This invention relates to the sensing of information relating to a boosting missile target, estimation of the future time at which a boosting missile staging event, such as burnout, is expected to occur, and use of such information to improve the guidance of antimissile defenses.
Ballistic missile defense has become a significant priority as national intelligence indicates a growing missile threat from rogue nations that might obtain weapons of mass destruction and use ballistic missiles to fire them at U.S. forces abroad, U.S. allies or the continental United States. A desirable engagement strategy against ballistic missiles is to intercept the target as early as possible during the boost phase or early ascent phase when the target is a large object and has not dispersed counter measures or multiple warheads. Such a strategy minimizes the requirements for warhead and decoy discrimination, and allows for multi-layered defense opportunities. A missile defense system supporting this strategy must include an accurate boost phase target state estimator. Without accurate target state estimates, a fire control system cannot obtain valid intercept solutions for launching the interceptor during boost, and intercepting during the early ascent phase. The problem of identifying, determining or estimating the state, and providing guidance of a kill vehicle toward a hostile missile is described generally in U.S. patent application Ser. Nos. 11/356,675 filed Feb. 16, 2006, now U.S. Pat. No. 7,552,669, 11/430,535 filed May 9, 2006, now U.S. Pat. No. 7,511,252, 11/430,644 filed May 9, 2006, now abandoned, and 11/430,647 filed May 9, 2006, now U.S. Pat. No. 7,473,876.
Challenges in developing a boost phase tracking algorithm include unpredictable target accelerations while the target is in powered flight, and uncertainty of its burn time. Targets powered by solid rocket motors present the additional challenge of irregular thrust acceleration profiles. Due to the significant changes in acceleration during the target's boost phase, filters that assume constant acceleration cannot meet the stringent accuracies required of most fire control systems. Current state-of-the-art template-based filters use position and velocity templates assuming constant accelerations or rocket equation acceleration modeling. Such templates are subject to error attributable to motor burn variations, energy management (lofted/depressed trajectories), ISP variations, and early thrust terminations.
In addition, uncertain knowledge of the time of launch of the target results in error in estimating the time after launch. The uncertainty in knowledge of the time after launch leads to error in time indexing into a thrust template, which in turn tends to introduce more error in the acceleration estimate. For example, if the estimate of time after launch in
Improved or alternative estimation of the future time of staging events such as burnout, and early identification after-the-fact of early thrust termination is also desired.
In the present description, a ^ notation is used to denote filter estimates of the respective variables, and a superscript
where
stageTimeĈurrênt=nominal current stage burnout time;
stageTimePast=nominal past stage burnout time;
stageTimePastEst=estimated value of the previous stage burnout time;
{circumflex over (K)} and de{umlaut over (l)}T=state estimates from the filter;
offsetError=initial difference between template_index and measured Time.
The estimated burnout time is used to aid in predicting the future location of the target.
According to another aspect of the invention, a method for determining early thrust termination of a boosting target comprises the step of sensing position of the boosting target, as for example from moment to moment, to thereby generate target position information. Current stage state estimates including position, velocity, time index error into the thrust acceleration template, and motor scale factor {circumflex over (K)} are generated. The motor scale factor is used to indicate if the target has early thrust terminated.
The Template Updated Boost Algorithm (TUBA) is a boost phase filter or processing that estimates variations with respect to nominal templates representing the target's kinematic motion.
Another boost phase filter is described in U.S. patent application Ser. No. 10/972,943 filed on Oct. 25, 2004, now U.S. Pat. No. 7,181,323, in the name of Boka et al. and entitled Computerized Method for Generating Low-Bias Estimates of Position of a Vehicle From Sensor Data. This boost filter is the Unified Unbiased Rocket Equation Extended Kalman Algorithm (UUREEKA). It differs from TUBA in that UUREEKA models target dynamics using the fundamental rocket equation and is ideal for tracking liquid-fueled targets whose thrust acceleration profiles can be modeled using the rocket equation. UUREEKA is less advantageous for solid fuel rocket motors that exhibit irregular thrust acceleration profiles. TUBA is well adapted for tracking solid-fuel targets that have irregular thrust acceleration profiles, which cannot be modeled by the rocket equation. As mentioned,
TUBA uses a template filter which utilizes a table of nominal target data which relates target time after launch (TAL) to boost acceleration, speed, altitude, and angle of attack. An example of a nominal target template data table 300 appears as
The entry point into the target template 300 of
The TUBA algorithm associated with block 412 of
More specifically, the TUBA process of
tInstage=template_index−stageTimePast (1)
where stageTimePast is the nominal stage time of the previous stage, as illustrated in
X=XM (2)
is the initial position vector (set to measured value);
{dot over (X)}={dot over (X)}M (3)
is the initial velocity vector (set to an initial estimate);
K=1 (4)
is the motor scale factor (set to nominal value);
delT=0 (5)
is the initial estimate of error in template_index; and
delA=0 (6)
is the initial estimate of error in angle of attack.
The TUBA Initialization function 514, represented as 600 of
Template_index=(tInstage−delT)*K+stageTimePast (7)
From block 620, the logic of
offsetError=template_index−tgtMeasTime (8)
where variable “tgtMeasTime” is the current system time, variously designated t or tm in
TUBA uses a nine-state Kalman filter which estimates the position and velocity vectors and three additional states. The three additional states are used to resolve the deficiencies associated with the use of a nominal acceleration profile. The TUBA filter equations are developed under the assumption that the target is either ballistic (falling under the force of gravity) or the specific force (such as thrust acceleration) is exactly known and can therefore be compensated for. It is also assumed that the target is not subject to significant atmospheric drag, which is reasonable in view of the high altitudes at which target tracking occurs. Alternatively, it is assumed that atmospheric drag can be properly compensated for. Equations (9), (10), and (11) model the target kinematics under these assumptions
where:
μ is the Earth gravitational constant, 3.986005*1014 m3/s2;
w is the magnitude of Earth's angular velocity, 7.29211574*10−5 rad/s;
|Tacc| is the boost acceleration magnitude; and
{circumflex over (T)} is the unit thrust vector.
The TUBA state vector is
where:
X and {dot over (X)} are three-dimensional position and velocity vectors, respectively;
K is a motor scale factor reflecting the target rocket motor, hot (K>1.0), cold (K<1.0), or nominal (K=1.0);
delT is the error in the initial time used to look up target parameters from the nominal templates; and
delA is the error in the estimate of the target's angle of attack.
The TUBA dynamics equations (i.e. the nonlinear TUBA state derivative equations) are
and are based on the assumed target kinematics set forth above. Additionally, it is assumed that K, delT, and delA are constants.
The thrust acceleration |Tacc|, is obtained from the nominal acceleration template using template_index and K estimate as
|Tacc|=K*BoostAccLookup(template_index) (14)
The unit thrust vector {circumflex over (T)} is calculated using the nominal angle of attack lookup, estimated position, velocity, and delA as
AoaEst=AOALookup(template_index)+delA (15)
yL2={dot over ({circumflex over (X)} (16)
zL2=({dot over ({circumflex over (X)}×{circumflex over (X)})×yL2 (17)
{circumflex over (T)}=yL2*cos(AoaEst)−zL2*sin(AoaEst) (18)
where the template_index is defined by equation (7).
Referring once more to
A 2nd order Runge Kutta algorithm might be used for the integration process. The incremental time step, Δt, refers to either the nominal update cycle time or the incremental time step from the last cycle time to the current measurement time tM (i.e. Δt=tm−ti−1).
From state time propagation block 518, the logic of
where components of the Jacobian corresponding to
are defined below in equations 21 to 26
Note that the [[•]] notation denotes a skew symmetric matrix of the vector argument.
are performed numerically by choosing some small value for ∂K and ∂delT. The resulting equations are
where:
dk=0.001
dt=0.01
a1=BoostAccLookup(template_index)
a2=BoostAccLookup(template_index+(tInstage+dt)*dk)
a3=BoostAccLookup(template_index+dt)
The partial derivative of acceleration with respect to the error in angle of attack,
is given by
where:
∂{circumflex over (T)}=−yL2*sin(AoaEst)−zL2*cos(AoaEst) (26)
The partial of {circumflex over (T)} is taken with respect to angle of attack only, since variations of the thrust vector with respect to position and velocity is minimal. {circumflex over (T)}, AoaEst, yL2, and zL2 are defined in equations (18), (15), (16), and (17), respectively.
From Jacobian computation block 520 of
The TUBA state covariance is defined as
P=E{(s−
Where
s is the TUBA state vector
E is the expected value of {*}
P is the TUBA state covariance matrix,
with
P11=state covariance matrix of X
P22=state covariance matrix of {dot over (X)}
P33=state covariance element for K
P44=state covariance element for delT
P55=state covariance element for delA
and
Time propagation of the TUBA error covariance matrix P is performed with the equation
P(ti)−=ΦP(ti−1)ΦT+Qi (28b)
where:
Q is the 9×9 TUBA state noise matrix whose diagonal elements are chosen based on tuning considerations.
From covariance propagation portion or block 522 of time update 516 of
The logic of
K=P(ti)−·HT·(H·P(ti)−·HT+R)−1 (29)
where:
H=[I3×303×303×3]
H is the measurement matrix, and R is the measurement noise covariance matrix associated with the currently reporting sensor.
The logic flows from block 528 of
ŝi=ŝi−+K·(Xm−H·{circumflex over (X)}i−) (30)
Finally, the logic of
P(ti)=(I−K·H)·P(ti)− (31)
and the logic returns to time update block 516, with updated time T=Tm+Δt for the next calculation cycle, by way of a path 540.
Template Parameter Update block 524 of
tInstage=tInstage+Δt (32)
where Δt is the measurement update interval
template_index=(tInstage−del{circumflex over (T)})*{circumflex over (K)}+stageTimePast (33)
where stagetimepast is the nominal past stage.
Note that the initial error in tInstage due to the initial guess at the value of target time after launch is removed in the calculation of template_index via the filter state del{circumflex over (T)}, and the acceleration profile variation due to motor differences is corrected by the filter state {circumflex over (K)}.
The TUBA target staging and early thrust termination_logic block 542 of
where:
stageTimeCurrent=nominal current stage burn out time
stageTimePast=nominal past stage burn out time
stageTimePastEst=estimated value of the previous stage burn out time
{circumflex over (K)} and del{circumflex over (T)}=state estimates from the filter
offsetError=initial difference between template_index and measured time.
Staging times for subsequent stages are updated relative to the current stage time estimate.
To account for the uncertainties in the estimated burnout time, a staging window (e.g. 3 to 4 seconds) is set on either side of the estimated current stage burnout time in block 542 of
K=1
delT=0
thisStage=thisStage+1
offsetError=stageTirneEstPast−tgtMeasTime
tInstage=tgtMeasTime−stageTimeEstPast
template_time=(tInstage−delT)*{circumflex over (K)}+stageTimePast (35)
where:
tgtMeasTime is current system time.
When the target has exited a staging window, the filter error covariance for K and delA are reset to their initial default values by the Staging Logic portion of block 542 of
Liquid-propellant rocket engines control the thrust by varying the amount of propellant that enters the combustion chamber. By stopping the flow of propellants into the combustion chamber, these targets can effectively terminate their thrust prior to the nominal end of boost time. Solid-propellant rockets are not as easy to control as liquid rockets. Once started, the propellants burn until they are gone. However, some solid-fuel engines have hatches on their sides that can be cut loose by remote control to release the chamber pressure and terminate thrust. Early thrust termination poses a particularly difficult problem for tracking since it is an unknown change in acceleration applied at an unknown time. If the filter continues to assume nominal boost acceleration when in actuality the rocket has early thrust terminated, potentially huge errors would result in the estimated states which might well render invalid any fire control solution. The early thrust termination logic portion of block 542 of
More particularly, from current stage burnout estimation block 816 of
Thus, a method according to an aspect of the invention is for estimating staging of a boosting target, as for example of a missile. The method comprises the steps of sensing position of the boosting target, as for example from moment to moment. This may be done by means of an infrared sensor or by a radar system, or by another other suitable method. This generates target position information. From the sensed target position information, target current stage state estimates are generated. The target stage state estimates include position, velocity, time index error into the thrust template, and motor scale factor {circumflex over (K)}. The method further comprises the step of determining estimated burnout time tBOEst of the current stage by use of the equation
where
stageTimeCurrent=nominal current stage burnout time;
stageTimePast=nominal past stage burnout time;
stageTime{umlaut over (P)}astËst =estimated value of the previous stage burnout time;
{circumflex over (K)} and de{circumflex over (l)}T=state estimates from the filter;
offsetError=initial difference between templateindex and measured Time.
The estimated burnout time is used to aid in predicting the future location of the target.
According to another aspect of the invention, a method for determining early thrust termination of a boosting target comprises the step of sensing position of the boosting target, as for example from moment to moment, to thereby generate target position information. Current stage state estimates including position, velocity, time index error into the thrust template, and motor scale factor {circumflex over (K)} are generated. The motor scale factor is used to indicate if the target has early thrust terminated.
Number | Name | Date | Kind |
---|---|---|---|
3116039 | Goldberg | Dec 1963 | A |
3156435 | Edward et al. | Nov 1964 | A |
3164339 | Schroader et al. | Jan 1965 | A |
3169727 | Schroader et al. | Feb 1965 | A |
3206143 | Von Munchihofen | Sep 1965 | A |
3527167 | Morse | Sep 1970 | A |
3560971 | Alsberg et al. | Feb 1971 | A |
3706096 | Hammack | Dec 1972 | A |
3741501 | Salkeld | Jun 1973 | A |
3741502 | Schroader et al. | Jun 1973 | A |
3883091 | Schaefer | May 1975 | A |
3951359 | Willhite | Apr 1976 | A |
3964695 | Harris | Jun 1976 | A |
3982713 | Martin | Sep 1976 | A |
3996590 | Hammack | Dec 1976 | A |
4093153 | Bardash et al. | Jun 1978 | A |
4470562 | Hall et al. | Sep 1984 | A |
4502650 | Yueh | Mar 1985 | A |
4568823 | Diehl et al. | Feb 1986 | A |
4589610 | Schmidt | May 1986 | A |
4791573 | Zemany et al. | Dec 1988 | A |
4856733 | Lachmann | Aug 1989 | A |
4925129 | Salkeld et al. | May 1990 | A |
5050818 | Sundermeyer | Sep 1991 | A |
5170440 | Cox | Dec 1992 | A |
5198607 | Livingston et al. | Mar 1993 | A |
5296861 | Knight | Mar 1994 | A |
5319556 | Bessacini | Jun 1994 | A |
5340056 | Guelman et al. | Aug 1994 | A |
5341142 | Reis et al. | Aug 1994 | A |
5379044 | Carlson et al. | Jan 1995 | A |
5379966 | Simeone et al. | Jan 1995 | A |
5414643 | Blackman et al. | May 1995 | A |
5429322 | Waymeyer | Jul 1995 | A |
5458041 | Sun et al. | Oct 1995 | A |
5464174 | Laures | Nov 1995 | A |
5471433 | Hammell et al. | Nov 1995 | A |
5474255 | Levita | Dec 1995 | A |
5506586 | Bull | Apr 1996 | A |
5537118 | Appriou | Jul 1996 | A |
5557347 | Johnson | Sep 1996 | A |
5660355 | Waymeyer | Aug 1997 | A |
5710423 | Biven et al. | Jan 1998 | A |
5757310 | Millward | May 1998 | A |
5765166 | Gotfried et al. | Jun 1998 | A |
5788179 | Wicke | Aug 1998 | A |
5793931 | Hillis | Aug 1998 | A |
5811788 | Wicke | Sep 1998 | A |
5862496 | Biven | Jan 1999 | A |
5912640 | Bradford et al. | Jun 1999 | A |
5959574 | Poore, Jr. | Sep 1999 | A |
5960097 | Pfeiffer et al. | Sep 1999 | A |
6011507 | Curran et al. | Jan 2000 | A |
6043867 | Saban | Mar 2000 | A |
6064332 | Cloutier | May 2000 | A |
6082666 | Windhorst et al. | Jul 2000 | A |
6091361 | Davis et al. | Jul 2000 | A |
6104336 | Curran et al. | Aug 2000 | A |
6209820 | Golan et al. | Apr 2001 | B1 |
6259974 | Bessacini et al. | Jul 2001 | B1 |
6262680 | Muto | Jul 2001 | B1 |
6278401 | Wigren | Aug 2001 | B1 |
6314204 | Cham et al. | Nov 2001 | B1 |
6404380 | Poore, Jr. | Jun 2002 | B2 |
6498580 | Bradford | Dec 2002 | B1 |
6527222 | Redano | Mar 2003 | B1 |
6543716 | Miller et al. | Apr 2003 | B1 |
6549158 | Hanson | Apr 2003 | B1 |
6561074 | Engel et al. | May 2003 | B1 |
6563450 | Wallace | May 2003 | B1 |
6568628 | Curtin et al. | May 2003 | B1 |
6575400 | Hopkins et al. | Jun 2003 | B1 |
6603421 | Schiff et al. | Aug 2003 | B1 |
6666401 | Mardirossian | Dec 2003 | B1 |
6674390 | Murphy, Jr. | Jan 2004 | B1 |
6720907 | Miron | Apr 2004 | B1 |
6736547 | Stevens et al. | May 2004 | B2 |
6739547 | Redano | May 2004 | B2 |
6750806 | Fischer | Jun 2004 | B2 |
6771205 | Barton et al. | Aug 2004 | B1 |
6799138 | Lawrence et al. | Sep 2004 | B2 |
6877691 | DeFlumere et al. | Apr 2005 | B2 |
7026980 | Mavroudakis et al. | Apr 2006 | B1 |
7137588 | Humphrey | Nov 2006 | B2 |
7181323 | Boka et al. | Feb 2007 | B1 |
7190304 | Carlson | Mar 2007 | B1 |
7348918 | Redano | Mar 2008 | B2 |
7394047 | Pedersen | Jul 2008 | B1 |
7400289 | Wolf | Jul 2008 | B1 |
7411543 | Boka | Aug 2008 | B1 |
7473876 | Pedersen et al. | Jan 2009 | B1 |
7511252 | Pedersen et al. | Mar 2009 | B1 |
7532669 | Wen et al. | May 2009 | B2 |
7552669 | Denis et al. | Jun 2009 | B1 |
20020008657 | Poore, Jr. | Jan 2002 | A1 |
20040004155 | DeFluemere et al. | Jan 2004 | A1 |
20050114023 | Williamson et al. | May 2005 | A1 |
20050128138 | McCabe et al. | Jun 2005 | A1 |
20060074558 | Williamson et al. | Apr 2006 | A1 |
Number | Date | Country |
---|---|---|
9858274 | Dec 1998 | WO |
Number | Date | Country | |
---|---|---|---|
20110025551 A1 | Feb 2011 | US |