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Derivation of the Fundamental Missile Guidance Equations, Lecture notes of Differential Equations

Before a missile is launched, that is, during the prelaunch phase, the missile needs to know where to go. It knows that it is supposed to go to the target, ...

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341
AARMS Vol. 14, No. 4 (2015) 341348.
Derivation of the Fundamental Missile Guidance
Equations
PAPP István,1 SZILVÁSSY László,2 ÓVÁRI Gyula3
In order to guide itself to a successful target intercept, the missile must obtain in- formation about the target.
The prelaunch and post launch information too, must be gathered. Before a missile is launched, that is, during
the prelaunch phase, the missile needs to know where to go. It knows that it is supposed to go to the target, but
it must be told where the target is. The missile is told where the target is by electrical signals entering through
the umbilical from the launcher. These signals are head aimed (to point the missile head at the target), English
bias (to point the missile at the intercept point), and an estimate of true target Doppler on the simu- lated
Doppler line.
Keywords: missile, equations of motion, guidance, derivation
Introduction
Then missile then flies (according to the proportional navigation guidance law), senses a change in the line-of-sight
angle between the missile velocity vector and the target. In addi- tion, the missile is given certain conditioning signals,
which let the missile adjust for varia- tions. These conditioning signals are the autopilot commands to adjust autopilot
responses, and auxiliary Doppler positioning signal (or signals). Furthermore, though the missile is de - signed to guide to
impact, an actual impact may not occur, and the missile may miss the target by some finite distance. Specific circuits in
the missile give an indication of closest missile approach to the target. These circuits then cause the warhead to be
triggered so as to explode as close to the target as possible. In addition, other circuits in the missile are designed to pro-
vide indications of a total miss. All of this logic and information is built into the missile, so that the missile knows what
to do before it is launched. [1]
Missile Guidance Types
Guidance systems can use any one of several methods or laws to coordinate a missile along a trajectory or flight-path to
intercept a target (for example an aircraft). The specific target flight path information required by the guidance
package depends on which law is used. In this section we will discuss the three types of pursuit courses, which are the
following:
pure pursuit;
deviated pursuit;
pure collision.
1 National University of Public Service, Budapest, Hungary, e-mail: pappi@uni-nke.hu
2 National University of Public Service, Budapest, Hungary, e-mail: szilvassy.laszlo@uni-nke.hu
3 National University of Public Service, Budapest, Hungary, e-mail: ovary.gyula@uni-nke.hu
pf3
pf4
pf5
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341

AARMS Vol. 14, No. 4 (2015) 341–348.

Derivation of the Fundamental Missile Guidance

Equations

PAPP István,^1 SZILVÁSSY László,^2 ÓVÁRI Gyula^3

In order to guide itself to a successful target intercept, the missile must obtain in- formation about the target. The prelaunch and post launch information too, must be gathered. Before a missile is launched, that is, during the prelaunch phase, the missile needs to know where to go. It knows that it is supposed to go to the target, but it must be told where the target is. The missile is told where the target is by electrical signals entering through the umbilical from the launcher. These signals are head aimed (to point the missile head at the target), English bias (to point the missile at the intercept point), and an estimate of true target Doppler on the simu- lated Doppler line. Keywords: missile, equations of motion, guidance, derivation

Introduction

Then missile then flies (according to the proportional navigation guidance law), senses a change in the line-of-sight angle between the missile velocity vector and the target. In addi- tion, the missile is given certain conditioning signals, which let the missile adjust for varia- tions. These conditioning signals are the autopilot commands to adjust autopilot responses, and auxiliary Doppler positioning signal (or signals). Furthermore, though the missile is de- signed to guide to impact, an actual impact may not occur, and the missile may miss the target by some finite distance. Specific circuits in the missile give an indication of closest missile approach to the target. These circuits then cause the warhead to be triggered so as to explode as close to the target as possible. In addition, other circuits in the missile are designed to pro- vide indications of a total miss. All of this logic and information is built into the missile, so that the missile knows what to do before it is launched. [1]

Missile Guidance Types

Guidance systems can use any one of several methods or laws to coordinate a missile along a trajectory or flight-path to intercept a target (for example an aircraft). The specific target flight path information required by the guidance package depends on which law is used. In this section we will discuss the three types of pursuit courses, which are the following:

  • pure pursuit;
  • deviated pursuit;
  • pure collision.

1 National University of Public Service, Budapest, Hungary, e-mail: pappi@uni-nke.hu 2 National University of Public Service, Budapest, Hungary, e-mail: szilvassy.laszlo@uni-nke.hu 3 National University of Public Service, Budapest, Hungary, e-mail: ovary.gyula@uni-nke.hu

I T

Figure 1. Types of the guidance. [1: 183]

After that, we develop the respective differential equations. The homing trajectory that a missile flies depends on the type of guidance law employed. The guidance law depends on the mathematical requirements or constraints of the engagement. Figure 1 will be used as the basis to derive these equations. In particular, the kinematics of an attack course, as illustrated in Figure 1, are based on the relationships between the:

  • interceptor (or missile) velocity V ;
  • the target velocity V ;
  • the interceptor lead angle λ ;
  • the target aspect angle α ;
  • the interceptor to target range R. The basic differential equations can be derived from considerations of the geometry. Re- ferring to Figure 1, the range rate can be written in the form

(1). where the angle reference is the interceptor-to-target range vector. The velocity compo- nents orthogonal to R consist of two parts: (1) the translational component, and (2) the tangential (or turning) component.

M T

M T

0

Where R is the range magnitude, θ is the orientation of the line of sight to the target, V is the interceptor missile velocity component, and V nontrivial cases of a stationary target or head/tail chase ( θ = ± 90°), we have

where κ = V

(5). Letting C be the constant of integration, the general solution of (5) assumes the form

Therefore,

From the identity

We have

The integration constant C can be determined from the initial conditions R0 and θ0 = ± 90°. Thus from (6) we obtain

θ = 0, ρ = 1, R = C.

From the above analysis, we note that the missile will intercept the target if its velocity is greater than that of the target. From (6), ρ ( θ ) can be plotted for different values of the param- eter κ (i.e., κ = 0.5, 1.0, 1.5, 2.0, 3.0). [1] [2]

Deviated pursuit

Deviated pursuit points the nose of the intercepting missile (or aircraft) by a fixed angle in front of the target (see Figure 1). In other words, an interceptor directing its velocity vector at a constant angle ahead of the target flies a deviated pursuit attack course. Since the inter- ceptor lead angle is constant for deviated pursuit, λ = λ. Therefore, from (1) and (2) we have the differential equations

(7a). (7b).

M T

M T

Figure 3. Deviated pursuit guidance. [1: 186]

In order to obtain the deviated pursuit algebraic equations, we will use Figure 3. The differential equations for the deviated pursuit case are (λ = constant)

(8a).

Solution of the differential equations for R and θ requires a given V initial values of R and θ. The normal acceleration for the deviated pursuit is obtained as (9). The angle off the target tail, at which θ is maximum, is obtained from the expression (10). where V intercept the target can be obtained from the expression

Pure collision

A pure collision course is a straight-line course flown by an interceptor so as to collide with the target. Referring to Figure 4.9, the differential equation assumes the form

θ = konstans

(12c).

Figure 4. Maximum manoeuvre capability. [1: 190]

The other factor influencing maximum turn rate is the roll orientation of the missile with respect to the manoeuvre plane. If the direction of the turn is perpendicular to either the pitch or yaw plane, then the turn will be confined only to that plane, and the maximum acceleration will be limited by the autopilot to 25 g’s. If the direction of the turn is halfway between the two planes, both autopilots will contribute, and the allowable turning acceleration is as high as 25√2, i.e., about 35 g’s. That the time for which the missile locks on the target can vary from about 0.6 to 1.0 second. Increased lock time can have a significant affect because of the rapidly changing geometry, and usually results in increased missile flight times to attain a successful intercept. Because lock time is an uncontrollable factor, a degree of uncertainty is introduced to the minimum-range zone. These relationship, we can see in Figure 4. [1] [4]

Figure 5. Geometry of the interception process. [1: 190]

At this point, simple interception model dynamics will be developed. Assuming that the target and the missile motions evolve in the same horizontal plane, the geometry of the in- terception process is shown in Figure 5. The interception is characterized by two variables, namely, the target range and the LOS angle. The kinematic equations are expressed by the following relations:

where r = missile - target range; λ = LOS angle; θ = pitch angle (or missile axis angle); u = longitudinal velocity component of the missile; w = normal velocity component of the missile. The rate of variation of the LOS , dλ/dt , is measured by the seeker, and the tracking error related to the system of measurement is neglected. In other words, the axis of the seeker is assumed to lie always along the LOS. The seeker head will be limited to a cone with a maxi- mum half-angle equal to 45°, which imposes the saturation constraint | λ − θ | ≤ 45°. [1] [3] [4]

References

[1] SIOURIS, G. M.: Missile Guidance and Control Systems. New York: Springer, 2003. http:// cdn.preterhuman.net/texts/terrorism_and_pyrotechnics/rocketry/Missiles_and_Warheads/ Missile%20Guidance%20&%20Control%20Systems.pdf (downloaded: 2015.07.15) [2] BALL, R. E.: The Fundamentals of Aircraft Combat Survivability Analysis and Design. Virginia: Virginia Polytechnic Institute and State University Blacksburg, 1985. [3] PALUMBO, N. F., BLAUWKAMP, R. A., LLOYD, J. M.: Modern Homing Missile Guidance Theory and Techniques. Johns Hopkins APL Technical Digest , 29 1 (2010). [4] LIN, C. M., HSU, C. F., CHANG, S. K., WAI, R. J.: Guidance – Law Evaluation for Missile Guidance Systems. Asian Journal of Control , 2 4 (2000), 243–250.