EP0269642A1 - Rocket propellant charge with negative pressure exponent - Google Patents
Rocket propellant charge with negative pressure exponentInfo
- Publication number
- EP0269642A1 EP0269642A1 EP87901295A EP87901295A EP0269642A1 EP 0269642 A1 EP0269642 A1 EP 0269642A1 EP 87901295 A EP87901295 A EP 87901295A EP 87901295 A EP87901295 A EP 87901295A EP 0269642 A1 EP0269642 A1 EP 0269642A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- charge
- propellant
- burning
- core
- rate
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
Classifications
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F02—COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
- F02K—JET-PROPULSION PLANTS
- F02K9/00—Rocket-engine plants, i.e. plants carrying both fuel and oxidant therefor; Control thereof
- F02K9/08—Rocket-engine plants, i.e. plants carrying both fuel and oxidant therefor; Control thereof using solid propellants
- F02K9/10—Shape or structure of solid propellant charges
- F02K9/12—Shape or structure of solid propellant charges made of two or more portions burning at different rates or having different characteristics
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F02—COMBUSTION ENGINES; HOT-GAS OR COMBUSTION-PRODUCT ENGINE PLANTS
- F02K—JET-PROPULSION PLANTS
- F02K9/00—Rocket-engine plants, i.e. plants carrying both fuel and oxidant therefor; Control thereof
- F02K9/08—Rocket-engine plants, i.e. plants carrying both fuel and oxidant therefor; Control thereof using solid propellants
- F02K9/26—Burning control
-
- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F05—INDEXING SCHEMES RELATING TO ENGINES OR PUMPS IN VARIOUS SUBCLASSES OF CLASSES F01-F04
- F05D—INDEXING SCHEME FOR ASPECTS RELATING TO NON-POSITIVE-DISPLACEMENT MACHINES OR ENGINES, GAS-TURBINES OR JET-PROPULSION PLANTS
- F05D2200/00—Mathematical features
- F05D2200/20—Special functions
- F05D2200/24—Special functions exponential
Definitions
- This invention relates to a novel method of making a solid propellant rocket motor or gas generator charge with a negative burning rate pressure exponent (nega ⁇ tive dr, /dP) .
- the negative exponent characteristic 5. can be obtained independently of burning rate and other bulk propellant properties allowing impulse, flame temperature, signature, mechanical properties to be chosen as required.
- Propellant burning rates are usually described as a function of pressure using Vieille's Law
- variable 15 area nozzles especially for gas generator applications, see Cohen, J. , Landers, L.C. and Lou, R.L., "Minimum- Response-Delay Controllable Solid-Propellant Gas Generators". J. Spacecraft, Vol. 14, No. 5, May 1977.
- a few examples of negative exponent propellants have been created as shown in Cohen et al above. However their ballistic properties are not fully understood. In the few examples of negative 5. exponent propellants, the negative exponent character ⁇ istic is usually gained at the expense of other desir ⁇ able ballistic properties.
- liquid fuels usually com ⁇ prised of separate reservoirs of oxidizing and oxid- izable materials, or solid fuels, usually comprised of a solid state mixture of oxidizing and oxidizable materials formed into a single fuel grain mass.
- fuel rockets depend upon burning which occurs with contact of the oxidizing and oxidizable materials, such burning is initiated by a small source of external heat while solid fuel rockets depend upon burning which is initiated by elevating the surface temperature
- the burning rate of a solid fuel rocket can be increased by preheating or raising the temper ⁇ ature of small areas in the fuel mass just prior to
- Solid fuel rockets are preferred for military and long mission uses because of their inherent simplicity and avoidance of the complex plumbing, mixing and control elements required in liquid fuel rockets and because 5. of the ease and safety with which the rocket fuel, or grain, can be handled and stored for future use.
- the design parameters, fuel selection tradeoffs, and operating characteristics of solid fuel rockets are well known in the art and are, for example, discussed 10. in the referenced textbook "Rocket Propulsion Elements", 2d ed., by G.P. Sutton, and “Propellant Chemistry” by Stanley F. Sarver. The disclosure of these referenced texts is hereby incorporated by reference into the present specification.
- Modulation or termination of the thrust-producing reaction once grain burn has been commenced poses some difficulty in a solid fuel rocket; this difficulty is a characteristic of solid fuel rockets and makes it desirable to employ apparatus such as is described
- the present apparatus is principally concerned with thrust modulation or burn rate control during 30. the grain burn of a solid fuel rocket.
- thrust modulation might, for example, also be desirable in tailoring the orbit of a spacecraft, in trading thrust magnitude for thrust duration in a particular rocket application, or in balancing the thrust applied to a parallel rocket vehicle, especially during the initial liftoff, low air velocity, flight portion.
- Burn rate control can also be useful in achieving fixed levels of thrust which are independent of fuel temperature 5. variations resulting from atmospheric conditions.
- the Trotel apparatus contemplates the separation of fuel increments by inhibitor layers which
- Picquendar Another example of a solid fuel rocket control apparatus is found in the patent of J.E. Picquendar, U.S. 3,398,537 which also employs externally supplied electrical energy to maintain a supply of combustible fuel to the thrust generating reaction.
- the Picquendar invention employs a grain composition that is selected to give a non-self sustaining burn; this provides a rocket motor that is responsive to externally applied heat energy.
- the Okamoto apparatus is principally concerned with the improvements achievable using the fundamental buried filament concept without extension of this concept-into a modulation
- the patent of A.P. Ada son, U.S. 3,065,597 discloses a solid fuel rocket which is capable of the extinguishing and re-ignition functions through the use of burn chamber pressure control.
- the Adamson invention is based on 30. the concept of burn in the rocket pressure vessel being dependent upon the presence of pressures above a certain threshold for continuation.
- the Adamson apparatus provides an arrangement for increasing the burn chamber temperature by external means up to the threshold of burn maintenance when re-ignition of the rocket is desired.
- solid fuel rocket motor control Other examples of solid fuel rocket motor control are found in the patents of R.L. Rod, U.S. 3,066,482 and G.H. Messerly, U.S. 3,182,451 which concern respec ⁇ tively the achievement of increased burn rate by the 25. addition of acoustic or other transponder-supplied elastic wave (vibratory) energy for increasing fuel combustion efficiency and the use of fluids in conductive tubes which pass through the body of the fuel grain for controlling the temperature of the fuel grain. Additional examples of solid fuel rocket motor burn rate control are to be found in the Patents of R.H. hitesides, JR., U.S. 4,345,427 R.L. Glick, U.S. 3,381,476 and L.H. Caveny, U.S. 3,630,028 which concern 5. improvement in the control apparatus employed with a retractable filament burn rate control variations of the retractable filament structure and the addition of grain cutter elements to the ends of retractable filaments, respectively.
- the object of the present invention is to provide certain improvements to thrust control of a rocket, and this is achieved according to this invention by 5. using a small quantity of high-negative-exponent pro ⁇ pellants as core material in charges, the bulk of which are made of conventional propellant materials.
- the bulk propellant is chosen to provide ballistic properties such as specific impulse, density, smoke, 10. flame temperature or other properties important in a particular application and not necessarily available from the negative exponent propellant.
- the charge is constructed with a core, or several cores of propellant with an intrinsically negative
- pressure exponent with the bulk of the propellant made up of any propellant with a lower burning rate than the core propellant over the pressure range of interest.
- the core propellant burning rate range can be adjusted to give the desired value by a method
- the result is a charge with pressure and temper ⁇ ature sensititivies determined by the cores, burning rate determined by the acceleration, and specific impulse and other bulk properties determined by the 25. bulk propellant.
- Suitable core materials and burning rate acceler ⁇ ation methods are referred to herein, and the use of such a charge in a rocket motor or gas generator with a variable area nozzle device to give controllable thrust is included.
- the resultant charge has a burning rate and pressure sensitivity determined by the core negative 5.
- exponent material but other ballistic characteristics such as specific impulse, flame temperature and smoke are determined by the properties of the bulk material.
- the charge design incorporates fibres or strands of core material embedded in the matrix of the bulk 10. propellant and aligned generally perpendicular to the intended burning face.
- the cross sectional area of the cores can be very small compared to the overall burning surface area, so that the mean properties are essentially those of the bulk propellant.
- Cone burning is forced around each core by arrang ⁇ ing that the core material over the operating pressure range of the motor has a higher burning rate than that of the bulk material.
- the core regresses faster than the bulk 20. propellant, exposing extra surface area in the bulk propellant in the form of a cone around the core, until the cones from adjacent cores intersect.
- This quasi-steady-state surface consisting of a large number of intersecting cones, now regresses at a linear 25. rate equal to the core burn rate.
- the bulk propellant is consumed at exactly the same rate as if the original planar surface had re ⁇ gressed at the core burn rate.
- the charge produces a gas whose properties are those of 5.
- a gas generator would now be acting as if it were a constant pressure source, as the quasi-steady-state burning rate has a negative pressure exponent.
- FIG. 1 is a schematic central section of a charge showing the bulk propellant, the core, and the inhibitor,
- FIG. 2 is a graph of burning rate against pressure 25. showing typical negative exponent propellants reported by Cohen, Landers and Lou
- FIG. 3 is a graph similar to FIG. 2 showing the negative exponent Extruded Double Base propellant produced by the applicant,
- FIG. 4 is a view similar to FIG. 1 showing the 5. development of burning surface from initial flat end to approximately conical surface by use of an axial line of spaced cavities,
- FIG. 5 is a longitudinal section of a negative exponent strand of Bradfield cavitie's
- FIGS. 6 and 7 show a negative exponent charge in diagramatic longitudinal and cross section respect ⁇ ively using strands of Bradfield cavities dispersed as spaced burning control means arranged as a regular pattern through the charge, and
- FIG. 8 shows the negative exponent charge controlled by means of a variable area nozzle device.
- the inhibitor 1 surrounds the bulk propellant 2 which in turn has the core 3 axially dispersed within it.
- the bulk burning rate r, 5. is greater than the core burning rate r, , then the charge burns planar and is of no interest. Therefore consideration is restricted to the pressure range where r ⁇ r ⁇ .
- the volume of propellant consumed per unit time is the same as the original flat surface would consume if it were burning at the accelerated burning rate r, , rather than r, .
- the charge produces gas 20. at a rate which is determined by the core burning rate, but the nature of the gas produced is that of the bulk propellant.
- This invention makes use of the fact that, by extension, if the core propellant burns with a negative burning rate pressure exponent, the entire charge produces gas at a rate determined by that negative pressure exponent characteristic.
- Control calculations are discussed in Winch and Irvine who have calculated the transition times for a variety of conditions, in units of D/2r, , the time taken to burn from the centre of the cylinder to the edge.
- the time taken to burn from one cone to another 10. is always at least D/2r, , but for cones steeper that 45°, the time is never greater than .
- the charge burning rate, set by the core burning rate r may be required to vary J over a set rang °e r,bc_m,m. to r,b threadc_m,aontically modified J charg °e
- the limit of infinite negative exponent is a step
- Landers and Lou above refer to this ratio as the tum- 30. down ratio.
- the resulting charge will, at equilibrium, burn at a constant pressure, regardless of nozzle area.
- the variable nozzle area device must be appropriate for the burning° rate rang°e r,bcmax to r,bcm. , but within that range the motor will find an equilibrium burning rate and an equilibrium surface area to match the nozzle.
- a negative exponent charge with infinite exponent is identical to a constant pressure source.
- the chamber pressure is constant, independent of the nozzle area, while the mass low is directly proportional to the nozzle area.
- a charge with a central core of negative exponent propellant and a bulk of slower burning propellant of different properties will have a burning rate at equilibrium equal to the negative exponent propellant, and gas properties of the bulk propellant.
- This transition time, ⁇ to reach equilibrium will be a limiting feature of the charge performance.
- the transition time can be reduced by reducing the charge diameter, or increasing the minimum core burning rate.
- the transition time can be reduced by incorporating many cores of negative exponent propellant, equally 30. spaced across the grain. Winch and Irvine have discussed the use of multiple cores for forced cone burning to minimise the transition time and their results. For multiple cores, the transition time becomes Z/r b . where Z is the mean distance between cores. If the cores are optimally spaced, Z is approximately equal to D/N where N is the number of fibres.
- the significant parameter is the ratio of the transition time ⁇ to the maximum duration of firing
- Table 1 lists the ratio ⁇ /t f for various L/D ratios and various numbers of cores, N. It can be seen, for instance, that to achieve a value of ⁇ / f 0 f less than 0.05 requires an L/D greater than 4, with N greater than 20, while a ⁇ /t f of less than 0.01 needs high values of L/D,
- the propellants quoted vary from cool propellants for gas generator applications with n of -2.7, and
- the propellant has been extruded in 6 mm, 3 mm and 15. 1 mm diameter strands without difficulty, and no variation in burning rate characteristics has been observed with change in diameter. Strands of the propellant have been incorporated into small charges by the applicant to investigate the practicality of this means of charge 20. manufacture.
- Winch and Irvine have reviewed a wide range of means of inducing accelerated burning rate in an end- burning charge by forced cone burning.
- the same ideas of forced cone-burning can be carried over to increasing the core burning rate. It will be seen that if the core strand had, for example, a central wire core as in the invention of B. Silver U.S. Patent 3140663 and the work of Caveny and Glick, the thermal feedback from the flame-zone would increase the burning rate of the core strand and the incorporation of such a wire is optional in this invention.
- cavities 4 are indicated.
- the resultant accelerated mean burning rate causes an approximate cone to form in the charge.
- the pulsed nature of the cavity line leads to a fluctuating slope on the conical surface but Bradfield has shown that the resultant
- any method which rapidly moves the flame front a distance of P-S produces the desired effect of increasing the burning rate without affecting the core pressure exponent or turn-down ratio.
- Figure 5 shows a suggested negative exponent strand made using Bradfield cavities to double the burning rate of the EDB propellant to a range 10 mm/s to 20 mm/s.
- Each strand is constructed of a large number of
- Figures 6 and 7 show a multi-core charge with a core burning rate of 10 mm/s to 20 mm/s, a bulk burning rate of 8 mm/s and a transition time from one burning surface area to another of 0.01 t, , where t, is the 30. time of burn at the lower rate.
- FIG. 6 shows the propellant 2 in a case 8 and shows how a multiplicity of spaced cores 3 are disposed. This assembly has combined several very useful pioperties.
- the actual burning rate range can be adjusted to give a useful mass flow rate range for a particular application.
- the bulk propellant can be chcsen from a wide range of available propellant formulations to give particular requirements, such as high impulse (aluminised CDB, for example), low smoke (non-alu inised CDB), or low
- Control response rate is improved because opening the nozzle instantly gives more thrust, and this is followed by an increase in burning rate to sustain the higher level of thrust with a higher rate of gas production.
- the negative exponent cored charge described in this invention has most of the advantages of a charge made entirely of negative exponent propellant.
- the pressure remains nearly constant, and thus the motor chamber and nozzle can be designed around that constant
- Each area can be independantly optimised, so that the resultant charge is no longer such a compromise, and the range of propellants available to the designer 20. is enormously increased.
- n less than -2.5 have been produced in EDB strands, with a turn-down ratio 25. of greater than 2.
- Cast composite propellants are also available, with n less than -1.0 and turn-down ratios greater than 2.0 (and up to 2.6).
- the designer having selected the core propellant, can then choose an accelerator (such as Bradfield cavities, or similar devices that cause the flame-front to progress very rapidly through a fixed fraction of the propellant) to raise the burning rate range of the core propellant to the range required by the application.
- an accelerator such as Bradfield cavities, or similar devices that cause the flame-front to progress very rapidly through a fixed fraction of the propellant
- Gas generators for pneumatic actuators are an application where controllability is the most important 20. feature. Rapid response rate, and the ability to choose low flame temperature propellants are particularly attractive.
- Such a charge could also be used in gas generator fuelled ram-jets or ducted rockets.
- gas generator fuelled ram-jets or ducted rockets Such a charge could also be used in gas generator fuelled ram-jets or ducted rockets.
- a very fuel rich propellant is burnt in a chamber, exhausted into a duct where it is mixed with air, and the resultant mixture is burnt and exhausted as a ram ⁇ jet.
- the control is used to give varying mass flow to compensate for varying air flow at different flight
- boost motors presently in use. For these applications, turn-down ratios of up to about 5 would be required, and these are not yet available. Further research into negative exponent propellants is needed before this use could be seriously addressed. Response time
- a bulk propellant which can be chosen to give optimum properties for the application intended without affecting the charge burning rate or negative exponent.
- the resultant charge has all the advantages of 15 " .. negative exponent charges produced entirely from negative exponent propellant, except for the almost instantaneous response of the completely homogeneous negative exponent charge.
- the negative exponent core charge can, however, be made with as small a response time as required, provided 20. sufficiently many closely spaced cores can be embedded in the charge.
- the cored charge has none of the major disadvantages of the homogeneous negative exponent charge, because the bulk propellant can be selected to give whatever performance is required.
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- Engineering & Computer Science (AREA)
- Chemical & Material Sciences (AREA)
- Combustion & Propulsion (AREA)
- Mechanical Engineering (AREA)
- General Engineering & Computer Science (AREA)
- Testing Of Engines (AREA)
Abstract
Une charge propulsive solide pour un moteur-fusée ou un générateur de gaz comprend un agent propulsif en masse (2) ayant des noyaux longitudinaux de matériau de régulation (3). Les noyaux de régulation offrent une vitesse de combustion supérieure à celle de l'agent propulsif en masse, laquelle diminue avec l'augmentation de la pression, de telle sorte que la vitesse de combustion de la charge propulsive solide décroît également au fur et à mesure que la pression augmente.A solid propellant charge for a rocket engine or gas generator includes a bulk propellant (2) having longitudinal cores of regulating material (3). The control cores provide a higher rate of combustion than that of the bulk propellant, which decreases with increasing pressure, so that the rate of combustion of the solid propellant charge also decreases as as the pressure increases.
Description
Claims
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AUPH483786 | 1986-02-28 | ||
AU4837/86 | 1986-02-28 |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0269642A1 true EP0269642A1 (en) | 1988-06-08 |
EP0269642A4 EP0269642A4 (en) | 1988-06-23 |
Family
ID=3771492
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP19870901295 Withdrawn EP0269642A4 (en) | 1986-02-28 | 1987-02-26 | Rocket propellant charge with negative pressure exponent. |
Country Status (2)
Country | Link |
---|---|
EP (1) | EP0269642A4 (en) |
WO (1) | WO1987005362A1 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP3072868B1 (en) * | 2010-06-15 | 2017-12-13 | Aerojet Rocketdyne, Inc. | End-burning propellant grain with area-enhanced burning surface |
CN117332724A (en) * | 2023-12-01 | 2024-01-02 | 南京理工大学 | Method for predicting inner trajectory of paste rocket engine |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3105350A (en) * | 1959-02-26 | 1963-10-01 | Thompson Ramo Wooldridge Inc | Monofuel propellant booster rocket |
US3107620A (en) * | 1959-10-20 | 1963-10-22 | Atlantic Res Corp | Propellent grains |
FR1357255A (en) * | 1963-05-06 | 1964-04-03 | Bombrini Parodi Delfino Spa | Improvements in devices enabling the combustion speed of solid fuel propellants for rockets and missiles to be modified at will |
US3292545A (en) * | 1963-10-01 | 1966-12-20 | Mitsubishi Heavy Ind Ltd | Propellant grain |
DE2034104A1 (en) * | 1970-07-09 | 1972-01-13 | Dynamit Nobel Ag | Solid propellant for rocket engines |
US4345427A (en) * | 1979-10-26 | 1982-08-24 | Thiokol Corporation | Rocket motor or gas generator having controlled thrust or mass flow output |
-
1987
- 1987-02-26 EP EP19870901295 patent/EP0269642A4/en not_active Withdrawn
- 1987-02-26 WO PCT/AU1987/000056 patent/WO1987005362A1/en not_active Application Discontinuation
Non-Patent Citations (2)
Title |
---|
No relevant documents have been disclosed. * |
See also references of WO8705362A1 * |
Also Published As
Publication number | Publication date |
---|---|
EP0269642A4 (en) | 1988-06-23 |
WO1987005362A1 (en) | 1987-09-11 |
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Legal Events
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PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
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Effective date: 19871117 |
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A4 | Supplementary search report drawn up and despatched |
Effective date: 19880623 |
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Effective date: 19890207 |
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STAA | Information on the status of an ep patent application or granted ep patent |
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18D | Application deemed to be withdrawn |
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RIN1 | Information on inventor provided before grant (corrected) |
Inventor name: IRVINE, ROBERT, DAVID Inventor name: WINCH, PETER, CLIVE |