CN102878872B - Guidance information processing method aiming at seeker loss-of-lock conditions - Google Patents

Guidance information processing method aiming at seeker loss-of-lock conditions Download PDF

Info

Publication number
CN102878872B
CN102878872B CN201210278133.6A CN201210278133A CN102878872B CN 102878872 B CN102878872 B CN 102878872B CN 201210278133 A CN201210278133 A CN 201210278133A CN 102878872 B CN102878872 B CN 102878872B
Authority
CN
China
Prior art keywords
mtd
msub
seeker
mtr
missile
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.)
Active
Application number
CN201210278133.6A
Other languages
Chinese (zh)
Other versions
CN102878872A (en
Inventor
尹永鑫
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Rainbow UAV Technology Co Ltd
Original Assignee
China Academy of Aerospace Aerodynamics CAAA
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by China Academy of Aerospace Aerodynamics CAAA filed Critical China Academy of Aerospace Aerodynamics CAAA
Priority to CN201210278133.6A priority Critical patent/CN102878872B/en
Publication of CN102878872A publication Critical patent/CN102878872A/en
Application granted granted Critical
Publication of CN102878872B publication Critical patent/CN102878872B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Aiming, Guidance, Guns With A Light Source, Armor, Camouflage, And Targets (AREA)

Abstract

The invention discloses a guidance information processing method aiming at seeker loss-of-lock conditions. The guidance information processing method comprises the following steps of: calculating a theoretical line-of-sight rate according to the position and speed information of a guided missile, and employing different switching methods between the actually measured line-of-sight rate and the theoretical line-of-sight rate under the condition that the seeker loses a target according to different distances between the guided missile and the target; and calculating a theoretical frame angle according to the position and attitude angle information of the guided missile, and presetting the frame angle of the seeker under the condition that the seeker loses the target.

Description

Guidance information processing method for seeker unlocking condition
Technical Field
And designing a low-cost tactical missile high-precision guidance control system.
Background
At present, the high performance of the missile is basically realized by the high performance of a guide head, an inertial navigation device and a rudder system. The seeker determines the performance of the missile to a great extent, but for low-cost missiles, the deficiency of the seeker performance can be made up only to a certain extent through an advanced guidance control algorithm. The defects are mainly reflected in the aspects of high noise of the line-of-sight angular velocity measurement, high probability of target loss of the seeker, low isolation between the seeker and the projectile body and the like. If the guidance control algorithm cannot improve the above adverse factors to a certain extent, the hit precision of the missile is finally influenced.
Advanced guidance control algorithms should be able to compensate for deficiencies in the hardware performance of the seeker system to some extent, such as reducing noise in line-of-sight angular velocity, increasing the probability of recapturing targets after the seeker is out of lock, increasing the accuracy of missile hits if the seeker loses a target, and the like. At present, a low-pass filter is generally designed to filter an actual measurement value of the line-of-sight angular velocity, and a conventional filtering method is already mature under the condition that a seeker locks a target in the whole course. However, for the guided missile adopting the laser guidance mode and the like, when the guided missile passes through a cloud layer or a target releases a smoke curtain, the phenomenon that the target is lost by a seeker cannot be avoided, and under the circumstances, an effective method for reference is not available on how to ensure the miss distance of the guided missile by utilizing the existing information.
Disclosure of Invention
The technical problem of the invention is solved: in order to solve the problem that the existing low-cost tactical missile cannot hit the target under the condition that the seeker loses the target, a guidance information processing method aiming at the condition that the seeker loses the lock is provided, and the miss distance can be reduced under the condition that the seeker loses the target.
The technical solution of the invention is as follows: a guidance information processing method aiming at the condition that a seeker is unlocked comprises the following steps:
(1) measuring the angular rate and overload of the missile by using a rate gyroscope and an adder table;
(2) carrying out strapdown resolving by utilizing the actually measured angular rate and overload to obtain the attitude angle, speed and position information of the missile;
(3) calculating theoretical line-of-sight angular velocity according to the missile velocity and the position information; calculating a theoretical frame angle according to the position and attitude angle information of the missile;
(4) when the seeker is unlocked, the processing of the guidance information comprises the processing of the visual angular velocity and the frame angle information; the line-of-sight angular velocity processing firstly needs to judge whether the remaining flight time of the missile is greater than the preset time T, if so, the seeker is in a remote unlocking state, the theoretical line-of-sight angular velocity calculated in the step (3) is used for replacing the actual line-of-sight angular velocity for filtering, otherwise, the seeker is in a close-distance unlocking state, and the actual line-of-sight angular velocity filtering output value at the moment before the seeker is unlocked is used as the input of the filtering; in the two-state processing process, when the target is locked again, the actually measured line-of-sight angular velocity is used as the input of filtering; and (4) frame angle information processing, namely presetting the frame angle of the seeker by adopting the theoretical frame angle calculated in the step (3), and searching on the basis of the preset frame angle.
Compared with the prior art, the invention has the beneficial effects that:
(1) the invention can provide available guidance information for the guidance law under the condition that the seeker is unlocked, and effectively overcomes the defect that the conventional technology cannot help the seeker unlocking phenomenon.
(2) Semi-physical simulation data show that the scheme can ensure that the missile hits the target under the conditions of remote unlocking of the seeker and remote recapture; it is possible to ensure that the amount of miss is reduced to within an acceptable range in the event that the seeker is short out of lock.
Drawings
FIG. 1 is a flow chart of the present invention;
FIG. 2 is a ballistic contrast curve for a long-range loss of lock;
FIG. 3 is a ballistic contrast curve for a short-range loss-of-lock condition;
figure 4 is an enlarged partial view of the ballistic tip of figure 3.
Detailed Description
The present invention will be described in detail with reference to the accompanying drawings, as shown in fig. 1, the steps of the present invention are as follows:
(1) measuring the angular rate and overload of the missile by using a rate gyroscope and an adder table;
(2) carrying out strapdown resolving by utilizing the actually measured angular rate and overload to obtain the attitude angle, speed and position information of the missile; the specific algorithm is as follows:
<math><mrow> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <msub> <mi>n</mi> <mi>xg</mi> </msub> </mtd> </mtr> <mtr> <mtd> <msub> <mi>n</mi> <mi>yg</mi> </msub> </mtd> </mtr> <mtr> <mtd> <msub> <mi>n</mi> <mi>zg</mi> </msub> </mtd> </mtr> </mtable> </mfenced> <mo>=</mo> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <mn>1</mn> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mi>cos</mi> <mi>&gamma;</mi> </mtd> <mtd> <mi>sin</mi> <mi>&gamma;</mi> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mo>-</mo> <mi>sin</mi> <mi>&gamma;</mi> </mtd> <mtd> <mi>cos</mi> <mi>&gamma;</mi> </mtd> </mtr> </mtable> </mfenced> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <mi>cos</mi> <mi>&theta;</mi> </mtd> <mtd> <mi>sin</mi> <mi>&theta;</mi> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mo>-</mo> <mi>sin</mi> <mi>&theta;</mi> </mtd> <mtd> <mi>cos</mi> <mi>&theta;</mi> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mn>1</mn> </mtd> </mtr> </mtable> </mfenced> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <mi>cos</mi> <mi>&psi;</mi> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mo>-</mo> <mi>sin</mi> <mi>&psi;</mi> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mn>1</mn> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mi>sin</mi> <mi>&psi;</mi> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mi>cos</mi> <mi>&psi;</mi> </mtd> </mtr> </mtable> </mfenced> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <msub> <mi>n</mi> <mi>xb</mi> </msub> </mtd> </mtr> <mtr> <mtd> <msub> <mi>n</mi> <mi>yb</mi> </msub> </mtd> </mtr> <mtr> <mtd> <msub> <mi>n</mi> <mi>zb</mi> </msub> </mtd> </mtr> </mtable> </mfenced> </mrow></math>
wherein n isxg、nyg、nzgRespectively overload three shafts of the missile under a ground coordinate system; psi, theta and gamma are respectively a yaw angle, a pitch angle and a roll angle of the missile; n isxb、nyb、nzbAnd respectively, missile triaxial overload under a missile coordinate system.
a xg b yg a zg = g 0 0 0 g 0 0 0 g ( n xg n yg n zg + 0 1 0 )
Wherein, axg、ayg、azgThe three-axis acceleration of the missile under a ground coordinate system is respectively; g is the acceleration of gravity.
<math><mfenced open='{' close=''> <mtable> <mtr> <mtd> <msub> <mi>V</mi> <mi>xg</mi> </msub> <mo>=</mo> <msub> <mi>V</mi> <mrow> <mi>xg</mi> <mn>0</mn> </mrow> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <msub> <mi>a</mi> <mi>xg</mi> </msub> <mi>dt</mi> </mtd> </mtr> <mtr> <mtd> <msub> <mi>V</mi> <mi>yg</mi> </msub> <mo>=</mo> <msub> <mi>V</mi> <mrow> <mi>yg</mi> <mn>0</mn> </mrow> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <msub> <mi>a</mi> <mi>yg</mi> </msub> <mi>dt</mi> </mtd> </mtr> <mtr> <mtd> <msub> <mi>V</mi> <mi>zg</mi> </msub> <mo>=</mo> <msub> <mi>V</mi> <mrow> <mi>zg</mi> <mn>0</mn> </mrow> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <msub> <mi>a</mi> <mi>zg</mi> </msub> <mi>dt</mi> </mtd> </mtr> </mtable> </mfenced></math>
Wherein, Vxg、Vyg、VzgThe three-axis speeds of the missile under a ground coordinate system are respectively; vxg0、Vyg0、Vzg0Respectively is the missile triaxial initial velocity under the ground coordinate system; and t is the missile flight time.
<math><mfenced open='{' close=''> <mtable> <mtr> <mtd> <msub> <mi>x</mi> <mi>g</mi> </msub> <mo>=</mo> <msub> <mi>x</mi> <mrow> <mi>g</mi> <mn>0</mn> </mrow> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <msub> <mi>V</mi> <mi>xg</mi> </msub> <mi>dt</mi> </mtd> </mtr> <mtr> <mtd> <msub> <mi>y</mi> <mi>g</mi> </msub> <mo>=</mo> <msub> <mi>y</mi> <mrow> <mi>g</mi> <mn>0</mn> </mrow> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <msub> <mi>V</mi> <mi>yg</mi> </msub> <mi>dt</mi> </mtd> </mtr> <mtr> <mtd> <msub> <mi>z</mi> <mi>g</mi> </msub> <mo>=</mo> <msub> <mi>z</mi> <mrow> <mi>g</mi> <mn>0</mn> </mrow> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <msub> <mi>V</mi> <mi>zg</mi> </msub> <mi>dt</mi> </mtd> </mtr> </mtable> </mfenced></math>
Wherein x isg、yg、zgThe three-axis positions of the missile under a ground coordinate system are respectively; x is the number ofg0、yg0、zg0The initial positions of the three axes of the missile are respectively in the ground coordinate system.
<math><mfenced open='{' close=''> <mtable> <mtr> <mtd> <mi>&psi;</mi> <mo>=</mo> <msub> <mi>&psi;</mi> <mn>0</mn> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <mfrac> <mrow> <msub> <mi>&omega;</mi> <mi>y</mi> </msub> <mi>cos</mi> <mi>&gamma;</mi> <mo>-</mo> <msub> <mi>&omega;</mi> <mi>z</mi> </msub> <mi>sin</mi> <mi>&gamma;</mi> </mrow> <mrow> <mi>cos</mi> <mi>&theta;</mi> </mrow> </mfrac> <mi>dt</mi> </mtd> </mtr> <mtr> <mtd> <mi>&theta;</mi> <mo>=</mo> <msub> <mi>&theta;</mi> <mn>0</mn> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <mrow> <mo>(</mo> <msub> <mi>&omega;</mi> <mi>y</mi> </msub> <mi>sin</mi> <mi>&gamma;</mi> <mo>+</mo> <msub> <mi>&omega;</mi> <mi>z</mi> </msub> <mi>cos</mi> <mi>&gamma;</mi> <mo>)</mo> </mrow> <mi>dt</mi> </mtd> </mtr> <mtr> <mtd> <mi>&gamma;</mi> <mo>=</mo> <msub> <mi>&gamma;</mi> <mn>0</mn> </msub> <mo>+</mo> <msubsup> <mo>&Integral;</mo> <mn>0</mn> <mi>t</mi> </msubsup> <mrow> <mo>(</mo> <msub> <mi>&omega;</mi> <mi>x</mi> </msub> <mo>-</mo> <mi>tan</mi> <mi>&theta;</mi> <mrow> <mo>(</mo> <msub> <mi>&omega;</mi> <mi>y</mi> </msub> <mi>cos</mi> <mi>&gamma;</mi> <mo>-</mo> <msub> <mi>&omega;</mi> <mi>z</mi> </msub> <mi>sin</mi> <mi>&gamma;</mi> <mo>)</mo> </mrow> <mo>)</mo> </mrow> <mi>dt</mi> </mtd> </mtr> </mtable> </mfenced></math>
Wherein psi0、θ0、γ0Respectively an initial yaw angle, a pitch angle and a roll angle of the missile; omegax、ωy、ωzThe three-axis attitude angular velocities of the projectile body are respectively.
(3) Calculating theoretical line-of-sight angular velocity according to the velocity and the position information; calculating a theoretical frame angle according to the position and attitude angle information of the missile;
<math><mfenced open='{' close=''> <mtable> <mtr> <mtd> <msub> <mi>q</mi> <mi>&epsiv;</mi> </msub> <mo>=</mo> <mi>arctan</mi> <mrow> <mo>(</mo> <mfrac> <msub> <mi>y</mi> <mi>g</mi> </msub> <msub> <mi>x</mi> <mi>g</mi> </msub> </mfrac> <mo>)</mo> </mrow> </mtd> </mtr> <mtr> <mtd> <msub> <mi>q</mi> <mi>&beta;</mi> </msub> <mo>=</mo> <mi>arcsin</mi> <mrow> <mo>(</mo> <mfrac> <msub> <mi>z</mi> <mi>g</mi> </msub> <msqrt> <msubsup> <mi>x</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>+</mo> <msubsup> <mi>y</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>+</mo> <msubsup> <mi>z</mi> <mi>g</mi> <mn>2</mn> </msubsup> </msqrt> </mfrac> <mo>)</mo> </mrow> </mtd> </mtr> </mtable> </mfenced></math>
wherein q isε、qβRespectively a theoretical pitch line-of-sight angle and a theoretical yaw line-of-sight angle.
<math><mfenced open='{' close=''> <mtable> <mtr> <mtd> <msub> <mover> <mi>q</mi> <mo>&CenterDot;</mo> </mover> <mi>&epsiv;</mi> </msub> <mo>=</mo> <mfrac> <mrow> <msub> <mi>V</mi> <mi>xg</mi> </msub> <msub> <mi>y</mi> <mi>g</mi> </msub> <mo>-</mo> <msub> <mi>x</mi> <mi>g</mi> </msub> <msub> <mi>V</mi> <mi>yg</mi> </msub> </mrow> <mrow> <msubsup> <mi>x</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>+</mo> <msubsup> <mi>y</mi> <mi>g</mi> <mn>2</mn> </msubsup> </mrow> </mfrac> </mtd> </mtr> <mtr> <mtd> <msub> <mover> <mi>q</mi> <mo>&CenterDot;</mo> </mover> <mi>&beta;</mi> </msub> <mo>=</mo> <mfrac> <mn>1</mn> <msqrt> <msubsup> <mi>x</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>+</mo> <msubsup> <mi>y</mi> <mi>g</mi> <mn>2</mn> </msubsup> </msqrt> </mfrac> <mfrac> <mrow> <mrow> <mo>(</mo> <msubsup> <mi>x</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>+</mo> <msubsup> <mi>y</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>)</mo> </mrow> <msub> <mi>V</mi> <mi>zg</mi> </msub> <mo>-</mo> <msub> <mi>z</mi> <mi>g</mi> </msub> <mrow> <mo>(</mo> <msub> <mi>x</mi> <mi>g</mi> </msub> <msub> <mi>V</mi> <mi>xg</mi> </msub> <mo>+</mo> <msub> <mi>y</mi> <mi>g</mi> </msub> <msub> <mi>V</mi> <mi>yg</mi> </msub> <mo>)</mo> </mrow> </mrow> <mrow> <msubsup> <mi>x</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>+</mo> <msubsup> <mi>y</mi> <mi>g</mi> <mn>2</mn> </msubsup> <mo>+</mo> <msubsup> <mi>z</mi> <mi>g</mi> <mn>2</mn> </msubsup> </mrow> </mfrac> </mtd> </mtr> </mtable> </mfenced></math>
Wherein,
Figure BSA00000760100900043
Figure BSA00000760100900044
respectively, a theoretical pitch line-of-sight angular velocity and a theoretical yaw line-of-sight angular velocity.
<math><mrow> <mi>G</mi> <mo>=</mo> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <msub> <mrow> <mi>cos</mi> <mi>q</mi> </mrow> <mi>&beta;</mi> </msub> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <msub> <mrow> <mo>-</mo> <mi>sin</mi> <mi>q</mi> </mrow> <mi>&beta;</mi> </msub> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mn>1</mn> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <msub> <mrow> <mi>sin</mi> <mi>q</mi> </mrow> <mi>&beta;</mi> </msub> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <msub> <mrow> <mi>cos</mi> <mi>q</mi> </mrow> <mi>&beta;</mi> </msub> </mtd> </mtr> </mtable> </mfenced> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <msub> <mrow> <mi>cos</mi> <mi>q</mi> </mrow> <mi>&epsiv;</mi> </msub> </mtd> <mtd> <msub> <mrow> <mi>sin</mi> <mi>q</mi> </mrow> <mi>&epsiv;</mi> </msub> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mo>-</mo> <msub> <mrow> <mi>sin</mi> <mi>q</mi> </mrow> <mi>&epsiv;</mi> </msub> </mtd> <mtd> <msub> <mrow> <mi>cos</mi> <mi>q</mi> </mrow> <mi>&epsiv;</mi> </msub> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mn>1</mn> </mtd> </mtr> </mtable> </mfenced> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <mi>cos</mi> <mi>&psi;</mi> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mi>sin</mi> <mi>&psi;</mi> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mn>1</mn> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mo>-</mo> <mi>sin</mi> <mi>&psi;</mi> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mi>cos</mi> <mi>&psi;</mi> </mtd> </mtr> </mtable> </mfenced> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <mi>cos</mi> <mi>&theta;</mi> </mtd> <mtd> <mo>-</mo> <mi>sin</mi> <mi>&theta;</mi> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mi>sin</mi> <mi>&theta;</mi> </mtd> <mtd> <mi>cos</mi> <mi>&theta;</mi> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mn>1</mn> </mtd> </mtr> </mtable> </mfenced> <mfenced open='[' close=']'> <mtable> <mtr> <mtd> <mn>1</mn> </mtd> <mtd> <mn>0</mn> </mtd> <mtd> <mn>0</mn> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mi>cos</mi> <mi>&gamma;</mi> </mtd> <mtd> <mo>-</mo> <mi>sin</mi> <mi>&gamma;</mi> </mtd> </mtr> <mtr> <mtd> <mn>0</mn> </mtd> <mtd> <mi>sin</mi> <mi>&gamma;</mi> </mtd> <mtd> <mi>cos</mi> <mi>&gamma;</mi> </mtd> </mtr> </mtable> </mfenced> </mrow></math>
And G is a coordinate transformation matrix from the missile coordinate system to the sight line coordinate system.
<math><mfenced open='{' close=''> <mtable> <mtr> <mtd> <msub> <mi>&theta;</mi> <mi>g</mi> </msub> <mo>=</mo> <mn>57.3</mn> <mo>&times;</mo> <mi>arctan</mi> <mrow> <mo>(</mo> <mfrac> <msub> <mi>G</mi> <mn>12</mn> </msub> <msub> <mi>G</mi> <mn>11</mn> </msub> </mfrac> <mo>)</mo> </mrow> </mtd> </mtr> <mtr> <mtd> <msub> <mi>&psi;</mi> <mi>g</mi> </msub> <mo>=</mo> <mn>57.3</mn> <mo>&times;</mo> <mi>arcsin</mi> <mrow> <mo>(</mo> <mo>-</mo> <msub> <mi>G</mi> <mn>13</mn> </msub> <mo>)</mo> </mrow> </mtd> </mtr> </mtable> </mfenced></math>
Wherein, thetag、ψgRespectively a theoretical pitching frame angle and a theoretical yawing frame angle; g11Is the 1 st row and 1 st column element in the matrix G; g12Is the 1 st row and 2 nd column element in the matrix G; g13Is the 1 st row, 3 rd column element in matrix G.
(4) When the seeker is unlocked, the processing of the guidance information comprises the processing of the visual angular velocity and the frame angle information; the line-of-sight angular velocity processing firstly needs to judge whether the remaining flight time of the missile is greater than the preset time T, if so, the seeker is in a remote unlocking state, the theoretical line-of-sight angular velocity calculated in the step (3) is used for replacing the actual line-of-sight angular velocity for filtering, otherwise, the seeker is in a close-distance unlocking state, and the actual line-of-sight angular velocity filtering output value at the moment before the seeker is unlocked is used as the input of the filtering; in the two-state processing process, when the target is locked again, the actually measured line-of-sight angular velocity is used as the input of filtering; the frame angle information processing is to preset the frame angle of the seeker by adopting the theoretical frame angle calculated in the step (3), and search (can be performed by adopting methods such as rectangular search) on the basis of the preset frame angle so as to improve the probability of recapturing the target or shorten the time for recapturing the target, thereby reducing the miss amount.
The preset time T is calculated according to the formula
T=K·Tb
Where K is the minimum control stiffness, TbIs the time constant of the projectile.
Examples of applications are as follows:
in the case of long-distance unlocking of the seeker (9-12 s after launching, the remaining flight time is greater than 8s), the trajectory pair is as shown in fig. 2, wherein the solid line is the trajectory obtained by using the scheme, the miss distance is 0.29m, the dotted line is the trajectory obtained without using the scheme, and the miss distance is 91 m. Therefore, under the condition that the seeker is remotely unlocked, the miss distance is obviously reduced by using the scheme, and the target can be directly hit.
Under the condition that the seeker is short-distance unlocked (18 s-21 s after launching and the residual flight time is less than 8s), the trajectory pair is shown in figure 3, the local magnification of the trajectory tail end is shown in figure 4, wherein the solid line is the trajectory obtained by using the scheme, the miss distance is 0.63m, the dotted line is the trajectory obtained by not using the scheme, and the miss distance is 8.7 m. Therefore, under the condition that the seeker is short-distance unlocked, the miss distance is obviously reduced by using the scheme, and the target can be directly hit.
The invention has not been described in detail in part of the common general knowledge of those skilled in the art.

Claims (1)

1. A guidance information processing method aiming at the condition that a seeker is unlocked is characterized by comprising the following steps:
(1) measuring the angular rate and overload of the missile by using a rate gyroscope and an adder table;
(2) carrying out strapdown resolving by utilizing the actually measured angular rate and overload to obtain the attitude angle, speed and position information of the missile;
(3) calculating theoretical line-of-sight angular velocity according to the missile velocity and the position information; calculating a theoretical frame angle according to the position and attitude angle information of the missile;
(4) when the seeker is unlocked, the processing of the guidance information comprises the processing of the visual angular velocity and the frame angle information; the line-of-sight angular velocity processing firstly needs to judge whether the remaining flight time of the missile is greater than the preset time T, if so, the seeker is in a remote unlocking state, the theoretical line-of-sight angular velocity calculated in the step (3) is used for replacing the actual line-of-sight angular velocity for filtering, otherwise, the seeker is in a close-distance unlocking state, and the actual line-of-sight angular velocity filtering output value at the moment before the seeker is unlocked is used as the input of the filtering; in the two-state processing process, when the target is locked again, the actually measured line-of-sight angular velocity is used as the input of filtering; the frame angle information processing is to preset the frame angle of the seeker by adopting the theoretical frame angle calculated in the step (3) and search on the basis of the preset frame angle; the preset time T is calculated as follows: t = K · Tb(ii) a Where K is the minimum control stiffness, TbIs the time constant of the projectile.
CN201210278133.6A 2012-08-07 2012-08-07 Guidance information processing method aiming at seeker loss-of-lock conditions Active CN102878872B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201210278133.6A CN102878872B (en) 2012-08-07 2012-08-07 Guidance information processing method aiming at seeker loss-of-lock conditions

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201210278133.6A CN102878872B (en) 2012-08-07 2012-08-07 Guidance information processing method aiming at seeker loss-of-lock conditions

Publications (2)

Publication Number Publication Date
CN102878872A CN102878872A (en) 2013-01-16
CN102878872B true CN102878872B (en) 2014-06-18

Family

ID=47480296

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201210278133.6A Active CN102878872B (en) 2012-08-07 2012-08-07 Guidance information processing method aiming at seeker loss-of-lock conditions

Country Status (1)

Country Link
CN (1) CN102878872B (en)

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103822636B (en) * 2014-03-18 2016-10-05 中国航天时代电子公司 A kind of Air-to-Surface Guided Weapon strapdown homing Line-of-sight reconstruction method
CN105785415B (en) * 2016-03-03 2018-01-05 北京航天控制仪器研究所 A kind of aerial trajectory predictions method of guided cartridge
CN107388904B (en) * 2017-06-13 2019-01-22 河北汉光重工有限责任公司 Laser signal resolves and servo control integrated processing system
CN107179021B (en) * 2017-06-14 2018-08-28 北京理工大学 More bullets cooperate with zero-miss guidance control methods under a kind of beam rider guidance system
CN108279005B (en) * 2017-12-21 2020-06-16 北京航天飞腾装备技术有限责任公司 Guidance information reconstruction method under seeker data failure mode
CN108254732B (en) * 2017-12-21 2020-07-14 彩虹无人机科技有限公司 Method for accurately capturing target in large field of view by small field of view laser detector
CN108983214B (en) * 2018-05-03 2022-04-08 西安电子工程研究所 Radar seeker target selection method
CN109669480B (en) * 2019-01-03 2021-11-09 西安航天动力技术研究所 Seeker control method for predicting target position
CN114061380B (en) * 2021-09-29 2023-11-03 湖北航天飞行器研究所 Sketch aiming guidance method
CN116182647A (en) * 2022-12-21 2023-05-30 西安现代控制技术研究所 Guided ammunition belt falling angle constraint guidance information extraction method suitable for image seeker

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101603800A (en) * 2009-07-02 2009-12-16 北京理工大学 The guidance information building method of the target-seeking target seeker of a kind of half strapdown
CN101666650A (en) * 2009-09-30 2010-03-10 北京航空航天大学 SINS/GPS super-compact integrated navigation system and implementing method thereof

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8558153B2 (en) * 2009-01-23 2013-10-15 Raytheon Company Projectile with inertial sensors oriented for enhanced failure detection

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101603800A (en) * 2009-07-02 2009-12-16 北京理工大学 The guidance information building method of the target-seeking target seeker of a kind of half strapdown
CN101666650A (en) * 2009-09-30 2010-03-10 北京航空航天大学 SINS/GPS super-compact integrated navigation system and implementing method thereof

Also Published As

Publication number Publication date
CN102878872A (en) 2013-01-16

Similar Documents

Publication Publication Date Title
CN102878872B (en) Guidance information processing method aiming at seeker loss-of-lock conditions
CN109597427B (en) Bomb random attack planning method and system based on unmanned aerial vehicle
CN105021092B (en) A kind of guidance information extracting method of strapdown homing target seeker
CN105258698B (en) A kind of high dynamic spin aerial Combinated navigation method of guided cartridge
CN105486307B (en) For the line-of-sight rate by line method of estimation of maneuvering target
CN105180728B (en) Front data based rapid air alignment method of rotary guided projectiles
CN107255924A (en) Method for extracting guidance information of strapdown seeker through volume Kalman filtering based on dimension expansion model
CN105115508B (en) Alignment methods in rotation guided cartridge Quick air based on rear data
CN106379559B (en) A kind of transition air navigation aid suitable for guided missile launched by airplane
CN106529073A (en) Analysis method of handover conditions of hypersonic-velocity target interception missile based on interception geometry
CN104503471A (en) Terminal guidance method for maneuvering aircraft multi-terminal constraint backstepping sliding mode
CN111504256A (en) Roll angle real-time estimation method based on least square method
CN106403934A (en) Shell-borne geomagnetic attitude measurement and processing algorithm
CN101403593B (en) Dual-shaft strapdown platform plain shaft ultra semi-sphere stabilization method based on rolling/deflecting structure
CN103869097B (en) Rotating missile course angle, angle of pitch angular rate measurement method
Solano-López et al. Strategies for high performance GNSS/IMU Guidance, Navigation and Control of Rocketry
CN105674988B (en) A kind of Transfer Alignment of the equivalent single-shaft-rotation inertial navigation of MEMS
CN115685778A (en) Radar-seeking aircraft miss distance estimation method based on radio frequency semi-physical simulation
Feng et al. Analysis of Near Space Hypersonic Glide Vehicle Trajectory Characteristics and Defense Difficulties
CN113031645B (en) Missile angular rate stability augmentation strapdown guidance method based on UKF filtering
Haopeng et al. Research on Searching Guidance of TV Guided Missile
Wang et al. Research on Searching Guidance of TV Guided Missile
Xinyao et al. Trajectory simulation of virtual three point guidance
Li et al. Research on aerial alignment method of guided projectiles based on INS/radar command combination
CN106643797A (en) Post-bombardment gyro bias correction method

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C41 Transfer of patent application or patent right or utility model
TR01 Transfer of patent right

Effective date of registration: 20170214

Address after: 065500 Guan Industrial Park, Langfang, Hebei

Patentee after: Rainbow UAV Technology Co., Ltd.

Address before: 100074 Beijing, Fengtai District Yungang West Road, No. 17

Patentee before: China Aerospace Aerodynamic Technology Institute