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Space vehicle correction engine test method |
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IPC classes for russian patent Space vehicle correction engine test method (RU 2535352):
Aircraft / 2521145
Aircraft comprises airframe, jet engines, fuel feed, ignition and flow control unit, unit of symmetric tapered combustion chambers, two units of exhaust nozzles and units of symmetric bent exhaust pipes with ends. Every combustion chamber is rigidly coupled with appropriate exhaust nozzle of the first unit of exhaust nozzles behind the combustion chambers and rigidly connected with appropriate exhaust nozzle of the second unit of exhaust nozzles ahead of combustion chamber. Every nozzle is rigidly connected with appropriate bent exhaust pipe inside the airframe located ahead. Hydraulic inputs of the unit of symmetric bent exhaust pipes are communicated with appropriate hydraulic outputs of control unit.
Facility for moving in outer space / 2520856
Invention relates to jet-propelled moving facilities, predominantly in free outer space. Proposed moving facility contains body (1), payload (2), control system and at least one ring system of superconductive focusing-deflecting magnets (3). Each magnet (3) is attached to body (1) by load-bearing element (4). It is preferable to use two described ring systems located in parallel planes ("one above the other"). Each ring system is designed for long-term storage of highest-energy electrically charged particle flux (5) (relativistic proton flux) circulating in this system. Fluxes in ring systems are mutually antithetical and are inserted in these systems before flight (on launch orbit). To output of one of the magnets (3) of "upper" ring system a device (6) for part of flux (7) extraction to outer space is attached. Similarly, part of flux (9) is extracted via device (8) of one of the magnets of "lower" ring system. Fluxes (7) and (9) create jet propulsion. Devices (6) and (8) can be made in the form of deflecting magnetic system, neutraliser of flux electric charge and undulator.
Method to control spacecraft placing into orbit of planet artificial satellite / 2520629
Invention relates to spacecraft (SC) motion control during placing it into orbit of planet artificial satellite using aeroassisted maneuver. In the phase of airbraking, following parameters are forecasted for the time of SC exiting planetary atmosphere: SC speed, angle to inclination to local horizon and altitude of transfer orbit apofocus. In this process in each of successive forecast points, SC motion is considered on remaining atmospheric flight segments for roll angles γ = 0 rad and γ = π. The mentioned above forecasted manoeuvring parameters are found for each of these angles. Their values are used during control of SC incidence change (close to its value corresponding to maximum quality) and issuing pulse of SC speed in transfer orbit apofocus.
Withdrawal of carrier rocket stage separated part from payload orbit and device to this end / 2518918
Invention relates to liquid-propellant rockets, accelerating units and can be used at starting the engines when liquid-propellant store residues do not exceed 3% of initial value. Proposed method consists in gasification of liquid residues of unusable fuel reserve in oxidiser and combustible tanks, generation of braking pulse by their combustion in combustion chamber of gas rocker engine and high-rate blowdown of combustion products into space. In compliance with this invention, solid-propellant gas generating compounds (SPGGC) are used for gasification of unusable rocket propellant reserve. SPGGC is fed to oxidiser tank with excess oxygen while SPGGC with limited content of oxygen is fed to fuel tank. Note here that chemical composition and mount of SPGGC at minimum possible residues of unusable rocket propellant components are defined proceeding from preset characteristic speed: where is characteristic speed, is pulse developed owing to minimum unusable residues of rocket propellant in both tanks required for their oxidation, is the pulse developed only by combustion of SPGGC gases in gas rocket engine. Proposed device comprises engine with oxidiser and fuel tanks, tank supercharge system, has rocket engine with power supply system and rocket propellant component residues gasification system. Note here that engine plant is equipped with solid-propellant gas generators with their outlets connected with gas feed devices. Said gas generators are equipped with pyro membranes fitted in fuel tanks with residues of liquid rocket fuel.
Method of control over carrier rocket boost phase / 2495800
Invention relates to rocketry. Proposed method consists in deflection of midflight engine swing part in preset plane of jet deflection plane with allowance for periodic computation of command signal in response to midflight engine swing part deflection subject to program angle, deflection and rate of deflection of carrier rocket distinguished point from launcher vertical axis, carrier rocket pitch rate and angle and simultaneous stabilisation of carrier rocket angular position in the plane perpendicular to preset one. Said deflection of midflight engine swing part is performed by assuming said program angle of said deflection of midflight engine swing part and command signal gain with respect to distinguished point deflection and deflection rate from launcher vertical axis by preset laws from periodically measured elevation above launcher horizontal plane, said distinguished points is assumed to be the center of said swing part.
Method of control over active space object to be docked to passive space object / 2490181
Invention relates to space engineering and may be used for docking of two space objects, one active and another passive. Active space objected is placed in reference orbit to define characteristics of approach pulses via nominal parameters of said reference orbit to be applied to active space object in initial orbit. Then, characteristics of approach pulses are defined from actual parameters of active space object and applied to next orbits.
Method of driving carrier rocket separable unit from payload orbit and device to this end / 2482034
Invention relates to space engineering, particularly, to space rockets with liquid-propellant engines. Gas rocket engine is intended for driving separable unit from payload orbit. Said engine makes separable unit spin about length axis and stabilises angular position of rocket carrier separable unit. Rocket gas engine runs on the principle of releasing supercharging gas before gasification of liquid components of rocket fuel components that increases efflux rate of combustion products from nozzle. Extra pneumoelectric valves are mounted ahead of mixing manifold to support rocket gas engine operation.
Method of safe launching of rocket with multiengine first stage / 2481251
Invention relates to aerospace engineering and may be used in clustered rocket bodies. In nonexplosive failure of one of the engines, crash rocket is withdrawn by turning it from pad structures through pitch and hunt angles preloaded in control program and by emergency programs through said angles per the number engines and two fields of drop in the area of space center. In flight, control system is used to computer coordinates of instantaneous fault point, to define failure of engine not accelerated to full thrust by integral criterion and characteristic parameters of rocket motion irrespective of engine onboard diagnostics transducer readings. Given the failure, drop field is selected depending upon failure detection time as well as appropriate emergency program of pitch and hunt angles to withdraw rocket from pad structures. Then, failed engine is cut off along with running engines provided coordinates of instantaneous drop point belong in aforesaid selected field of rocket drop. In the case of normal operation of the engines, flight is controlled in compliance with standard program pf pitch and hunt angles.
Method of withdrawing accelerating rocket module from spaceship flight path / 2478064
Invention relates to aerospace engineering, particularly, to rocket acceleration module and its components intended for its stabilisation and withdrawal from separated spaceship. Proposed method comprises issuing command for accelerating module engine shutdown and issuing command with time delay Δt1 for separating accelerating module from spaceship and imparting them a relative velocity. It comprises also issuing the command for actuation of accelerating module withdrawal system to separate said module from spaceship with time delay Δt2. Prior to issuing command for accelerating module engine shutdown at preset flight parameters of spaceship, the latter and accelerating module are oriented relative to preset transverse axis at position of separation and stabilised at said position. Withdrawal of accelerating module is combined with spinning it relative to common longitudinal axis.
Method of spacecraft stage separation part descent / 2475429
Invention relates to aerospace engineering and may be used for programmable displacement of coordinates of spacecraft separation stages fall points. Rocket gas engine and separation stages control program is divided into extra-atmospheric and atmospheric sections. Said sections are divided into finite number of time intervals to define the program of separation stage angular turn and motion at every said interval.
Method for generation of control actions on spacecraft / 2533873
Invention relates to spacecraft (SC) motion control using solar radiation pressure forces distributed over SC working zones. The latter are formed as flat parallel optically transparent droplet flows. Distance between droplets of R radius in each flow in its lengthwise direction (Sx) and frontal-lateral direction (Sy) is divisible by . Number of flows is . By mutual bias of flows in direction of their motion for distance droplet mist flows are generated in number of . Each of the mentioned flows is biased relative to previous flow for distance in frontal-lateral direction. Thus opacity in frontal-lateral direction and transparency in direction of plane perpendicular to a flow is created. Unit distributed light pressure force is regulated by changing radius and number of droplets coming to point of it application in unit time. Total action value is regulated by changing number of droplet jets.
Method of clearing space debri from orbit / 2531679
Invention can be used to move space debris from working orbits to recycling orbits. The method includes taking towing spacecraft and a self-contained docking module into the region of an orbit from which space debris is to be cleared. The sequence of removing space debris is selected by comparing a criterion, for example the probability of the space debris colliding with other space objects, for each space debris. Compensation for accumulated errors of motion parameters of the towing spacecraft during previous manoeuvres, as well as the pointing system is distributed between correcting pulses of the towing spacecraft at the long-range guidance step and of the self-contained docking module at the self-guidance portion.
Antifailure protection of rocket multiplex control system / 2521117
Proposed method comprises generation of data signal in every channel corresponding to a definite combustion chamber as the difference between command signal and feedback signal, generation of control system channel cut-off signal as the signal of setting actuator rod on said channel to mid position. Channel cut-off signal is generated in case the data signal modulus integral calculated at preset-duration time interval exceeds the preset threshold. Note here that command signals of other channels are generated as sums of or difference in pitch, yaw and bank control signals and cut-off channel feedback signal with coefficients depending on cut-off channel number so that required summed pitch, yaw and bank control moments are actuated.
Method to control spacecraft placing into orbit of planet artificial satellite / 2520629
Invention relates to spacecraft (SC) motion control during placing it into orbit of planet artificial satellite using aeroassisted maneuver. In the phase of airbraking, following parameters are forecasted for the time of SC exiting planetary atmosphere: SC speed, angle to inclination to local horizon and altitude of transfer orbit apofocus. In this process in each of successive forecast points, SC motion is considered on remaining atmospheric flight segments for roll angles γ = 0 rad and γ = π. The mentioned above forecasted manoeuvring parameters are found for each of these angles. Their values are used during control of SC incidence change (close to its value corresponding to maximum quality) and issuing pulse of SC speed in transfer orbit apofocus.
Method of spaceship orienting and device to this end / 2519288
Proposed method comprises generation of signals for estimation of: spacecraft orientation angle, spacecraft sing angle and control. Signal difference of said parameters and their estimates are defined. Several formulas are used to calculate the correction signals of setting and estimation of external interference. Said corrections are allowed for at correction of orienting angle estimate signals and angular velocity signal. The latter are applied in spacecraft orientation control circuit. Proposed device comprises the following extra units: memory, adders, amplifiers, integrators interconnected and connected with other elements via system of switches. Proposed device incorporates models of the spacecraft orientation main circuit and flywheel engine.
Method of spaceship orienting and device to this end / 2514650
Invention relates to aerospace engineering, particularly, to spacecraft orientation. Proposed method comprises the steps that follow. Generation of angle estimate and spacecraft spin rate estimate signal are generated. Determination of difference in angle signal and angle estimate signal. Determination of difference in spin rate and spin rate estimate signal. Corrected angle estimate signal and corrected spin rate estimate signal are defined. Control signal is generated using said corrected angle estimate signal and corrected .spin rate estimate signal Proposed device comprises engine-flywheel model, four integrators, four adders, four normally closed switches and two normally-open switches. Output of 2nd adder is connected via engine-flywheel model, 1st integrator, 4th adder, 2nd integrator, 5th adder, 6th adder, 1st switch and 3rd integrator, all being connected in series, with 5th adder 2nd input. Output of the latter is connected via 1st switch with 2nd input of 1st adder. Output of 4th adder is connected via 7th adder, 2nd switch and 4th integrator, all being connected in series, with 4th adder 2nd input. Output of the latter is connected via 2nd switch with 3rd input of 2nd adder. Output of spin rate transducer is connected with 7th adder 2nd input and, via 3rd switch, with 2nd amplifier input.
Method of spaceship orienting and device to this end / 2514649
Invention relates to aerospace engineering, particularly, to spacecraft orientation. Proposed method comprises the steps that follow. Generation of angle estimate signal and signal of spacecraft spin rate. Generation of control estimate signal. Determination of difference in angle signal and angle estimate signal. Determination of difference in spin rate and spin rate estimate signal. Determination of difference in control signal and control estimate signal and determination of corrected angle estimate signal, corrected spin rate estimate signal and outer interference estimate signal. Then, generated are control signal with corrected angle estimate signal, corrected spin rate estimate signal and external interference estimate signal. Proposed device to this end comprises five normally-closed switches, two normally-open switches, seven adders, model of engine-flywheel, two amplifiers and five integrators.
Device to control spacecraft position in space with help of orbital gyrocompass / 2509690
Device for control over spacecraft position in space with the help of orbital gyrocompass. Control device comprises local vertical plotter, adders, amplifier-converter units, integrators, compensation units and gyro meter of angular velocity, spacecraft position setting device, cosine angle transducers, sine angle transducers, spacecraft veering control unit and spacecraft bearing setting unit. Connection between device elements are configured to allow spacecraft turn the course through arbitrary angle without loss in orientation relative to orbital system of coordinates. Note here that contour of correction from local vertical plotter is in operating mode. Spacecraft can either spin along the course or stay in definite position relative to orbital system of coordinates with loss in precision of orientation.
Method of descending space rocket stage separation part and device to this end / 2506206
Invention relates to aerospace engineering and may be used for descending space rocket stage separation parts (SRSSP) from orbits of payloads. SRSSP comprises propellant compartment and power compartment with bottoms. Upper bottom accommodates rotary chambers of rocket gas engine while lower bottom accommodates mid-fight engine (MFE) with elongated charge electrically connected via switchboard with power supply. SRSSP is oriented and stabilised by energy of liquid propellant gasified residues at application of velocity pulse defined by radii of SP MFE descending path apogee and perigee.
Stabilisation of unstable fragments of space garbage / 2505461
Proposed method comprises application of force to the fragment at its design points. Said force is created by air effects applied by gas flare to said fragment produced by satellite located nearby said fragment. Said gas flare can be generated by device, for example, various jet engines. Note here that space garbage fragment orbit can be changed simultaneously.
Method of three-axis orientation of spacecraft in orbital coordinate system / 2247684
Proposed method is performed by information of orientation unit to Sun by introducing the orbit parameters into on-board computer followed by calculating the Sun position in observation field of orientation unit for each point of orbit for orientation of axes in orbital coordinate system; search angular velocity is set for spacecraft to ensure capture of Sun by observation field of orientation unit, after which angular velocity is decreased to zero ensuring position of Sun in observation field of orientation unit. Then spacecraft is turned in such way that Sun should move to required initial point; turning the spacecraft to preset points is continued for each orbital point.
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FIELD: instrumentation. SUBSTANCE: invention relates to control of movement of space vehicle (SV). According to the proposed method, thrusts of correction engines (CE) (control accelerations) are determined as per total changes in a period of SV revolution from correction to correction. The latter are performed with one and the same CE and a thrust level of those CE is estimated. For reliable understanding of thrusts of a pair of mutually opposite located CE, series control activations of the same pair are performed from time to time with equal pulses. Discrepancy as to total pulse of thrust is entered in equal parts with an opposite sign to the implemented pulses. As a result, reliable thrust levels of CE in operation are obtained. EFFECT: reduction of costs and improvement of CE thrust determination accuracy as per the data of trajectory measurements, as well as improvement of SV orbit correction accuracy.
The present invention relates to the field of space technology and can be used to adjust the parameters of motion of the SPACECRAFT (SC). 1. The company from the prior art known method of correcting elements of the orbit of geostationary spacecraft, based on the determination of rods of engines according to the trajectory of ground-based measurements. The essence of this method consists in the following. 1. Spend trajectory measurements. Trajectory measurements were carried out using funds from a ground control center (GCC), mutually spaced around the territory of the Russian Federation for long distances. Trajectory measurements can be performed as a radio and optical means, while the measured parameters may be inclined range (measuring point - KA), the rate of change of slant range and Equatorial coordinates right ascension and declination of the SPACECRAFT. Measuring information transmitted from the measuring points in GCC ballistic centers, processing this information and determine the actual orbital elements of the SPACECRAFT. Trajectory measurements represent the standard measurement cycle current navigation parameters (ITP), the number of sessions of measurements and the number of intervals between sessions of the pillar is t for the daily interval and having two points of ground-based measurements from 4 to 6. 2. Make a test exposure. To do this, at the scheduled time, switch on the engine correction (DC) of the desired thrust direction and work out the pulse, providing the change of the adjustable parameter, such as the orbital period. The duration of the test exposure is chosen such that it is, on the one hand, led to small changes of the orbital elements, and on the other hand, that these changes were sufficient for reliable determination of the magnitude of the thrust DK. For example, when the thrust of the engine 0,08 N (8 HS) the duration of the test exposure for a SPACECRAFT with a mass of 2000 kg in geostationary orbit is about 2 h, and the corresponding tranversely pulse ~575 NS, which corresponds to the change of the orbital period of the SPACECRAFT, depending on the angles DK, (2,5-24,5) C. When the error of the determination of this parameter is 0.1 s, the error in determining the thrust is less than 5% is a good result. The random component of error implementing thrust is 3%, then the true thrust will be determined with an error of F(1±0,03)·0,05=0,05 F, i.e., the same 5%. 3. Spend trajectory measurements. Trajectory is measured similarly to p. 1. Pull the DC is determined by the actual value of the change in the adjustable parameter is the orbital period. 4. Determine the actual value of the change in corrector is imago parameter and determine cravings DC. Pull the DC is determined by the actual value of the change in the adjustable parameter is the orbital period. As necessary, PP.1-4 is repeated for each of the DC motor correction. After a certain period of time, as the lifespan of the systematic component of the thrust variable, repeat the full cycle (PP.1-4) testing of all DC. 5. Take corrective action. For this purpose the estimated time switch on DK desired thrust direction. Duration of JC set based on the value of thrust produced when the test enable. Inclusion of DK is changing the adjustable parameter, such as the orbital period of the SPACECRAFT. However, due to the fact that the engine thrust correction may change the required values of the adjustable parameter, as a rule, cannot be implemented in a single application of corrective action. 6. Spend trajectory measurements and precise traction DK. The operation was performed similarly to PP.3, 4. 7. Take corrective action. Switch on the DC required thrust direction at the time determined on the basis of traction DK, obtained by the test and the previous inclusions. If necessary, PP.6, 7 is repeated to achieve the required accuracy of the spine of the adjustable parameter. The disadvantage of method 1 is that: 1 - full cycle of testing all of the DC, including redundant circuits on the SPACECRAFT reaches up to 16 arbitrary numbers, collectively stretches, at least a month and includes in addition to the standard schedule 16 full-time cycles ITP; 2 - the required value of the adjustable parameter is achieved, as a rule, two corrections within 2 days, this requires planning two regular cycles ITP. This is a very expensive way, which, although it is extremely reliable as possible we have to go. It was used when the correction parameters of the orbit was performed no more than once per month. Currently, when the correction parameters of the orbit can be conducted with a frequency of once a day or even less, it can be argued that: 1 - in the absence of Autonomous on-Board navigation or daily ICNP means NKU way practically not applicable; 2 - in the presence of Autonomous on-Board navigation or daily ICNP means NKU has a more efficient way of definition (specification) of thrust DK set forth below. 2. In the practice of the JSC "ISS" is more often used another way to Refine rods DK. It uses a heuristic approach: there are initial conditions (WELL) the motion for the previous ITP, there are the current settings (so what) movement, have spent a plan of correction that includes up to two arbitrary numbers DK, solved the problem of forecasting the movement of the parish in current traffic conditions) without much error. In the method-analogue 2 performs the following sequence of operations (irrelevant details are omitted). 1. Worked out a plan of correction. 2. Spend trajectory measurements. With an auxiliary (side) navigation trajectory measurements are conducted in a continuous mode. 3. Implementing program to determine the parameters of motion of the center of mass of the SPACECRAFT. 4. Precise control of acceleration change of the orbital parameters. Refinement is not possible to determine the control acceleration more precisely the range of values of the accelerations specified by the manufacturer. It guarantees the tracking of abnormal JC, and, in the case of prolonged and possibly permanent situation, when (while) the refusal DK not recorded on Board the SPACECRAFT, still expect a plan of correction. 5. Perform the calculation program (compilation) plan corrections KA at step interval. Step interval is 1 day in the presence of Autonomous on-Board navigation or daily ITP (daily trajectory measurements - HILDREN) days or more - in the absence of THESE. 6. Depending on the organization ballistic flight support KA on the ORT CA are written plan of correction and control of acceleration or only specified control acceleration. Next paragraphs.1-6 are repeated during the whole time the AC for its intended purpose. The accuracy of this method exceeds the tolerance specified by the manufacturer of the propulsion system. The fact that the definition of thrust two DC in the range of plan (1 day) and even the definition of thrust of one of the DC, with a single-turn on a small (usually) the duration when the QUESTION is not solved satisfactorily task. The problem of determining the thrust of more than two DC solution is not. If there HILDREN importantly, when calculating the correction parameters (one-two on the engine(s) on the daily interval) always assume that a change of control of the adjustable parameter, which is often the period of circulation (it always changes when adjustments longitude and corrections inclination) can be regarded as error-free management center of mass of the SPACECRAFT, since the latter do not have time to affect the results of the corrections, as THESE exclude the possibility of their accumulation. However, the use of control (in terms of determining the orbital period) plane, for example, geostationary satellites, traditionally coincides with the plane XOZ inertial geocentric Equatorial coordinate system (the X-axis to the point Spring) when conducting daily corrections and HILDREN, it is not possible t is updated to exclude the methodical error of the calculation of the period of circulation and its changes for the correction the first of which can greatly affect the quality of the process of keeping the AC. The error δ t1determine the sidereal period is estimated means for trajectory measurements in 0.1 s; the change of the period for correction [mood] of the orbit on the day is nominally (1-2), and refinement of the accelerations from the engines (relative error, according to method 1, 5%) makes it possible respectively to rely on the accuracy Δ2 knowledge [change] period of not more than 0.1 s AND δ t and δ t2- size small, but the actual deviation of the sidereal orbital period from the expected amounts to 1.5 C. the Reason is explained in this example. If the middle of the active site (AU) corresponds to time tAUand the intersection of the plane XOZ, the sidereal orbital period is traditionally taken as the control corresponds to the time tXOZoff-tAUon the bottom half (the sidereal period of the prior correction believe is true), we obtain the sidereal period, which will include only half implemented for the correction of the average speed of the SPACECRAFT, and at close values of tAUand tZwhen tXOZ>tAUin the sidereal period implemented for the correction of the average speed of the SPACECRAFT and will not be reflected. And plan of correction is necessary for each and every day. The specified accuracy of 100% (1,5 who), of course, unacceptable, and if we're talking about geostationary satellites, does not allow to count on the hold narrow areas and conduct a thin collocation (hold multiple SPACECRAFT in one area). This error leads to the fact that the link is only one DK in step adjustments, consisting of the work of this DK, calculated according to HILDREN (best option refinement of thrust) often differs from the actual prescribed by the manufacturer more than the amount prescribed by the same manufacturer (for example, more than 11% of the nominal value for the stationary plasma DK). This error, though not fully, occurs in the calculation of the correction parameters because of perceptions that immediately after the time of intersection of the reference plane must AY that implemented the momentum of the whole must go to the corresponding change in the orbital period. In the Appendix shows an example in which from the WELL produced: prediction of parameters of passive motion of the center of mass of the SPACECRAFT for two days; forecasting the parameters of motion of the center of mass of the SPACECRAFT with thrust on AU, located just behind the tZ(1)predicting the parameters of motion of the center of mass of the SPACECRAFT with thrust on AU, located midway between tXOZ(1)and tXOZ(2)predicting the parameters of motion of the center of mass of the SPACECRAFT with thrust on AU, located directly in front of t . Time tXOZ(0)coincides with the time WELL. Plus all of the above is the forecast error of the points of intersection of the reference plane because of the inaccuracy of the knowledge thrust DK. HILDREN do not allow, even with a rough knowledge rods DK, accumulate error management center of mass of the SPACECRAFT. However, the quality control is directly related to the requirements of maintaining satellite systems during normal operation of the SPACECRAFT. A rough knowledge of the rods DK leads to gross errors of forecasting the motion of the SPACECRAFT, which does not allow using corrections to rely on a high quality realization of the evolution of the SPACECRAFT in orbit. The aim of the invention is to provide a reliable and rapid method for determining the thrust DK and improving the accuracy of the correction parameters of movement of the center of mass of the SPACECRAFT. This goal is achieved by testing DK KA, namely, that exert a corrective influence by incorporating DK; conduct daily trajectory measurements; determine the parameters of the motion of the center of mass of the SPACECRAFT; selected, for reasons of stability of the systematic component of the error draughts DK, the interval of time trying to enter statistics on developments DK - actual duration and conditional non DK, and changes in the orbital period of the AC; from the existing data set, choose those that meet the river the view of following one after the other inclusions of the same DK; data summarize and calculate the average thrust for each working DK; make the test stimulus to the body KA successive inclusions of two DK opposite direction thrust equal pulses, the difference from zero of the implemented increment period is transferred to the residual error for the total impulse, which contribute equally with opposite sign in the implemented pulses, and get the correct levels draughts working DC. Implementation of the proposed method involves the following sequence of operations. 1. Worked out a plan of corrections. This operation is similar to the 1 way 2. 2. Spend trajectory measurements. This operation is similar to the 2 way 2. With an auxiliary (side) navigation trajectory measurements are conducted in a continuous mode. 3. Implementing program to determine the parameters of motion of the center of mass of the SPACECRAFT. The operation is similar to the 3 way 2. The result is of interest to the orbital period of the SPACECRAFT. 4. Trying to enter data on operating time of the DC - actual duration and conditional number DK, also change the orbital period. When a continuous process ballistic ensure flight KA always have data from previous trajectory measurements. The accumulation interval data is selected for reasons of stability of the systematic status is engaged errors rods DK. He is about 2 months. 5. From the available data set, choose those that meet the condition of following one after the other inclusions of the same DC. In the sample will not be accepted include DC, between which happened clarifying the change of the level of thrust. 6. Data summarize and calculate the average thrust for each working DK. Traction on the results of measurements of the trajectory calculated by known methods, for example, by the formula [P. E. Eliasberg "introduction to theory of flight satellites, M.: Nauka, 1965]: , where FUNIVERSITY- pull DC, N; ΔiτOnaccordingly, the increment of the orbital period and the duration of JC with conditional number (ln) is the i-th row of data; mCA- SPACECRAFT mass, kg; µ⊕is the gravitational parameter of the Earth, m3/s2; R is the radius of the circular orbit, m The essence of the approach to determining the thrust for change is the orbital period is what if the correction to the N-day interval are held regularly (daily) about the same sidereal time, the same DC and have the same duration, the change in the orbital period affects only the operation of the DC, the difference between the forecast errors of the SPACECRAFT location at HILDREN on the long interval of the data set on the groundwork of DK is equal to zero. 7. Make a test exposure. For validation of the obtained rods DK and adequacy of the selected data on operating time DC need experimental verification of consistency of rods mutually opposite DC. Only after such verification with the successful outcome of the calculated thrust may be real. To do this, at the scheduled time carried out directly following each other include two DC mutually opposite directions of thrust is equal to the pulse when the duration of each turn provides the change in the orbital period to the same value. 8. Spend trajectory measurements. This operation is similar to p. 2. 9. Implementing program to determine the parameters of motion of the center of mass of the SPACECRAFT. The results of the determination of the orbital period before and after the test enable DK determine the change in the orbital period δ tMESM. The operation is similar to PP.3, 4. 10. Define the residual error for the total momentum of the Yaga. The discrepancy ΔJ determined by the ratio of: . 11. The discrepancy ΔJ contribute equally with opposite sign in the implemented pulses and receive significant levels of linkage DK worked. Significant levels of rods running DK is obtained from the relations: for one DK of the pair and for another DK of the pair. Next paragraphs.1-10 are repeated during the whole time the AC for its intended purpose. It should be noted. 1. DL the successful implementation of the plan of correction requires not only good knowledge of the thrust DK (same - changes of the adjustable parameter of the movement), but accurate prediction of motion parameters at the moment of calculation of the correction parameters. All motion parameters at any given time are determined by the oscillating, i.e., the instantaneous current. In addition to our interest period. It is important to bear in mind everything that was said above about the position of the reference plane. However, this goes beyond the testing center and relates to the correction method of the orbital parameters. Yes, exactly the current period are dealing with, we do not know, but the change in the orbital period for correction of the same DK know, therefore, know good traction DK, and this, in the end, turns out to be the most important in the realization of ballistic flight support KA. 2. After determining reliable values of the levels of the pair of rods DK you can use the entire dataset for these DK, except adjacent data on other DK, for further clarification, and, importantly, the data obtained can be used in the event of a change in the regime of ballistic flight support KA, which is described in method 2, i.e., when the trajectory measurements (ITP) is held once a week and less. The proposed method of testing DK KA allows you to define thrust (control acceleration without the unnecessary costs and precisely what thew, sequentially, as needed, for each DC. The testing engine of correction of the SPACECRAFT (SC), namely, that exert a corrective influence by including engines correction (DC), is carried out daily trajectory measurements, determine the parameters of the motion of the center of mass of the SPACECRAFT at the time interval selected for reasons of stability of the systematic component of the error draughts DK, collect statistics on developments DK - actual durations of work and contingent DK rooms, as well as changes in the orbital period of the SPACECRAFT, from the available data set, choose those that meet the condition of following one after the other inclusions of the same DK, the selected data summarize and calculate the average thrust for each working DK, make a test exposure to the chassis KA equal pulses by successive inclusions of two DK opposite direction of thrust, the difference from zero of the implemented increment period is transferred to the residual error for the total impulse, which contribute equally with opposite sign in the implemented pulses, and get the correct levels rods worked DK.
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