2007 EP
1860750 Nov 2007 EP
1939396 Jul 2008 EP
2028104 Feb 2009 EP
1638184 Mar 2009 EP
1648096 Jul 2009 EP
2108828 Oct 2009 EP
1728990 Nov 2009 EP
2161444 Mar 2010 EP
2169800 Mar 2010 EP
1713141 May 2010 EP
1728304 Jun 2010 EP
1468180 Jul 2010 EP
2467286 Nov 1985 FR
2637942 Apr 1990 FR
2645908 Oct 1990 FR
2755319 Apr 1998 FR
2848647 Jun 2004 FR
612817 Nov 1948 GB
671379 May 1952 GB
673961 Jun 1952 GB
706743 Apr 1954 GB
731735 Jun 1955 GB
761955 Nov 1956 GB
768047 Feb 1957 GB
784119 Oct 1957 GB
786001 Nov 1957 GB
789589 Jan 1958 GB
807267 Jan 1959 GB
817507 Jul 1959 GB
834550 May 1960 GB
864712 Apr 1961 GB
874251 Aug 1961 GB
877838 Sep 1961 GB
878552 Oct 1961 GB
885184 Dec 1961 GB
917392 Feb 1963 GB
919540 Feb 1963 GB
920408 Mar 1963 GB
924078 Apr 1963 GB
931926 Jul 1963 GB
937278 Sep 1963 GB
937681 Sep 1963 GB
950015 Feb 1964 GB
950506 Feb 1964 GB
977402 Dec 1964 GB
993039 May 1965 GB
1004953 Sep 1965 GB
1008310 Oct 1965 GB
1009115 Nov 1965 GB
1012909 Dec 1965 GB
1043271 Sep 1966 GB
1083943 Sep 1967 GB
1097623 Jan 1968 GB
1103032 Feb 1968 GB
1127856 Sep 1968 GB
1137691 Dec 1968 GB
1138807 Jan 1969 GB
1141019 Jan 1969 GB
1148179 Apr 1969 GB
1158271 Jul 1969 GB
1172126 Nov 1969 GB
1174207 Dec 1969 GB
1211607 Nov 1970 GB
1270011 Apr 1972 GB
1275753 May 1972 GB
1275754 May 1972 GB
1275755 May 1972 GB
1301104 Dec 1972 GB
1348797 Mar 1974 GB
1392271 Apr 1975 GB
1454766 Nov 1976 GB
1460590 Jan 1977 GB
1516664 Jul 1978 GB
2019494 Oct 1979 GB
2074254 Oct 1981 GB
2089433 Jun 1982 GB
2123154 Jan 1984 GB
2174824 Nov 1986 GB
2184609 Jun 1987 GB
2199083 Jun 1988 GB
2211285 Jun 1989 GB
2218255 Nov 1989 GB
2232207 Dec 1990 GB
2341897 Mar 2000 GB
2355286 Apr 2001 GB
2420615 May 2006 GB
2426043 Nov 2006 GB
2435529 Aug 2007 GB
2436708 Oct 2007 GB
2441924 Mar 2008 GB
2442585 Apr 2008 GB
2456336 Jul 2009 GB
2456672 Jul 2009 GB
2447514 Dec 2009 GB
4946DELNP2006 Aug 2007 IN
4341DELNP2005 Oct 2007 IN
5879DELNP2008 Sep 2008 IN
2502DEL2005 Oct 2009 IN
55DEL2010 Jul 2010 IN
1913DEL2009 Jul 2010 IN
2013DEL2009 Jul 2010 IN
1173399 Jun 1987 IT
1194590 Sep 1988 IT
MI911564 Jan 1992 IT
51-065252 Jun 1976 JP
56-088920 Jul 1981 JP
56-148624 Nov 1981 JP
56-148625 Nov 1981 JP
S59-010709 Jan 1984 JP
60-184973 Sep 1985 JP
S60-184906 Sep 1985 JP
61-182489 Aug 1986 JP
3182638 Aug 1991 JP
6201891 Jul 1994 JP
2519620 Jul 1996 JP
10-054561 Feb 1998 JP
10-061660 Mar 1998 JP
10-115229 May 1998 JP
10-122180 May 1998 JP
11-324727 Nov 1999 JP
2000-054855 Feb 2000 JP
2000-130319 May 2000 JP
2000-329096 Nov 2000 JP
2002-030942 Jan 2002 JP
2002-115565 Apr 2002 JP
2003-009593 Jan 2003 JP
2003-013744 Jan 2003 JP
2003-041906 Feb 2003 JP
2004-163087 Jun 2004 JP
2005-345095 Dec 2005 JP
2006-022811 Jan 2006 JP
2006-170208 Jun 2006 JP
2006-174694 Jun 2006 JP
2006-200438 Aug 2006 JP
2007-231949 Sep 2007 JP
2008-111438 May 2008 JP
2008-132973 Jun 2008 JP
2009-108756 May 2009 JP
2009-108860 May 2009 JP
2009-209931 Sep 2009 JP
2009-216085 Sep 2009 JP
2009-250040 Oct 2009 JP
2010-014114 Jan 2010 JP
2010-106835 May 2010 JP
19840002483 Dec 1984 KR
880002362 Oct 1988 KR
890001170 Apr 1989 KR
1020010007189 Jan 2001 KR
1020020024545 Mar 2002 KR
1020030032864 Apr 2003 KR
1020060096320 Sep 2006 KR
1020070078978 Aug 2007 KR
1020070113990 Nov 2007 KR
1020080033866 Apr 2008 KR
1020090121248 Nov 2009 KR
7903120 Oct 1979 NL
437543 Mar 1985 SE
9901718 May 1999 SE
0103180 Mar 2003 SE
WO 8501326 Mar 1985 WO
WO 9207221 Apr 1992 WO
WO 9524072 Sep 1995 WO
WO 9722176 Jun 1997 WO
WO 9722789 Jun 1997 WO
WO 9726491 Jul 1997 WO
WO 9825014 Jun 1998 WO
WO 9854448 Dec 1998 WO
WO 9919161 Apr 1999 WO
WO 0140644 Jun 2001 WO
WO 0182448 Nov 2001 WO
WO 0202920 Jan 2002 WO
WO 0229225 Apr 2002 WO
WO 0239045 May 2002 WO
WO 0240844 May 2002 WO
WO 0242611 May 2002 WO
WO 0244574 Jun 2002 WO
WO 0250618 Jun 2002 WO
WO 02037638 Sep 2002 WO
WO 03093652 Nov 2003 WO
WO 2004077637 Sep 2004 WO
WO 2005045345 May 2005 WO
WO 2005099063 Oct 2005 WO
WO 2008044972 Apr 2008 WO
WO 2008044973 Apr 2008 WO
WO 2008082334 Jul 2008 WO
WO 2008082335 Jul 2008 WO
WO 2008082336 Jul 2008 WO
WO 2009067048 May 2009 WO
WO 2010050856 May 2010 WO
WO 2010082893 Jul 2010 WO
8608745 Jul 1987 ZA
Non-Patent Literature Citations (12)
Entry
U.S. Appl. No. 13/210,121, filed Aug. 15, 2011, Donnelly et al.
U.S. Appl. No. 13/226,156, filed Sep. 6, 2011, Donnelly et al.
U.S. Appl. No. 13/372,998, filed Feb. 14, 2012, Nash et al.
U.S. Appl. No. 13/481,469, filed May 25, 2012, Wilson.
“Analysis of Technology Options to Reduce the Fuel Consumption of Idling Trucks,” Stodolsky, F., L. Gaines, and A. Vyas, Argonne National Laboratory, ANL/ESD-43, Jun. 2000, 40 pages.
“Why Gas Turbines have a Future in Heavy Duty Trucks.” Capstone Turbine Corporation, Brayton Energy, LLC, Kenworth Truck Company, a PACCAR Company, Peterbilt Truck Company, a PACCAR Company, Apr. 2009, 10 pages.
Balogh et al. “DC Link Floating for Grid Connected PV Converters,” World Academy of Science, Engineering and Technology Apr. 2008, Iss. 40, pp. 115-120.
Mackay et al. “High Efficiency Vehicular Gas Turbines,” SAE International, 2005, 10 pages.
Nemeth et al. “Life Predicted in a Probabilistic Design Space for Brittle Materials With Transient Loads,” NASA, last updated Jul. 21, 2005, found at http://www.grc.nasa.gov/WWW/RT/2004/RS/RS06L-nemeth.html, 5 pages.
Wolf et al. “Preliminary Design and Projected Performance for Intercooled-Recuperated Microturbine,” Proceedings of the ASME TurboExpo 2008 Microturbine and Small Turbomachinery Systems, Jun. 9-13, 2008, Berlin, Germany, 10 pages.
“Remy HVH250-090-SOM Electric Motor,” Remy International, Inc., 2011, 2 pages.
Gieras et al., “Performance Calculation for a High-Speed Solid-Rotor Induction Motor,” IEEE Transactions on Industrial Electronics, 2012, vol. 59, No. 6, pp. 2689-2700.
Related Publications (1)
Number Date Country
20140196457 A1 Jul 2014 US
Provisional Applications (1)
Number Date Country
61488575 May 2011 US