Abstract:
The invention, intended primarily for use in a steel flywheel power source ( 30 ), provides a vacuum system and a method of maintaining a vacuum inside a flywheel chamber ( 32 ) for the life of the power source ( 30 ). The vacuum system combines the use of cleaning and de-gassing treatments in the chamber ( 32 ) and vacuum tempering of the steel flywheel ( 31 ) with the use of a chemical type metal alloy nonevaporable getter, such as zirconium-vanadium-iron, that cooperatively matches the outgassing of the flywheel ( 31 ) and chamber ( 32 ) by sorbing those gases that are released. The getter may be reactivated throughout the life of the flywheel system by reheating it with an integral heater that is triggered by a timer instead of a vacuum gauge to increase the system reliability, using power taken directly from the energy stored in the flywheel. The electronics ( 45 ) of the flywheel power source are used to signal an alarm or prevent achieving or maintaining full speed of the flywheel when the vacuum in the chamber degrades.

Description:
[0001]    This invention pertains to a vacuum system for energy storage flywheels and more particularly to a vacuum system and method of maintaining vacuum in a flywheel power source that employs a steel flywheel for storing energy. The vacuum system maintains the required low pressure inside a flywheel chamber to prevent excessive aerodynamic drag for the life of the power source and is reliable, maintenance-free and low cost.  
         BACKGROUND OF THE INVENTION  
         [0002]    Flywheels have been used for many years as energy storage devices. They have often been used as power smoothing mechanisms for internal combustion engines and other kinds of power equipment. More recently, flywheels have been recognized as a very attractive energy storage technology for such electrical applications as uninterruptible power supplied utility load leveling systems and electric vehicles.  
           [0003]    Modern flywheel energy storage systems convert back and forth between a spinning flywheel&#39;s rotational energy and electrical energy. A flywheel energy storage stem includes a flywheel, a motor generator, a bearing system and a vacuum enclosure. The rotating flywheel stores mechanical energy, the motor generator converts electrical or mechanical energy to mechanical or electrical energy, respectively, and the bearing system physically supports the rotating flywheel.  
           [0004]    In almost all energy storage applications, whether quick discharge type (power ride-through), where discharge time is measured in seconds, or long-term discharge type (power backup), where discharge time is measured in hours, flywheels directly compete with electrochemical batteries. Two key advantages of flywheels used for electrical energy storage over electrochemical battery systems are its longevity and reliability. Electrochemical batteries, in particular, lead-acid batteries, have short lifetimes, between six months and seven years depending on operating conditions. These batteries require periodic maintenance and can fail unpredictably. In contrast, flywheel energy storage systems are expected to have maintenance-free lifetimes of twenty years.  
           [0005]    To achieve a maintenance-free life of many years, the vacuum system that is used to prevent excessive drag and aerodynamic heating of the flywheel must be capable of reliably maintaining an adequate level of vacuum. To date several approaches have been used to create and or maintain vacuum in flywheel systems. The simplest and most widely used approach is to attach an external mechanical vacuum pump to the flywheel chamber. The vacuum pump can then either run continuously or can just turn on when a vacuum gauge indicates that the vacuum has reached an unacceptable pressure. In either case, most vacuum pumps require regular maintenance and have less than twenty-year lives along with the vacuum gauges.  
           [0006]    Another method for creating vacuum in a flywheel chamber is to use the flywheel&#39;s rotation to drive a molecular drag pump. The flywheel shaft spans two different chambers and a drag pump gear on the shaft pumps gases from the flywheel chamber to the external chamber. The external chamber, which is at a higher pressure, contains physical type getters to trap the gas molecules. Unfortunately, the drag pump is very inefficient at low speeds and could cause the flywheel to take a much longer time to reach full speed if the vacuum level is substantially low. The physical type getters are also found to be not very effective at ambient temperatures either.  
           [0007]    Vacuum creation schemes for flywheel systems have also included using pumping action directly from the rotating flywheel itself with the molecules passing through a semi-porous membrane surrounding the flywheel to create the vacuum It is not clear what membrane material could perform this function although, if possible, the structure is likely expensive. Not to mention, this method also suffers from having a lack of vacuum until the flywheel is at high speed. Thus the charging of the flywheel power source would take an extended period of time and much excess power.  
           [0008]    To get around the problems of excess low speed drag loss, it is preferable to always have an adequate vacuum regardless of the flywheel speed. Physical type getters such as activated charcoal or zeolites have been proposed for use in sorbing large quantities of gases. Physical type getters trap molecules by having a very porous internal structure in which a small volume of material has an extremely large surface area to which molecules can stick. Unfortunately, as described above, sorption is related to temperature and at room temperature their efficiency is very poor because of the higher energy of the molecules preventing or inhibiting their sticking. They also are not effective for sorbing hydrogen, which may be the largest outgassing component depending on the type of flywheel&#39;s construction  
           [0009]    To get around the temperature dependence problems of physical getters, evaporable chemical type getters have been proposed. Evaporable getters work by having a base getter material that is continuously heated and vaporized inside the flywheel chamber. The material that is vaporized will condense on the inner walls of the chamber as a clean surface. The clean surface then allows chemical adsorption of gas molecules, which maintains the vacuum. This method can be maintenance-free if enough getter material is included with the flywheel power source. Unfortunately, non-evaporable getters are best suited for very low pressure vacuum because the film can only be deposited at a slow rate. Thus, the gas molecules of a medium pressure vacuum, which is all that is required for a rotating flywheel, would overpower the getter. The getter would also have a limited life.  
           [0010]    Compounding the problems of mining the vacuum for an extremely long time inside a flywheel power source, flywheel systems have a couple of uniquely problematic attributes compared with other evacuated devices. Flywheel systems have an unusually large internal surface area for their enclosed volume. The large surface area, which is the result of filling the chamber mostly with the flywheel creates much higher gas evolution For performance reasons, such as reducing the turbulent drag on the flywheel through reduction of the gap between the flywheel and the stationary chamber walls, as well as for shipping and handling purposes, the size of the flywheel chamber is preferably made small. The lower internal volume from the large internal flywheel and small outer chamber means that the internal volume becomes very small. Thus, it does not take much outgassing of molecules before the pressure inside the chamber rises to acceptable levels.  
         SUMMARY OF THE INVENTION  
         [0011]    The invention is a vacuum system and method of maintaining vacuum in a flywheel power source that maintains the low pressure inside a flywheel chamber for the life of the power source. The vacuum system works by combining the use of a steel flywheel housed inside a metal vacuum chamber of the power source, with the use of a chemical type metal alloy non-evaporable getter that cooperatively matches the outgassing of the flywheel and chamber by sorbing those gases that are released. In contra, use of higher speed and lighter weight composite material flywheels for storing energy in the power source would result in up to 1000 times or greater outgassing load, which would make removal of the gases by this method extremely difficult. Not only would the quantity and rate of gas evolution be extremely large for a system employing a composite material flywheel, the gases include much water vapor as well as larger molecules which are much more difficult to getter by chemical type getters. The use of a steel flywheel has been found to outgas primarily hydrogen and this is gas most readily sorbed by the chemical type metal alloy non-evaporable chemical type getters. In contrast, physical type getters are can not effectively trap hydrogen Although, steel flywheels contain nearly 70 times more internal nitrogen gas, the hydrogen is many times more soluble in the steel and thus outgases at a higher rate. Therefore, sorbing the large quantity of hydrogen is required to maintain the vacuum. Because both the getter material and the flywheel are constructed of metals, it becomes understandable that both would have similar differing solubilities for different gasses. The hydrogen that is readily released from the flywheel in vacuum due to its higher internal concentration, becomes readily sorbed by the alloy getter material. Other gases such as carbon monoxide, carbon dioxide, nitrogen and oxygen are also outgassed and sorbed, but at slower rates. The non-evaporable getter has the ability to take in these gases at a lower temperature than the steel of the flywheel because of the elements in its construction and because of use of alloying which lowers the activation and operation temperature. One common commercially available metal alloy non-evaporable getter material that is preferable for use with the invention is zirconium-vanadium-iron  
           [0012]    Hydrogen is uniquely absorbed to the center of the getter material, while other gases stick to the getter surface until the getter is reactivated by heating it such the gases permeate to the center also. The non-evaporable getter material is preferably in the form of granular or other finely divided form such as pellets or grains, so that it has a larger volume of material than in coated strip form and the capacity for hydrogen becomes extremely large matching the outgassing of the flywheel for the life of the system.  
           [0013]    In one embodiment of the invention, the getter in the flywheel power source is reactivated throughout the life of the flywheel system by reheating it through use of an integral heater. The heater is preferably triggered by a timer instead of a vacuum gauge to increase the system reliability. The power for the heater can be taken directly from the energy stored in the flywheel. When the getter is being reactivated, some stored hydrogen becomes released and is later sorbed. Because the flywheel is constructed of steel, it has a high thermal conductivity, capacity and capability along with a lower operating tip speed because of its mass. This makes the release of hydrogen during reactivation not problematic when the flywheel is spinning. The vacuum can be regenerated without shutting the system down Although it is common to heat non-evaporable getters continuously in operation at a lower temperature than the activation temperature to increase the sorption rate of gases, this could potentially use up the getter in a flywheel system much too quickly by yielding a lower pressure than required for a shorter time.  
           [0014]    In a further embodiment of the invention, the outgassing of the steel flywheel can be reduced by performing the steel tempering operation in a vacuum prior to installation in the containment vessel. This reduces the quantity of non-evaporable getter required to maintain the vacuum The steel in the flywheel must be heat treated, quenched and tempered to achieve the high strength and toughness required for high speed operation. The tempering process involves heating the steel to a tempering temperature, in many cases between 800° F. and 1200° F. and holding it at that temperature for several hours. The brittle martensite internal structure produced during heat treatment becomes transformed to tempered martensite. Because the solubility of gases in metals is related to the temperature, the steel flywheel material can have much of its gas removed while being held at this high temperature. Vacuum furnaces are many times used to improve the mechanical properties and appearances of metals. In this case, the use of vacuum in the tempering process reduces the outgassing load of the steel flywheel in operation in vacuum. Upon removal from the tempering, water and other molecules become attached to the material surface and the flywheel outgassing would still benefit from some lower temperature heating during installation of the flywheel system vacuum. However, the longer term outgas rate can be reduced by the process.  
           [0015]    In yet a further embodiment of the invention, the electronics of the flywheel power source are used to signal an alarm and or prevent achieving or maintaining fill speed of the flywheel when the pressure in the vacuum chamber is found to be too high. This can be done either by simply current limiting to the motor power since the flywheel is constructed from steel and is less likely to overheat, or alternatively the electronics calculating the drag through use of the motor power, flywheel speed and flywheel acceleration. The calculation method allows the flywheel to detect any vacuum level problems and also any bearing or motor/generator problems prior to accelerating to full speed. The determination of excess drag for a given state of flywheel operation can also be used to trigger reactivation of the getter for improving the vacuum. 
       
    
    
     DESCRIPTION OF THE DRAWINGS  
       [0016]    [0016]FIG. 1 is a schematic elevation of a flywheel power source with a vacuum system in accordance with the invention;  
         [0017]    FIGS.  2 A- 2 C are graphs of the vacuum housing pressure, getter gas adsorption and getter pumping speed without a non-evaporable getter pump;  
         [0018]    [0018]FIG. 3A- 3 C are graphs of the vacuum housing pressure, getter gas adsorption and getter pumping speed with a non-evaporable getter pump that is activated but once;  
         [0019]    FIGS.  4 A- 4 C are graphs of the vacuum housing pressure, getter gas adsorption and getter pumping speed with a non-evaporable getter pump that is repeatedly reactivated 
     
    
     DESCRIPTION OF THE PREFERRED EMBODIMENT  
       [0020]    Tuning to the drawings, wherein like reference characters designate identical or corresponding parts, FIG. 1 shows a flywheel power source  30  that has been disconnected from an external initial vacuum-pumping system  20 . In accordance with the invention, the flywheel power source  30  uses a steel flywheel  31  that is enclosed inside a metal chamber  32  for storing energy. The flywheel steel is preferably an alloy for high strength and deep hardenability with 4340 being preferred for having relatively good properties at low cost. The chamber is maintained internally at a low pressure for reduction of aerodynamic drag on the flywheel  31 . The container  32  can be constructed of steel, stainless steel aluminum or of other metals, however carbon steel is preferred for low cost. Although some prior art flywheel systems have used ‘O’ rings or epoxy bonding to seal the vacuum, the vacuum chamber of the invention is preferably sealed using metal welding, brazing or soldering for lower outgassing and gas permeability from the outside of the chamber. Metal gasket seals could be employed but these are expensive in large diameters needed to allow insertion of the flywheel.  
         [0021]    The flywheel is supported for rotation about a vertical axis using upper and lower bearings  38  and  39 . The bearings  38 ,  39  can be magnetic, as shown, mechanical or a combination of the two. Use of magnetic bearings has the benefit of not requiring lubricants that could contaminate the vacuum along with a long life without any wear.  
         [0022]    To accelerate and decelerate the flywheel  31  for storing and retrieving energy, the flywheel uses an attached motor/generator  41 . The motor/generator is preferably of the brushless type so there are no wearing surfaces of generation of particles inside the chamber  32 . As shown, the motor/generator is a 3-phase permanent magnet type for high efficiency, however reluctance motor/generator designs can also be used as is well known in the art. It is also contemplated that a separate motor and generator could also be used as well as an integrated flywheel and motor/generator. The. motor generator  41  uses permanent magnets  42  that are aced to the flywheel shaft  40  using a thin high strength sleeve, not shown. Rotational torque is generated in cooperation with the magnets  42  using a surrounding laminated ferromagnetic stator  43 . The laminations in motor stators are used support the windings mechanically and provide a relatively efficient magnetic flux path for the rotating magnetic fields. Air core motor/generators are also commonly employed in flywheel systems for the purpose of achieving the highest levels of efficiency due to a lack of magnetic iron losses and they also have reduced inductances for increased power delivery response time. Unfortunately, air core motor/generators typically require use of a plastic support structure along with excessive potting to hold the windings and eliminate the losses. These materials outgass significantly and are therefore a laminated ferromagnetic core type motor/generator is preferred for use with the invention.  
         [0023]    The flywheel power source  30  preferably also includes a separate non-evacuated chamber  47  for malting electrical connections and for potential placement of some electronics, not shown Power and control wires  48  from the flywheel chamber exit to the non-evacuated chamber  47  through use of electrical feedthroughs  35 . Electrical feedthroughs  35  are hermetically sealed connections that allow electrical power to pass into vacuum housing  32  without causing the vacuum to be lost. A vacuum inlet port  36  is used for initially pulling vacuum on the flywheel chamber  32  using the external vacuum pumping system  20 . The vacuum inlet port  36  is preferably fabricated from copper tubing for easy crimping and sealing of the vacuum although stainless steel tubing could be used. The port  36  is originally part of connection tube  25 , but is crimped off and cut once vacuum-pumping system  20  is no longer required. Crimping off vacuum inlet port  36  from connection tube  25  is the preferred method of disconnecting energy storage flywheel system  30  from vacuum-pumping system  20 . Alternatively, a valve could be attached on to the vacuum inlet port  36  and this could be used to seal the vacuum but with more cost.  
         [0024]    The flywheel power source  30  can have its control and power conversion electronics  45  inside the non-evacuated chamber  47  or located separately as shown. Interconnection cabling  44  connects the flywheel power source  30  to the control electronics  45  while interface cabling  46  connects the power electronics to utility or auxiliary power sources, not shown. The power electronics  45  converts power from the utility power to energy stored the rotating flywheel  31  and vice-versa The power electronics  45  also control the rate of energy storage and delivery as well as monitor the overall health of the power source  30 .  
         [0025]    In accordance with the invention, the vacuum inside the flywheel chamber  32  is maintained against the outgassing of the flywheel, chamber and other internal components, after the initial vacuum pumping system  20  has been disconnected, through the use of a chemical type metal alloy non-evaporable getter in the form of a getter pump  37 . The non-evaporable getter pump  37  contains preferably pills or pellets of an alloy of special metal alloys that are effective in absorbing hydrogen via solid solution formation and adsorbing various gas species by forming molecular compounds, e.g., nitrides, oxides and carbides, at room temperature. The great affinity to absorb hydrogen by the getter directly matches and cooperates with the majority composed hydrogen gas that outgasses from the flywheel  31  and also the vacuum chamber  32 . Use of a composite flywheel would outgas much water vapor and other larger molecules which are not directly absorbed by the non-evaporable getter. Besides the much lower and matched outgassing and sorption with use of a steel flywheel, the steel flywheel also rotates at a lower tip speed, has a higher thermal conductivity and temperature capability than a composite flywheel. Thus, in a steel flywheel system; the main concern for the vacuum level is reduction of drag power loss instead of preventing a surface overheating failure. The required level of vacuum is approximately 10 −2  Torr for a steel flywheel compared to 10 −3  for a composite flywheel which makes the vacuum maintenance another ten times easier.  
         [0026]    Alternatively to use of a non-evaporable getter, use of a evaporable getter would have difficulty in keeping up with the higher outgassing rate and also potentially with surviving the life of the flywheel power source. A common physical type getter such as zeolite would also not be effective even in large quantities due to its inability to sorb the small molecules of hydrogen A preferred chemical type non-evaporable getter material for use in the vacuum system is a zirconium-vanadium-iron alloy, in particular an alloy that is 70 weight percent (70 w %) zirconium, 24.6 w % vanadium and 5.4 w % iron, denoted as ST707™ by SAES Getters S.p.A. To activate ST707™ it is heated to 450° C. for 15 minutes within a vacuum enclosure at a pressure of 10 −4  torr or below. A zirconium-aluminum alloy, in particular an alloy that is 84 w % zirconium and 16 w % aluminum denoted as ST 101™ by SAES Getters S.p.A, could be used but it is not preferred because of its very high activation temperature (&gt;700° C.). The use of alloying more than one metal allows the getter to be activated at a lower temperature than a single material would be. Alloys of three or more metals generally, depending on the metals, provide lower activation temperatures that are more easily achieved and are thus preferred..  
         [0027]    In one embodiment of the invention, the activation of the getter is done using a heater that is integral with the flywheel power source. The pellets in the pump would be placed in contact with an electric heater. By having a heater integral with the flywheel the getter material can be reactivated when the pressure in the vacuum chamber becomes too high, thereby extending the life of the flywheel system. In the activation process, the non-inert gas species, excluding hydrogen, that have formed molecular compounds with the getter material diffuse from the surface of the getter material into its center, leaving chemically reactive sites on the sure. The getter surface now “activated” is able to adsorb additional non-inert gas species, excluding hydrogen.  
         [0028]    During activation, hydrogen is desorbed from the getter material and is released into vacuum housing  32 . However, that hydrogen can be reabsorbed by NEG pump  37  after the activation process has been completed and the getter material cools. When some hydrogen desorbs in the reactivation process, the hydrogen partial pressure inside the flywheel chamber  32  can increase. However, hydrogen is a small molecule and exerts relatively little drag, and, because the flywheel is constructed of steel, the flywheel is not in danger of a catastrophic failure. Steel has a much higher thermal conductivity to transfer surface gas friction heating, a larger thermal mass to absorb the heat energy and also hundreds of degrees higher temperature capability than composites. The steel flywheel also typically operates with a slower peripheral speed than the composite flywheel so less heat is generated. Because of this, the vacuum system of the flywheel power source can safely be regenerated without discharging the flywheel.  
         [0029]    Although a getter material is available in the form of thin, coated strips, which typically preferred because they can pump faster per amount of material due to greater exposed surface area, use of getter material in the form of pellets minimizes the cost and also increases the total gas sorbing capacity over the life of the flywheel system. In one embodiment of the invention, the non-evaporable getter of the steel flywheel system is reactivated through the triggering from a timer. Because vacuum gauges such as thermocouple type and ion gauges add extra cost and are likely unreliable to last the desired life the flywheel power source, they are preferably eliminated. A timer is then used to trigger reactivation of the getter which is made possible by knowing the outgas rates of the different gas species inside the flywheel chamber. A residual gas analyzer, not shown, temporarily connected to the inlet port  36  can perform this function.  
         [0030]    In a further embodiment of the invention, the flywheel electronics  45  are used to maintaining or achieving full flywheel speed if the chamber pressure or drag is too high. Because the flywheel is constructed of steel and unlikely to overheat, the speed limiting can be done using simple current liming to the motor. Another method that can be employed is for the electronics to calculate if the drag is higher than allowable at any given speed by measuring the motor power or current, flywheel speed and flywheel acceleration. This method can determine an inadequate vacuum prior to achieving full speed or alternatively detect increased drag resulting from other components including the motor/generator or bearings. The detection of increased drag can be used to trigger an alarm and even be used to trigger reactivation of the vacuum.  
         [0031]    In order to initially establish a vacuum inside the chamber  32 , the external vacuum pumping system  20  is preferably used. This allows establishment of an initial high vacuum and prevents unnecessarily using up the getter pump  37 . The vacuum-pumping system  20  can be comprised of combined diaphragm and turbo-drag pump  21 , ultra-high vacuum Bayard-Alpert ion gauge  22 , right-angle valve  23 , bellows  24  and connection tube  25 . Combined oil-free diaphragm and turbo-drag pump  21 , are preferably chosen to avoid the possibility of oil contamination of energy storage flywheel system  30  via backstreaming. Other oil free pumps could also be used and oil type pumps might be applicable if a sufficient trap could be made, however this is less preferable. The vacuum pumping system  20  reduces the pressure in energy storage flywheel system  20  from 1 atmosphere (760 torr) to 10 −6  torr. Ultra-high vacuum Bayard-Alpert ion gauge  22  is used to measure the pressure of the system. Right-angle valve  23  is used to isolate ultra-high vacuum Bayard-Alpert ion gauge  22  from atmospheric pressure when vacuum inlet port  36  is crimped from connection tube  25 . If the gauge were to be exposed to atmospheric pressure while energized, it would be destroyed. In addition, right-angle valve  23  minimizes the amount of water-vapor contamination to which vacuum-pumping system  20  is exposed, thereby improving the efficiency of vacuum-pumping system  20 . Bellows  24  is a flexible-piping element that is used to avoid problems associated with the misalignment between the two independent systems  20  and  30 . The function of connection tube  25  was previously described.  
         [0032]    The following describes the procedure for establishing vacuum in the flywheel power source  30 . Each component of energy storage flywheel system  30  must be thoroughly cleaned during assembly to remove all sources of contamination, in particular all greases and oils. Once the energy storage flywheel system  30  is assembled and is connected to vacuum-pumping system  20 , it is preferable if energy storage flywheel system  30  is heated uniformly to the maxim temperature to which its components can withstand without loss or degradation of their performance. This elevated temperature “bakeout” will increase the mobility of gas molecules on the internal free surfaces of energy storage wheel system  30 , thereby increasing their desorption rate. Once the temperature within energy storage flywheel system  30  is uniform, vacuum pump  21  is used to reduce the pressures within vacuum housing  32 . The higher initial desorption rate of this vacuum baking process increases the number of gas molecules that can be removed by vacuum pump  21 , thereby decreasing the gas desorption rate after vacuum-pumping system  20  has been disconnected.  
         [0033]    Typically, vacuum chambers are vacuum baked at temperatures of 250° C. or greater to reduce, in particular, the water desorption rate to below 10 −13  torr-liters per second per square centimeter of surface area (3.5 million gas molecules per second per square centimeter). However, the motor generator and magnetic bearings, if used, may utilize low cost, high-field strength neodymium-iron-boron magnets. Temperatures above 120° C. can damage and even demagnetize the magnets. Thus, if neodymium-iron-boron magnets are used the maximum bakeout temperature of energy storage flywheel system  30  is linked to 120° C. The water desorption rate of a vacuum chamber after a vacuum bakeout at 120° C. is approximately 20 times greater than the water desorption rate of a 250° C. vacuum bakeout. This higher desorption rate would therefore require 20 times the amount of getter material to be used in NEG pump  37 . Once energy storage flywheel system  30  has been evacuated to a pressure level of 10 −6  torr and a long-term gas desorption rate has been determined, non-evaporable getter pump  37  is “activated.” It is preferable to activate non-evaporable getter pump  37  while vacuum pump  21  is being utilized to reduce the pressure within system  30 . The pressure in vacuum housing  32  should be I torr or below before activation. In this invention, it is preferable if a substantial portion of the hydrogen that is desorbed from the getter material during activation is removed from energy storage flywheel system  30  by vacuum pump  21  rather than readsorbed by NEG pump  37 . This process will maximize the absorption capacity of non-evaporable getter pump  37 . Once non-evaporable getter pump  37  has been activated, right-angle valve  23  is closed to isolate ultra-high vacuum Bayard-Alpert ion gauge  22 . Connection tube  25  is then crimped off.  
         [0034]    In another embodiment of the invention, the long term outgassing of the flywheel is reduced prior to being assembled in the power source  30 . It is preferable to minimize the gas desorption rate of energy storage flywheel system  30  and thereby minimum the size and cost of non-evaporable getter pump  37 . As flywheel  31  comprises at least a quarter of the total surface area of system  30 , minimization of its gas desorption rate can effectively reduce the gas desorption rate of the entire system Flywheel  31  is preferably 4340, a high-strength alloy steel, or one of its variations. To obtain high strength in the flywheel, the steel must be heat-treated and quenched. The raw round must first be rough machined to remove the carburized scale off of the surface prior to heat treatment. Removing roughly 0.300 inches from the surface ensures removal of any seams in the steel that can potentially crack the round upon quenching. Heat treatment is then usually performed at 1500-1600° F. for roughly 30 minutes per inch in diameter. The quenching method depends on the alloy of steel. Oil or liquid polymer quenching is typical for 4340.  
         [0035]    After quenching, the round must be tempered to increase the toughness of the steel and to relieve internal residual stresses. In accordance with the invention, the steel tempering can be combined with the outgas baking of the flywheel for the benefits of significantly more gas removal and reduction of the flywheel outgassing in operation at the same time as the steel toughness is being increased. The tempering is therefore done in a vacuum. The pressure in the chamber is preferably 10 −4  torr, or lower, so as to sufficiently remove the gases from the steel. At the elevated tempering temperature, typically between 800 and 1200 F., the mobility of the gasses in the steel is greatly increased. When combined with the low chamber pressure, a high rate of gas desorption from the metal occurs. Vacuum furnaces to conduct this procedure are readily available at many heat-treating companies although they are normally used for different purposes. Vacuum furnaces have typically been used for solution treating stainless steels or for bright hardening, which yields an attractive and improved surface that would otherwise be discolored from conventional atmospheric heat treatment. The tempering of the flywheel round is preferably conducted for roughly 1 hour per inch of diameter to insure adequate heating and equalizing of the internal structure. For a 4340 steel round, 1000° F. tempering temperature yields a good combination of strength and toughness of the steel. At this temperature, the gas desorption rate is expected to be roughly 100 times more than if vacuum baking was done later at only 800° F.  
         [0036]    Vacuum furnaces typically heat parts under vacuum and then cool the parts by gas circulation. Nitrogen or argon is typically used. For flywheels, argon is preferably used because all noble gases are completely insoluble in metals and thus no further gas will be absorbed during cool down from the high temperature. However, argon is much more expensive than nitrogen. The cool down time can be as short as a couple of minutes compared to the more than 10 hours if the steel flywheel material was cooled under vacuum. Therefore if nitrogen is used as the cooling gas, it is unlikely that a significant amount will be absorbed into the metal bulk When steel and other nitride-forming metals are heated in nitrogen, the amount of nitrogen, which act enters into solution, is of the order of 1 per cent or less by weight, and there is no tendency to form a nitride. Hydrogen, carbon monoxide and carbon dioxide typically diffuse from the bulk at 2250° F. and lower, whereas the removal of nitrogen and oxygen requires much higher temperatures. The temperature where this cooling could also be done in vacuum by letting the steel round cool for many hours but it is expensive to use the vacuum furnace for such a long period of time. The primary gases removed from the steel during the treatment are hydrogen, carbon monoxide and carbon dioxide. After the flywheel preparation treatment is completed, the steel round is then machined into flywheel  31 . This flywheel preparation treatment could also be applied to other components of the flywheel power source that also require quenching and tempering to meet their required service properties.  
         [0037]    Assuming that windage losses are acceptable for a given flywheel system at a maximum vacuum chamber pressure of 10 −2  Torr, FIGS.  2 A-C,  3 A-C and  4 A-C illustrate the advantage of integrated and reactivatable non-evaporable getter pump of the invention and the benefits of repeatedly reactivating the getter material during the life of the flywheel power source  30 . As described prior, the hydrogen is absorbed directly into the center of the getter pellets. However, the gasses of other species with larger molecules are adsorbed onto the getter surface. Once the getter surface is fill, the pumping action slows or stops. The getter then needs to be reactivated by heating which allows the larger molecules to be absorbed also to the center of the getter material, leaving fresh surfaces for adsorption One of the major gas components that outgases from the flywheel and chamber, and is not absorbed by the getter like hydrogen, is carbon monoxide.  
         [0038]    [0038]FIGS. 2A, 3A and  4 A show plots of the chamber pressure from outgassing from the flywheel and internal surfaces of the chamber along with the quantity of gas that is adsorbed by the getter material and the getter pumping speed of the gas. FIGS.  2 A-C shows the case of a flywheel power source without the getter pump and not in accordance with the invention Consequently, the amount of gas adsorbed remains at 0 torr-liters and the speed at which it is adsorbed is 0 liters per hour. More importantly, the vacuum chamber reaches the maximum chosen acceptable pressure of 10 −2  Torr in approximately 90 hours, far less than the desired 20 years (approximately 175000 hours). FIGS.  3 A-C show the same flywheel power source with the inclusion of the non-evaporable getter pump in accordance with the invention. The pressure in the chamber quickly drops from 10 −6  to 10 −9  Torr after the non-evaporable getter is activated. It remains at this pressure for more than 1400 hours until the surface are of the getter material becomes saturated, as indicated by the rapid drop off in pumping speed. Approximately 90 hours after the surface of the getter material becomes saturated, the maximum acceptable pressure is reached. While the pressure in the chamber remains below the acceptable pressure for a period of time that is 15 times longer that without the getter, the duration is still insufficient using the chosen conditions.  
         [0039]    It is possible to increase the amount of getter material from a few grams to several kilograms and thereby achieve the 20 year life, but at higher than desirable cost. It is therefore preferable to regularly reactivate the getter material in the flywheel power source. This differs from the application of getters in typical static systems such as vacuum bottles where they are activated only once and the heat source is typically external and removed from the product after activation. For other applications that allow reactivation of non-evaporable getters it is also usually only done for process applications where the getter material is easily replaceable after being exhausted and not in a sealed commercial products, such as a flywheel systems. FIGS.  4 A-C show the flywheel power source with the non-evaporable getter pump in accordance with the invention and using the further embodiment of regular reactivation using an integral heater. As illustrated, once the pressure reaches the maximum acceptable pressure, the getter material is reactivated and the pressure returns to a quasi-equilibrium with adequate vacuum level. The getter material can be regularly reactivated to achieve the 20 year life or until exhausted.  
         [0040]    Obviously, numerous modifications and variations of the described preferred embodiment are possible and will occur to those skilled in the art in light of this disclosure of the invention. Accordingly, I intend that these modifications and variations, and the equivalents thereof be included within the spirit and scope of the invention as defined in the following claims, wherein I claim: