This invention relates generally to chemicals used as propellants and, more particularly, propellants having relatively high specific impulse.
One enduring problem in spacecraft design is to minimize the non-payload weight of the spacecraft, i.e. the mass of the spacecraft structure and the expendables (e.g. propellant) stored on the spacecraft. This problem arises because every extra kilogram (kg) of mass in the spacecraft means less mass allocation available for the payload. Given that the cost of delivering payloads to space is high (from about $10K/kg for bulk deliveries to low Earth orbit to upwards of $1 million/kg for hardware soft-landed on Mars) there is a powerful incentive to reduce the mass of the payloads, the launch vehicle, the spacecraft, the constituent components of these devices, and the onboard expendables. Another enduring problem is the need to minimize the total volume of the spacecraft. Similar to the situation with the mass of the spacecraft, every cubic centimeter devoted to the spacecraft reduces the volume available to the payload. Thus, a need also exists to minimize the volume devoted to the propellants and spacecraft structure.
A common way to address the mass and volume challenges is through the development of new propellants. New propellants, though, must meet or exceed the performance requirements associated with the propellants that are being replaced. Also, the new propellants must be chemically compatible with existing fluid systems and rocket engines. If the new propellants are not compatible, then the systems and engines may need redevelopment in order to use the new propellant. Additionally, because of the harsh environments created within typical engines, each new propellant must be characterized for a variety of properties and conditions such as thermal stability, shock stability, ignition pressure surges, combustion instability, catalyst bed poisoning, and the like. Further, as chemicals, these propellants (and related ground systems) must meet stringent environmental regulations. For these reasons, the development of a new propellant is an expensive undertaking.
Thus, a need exists for propellants that are similar to existing propellants in every way, except that they have a different density.
The present invention provides, inter alia, methods of using isotopically enriched materials for propellants. The materials may be enriched in heavier isotopes and depleted in lighter isotopes. Enriching a propellant with heavier isotopes yields a propellant that is denser than the unenriched propellant. Otherwise the enriched propellant has properties that are identical to the properties of the unenriched propellant. These embodiments are well suited for use in electric propulsion systems.
In the alternative, the material may be enriched in lighter isotopes and depleted in heavier isotopes. Enriching a propellant with lighter isotopes yields a propellant that is less dense than the unenriched propellant. Otherwise the enriched propellant has properties that are identical to the properties of the unenriched propellant. These embodiments are well suited for use with thermal (chemical) propulsion systems. Additionally, the present invention provides mobile platforms (e.g. satellites, spacecraft, or launch vehicles) that are adapted to use isotopically enriched propellants.
In a first preferred embodiment, the present invention provides a propellant. The propellant includes a portion of an element with two isotopes each having a natural abundance in the element. The portion of the element is enriched with the first isotope and is adapted to be ionized. Preferably, the element is xenon.
In a second preferred embodiment, the present invention provides a method of operating a mobile platform. The method includes enriching a portion of an element with a first isotope of the element, ionizing the enriched portion of the element, and using the enriched and ionized portion of the element to produce thrust. Preferably, the method includes sizing a propellant tank based on the enriched portion of the element. Also, the enriching of the propellant may densify the propellant or may increase the specific impulse of the ionized propellant. Further, the enriched propellant may be stored on the mobile platform. The method preferably includes performing a cost/benefit analysis to determine an enrichment level for the propellant.
In a third preferred embodiment, the present invention provides a mobile platform including a rocket engine and a propellant container that is sized and dimensioned to store a propellant. The propellant includes a portion of an element with two isotopes each having a natural abundance in the element. The portion of the element is enriched with the first of the isotopes and is adapted to be ionized. The rocket engine communicates with the propellant container to receive and ionize the enriched propellant. Preferably, the mobile platform is a geosynchronous satellite with a xenon electric propulsion system.
In yet another preferred embodiment, the present invention provides a mobile platform. The mobile platform includes a propellant container and a rocket engine. The propellant container is sized and dimensioned to store a first mass of a propellant that has natural isotopic abundances. The container, though, stores a second mass of a propellant that is enriched in an isotope of the propellant. Preferably, the density of the enriched propellant is greater than the density of the natural propellant. Additionally, the rocket engine can ionize the enriched propellant.
In still another preferred embodiment, the present invention provides a propellant combination. The propellant combination includes portions of a first and a second element. The portion of the first element is isotopically enriched and is adapted to combine with the portion of the second element. Preferably, the first element is chlorine, boron, or bromine.
In another preferred embodiment, the present invention provides still another mobile platform. The mobile platform of the present invention includes two propellant containers and a rocket engine. The first of the containers is sized and dimensioned to store a first isotopically enriched propellant while the second container is sized and dimensioned to store a second propellant. The rocket engine communicates with both propellant containers and is adapted to chemically combine the propellants.
Yet another mobile platform is provided by the present invention in another preferred embodiment. The mobile platform of the current embodiment includes two propellant containers and a rocket engine. Both propellant containers are sized and dimensioned to store their respective propellants that have natural isotopic abundances. The rocket engine communicates with the propellant containers to receive and combine the propellants. However, one of the propellants stored in the containers is isotopically enriched.
Further features and advantages of the present invention, as well as the structure and operation of various embodiments of the present invention, are described in detail below with reference to the accompanying drawings.
The accompanying drawings, which are incorporated in and form a part of the specification, illustrate embodiments of the present invention and together with the description, serve to explain the principles of the invention. In the drawings:
Referring to the accompanying drawings in which like reference numbers indicate like elements,
The exemplary satellite 10 illustrated by
The bus 14, however, cannot be neglected because it contains many systems that support the payload 12. These support systems include a solar energy subsystem 16, a structural subsystem 18, and a propulsion system 20. During ascent from Earth on a launch vehicle (such as the Delta IV, Evolved, Expendable, Launch Vehicle that is also available from The Boeing Company), the structural subsystem 18 carries the loads imposed on the satellite 10. On orbit, the power subsystem supplies 16 the payload 12 and bus 14 with regulated power so that the satellite 10 can accomplish its mission.
The propulsion system 20 supports the payload 12 by allowing the satellite 10 to maneuver for such purposes as stationkeeping, orbital adjustments, and avoidance of space debris. To accomplish these maneuvers, the propulsion system 20 includes propellant tanks 22 and rocket engines 24 connected to the tanks 22 by propellant lines (not shown). Recently, The Boeing Company has outfitted many satellites 10 with Xenon Ion Propulsion Systems (XIPS) 20. A typical XIPS system 20 is illustrated schematically in
With reference again to
In accordance with the principles of the present invention, an alternative to trading mission life for payload 12 mass is using isotopic enrichment to increase the density of the propellant(s). Since the propellant is made denser by enrichment, the propellant tanks 22 and associated structure can be smaller and less massive than conventional propellant tanks and associated structure. The increase in density operates to decrease the size of the propellant tanks as follows. The approximate delta velocity (ΔV) imparted to a vehicle by a mass of propellant (Mprop) is given by
ΔV=Vex*ln(minitial/mfinal) where
Vex is the exhaust gas velocity, minitial is the initial mass of the vehicle, and mfinal is the final mass of the vehicle. Of course
minitial=mfinal+mpropellant.
Therefore, for a given delta velocity and a given exhaust velocity, a certain mass of propellant will be required. If the propellant is an isotopically densified gaseous propellant, then fewer atoms (or molecules) of the propellant are required to yield the required propellant mass. As a result, fewer moles of the gaseous propellant are required. Since the volume of a quantity of gas depends on the number of moles of the gas, the size of the propellant tank (for a given gas, pressure, and temperature) is reduced accordingly for the densified propellant as compared with the same propellant that has not been isotopically densified, Moreover, the resulting increase in the average mass of the propellant atoms thereby lowers the energy required to ionize a given mass of propellant. Because fewer ions are needed to yield the same propellant mass, the invention improves the efficiency of ion and plasma-dynamic thrusters 24 typically used in electric propulsion systems 20. The increased efficiency, in turn, reduces the power system's mass which allows the satellite to have yet smaller tanks or a longer maneuvering lifetime. Moreover, as the propellant tank decrease in size, the moment of inertia of the vehicle decreases. As a result, the size of the attitude control system and the amount of propellant used for attitude control also decreases.
Those skilled in the art will also understand that the denser propellants provided by the present invention are more efficient at converting the electric energy (provided by an ion engine) to exhaust gas kinetic energy. This result occurs because the ionization energy per atom of propellant remains the same while the kinetic energy per atom for a given exhaust velocity increases with increasing atomic weight. In some applications it may be desirable to increase the voltage of the accelerating grid of the ion engine to impart the increased kinetic energy to the exhaust ions. The increase in the grid voltage can be determined as follows. First exhaust gas velocity, Vex, is given by:
Vex=√{square root over ((2*E/m))} and E=qV
Where E is the kinetic energy, m is the ion mass, q is the amount of charge on the exhaust gas, and V is the grid potential. Since higher mass requires proportionally higher kinetic energy, the grid potential (V) increases in proportion to the ion mass. Even though there may be an increase in the weight of the electrical insulation (to account for the somewhat higher voltage), the higher voltage also means that the necessary current will decrease. So any increase in the mass of the insulation will be more than offset by the smaller radiator required to reject waste heat (generated by IR2 resistance heating) from the system. On the other hand, the propellant for an ion engine can be enriched with a lighter isotope which would give a higher Isp at the same voltage, but would make the propellant less dense thereby offsetting some of the weight savings associated with the higher Isp.
Thus, according to a preferred embodiment of the present invention, at least one element that is a constituent of a propellant is enriched with at least one heavier isotope. More particularly, those elements that
1.) have a large relative variance in their isotopic mass and
2.) have enough of both light and heavy isotopes that changing the concentration of the isotopes in favor of the heavier isotopes causes a change in density of the element are isotopically enriched for use as a propellant. Of course, the present invention is not limited to just those cases in which the enrichment can be made economically because, in some applications, the benefits of a density increase may be of greater moment than mere economic considerations. For instance, isotopic densification may allow some missions that would otherwise not be possible.
In particular, xenon, lithium, and carbon are well suited for isotopic enrichment to improve the propulsion system 20 performance. More particularly, xenon, the propellant used in The Boeing Company's 702 satellites 10 (see
Also, lithium has two isotopes 6Li and 7Li with natural abundances of, respectively, 7.59% and 92.41%. Thus, a density increase of about 1% is achievable. Further, lithium has been tested as a propellant for electric thrusters (e.g. engines 24) thereby providing a high level of assurance that enriched lithium should perform well as a propellant.
Similarly, carbon has been proposed as a candidate propellant for future ion propulsion systems 20. The particular form of carbon proposed for this use is known as Buckminsterfullerene (e.g. C60 or C70). Buckminsterfullerene possesses a large molecular mass and low ionization energy which makes it a good candidate for isotopic enrichment. Carbon also has two isotopes 12C (with a natural isotopic abundance of 98.89%) and 13C (natural abundance of 1.11%). Further, the natural abundance of the heavier 13C isotope is large enough that enrichment of carbon by a factor of ten is practicable and yields almost a 1% increase in density.
Turning now to
To provide for these lighter exhaust gases, the current embodiment includes at least one propellant that is isotopically enriched in a lighter isotope. When the raw propellants combine in a rocket engine, the resulting atoms and molecules that include the lighter isotopes become constituents of the exhaust gas. As a result, the exhaust gas has a lower average molecular weight than exhaust gases produced from conventional propellants. Thus, the Isp of the propellant combinations (and engines adapted to use the isotopically enriched propellants) are higher than the specific impulses of previously available propellant combinations. Moreover, because of the improved Isp, a smaller mass of propellant is needed to achieve the same delta-V as achieved with unenriched propellant.
Exemplary liquid propellants that contain elements suitable for isotopic lightening include chlorine trifluoride (ClF3), triethylboron (C6H15B), bromine pentafluoride (BrF5), and pantaborane (B5H9). The exemplary elements include boron, bromine, and chlorine which have the following isotopes (and natural abundances):
In addition to enriched liquid propellants, the present invention also provides enriched solid propellants. In particular, a common solid propellant ammonium perchlorate used in the SRBs 106 and 108 of the Space Shuttle 100 (
If it is desired to provide the same total impulse as provided by the non lightened propellant then additional moles (and volume) of propellant will be required. The reason that lightening the propellant reduces the total impulse is that the impulse depends on the mass of the exhaust gas as shown by the following equation:
vex=sqrt(2*Ec/mavg)
where vex is the exhaust gas velocity, Ec is the combustion energy per molecule, and mavg is the average mass of molecules in the exhaust. Further, the total impulse depends on the average mass as follows:
P=N*mavg*vex
Or, rewriting the equation:
P=N*sqrt(2*Ec*mavg)
where N is the number of molecules in the exhaust. Thus, if mavg is 0.66% lower (which it will be if the chlorine is enriched to 87.5% 35Cl), N will need to increase by about 0.33% to get the same total impulse, P. The net result is that, even with the desire to maintain the total impulse available, a mass of enriched propellant approximately equal to 99.67% of the mass of the un-enriched propellant is required. Thus, the weight savings per Shuttle flight will still be about 2635 pounds. An additional savings will also be available because propellant is not required to lift the 2635 pounds saved. Thus, the savings will be somewhat more than 2635 pounds.
Turning now to
Preferably, once the elements are enriched, the compounds constituting the propellant(s) may be manufactured as in operation 206. Since the enriched elements, and compounds, behave similarly to those that are not enriched, the manufacture of the propellants can be via conventional systems and processes. In operation 208 the enriched propellant(s) can be loaded on to a mobile platform (or ground based) propellant tank for storage. When it is desired to use the propellant to produce thrust, appropriate steps are taken to either ionize, or chemically combine, the propellant(s) as in, respectively, operations 210 and 212. Once ionized, or chemically combined, the resulting exhaust gas can then be expelled from an engine to produce the desire thrust. See operation 214.
Various modifications could be made in the constructions and methods described without departing from the scope of the invention. All matter contained in the description or shown in the accompanying drawings shall be interpreted as illustrative rather than limiting. Thus, the breadth and scope of the present invention should not be limited by any exemplary embodiment, but should be defined only in accordance with the following claims and their equivalents.
This application is a continuation in part of co-owned, co-pending U.S. patent application Ser. No. 10/988,055, filed by Tillotson on Nov. 12, 2004, entitled Isotopic Lightening, and incorporated in this application as if set forth in full.
Number | Date | Country | |
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Parent | 10988055 | Nov 2004 | US |
Child | 11013232 | Dec 2004 | US |