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A Novel Guidance Law with Line-of-Sight Acceleration Feedback for
Missiles against Maneuvering Targets
Kemao Ma, Xiaoyu Zhang
Abstract
Terminal guidance law design and its implementation are considered for homing missiles against maneuvering targets. The lateral
acceleration dynamics are taken into account in the design. In the guidance law design, the ling-of-sight acceleration signals are
incorporated into the acceleration reference signals to compensate for the targets’ maneuvers. Then the commanded accelerations are
designed and the convergent tracking of the lateral accelerations to these signals is proven theoretically. In the guidance implementation,
a linear high-gain differentiator is used to estimate the line-of-sight rates and the line-of-sight acceleration signals. To avoid the
magnifying effects of higher order differentiation, a practical design of commanded accelerations is given to realize approximate
tracking of the lateral accelerations to the given reference signals. Simulation is conducted for both cases with and without measurement
noises. The simulation results justify the feasibility of the design and the implementation.
Keywords: homing missiles, maneuvering targets, guidance law implementation.
I. I NTRODUCTION
For terminal guidance laws of the homing missiles against maneuvering targets, two of the most important factors affecting
the guidance precision are the targets’ maneuvers and the lateral acceleration dynamics of the missiles[1]. If these two factors
are ignored in mathematical performance analysis, then the conventional proportional navigation guidance (PNG) laws, which
provide for missiles lateral acceleration commands proportional to the line-of-sight rates, are optimal in the sense that both the
miss distance and control efforts are accounted for in the performance cost functional[2]. This result motivated many guidance
laws based on PNG. For a maneuvering target, an augmented PNG law consists of conventional PNG and a compensation
term for the target’s maneuvering acceleration. Thus, the target’s maneuver is canceled out in the relative kinematics of the
missile and the target, and the performance of PNG against a non-maneuvering target is recovered. Since the target’s maneuver
is generally unknown, the remaining problem is how to estimate the target’s maneuver in guidance law implementation. For a
seeker with bearing only measurement, such as an infrared seeker, the acceleration components of the target’s maneuver are
not observable. Therefore, Kalman Filter technique, as well as conventional state observer technique, would be practical only
if an appropriate maneuvering model for the target’s maneuver was designed for the observability condition to be met[3]. By
extending the observer states, however, extended state observer technique can be used to estimate the target’s maneuver without
making any a priori assumptions on target’s maneuver[4][5]. In fact, extending the observer states is equivalent to a constant
acceleration (CA) model being adopted, and the discrepancy between the actual target’s maneuver and the output of the CA
This work was supported in part by the National Natural Science Foundation of China under grant numbers 61174001, 61321062.
Kemao Ma is with the Control and Simulation Center, School of Astronautics, Harbin Institute of Technology, Harbin, China, 150080. China.
makemao@hit.edu.cn
Xiaoyu Zhang is with Automation College, Harbin Engineering University, Harbin, China, 150001. Corresponding author.
zhangxiaoyu@hrbeu.edu.cn
model is treated as an uncertain term in the observer error dynamics and is suppressed via high-gain feedback. Thus no further
delicate models of the target’s maneuver are necessary.
The compensation for the targets’ maneuvers is a feed-forward method. The targets’ maneuvers can also be treated in a
feedback paradigm. In this case, the maneuvers of the targets are thought of as external disturbance inputs for the guidance
systems, and feedback control methods with good disturbance rejection, or attenuation, can be used to design the guidance
laws. Indeed, based on sliding mode control, various guidance laws are designed in which a switching term is added to the
PNG term[6][7]. The sliding-mode guidance laws are non-smooth, which may result in theoretical difficulties in guidance law
implementation when the lateral acceleration dynamics of the missiles are considered.
Both theoretical analysis and numerical simulation show that the lateral acceleration dynamics of the missiles can induce
miss distance, especially when the time constants are large. There are two approaches to solving this problem. One approach
is to improve the response characteristics of the lateral acceleration dynamics by adopting novel techniques such as lateral
jets[8], and the guidance and control systems are in a decoupled structure and designed in separately. The introduction of the
lateral jets endows the missiles with features of heterogeneous multiple actuators and substantial uncertainties due to the side jet
interaction effects[9], which bring potential difficulties in the design of the guidance and control systems. The other approach
is to conduct an integrated design of guidance and control[10]. In an integrated design, the guidance, control and guidance
information estimation are treated as a whole coupled system for which certain performance index is to be optimized. The
integrated system is quite complex with multiple constraints compared with the guidance system or the control system in a
decoupled structure, and there are still difficulties to be tackled in both theory and application.
In this paper, a novel guidance law is designed for missiles against maneuvering targets. In the guidance law, the target’s maneuvers are compensated for via incorporating the line-of-sight accelerations into the guidance commands, instead of constructing
a filter or an observer. Also incorporated into the commands are the dynamics of the missiles via a robust control design. The
idea is to design the guidance and control separately, then to redesign the lateral acceleration commands issued by the guidance
laws by incorporating the closed-loop lateral acceleration dynamics into the commands. By so doing, a high guidance precision
is reached. The rest of the paper is organized as follows. In Section II, the three-dimensional relative kinematics of a missile
and its maneuvering target are given, and the problem of terminal guidance law design is formulated. In Section III, a guidance
law is designed via incorporating into guidance commands the line-of-sight accelerations and the lateral acceleration dynamics
of the missile. In the following section, guidance law implementation is considered, and a practical design of the acceleration
commands is given. In Section V, numerical simulation is conducted. The conclusion is given in Section VI.
II. P ROBLEM F ORMULATION
We assume the terminal guidance scenario of a missile against a maneuvering air target. It is convenient to describe the
kinematics of the relative motion between the missile and its target in the line-of-sight coordinate system, denoted by OxL yL zL
and shown in Fig. 1. The origin O of OxL yL zL is set to the mass center of the missile (denoted by M); the axis OxL is
aligned with the line-of-sight (denoted by LOS), the half-line originated from O and pointing to the target (denoted by
T); the axis OyL is in the vertical plane, pointing upward and normal to OxL ; and the axis OzL is normal to both OxL
and OyL with its positive direction decided by the right-hand rule. We take the earth-fixed coordinate system Axyz as an
inertial reference. OxL yL zL can be obtained through a translation of Axyz, followed by two consecutive counterclockwise
rotations, first with an Euler angle qβ with respect to Ay, and second with an Euler angle qε with respect to OzL , as
shown in Fig. 1 where, for clarity of illustration, the origin A of Axyz is already translated to coincide with the origin O
of OxL yL zL , and the rotations are indicated with dotted curved arrows. Thus, the orientation of OxL yL zL with respect to Axyz
is characterized by qε and qβ , known as line-of-sight angles. The relative range vector, i.e. the radius vector of the target in
OxL yL zL originating from M towards T along LOS, is denoted by ⃗R, and its magnitude, the relative range, is denoted by R.
y
yL
T
xL
R
LOS
q
q
q
O( A)
M
x
q
z
zL
Fig. 1. Orientation of OxL yL zL with respect to Axyz
Next, we construct the mathematical description of the relative motion of the missile and the target in OxL yL zL . Denote the
respective unit vectors of OxL , OyL , and OzL by ⃗iL , ⃗jL , and ⃗kL , and we have
⃗R = R⃗iL + 0⃗jL + 0⃗kL ,
(1)
Denote the unit vectors of Ax, Ay, and Az by ⃗i, ⃗j, and ⃗k, respectively. Fig.1 shows that




⃗iL
⃗i




 ⃗ 


 jL  = L(qε , qβ )  ⃗j  ,




⃗kL
⃗k
where


cos qε
sin qε
0
cos qβ
0




L(qε , qβ ) =  − sin qε cos qε 0  
0
1


0
0
1
sin qβ 0

sin qε − cos qε sin qβ
cos qε cos qβ


=  − sin qε cos qβ cos qε
sin qε sin qβ

sin qβ
0
cos qβ
(2)
− sin qβ
0





cos qβ



.

Consider the two consecutive rotations shown in Fig. 1, and we have the expression of the angular velocity of OxL yL zL with
respect to Axyz as follows
⃗ =q˙β ⃗j + q˙ε⃗kL
ω
=q˙β sin qε⃗iL + q˙β cos qε ⃗jL + q˙ε⃗kL ,
(3)
where the latter equality is obtained using (2). The relative velocity between the missile and the target is
⃗R˙ =R˙⃗iL + ω
⃗ × R⃗iL
=R˙⃗iL + Rq˙ε ⃗jL − Rq˙β cos qε⃗kL ,
(4)
which further leads to
⃗R¨ =R¨⃗iL + R˙⃗i˙L + (R˙ q˙ε + Rq¨ε )⃗jL + Rq˙ε ⃗j˙L
˙
− (R˙ q˙β cos qε + Rq¨β cos qε − Rq˙β q˙ε sin qε )⃗kL − Rq˙β cos qε⃗kL ,
(5)
where
⃗i˙L =⃗
ω ×⃗iL
=q˙ε ⃗jL − q˙β cos qε⃗kL ,
⃗j˙L =⃗
ω × ⃗jL
= − q˙ε⃗iL + q˙β sin qε⃗kL ,
⃗k˙ L =⃗
ω ×⃗kL
=q˙β cos qε⃗iL − q˙β sin qε ⃗jL .
Substitute these expressions into (5), and we have
⃗R¨ =(R¨ − Rq˙ε2 − Rq˙2 cos2 qε )⃗iL
β
+ (2R˙ q˙ε + Rq¨ε + Rq˙2β sin qε cos qε )⃗jL
+ (−2R˙ q˙β cos qε + Rq˙ε q˙β sin qε − Rq¨β cos qε + Rq˙ε q˙β sin qε )⃗kL .
(6)
Denote the projections of the target’s acceleration on OxL , OyL , and OzL by aTr , aT ε and aT β , respectively, and denote the
projections of the missile’s acceleration by a , a and a , respectively. Account for the contributions to ⃗R¨ of these projections,
Mr
Mε
Mβ
and we have
⃗R¨ = (aTr − aMr )⃗iL + (aT ε − aM ε )⃗jL + (aT β − aM β )⃗kL .
(7)
Equating (6) to (7) gives the following mathematical description of the relative motion between the missile and its target:
R¨ =Rq˙ε2 + Rq˙β2 cos2 qε + aTr − aMr ,
2R˙
aT ε − aM ε
q˙ε − q˙β2 sin qε cos qε +
,
q¨ε = −
R
R
aT β − aM β
2R˙
q˙ + 2q˙ε q˙β tan qε −
.
q¨β = −
R β
R cos qε
(8)
(9)
(10)
In equations (9) and (10), the target’s acceleration components aT ε and aT β are unknown and can be thought of as external
disturbances. The acceleration components aM ε and aM β are provided by the missile acceleration dynamics which can be
modeled as follows
a¨M ε = − 2ζ ωn a˙M ε − ωn2 aM ε + ωn2 aM ε c + ∆ε (aM ε , a˙M ε ,t),
(11)
a¨M β = − 2ζ ωn a˙M β − ωn2 aM β + ωn2 aM β c + ∆β (aM β , a˙M β ,t),
(12)
where the dynamics are modeled as second-order linear dynamics with damping ratio ζ > 0 and natural frequency ωn > 0, and
aM ε c and aM β c are guidance commands to be designed. The differences of the second-order models from the real dynamics of
the missile are lumped into the uncertainties ∆ε (aM ε , a˙M ε ,t) and ∆β (aM β , a˙M β ,t) which satisfy, uniformly in t, the following
inequalities
|∆ε (aM ε , a˙M ε ,t)| 6 a¯M ,
(13)
|∆β (aM β , a˙M β ,t)| 6 a¯M ,
(14)
where a¯M is a known constant.
Classical guidance theory shows that if the line-of-sight rates q˙ε and q˙β are convergent to zero, then a satisfactory miss
distance can be guaranteed. Thus the guidance law design problem can be formulated as follows: With the existence of the
external disturbances aT ε and aT β and uncertainties ∆ε (aM ε , a˙M ε ,t) and ∆β (aM β , a˙M β ,t) satisfying (13) and (14), design aM ε c
and aM β c in equations (11) and (12) such that aM ε and aM β in equations (9) and (10) can make q˙ε and q˙β convergent to zero.
III. G UIDANCE L AW D ESIGN BASED ON L INE - OF -S IGHT ACCELERATION F EEDBACK
If the following equalities hold:
aM ε =aT ε − 2R˙ q˙ε − Rq˙2β sin qε cos qε + kRq˙ε ,
(15)
aM β =aT β + 2R˙ q˙β cos qε − 2Rq˙ε q˙β sin qε − kRq˙β cos qε .
(16)
where k is a positive constant, then equations (9) and (10) become
q¨ε = − kq˙ε ,
(17)
q¨β = − kq˙β ,
(18)
Equations (17) and (18) guarantee the exponential convergence of the line-of-sight rates, and the convergence rates are determined
by parameter k. Generally speaking, equalities (15) and (16) do not hold. However, if commanded acceleration components aM ε c
and aM β c are designed such that the left-hand sides of (15) and (16), aM ε and aM β , can track the respective right-hand sides,
then the dynamics of line-of-sight rates (17) and (18) will hold in an approximation sense. Thus the right-hand sides of (15)
and (16) should be incorporated into aM ε c and aM β c as reference signals for aM ε and aM β to track. To deal with the unknown
terms aT ε and aT β , we rewrite the equations (9) and (10) as
Rq¨ε + aM ε =aT ε − 2R˙ q˙ε − Rq˙2β sin qε cos qε ,
aM β − Rq¨β cos qε =aT β + 2R˙ q˙β cos qε − 2Rq˙ε q˙β sin qε .
(19)
(20)
Comparing the right-hand sides of (15) and (16) with those of (19) and (20) suggests taking the reference signals in the form of
aM ε r =aM ε + Rq¨ε + kRq˙ε ,
(21)
aM β r =aM β − Rq¨β cos qε − kRq˙β cos qε ,
(22)
based on which the commanded accelerations are in the form of
aM ε c =aM ε r + Kε ,
(23)
aM β c =aM β r + Kβ ,
(24)
where Kε and Kβ are yet to be designed. In (21) and (22) line-of-sight accelerations, q¨ε and q¨β , are used to compensate for
the target’s unknown maneuvers. The compensation effect depends on the tracking of aM ε and aM β to the respective right-hand
sides of (15) and (16). In the sequel, we design Kε (aM ε , a˙M ε ) and Kβ (aM β , a˙M β ) to guarantee the tracking, as well as to account
for the uncertainties in (11) and (12).
Define the tracking error vectors as
[
eε =
[
]T
eε 1
eε 2
]T
,
aM ε − aM ε r a˙M ε − a˙M ε r
[
]T
eβ = eβ 1 eβ 2
]T
[
= aM β − aM β r a˙M β − a˙M β r
,
=
(25)
(26)
and, according to (11) and (12), we have the error dynamics as follows
1
∆ε (aM ε , a˙M ε ,t)),
ωn2
1
e˙β =Aeβ + B(aM β c − aM β r + fβ + 2 ∆β (aM β , a˙M β ,t)),
ωn
e˙ε =Aeε + B(aM ε c − aM ε r + fε +
(27)
(28)
where
2ζ a˙M ε r a¨M ε r
− 2 ,
ωn
ωn
2ζ a˙M β r a¨M β r
− 2 ,
fβ = −
ωn
ωn




0
1
0
, B = 
.
A =
ωn2
−ωn2 −2ζ ωn
fε = −
(29)
(30)
(31)
Substitute (23) and (24) into (27) and (28), and we have
1
∆ε (aM ε , a˙M ε ,t)),
ωn2
1
e˙β =Aeβ + B(Kβ + fβ + 2 ∆β (aM β , a˙M β ,t)),
ωn
e˙ε =Aeε + B(Kε + fε +
(32)
(33)
Since ζ > 0 and ωn > 0, A in (31) is a Hurwitz matrix. Therefore, for any Q > 0, there is a P > 0, such that the following
Lyapunov equation holds:
AT P + PA = −Q.
(34)
For error dynamics (32) and (33), define the Lyapunov function candidate asV = eTε Peε + eTβ Peβ , and we have
V˙ =eεT (AT P + PA)eε + eβT (AT P + PA)eβ
+ 2eTε PB(Kε + fε +
1
1
∆ε (aM ε , a˙M ε ,t)) + 2eTβ PB(Kβ + fβ + 2 ∆β (aM β , a˙M β ,t)).
ωn2
ωn
(35)
Substitute (34) into (35) and consider (13) and (14), and we have
V˙ 6 − eTε Qeε − eTβ Qeβ
+ 2eTε PB(Kε + fε ) + 2eTβ PB(Kβ + fβ ) +
2a¯M
(∥PBeε ∥ + ∥PBeβ ∥).
ωn2
(36)
If we design Kε and Kβ as follows
2a¯M
sign(BT Peε ),
ωn2
2a¯M
Kβ = − fβ − 2 sign(BT Peε ),
ωn
Kε = − fε −
(37)
(38)
then from (36) we have V˙ 6 −eTε Qeε − eTβ Qeβ , which justifies the asymptotic convergence of error vectors eε and eβ .
IV. G UIDANCE L AW I MPLEMENTATION
Here we assume that the radar seeker of the missile can provide relative range, relative range rate, and line-of-sight angles
for guidance law implementation. Since angular rates and accelerations of line-of-sight angles are used in the guidance law, the
implementation is focused on numerical differentiation algorithms. Here we employ the following linear differentiator
k1
(x1 − f (t)),
ε
k
x˙2 =x3 − 22 (x1 − f (t)),
ε
k
x˙3 = − 33 (x1 − f (t)),
ε
x˙1 =x2 −
(39)
(40)
(41)
where f (t) is the input signal to be differentiated, ε > 0 is a small design parameter, and k1 > 0, k2 > 0 and k3 > 0 are such
that
s3 + k1 s2 + k2 s + k3
(42)
is a Hurwitz polynomial. Here we assume that the third order derivative of f is bounded, i.e., there exists a constant K f such
that
| f (3) (t)| 6 K f , ∀t.
Define


e1


e =  e2

e3

 
 
=
 
(43)

x1 − f (t)
ε2
x2 − f˙(t)
ε2
x3 − f¨(t)


,

(44)
and from (39) - (41) we have
ε e˙ = Ae e + ε Be f (3) (t),
where

−k1


Ae =  −k2

−k3

1
0
0
0
(45)


0






1  , Be =  0  .



0
1
Since (42) is a Hurwitz polynomial, A is Hurwitz. Therefore, for any given Qe > 0, there exists a P > 0, such that
ATe P + PAe = −Qe .
(46)
Taking Ve (e) = eT Pe e, and it is easy to show that system (45) is input-to-state stable[11] with f (3) (t) thought of as an external
input, and V˙ (e) 6 0 whenever ∥e∥ >
2ε ∥Pe Be ∥K f
λmin (Qe )
. This means that the state of the system (45), the error defined in (44), will
converge in finite time T (ε ), dependent on ε , to the following set
{
}
2ε ∥Pe Be ∥K f
S(ε ) = e ∈ R3 ∥e∥ 6
,
λmin (Qe )
(47)
which is dependent on the parameter ε , and shrinks to zero as ε tends to zero from above. Thus for an input signal f satisfying
(43), the error variables defined in (44) are bounded, and
lim x1 (t) = f (t),
(48)
lim x2 (t) = f˙(t),
(49)
lim x3 (t) = f¨(t).
(50)
t→∞,ε ↓0
t→∞,ε ↓0
t→∞,ε ↓0
We can also see from (45) that the converging rates of (48) - (50) increase with the decrease of the value of ε :
lim T (ε ) = 0,
ε ↓0
and the bound K f in (43) can be arbitrarily large provided ε is small enough. However, with the decrease of ε , the error variables
ei (t), i = 1, 2, 3, 0 < t < T (ε ) will become very large, known as the peaking phenomenon[12]. To attenuate the peaking with the
set S(ε ) unchanged, we can introduce a satiation function to the differentiator (39) - (41). Here the details will not be discussed
theoretically, but we note that numerical simulation we conducted has revealed the effectiveness of this technique.
β
We denote the state of the differentiator (39) - (41) by xiε , i = 1, 2, 3 when the input signal is qε , and by xi , i = 1, 2, 3 when
the input signal is qβ . Therefore, the reference signals given in (21) and (22) are implemented by replacing q˙ε , q¨ε , q˙β , q¨β by
β
β
x2ε , x3ε , x2 and x3 , respectively, provided R, qε and qβ are available. As far as measurement noises are concerned, we need to
limit the order of differentiation operations as low as possible, especially to avoid very high order differentiations. Here only
first and second order differentiations are necessary, and we can limit the effects of noises by limiting the value of the parameter
ε . If we used the differentiator to implement Kε and Kβ in (37) and (38), the further differentiation operations on aM ε r and
aM β r required in (29) and (30) would have significantly magnified the noises of the measured signals qε and qβ , since third
and fourth order differentiations are involved. To avoid this, here we give a practical design of aM ε r and aM β r , instead of the
theoretical design given in (37) and (38). The idea is to treat the bounded uncertainties ∆ε and ∆β as input signals to dynamics
(11) and (12), and to reduce the gain of ∆ε and ∆β as well as to increase the frequency bandwidths of aM ε r and aM β r .
Let
2ζ (K − 1)
a˙M ε − (K 2 − 1)aM ε + (K 2 − 1)aM ε r ,
ωn
2ζ (K − 1)
a˙M β − (K 2 − 1)aM β + (K 2 − 1)aM β r ,
Kβ = −
ωn
Kε = −
(51)
(52)
where K > 1 is a design parameter, and substitute (51) and (52) into (11) and (12), and we have
a¨M ε = − 2ζ (K ωn )a˙M ε − (K ωn )2 aM ε + (K ωn )2 aM ε r + ∆ε (aM ε , a˙M ε ,t),
(53)
a¨M β = − 2ζ (K ωn )a˙M β − (K ωn )2 aM β + (K ωn )2 aM β r + ∆β (aM β , a˙M β ,t).
(54)
We can see from (53) and (54) that the gains of uncertain input signals ∆ε and ∆β are reduced K 2 times, with the gains of
aM ε r and aM β r unchanged and the bandwidths increased K times. Although Kε and Kβ in (51) and (52) cannot guarantee
asymptotic convergence of aM ε and aM β to their respective reference signals aM ε r and aM β r , as guaranteed by (37) and (38),
but a satisfactory tracking can be guaranteed provided K is sufficiently large.
V. S IMULATION
Here we consider the terminal guidance phase with the following initial conditions
˙
R(0) = 6000m, R(0)
= 600m/s, qε (0) = 27◦ , q˙ε (0) = 1.5◦ /s, qβ (0) = 30◦ , q˙ε (0) = −1.25◦ /s.
The sampling period of the guidance system is assumed to be T =5ms. Since the time horizon of a typical terminal guidance
phase ranges over a time interval of several seconds or just over ten seconds, we can employ the Euler integration as the
numerical implementation of differentiator (39) - (41) without much loss of precision, i.e.
[
]
x1 (kT ) − f (kT )
x1 ((k + 1)T ) =x1 (kT ) + T x2 (kT ) − k1 sat(
) ,
Ks ε
]
[
x1 (kT ) − f (kT )
x2 ((k + 1)T ) =x2 (kT ) + T x3 (kT ) − k2 sat(
) ,
Ks ε 2
]
[
x1 (kT ) − f (kT )
) ,
x3 ((k + 1)T ) =x3 (kT ) + T −k3 sat(
Ks ε 3
where the parameter Ks is set to 80, ε is set to 0.011, and the parameters k1 , k2 and k3 are set to 3, 3, and 1, respectively.
All the initial values of the differentiator are set to zero. The parameters in the dynamics (11) and (12) are set to ζ = 0.7 and
ωn = 8. The maximum acceleration the missile can provide is assume to be a¯M = 200m/s2 , and the commanded accelerations
issued by the guidance system take the following form
aM ε r + Kε
),
a¯M
aM β r + Kβ
aM β c =a¯M sat(
),
a¯M
aM ε c =a¯M sat(
where aM ε r and aM β r are given in (21) and (22) with k = 5, and Kε and Kβ are given in (51) and (52) with K = 4. The minimum
range for the seeker to operate is assumed to be R¯ b = 100m, and when R < R¯ b , both aM ε c and aM β c are set to zero.
Numerical simulation is conducted for the above scenario with an integration step 0.0001s. For a non-maneuvering target, the
interception time is 10.0577s, and the miss distance is 0.0475m. Then we consider the case where the maneuver of the target
takes the following form
aT ε =100 sin(2π fε + θε )m/s2 ,
aT β =100 sin(2π fβ + θβ )m/s2 ,
where fε =0.35Hz, θε = π5 , fβ =0.5Hz, θβ = π5 . The interception time is 10.1039s, and the miss distance is 0.1343m. The lineof-sight rates q˙ε , q˙β and their respective estimates are shown in Fig. 2 and Fig. 3, and a satisfactory tracking is obtained. The
acceleration acceleration components of the missile are shown in Fig. 4.
To validate the proposed guidance law and its implementation when measurement is corrupted by noises, the simulation is also
conducted with qε and qβ added with a normal stochastic noise with zero mean and standard deviation σ = 30µ rad. Numerical
simulation is repeated for 100 times. The miss distance values, with a mean value of 0.4856m and a standard deviation of
0.3372m, are shown in Fig. 5. The line-of-sight rates q˙ε , q˙β and their respective estimates under the noisy condition are shown
in Fig. 6 and Fig. 7. The lateral acceleration components of the missile are shown in Fig. 8.
6
actual signal
estimated signal
line−of−sight rate: d/dt qε / (°/s)
4
2
0
−2
−4
−6
0
2
4
6
tmie / s
8
10
Fig. 2. line-of-sight rate q˙ε and its estimate: without noises
6
actual signal
estimated signal
line−of−sight rate: d/dt qβ / (°/s)
4
2
0
−2
−4
−6
0
2
4
6
tmie / s
8
10
Fig. 3. line-of-sight rate q˙β and its estimate: without noises
200
acceleration components of the missile / (m/s2)
aMε
aMβ
150
100
50
0
−50
−100
−150
−200
0
2
4
6
time / s
8
10
Fig. 4. The acceleration components of the missile: without noises
1.4
miss distance values / m
1.2
1
0.8
0.6
0.4
0.2
0
0
20
40
60
simulation times
80
100
Fig. 5. The miss distance values: with noises
6
actual signal
estimated signal
line−of−sight rate: d/dt qε / (°/s)
4
2
0
−2
−4
−6
0
2
4
6
tmie / s
8
10
Fig. 6. line-of-sight rate q˙ε and its estimate: with noises
6
actual signal
estimated signal
line−of−sight rate: d/dt qβ / (°/s)
4
2
0
−2
−4
−6
0
2
4
6
tmie / s
8
10
Fig. 7. line-of-sight rate q˙β and its estimate: with noises
VI. C ONCLUSION
A noel terminal guidance law design and its implementation are considered for missiles against maneuvering targets. The
targets’s maneuvers are compensated for via feeding back the line-of-sight accelerations. Therefore no maneuver models for the
targets are necessary. The lateral acceleration dynamics are also incorporated into the guidance commands. The implementation
of the guidance laws only requires the first and second order derivative signals of the line-of-sight angles. A high gain
linear differentiator is used in the guidance law implementation. Numerical simulation is conducted to validate the design
and implementation. In the simulation, both cases with and without measurement noises are considered. The results show the
effectiveness. We note that in the implementation, the differentiator employs no statistical features of the noises, which deserves
further investigation to improve the performance of the given design.
200
acceleration components of the missile / (m/s2)
aMε
aMβ
150
100
50
0
−50
−100
−150
−200
0
2
4
6
time / s
8
10
Fig. 8. The acceleration components of the missile: with noises
Acknowledgment
This work was supported in part by the National Natural Science Foundation of China under grant numbers 61174001,
61321062.
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