lateral control for uavs using sliding mode technique
DESCRIPTION
Abstract: This paper presents sliding mode based lateral control for UAVs using a nonlinear sliding approach. The control is shown to perform well in different flight conditions including straight and turning flight and can recover gracefully from large track errors. Saturation constraints on the control input are met through the nonlinear sliding surface, while maintaining high performance for small track errors. Stability of the nonlinear sliding surface is proved using an appropriate Lyapunov function. The main contribution of this work is to develop a robust lateral control scheme that uses readily available sensor information and keeps the track error as small as possible without violating control constraints. In the proposed scheme the only information used in the control law is the lateral track error and the heading error angle. No information is required about the desired path/mission, which therefore can be changed online during runtime. This scheme is implemented on a high fidelity nonlinear 6-degrees-of-freedom (6-dof) simulationand different scenarios are simulated with large and small track errors in windy and calm conditions.Simulation results illustrate the robustness of the proposed scheme for straight and turning flight, in thepresence of disturbances, both for large and small track errors. Furthermore it is shown that the saturation limits of the control input are not exceeded in all cases.TRANSCRIPT
Lateral Control for UAVs using Sliding Mode Technique
M. Zamurad Shah*, R. Samar**, A.I. Bhatti**
* Mohammad Ali Jinnah University, Islamabad, Pakistan, (Ph.D. Student, email: [email protected])
** Mohammad Ali Jinnah University, Islamabad, Pakistan
Abstract: This paper presents sliding mode based lateral control for UAVs using a nonlinear sliding
approach. The control is shown to perform well in different flight conditions including straight and turning
flight and can recover gracefully from large track errors. Saturation constraints on the control input are met
through the nonlinear sliding surface, while maintaining high performance for small track errors. Stability
of the nonlinear sliding surface is proved using an appropriate Lyapunov function. The main contribution
of this work is to develop a robust lateral control scheme that uses readily available sensor information and
keeps the track error as small as possible without violating control constraints. In the proposed scheme the
only information used in the control law is the lateral track error and the heading error angle. No
information is required about the desired path/mission, which therefore can be changed online during run-
time. This scheme is implemented on a high fidelity nonlinear 6-degrees-of-freedom (6-dof) simulation
and different scenarios are simulated with large and small track errors in windy and calm conditions.
Simulation results illustrate the robustness of the proposed scheme for straight and turning flight, in the
presence of disturbances, both for large and small track errors. Furthermore it is shown that the saturation
limits of the control input are not exceeded in all cases.
1. INTRODUCTION
Two approaches are used for trajectory tracking of UAVs. In
first approach, UAV guidance and control problem is
separated into an outer guidance and an inner control loop.
Based on lateral track error and heading angle, outer
guidance loop generates a desired reference bank (roll) angle
and inner control law generates command to control surface
to follow the desired reference bank angle. In the second
approach, guidance and control laws are designed together in
a single framework.
In most applications, the separate inner and outer loop
approach is commonly used since it is simpler and well-
established design methods are available for inner loop
vehicle control. For outer guidance loop, different approaches
have been used in the past. Linear proportional and derivative
(PD) control (Siouris, 2004; Pappoullias, 1994) has been used
in many UAV applications. But during curved path following
in the present of a persistent disturbance (e.g. wind),
performance of PD control degrades. A nonlinear scheme has
been given by (Park, 2004; Park, 2007) showing improved
performance than PD scheme. But in the case of large track
error, control output of this nonlinear scheme saturates and
there is no stability proof during control saturation. A
conventional linear proportional and derivative lateral control
with some non-linear modifications has been given by
(Samar, 2007) which enhance the tracking performance. But
the control proposed by (Samar, 2007) is an ad-hoc solution
and as such no stability proof exists. In literature, other
different approaches have been proposed by (Nelson, 2006;
Regina 2009; Jia, 2010; Shtessel, 2009).
Sliding mode control is a technique derived from variable
structure control. Ideal sliding mode control is insensitive to
parameter variations and external disturbances, regardless of
nonlinearity and uncertainty (Bandyopadhyay, 2009). For a
certain class of systems, sliding mode controller design
provides a systematic approach to the problem and guarantee
system insensitivity with respect to the matched disturbance
and model uncertainty. The controller so designed is unique
since the performance of the controller depends on the design
of sliding surface and not the states tracking directly [Slotine,
1991]. Idea is to force the trajectory states towards the sliding
surface and once achieved, the states are constrained to
remain on the surface. Although the technique has good
robustness properties, pure sliding mode control presents
drawbacks that include large control requirements and
chattering. Chattering may be settled by smoothing the
control input using boundary layer or bandwidth limited
sliding mode control. Saturations and sigmoid functions are
used, for example as “filters” for the output of a
discontinuous signal in order to obtain a continuous one that
is realizable by mechanical hardware.
In this work, the approach used is to divide the UAV
guidance and control problem into an outer guidance and an
inner control loop (Fig. 1). Here, it is assumed that a fast
inner control law is already designed that can track the
desired (reference) roll angle command with minimal
overshoot. A Sliding mode based outer guidance loop is
proposed here in this paper for robust tracking. Main concern
here is the robustness and performance with minimum
information. The only inputs of guidance loop are lateral
track error & current heading error angle, and output is
desired/reference roll angle. In order to meet the constraints
of high performance in small track error and a bounded
Preprints of the 18th IFAC World CongressMilano (Italy) August 28 - September 2, 2011
Copyright by theInternational Federation of Automatic Control (IFAC)
11121
heading error angle in the case of large track error, a non-
linear sliding surface is proposed here.
Fig. 1: Guidance & Control approach used in this work
The stability of this non-linear sliding surface is proved with
the help of a Lyapunov function. Also the proposed scheme is
implemented in non-linear 6-dof simulation and simulation
results of different cases are shown here, that validate the
robustness of this proposed scheme.
2. PROBLEM DEFINITION
Notation of different variables used in this paper is same as
used in (Siouris 2004; Samar, 2007). Here, „𝑦‟ is the cross
track error, „𝜓𝐺 ‟ is the velocity heading, „𝜓𝑅‟ is the reference
heading and 𝜓𝐸 = 𝜓𝐺 − 𝜓𝑅 (Fig. 2). Note that magnitude of
𝜓𝐸 should be less than 90 degrees.
Fig. 2: Definition of cross track (𝑦), „𝜓𝐺 ‟, „𝜓𝑅‟ and „𝜓𝐸‟
2.1 Assumptions
For way point tracking during straight path 𝜓 𝑅 = 0, while
during circular path 𝜓 𝑅 is non-zero but may be small
depending on the mission. In this paper, 𝜓 𝑅 is assumed small
and neglected here.
While designing this outer guidance loop it is assumed that a
fast inner control loop is already designed. As the inner
control loop is fast enough (at least 5 times), so we assumed
here that the actual roll angle (𝜙) is approximately equal to
the desired/reference roll angle (𝜙𝑅).
2.2 Model of System Dynamics
During steady turn when vehicle is banked at an angle 𝜙, Lift
(L) is resolved into two components 𝐿 cos 𝜙 and 𝐿 sin 𝜙 that
balance the weight and centrifugal force respectively (Fig. 3)
𝐿 cos 𝜙 = 𝑚𝑔, 𝐿 sin 𝜙 =𝑚 𝑉2
𝑅 (1)
where 𝑚 is the mass, 𝑔 is the gravitational acceleration, V is
the velocity of Aircraft/UAV and R is the radius of turn.
From (1) we have
tan 𝜙 =𝑉2
𝑅 𝑔 (2)
Moreover we also know that during steady turn 𝑉 = 𝑅 𝜓𝐺 , so
(2) becomes
tan 𝜙 =𝑉 𝜓𝐺
𝑔 (3)
Resolving the components of velocity vector in Fig. 2, we
have
𝑦 = 𝑉 sin 𝜓𝐸 (4)
Using 𝜓𝐸 = 𝜓𝐺 − 𝜓𝑅 and assumption 𝜓 𝑅 = 0, (3) becomes
tan 𝜙 =𝑉 𝜓𝐸
𝑔 (5)
Fig. 3: Components of Lift (L) during steady turn
Using assumption 𝜙 ≅ 𝜙𝑅, (5) becomes
tan 𝜙𝑅 =𝑉 𝜓𝐸
𝑔 (6)
In summary, the overall dynamics of the outer guidance loop
is governed by (4) and (6) which can be also written in state-
space form as
𝑦 = 𝑉 sin 𝜓𝐸 (7)
𝜓𝐸 =
𝑔 tan 𝜙𝑅
𝑉 (8)
where cross track error „y‟ and „𝜓𝐸‟ are the state variables
and reference bank/roll angle „𝜙𝑅‟ is the output of outer
guidance loop. Also note that in case of small 𝜓𝐸 , 𝑦 ≅ 𝑉𝜓𝐸
that means that state „𝜓𝐸‟ is approximately equal to „𝑦
𝑉‟.
Yaw rate
roll angle
Ref Roll angle
Current Position & Heading angle
Desired Position &
Heading angle
Aileron
Rudder
Mission
Guidance
Control
Lateral Dynamcis
Preprints of the 18th IFAC World CongressMilano (Italy) August 28 - September 2, 2011
11122
2.3 Control Task
Using readily available sensor information „y‟ and „𝜓𝐸‟,
control task is to keeps the track error as small as possible by
generating an appropriate „𝜙𝑅‟. Also the output „𝜙𝑅‟ of
control system should be a bounded number (magnitude <30
degrees).
3. PROPOSED LATERAL CONTROL SCHEME
3.1 Why Non-Linear Sliding Surface?
In case of bank-to-turn, the UAV roll angle should be
bounded by some finite number (say approximately 𝜋
6). Hence
the output of guidance block (reference roll angle) should
also be bounded ( 𝜙𝑅 < 𝜙𝑚𝑎𝑥 =𝜋
6). During flight, large
track error is possible due to loss of GPS for long time so the
possibility of large track error can‟t be ignored during flight.
Suppose we choose a linear sliding surface 𝑆 = 𝜓𝐸 + 𝜆 𝑦 for
some positive scalar 𝜆. For performance in case of small
track error, we need a large 𝜆 so that we can reach the origin
𝑦, 𝜓𝐸 = (0,0) in minimum time. But on the other hand
choosing a large 𝜆 implies that in case of large track error we
should have a large 𝜓𝐸 (> 90 degrees) which is not possible
as magnitude of 𝜓𝐸 could not exceed 𝜋
6. So choice of 𝜆 is
trade-off between performance in the case of small track error
and a realizable magnitude of 𝜓𝐸 in the case of large track
error, and both constraints cannot be satisfied at the same
time with a linear sliding surface.
Fig. 4: Linear sliding surface (S) for some positive 𝜆
3.2 Non-Linear Sliding Surface
For performance in case of small track error and also
magnitude of 𝜓𝐸 less than 90 degrees, we choose a non-linear
sliding surface
𝑆 = 𝜓𝐸 + 𝛼 tan−1(𝛽𝑦) (9)
where 𝛼 and 𝛽 are scalars and later we will show that for
stability of sliding surface 𝛼𝛽 > 0. Performance in case of
small track error can be changed by changing parameter 𝛽
while another parameter 𝛼 can be used to keep the magnitude
of 𝜓𝐸 less than 90 degrees ( 𝛼 ≤ 1). A graph of above
sliding surface is shown in Fig. 5 for some particular 𝛼 and 𝛽.
Now an important question arises, is the motion on sliding
surface stable? Motion on sliding surface is described
by 𝑆 = 0, that is
ψE + 𝛼 tan−1(𝛽𝑦) = 0 (10)
The stability of (10) can be proved using Lyapunov theory,
Lyapunov candidate function (𝐕) for stability of (10) is
𝐕 =1
2 y2 + ψE
2 = 1
2 y2 + 𝛼 tan−1 𝛽𝑦 2 (11)
And the derivative of Lyapunov function 𝐕 is
𝐕 = −𝑉𝑦 sin 𝛼 tan−1 𝛽𝑦
−𝛼2𝛽 𝑉
1 + 𝛽2𝑦2tan−1 𝛽𝑦 sin 𝛼 tan−1 𝛽𝑦 12
as −𝜋
2≤ tan−1 𝛽𝑦 ≤
𝜋
2 and 𝛼 ≤ 1, sin 𝛼 tan−1 𝛽𝑦 will
have a same sign as 𝑦 if 𝛼𝛽 > 0. So the derivative of
Lyapunov function 𝐕 in (12) is negative definite if 𝛼𝛽 > 0
and 𝛼 ≤ 1.
In summary, the proposed non-linear sliding surface (9) is a
stable sliding surface subject to the above stated conditions
𝛼𝛽 > 0 and 𝛼 ≤ 1.
3.3 Equivalent Lateral Control
Equivalent control is interpreted (Slotine, 1991) as a
continuous control law that would maintain 𝑆 = 0 if the
dynamics were exactly known. In our case
𝑆 = 𝜓 𝐸 +
αβ
1 + β2y2y (13)
Fig. 5: Nonlinear Sliding Surface 𝑆 = 𝜓𝐸 + 𝛼 tan−1(𝛽𝑦)
𝑆 = 0 implies
0 =𝑔 tan(𝜙𝑅_𝑒𝑞𝑣 )
𝑉+
𝛼𝛽
1 + β2y2𝑉 sin 𝜓𝐸 (14)
From (14), equivalent control can be derived as
𝜙𝑅_𝑒𝑞𝑣 = tan−1 −𝑉2
𝑔
𝛼𝛽
1 + 𝛽2𝑦2sin 𝜓𝐸 (15)
-2000 -1500 -1000 -500 0 500 1000 1500 2000-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
Cross track error (y) in meters
E i
n r
ad
ian
s
-2000 -1500 -1000 -500 0 500 1000 1500 2000-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
Cross track error (y) in meters
E i
n r
ad
ian
s
Preprints of the 18th IFAC World CongressMilano (Italy) August 28 - September 2, 2011
11123
3.4 Existence of Sliding Mode
A control law should be chosen in such a way that from any
initial condition, the system trajectory is attracted towards the
sliding surface and then slides along the sliding surface
(Bandyopadhyay, 2009). To see the reachability condition,
Lyapunov candidate function 𝐕 =1
2S2 is selected. And the
derivative of Lyapunov function 𝐕 is
𝐕 = 𝑆𝑆
= 𝑆 𝑔
𝑉tan 𝜙𝑅 +
𝛼𝛽
1 + β2y2𝑉 sin 𝜓𝐸 (16)
Let us assume
tan 𝜙𝑅 = −𝐾 𝑠𝑖𝑔𝑛 𝑆 (17)
and replace it in (16), derivative of Lyapunov function 𝐕
becomes
𝐕 = 𝑆 −𝑔
𝑉𝐾 𝑠𝑖𝑔𝑛(𝑆) +
𝛼𝛽
1 + β2y2𝑉 sin 𝜓𝐸 (18)
𝐕 is negative definite if 𝑔
𝑉𝐾 >
𝛼𝛽
1+β2y2 𝑉 sin 𝜓𝐸
or
𝐾 >𝑉2
𝑔
𝛼𝛽
1 + β2y2 sin 𝜓𝐸
In extreme case, the maximum value of right side occurs in
the situation when sin 𝜓𝐸 = 1 and 𝑦 = 0. So (18) is
negative definite in whole flight envelope if
𝐾 >𝑉2
𝑔αβ (19)
3.5 Total Lateral Control
From equations (17) and (19), we have
𝜙𝑅 = tan−1 −𝐾 𝑠𝑖𝑔𝑛 𝑆 where 𝐾 >𝑉2
𝑔αβ
or
𝜙𝑅 = − tan−1 𝐾 𝑠𝑖𝑔𝑛 𝑆 (20)
Total lateral control is the sum of (15) and (20)
𝜙𝑅 = − tan−1 𝑉2
𝑔
𝛼𝛽
1 + 𝛽2𝑦2sin 𝜓𝐸
− tan−1 𝐾 𝑠𝑖𝑔𝑛 𝑆 (21)
where first part is continuous one and the second one is
discontinuous. From practical implementation point of view,
second discontinuous part can be approximated by a
continuous one.
4. CONTROL EFFORT BOUNDEDNESS
As discussed earlier that output of guidance block should be a
bounded number, in this section we have derived conditions
to keep 𝜙𝑅 ≤𝜋
6 during motion on sliding surface. Motion on
sliding surface is described by (10), that is
ψE + 𝛼 tan−1(𝛽𝑦) = 0 (22)
Differentiating (22), we get an expression (15) for equivalent
control that would maintain 𝑆 = 0 if the dynamics were
exactly known. So the equivalent control should always be
less 30 degrees ( 𝜙𝑅_𝑒𝑞𝑣 ≤π
6).
𝑉2
𝑔
𝛼𝛽
1 + 𝛽2𝑦2sin 𝜓𝐸 ≤ tan
π
6 (23)
In above inequality (23), replacing value of 𝜓𝐸 from (22)
𝑉2
𝑔
𝛼𝛽
1 + 𝛽2𝑦2sin(−𝛼 tan−1(𝛽𝑦)) ≤ tan
π
6
That can be written as
𝛼𝛽
1 + 𝛽2𝑦2sin(−𝛼 tan−1(𝛽𝑦)) ≤ tan
π
6
𝑔
𝑉2 (24)
In summary, the choice of 𝛼 and 𝛽 should be such that it
satisfies the inequality (24) in order to avoid the control
saturation during motion on sliding surface.
5. SIMULATION RESULTS
The proposed scheme is implemented in non-linear 6-dof
simulation of a UAV. Prior to implementation of this outer
guidance loop, a robust linear 𝐻∞ based linear control law
was implemented for inner control loop. To implement the
lateral control law (21), signum function is approximated
by 𝑆𝑖𝑔𝑛(𝑆) ≈𝑆
𝑆 +𝜖, where 𝜖 is a small scalar positive
number, in our case its value is 0.1. After a number of
simulation runs, 𝛼 and 𝛽 values are kept at 0.3333 and 0.003
respectively for better performance and robustness.
Fig. 6: Validation of inequality (21) for particular 𝛼 and 𝛽
0 500 1000 1500 20000
0.5
1
1.5x 10
-4
Lateral Track Error [m]
LHS
RHS
Preprints of the 18th IFAC World CongressMilano (Italy) August 28 - September 2, 2011
11124
Fig. 7: Performance for 2000m cross track error (No wind)
The above selected values of 𝛼 and 𝛽 also satisfy the
inequality (21) and maximum control effort during motion on
sliding surface is expected at cross track error of ~ 250
meters (Fig. 6). For the above selected 𝛼 and𝛽, the minimum
value of K in (21) should be greater than 4 (K=10 used in all
simulation results).
Straight Path Following
Simulation results for 2000m track error in the absence of
wind and in the presence of 30m/s side wind are shown in
Fig. 7 and Fig. 8 respectively. In the absence of wind, it takes
~26.72 seconds to reach the sliding surface and the
subsequent motion takes place on the sliding surface. On the
other hand in the case of side wind of 30m/s, it takes ~0.78
seconds more to reach the sliding surface. In both cases (with
& without wind), there is no overshoot in cross track error
and magnitude of steady state track error is less than 2.5
meters. Fig. 7 and Fig. 8 also validate that during motion on
sliding surface maximum control effort is at ~250 meters
cross track error.
Circular Path Following
In Fig. 9, the simulation results are plotted for a curved
(~circular) path in the presence of a north wind of 30m/s.
Even in this worst case scenario, the maximum magnitude of
cross track error is less than 45 meters.
6. CONCLUSIONS
A new scheme of lateral control for UAVs is proposed here
in this paper. This new scheme is based on a sliding mode
technique with a non-linear sliding surface. Due to limitations
of performance in the case of small track error and keep
𝜓𝐸 ≤ 𝜋
2 for whole flight envelope, a single linear sliding
surface is not a feasible solution. So a non-linear sliding
surface that can meet both these limitations is proposed here
in this paper and stability of that non-linear sliding surface is
proved with the help of a Lyapunov function. After the
selection of non-linear sliding surface, a sliding mode based
lateral control law is proposed and condition for reachability
to sliding surface is derived using a Lyapunov function.
Another limitation of guidance block output saturation
(reference roll angle saturation) is also addressed here in this
paper and conditions for saturation avoidance are derived
here.
Above proposed law is implemented in simulation (with
approximation of signum function), and simulation results are
shown here for straight & curved path. To see the robustness
of this proposed algorithm, simulations are performed in the
presence of disturbance (wind). Maximum steady state error
in the case of straight path following and circular path
following is 2.5 meters and 45 meters respectively even in the
presence of a lateral wind of 30m/s. Simulation results also
validate that there is no control effort saturation during
motion on sliding surface. In reaching phase (initial phase
when the system trajectory has not reached the sliding
surface), there is control saturation but reaching phase can be
eliminated using different techniques like a method discussed
in (Bandyopadhyay, 2009).
Problem of chattering in standard sliding mode technique is
settled by smoothing the control input using boundary layer
during implementation of this proposed algorithm. But in a
future work, this problem will be settled by using higher
order sliding mode (HOSM).
40 60 80 100 120 140 1600
1000
2000
3000
Time [sec]
Cro
ss T
rack E
rror
[m]
40 60 80 100 120 140 160-40
-20
0
20
Time [sec]
E [
deg]
-1000 -500 0 500 1000 1500 2000 2500-0.5
0
0.5
X: 1544
Y: -0.435
Z: 76.72
Cross Track Error [m]
E [
rad]
Sliding Surface
UAV Phase Portrait
40 60 80 100 120 140 160-40
-20
0
20
40
X: 76.72
Y: -8.212
Time [sec]
Roll
Refe
rence [
deg]
Preprints of the 18th IFAC World CongressMilano (Italy) August 28 - September 2, 2011
11125
Fig. 8: Performance for 2000m cross track error (30m/s wind)
REFERENCES
B. Bandyopadhyay, F. Deepak, and K.S. Kim (2009). Sliding
Mode Control Using Novel Sliding Surfaces. Springer-
Verlag, Berlin Heidelberg.
D. Nelson, B. Barber, T. McLein, R. Beard. (2006). Vector
field path following for small unmanned air vehicles.
Proceedings of the IEEE American control conference,
IEEE, Piscatawey, NJ.
George M. Siouris (2004). Missile Guidance and Control
Systems. Springer-verlag, USA.
Lei jia and Meng Xiuyun (2010). Application of Sliding
Mode Control Based on DMC in Guidance Control
System. 2nd
International Conference on Advanced
Computer Control, Shenyang, China
Marius Niculescu (2001). Lateral Track Control Law for
Aerosonde UAV. 39th AIAA Aerospace Sciences
Meeting and Exhibit. Reno, NV, USA.
N. Regina and M. Zanzi (2009). 2D Tracking and Over-
Flight of Target by Means of a Non-Linear Guidance
Law for UAV. IEEE Aerospace Conference, Big Sky,
MT.
R. Samar, S. Ahmed and F. Aftab (2007). Lateral Control
with Improved Performance for UAVs. 17th
IFAC World
Congress. Seoul, Korea.
Sanghyuk Park (2004). Avionics and Control System
Development for Mid-Air Rendezvous of Two Unmanned
Aerial Vehicles. Ph.d. Thesis, Chapter 3. Massachusetts
Institute of Technology. USA.
Sanghyuk Park, John Deyst, Jonathan P. How (2007),
Performance and Lyapunov stability of a nonlinear
pathfollowing guidance method, Journal of guidance,
control and dynamics, Vol. 30, No. 6, 1718–1728.
Slotine, J.-J. E. and Li, W., Applied Nonlinear Control,
chapter- 7, Prentice Hall, 1991.
Y.B. Shtessel, I.A. Shkolnikov and A. Levant (2009).
Guidance and Control of Missile Interceptor using
Second-Order Sliding Modes. IEEE Transaction on
Aerospace and Electronic Systems, Vol. 45, No. 1.
Fig. 9: Performance for curved path (30m/s North wind)
40 60 80 100 120 140 1600
500
1000
1500
2000
2500
Time [sec]
Cro
ss T
rack E
rror
[m]
40 60 80 100 120 140 160-40
-20
0
20
Time [sec]
E [
deg]
-1000 -500 0 500 1000 1500 2000 2500-0.5
0
0.5
X: 1494
Y: -0.4341
Z: 77.5
Cross Track Error [m]
E [
rad]
Sliding Surface
UAV Phase Portrait
40 60 80 100 120 140 160-40
-20
0
20
40
Time [sec]
Roll
Refe
rence [
deg]
X: 77.5
Y: -6.472
1300 1400 1500 1600 1700 1800-20
0
20
40
60
Time [sec]
Cro
ss T
rack E
rror
[m]
1300 1400 1500 1600 1700 1800-2
-1
0
1
2
Time [sec]
E [
deg]
1300 1400 1500 1600 1700 1800-30
-20
-10
0
10
Time [sec]
Roll
Refe
rence [
deg]
63.4 63.5 63.6 63.7 63.8
25.4
25.45
25.5
25.55
25.6
25.65
Track( Lat/Long )
long (deg)
lat
(deg)
0
1
2
3
4
8
9
Preprints of the 18th IFAC World CongressMilano (Italy) August 28 - September 2, 2011
11126