Chinese Journal of Aeronautics 22(2009) 250-256
Chinese 
Journal of 
Aeronautics 
www.elsevier.com/locate/cja
Design of Flight Control System for a Small   
Unmanned Tilt Rotor Aircraft 
Song Yanguo*, Wang Huanjin 
National Key Laboratory of Rotorcraft Aeromechanics, College of Aerospace Engineering,   
Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China 
Received 23 May 2008; accepted 25 March 2009 
Abstract 
A tilt rotor is an aircraft of a special kind, which possesses the characteristics of a helicopter and a fixed-wing airplane. How-
ever, there are a great number of important technical problems waiting for settlements. Of them, the flight control system might 
be a critical one. This article presents the progresses of the research work on the design of flight control system at Nanjing Uni-
versity of Aeronautics and Astronautics (NUAA). The flight control law of the tilt rotor aircraft is designed with the help of an 
inner/outer loop control structure and an eigenstructure assignment algorithm on the basis of a proper mathematical model al-
ready verified by the wind tunnel tests. The proposed control law has been born out through the construction of the flight control 
system and the flight tests. Now, the flight tests are still underway on a prototype of small unmanned tilt rotor aircraft. The results 
have evidenced the credibility of the aircraft design and the effectiveness of the flight control system for the tilt rotor working in 
the helicopter mode. A full envelope flight test is planned to carry out further researches on the flight control law. 
Keywords: tilt rotor aircraft; control; aircraft models; flight dynamics   
1.  Introduction1 
A  growing  number  of  countries  have  been  paying 
close attention to the development of tilt rotor aircraft, 
which  combines  the  vertical  lift  ability  of  helicopters 
and the speed and range of fixed-wing airplanes[1-6] and 
has found wide applications in both military and civil 
fields.   
The critical technological problem that is facing de-
signers and researchers of tilt rotor aircrafts is design 
of  flight  control  system.  To  find  out  the  solution,  a 
prototype of small unmanned tilt rotor aircraft has been 
designed and constructed, and a model for wind tunnel 
tests has been made to throw light on its aerodynamic 
performance.  And  the  wind  tunnel  test  results  have 
been  used  to  verify  and  improve  the  mathematical 
model.  Based  on  this  mathematical  model,  an  in-
ner/outer  loop  control  structure  and  an  eigenstructure 
assignment  algorithm  are  used  to design  the  tilt  rotor 
flight control law. The proposed control law is verified 
through  construction  of  a  flight  control  system  and 
                                                 
*Corresponding author. Tel.: +86-25-84895973. 
E-mail address: songyg@nuaa.edu.cn 
Foundation item: National Natural Science Foundation of China 
(60705034) 
 
1000-9361/$ - see front matter © 2009 Elsevier Ltd. All rights reserved. 
doi: 10.1016/S1000-9361(08)60095-3 
 
accomplishment of flight tests, which are being under-
way. 
The design of flight control law plays an significant 
role in future research on the development of this kind 
of  aircraft.  This  article  will  make  a  concise  introduc-
tion  to  the  progresses  of  the  work  on  it  at  Nanjing 
University of Aeronautics and Astronautics (NUAA).   
2. Mathematical Modeling of Flight Dynamics 
In  modeling  tilt  rotor  flight  dynamics,  as  a  tool  of 
utmost  importance,  the  aerodynamic  model  of  rotor 
must  include  the  aerodynamic  model  of  aerofoil,  the 
induced velocity model, and the blade flapping model. 
For the details of calculating the aerodynamic forces of 
a rotor, one can refer to Refs.[7-8]. In order to ensure 
the  real-time  calculation  of  a  flight  dynamics  model, 
an  aerodynamic  interference  coefficient  is  introduced 
to consider the disturbance between the rotor and the 
wing.  According  to  the  analysis  of  wind  tunnel  test 
results  (see  Fig.1)  and  calculated  model  results,  the 
interference coefficient is reasonably chosen to be 0.87 
for this model. 
Assume that the aerodynamic model of the wing is 
rigid without elastic deformation. In the free wake, the 
aerodynamic force models of wing, fuselage, horizon-
tal tail, vertical tail, and nacelle can be obtained from 
Ref.[9] while the method to calculate the aerodynamic 
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Song Yanguo et al. / Chinese Journal of Aeronautics 22(2009) 250-256 
· 251 · 
attested to high reliability of the flight dynamic model 
of the tilt rotor developed by the authors, which could 
be applied well to flying quality evaluation and design 
of  flight  control  system  after  further  verification  and 
modification. 
Fig.1    Wind tunnel test. 
 
force  model of  the wing  in  the rotor-disturbed  region 
from Ref.[10]. 
According  to  the  above-cited  modeling  method,  is 
built  in  the  simulated  environment  of  MATLAB/ 
SIMULINK a complete nonlinear flight dynamic  ma- 
thematical model of the unmanned tilt rotor aircraft, of 
which  the  primary  purposes  are:  ①  to  calculate  the 
flight  envelope  of  the  tilt  rotor  and  the  conversion 
characteristics,  etc.,  ②  to  acquire  the  linear  model  in 
the trim point to design the flight control system and 
analyze  the  control  stability,  and  ③  to  calculate  the 
control  response  of  the  nonlinear  model  and  evaluate 
the  flying  quality  through  the  flight  dynamic  simula-
tion. 
In order to validate the flight dynamic mathematical 
model  of  a  tilt  rotor  and  ascertain  its  aerodynamic 
characteristics  in  flights  in  helicopter,  airplane,  and 
conversion modes (three modes of full envelope flight), 
as  well  as  aerodynamical  interference  between  com-
ponents,  have  been  planned  and  fulfilled  wind  tunnel 
tests (see Fig.1). Fig.2 shows the change of lift of an 
experimental  aircraft  with  the  pitch  angle  in  an  un-
powered  experiment  when  the  nacelle  angle  is  90°   
and the wind speed 30 m/s. Fig.3 illustrates the change 
of  the  thrust of  an  experimental  aircraft  with  the  col-
lective pitch in helicopter mode in a powered experi-
ment when the nacelle angle is 90° and the wind speed 
is 0 m/s. Fig.4 shows the change of lift of an experi-
mental aircraft according to pitch angle at the typical 
conversion  point  in  a  powered  experiment  when  the 
nacelle angle is 60° , the wind speed 14 m/s, and the 
collective pitch 14° . Fig.5 displays the change of the 
thrust  of  an  experimental  aircraft  with  the  collective 
pitch in a powered experiment when the nacelle angle 
is 0° and the wind speed 0 m/s. The minor differences 
between the test results and the theoretical results have 
Fig.3    Change of  thrust  with collective  pitch  (powered ex-
periment, nacelle angle is 90° , and wind speed 0 m/s). 
 
Fig.4    Change of lift with pitch angle at a typical conversion 
point (powered experiment, nacelle angle is 60° , wind 
speed 14 m/s, and collective pitch 14° ). 
 
Fig.5    Change of  thrust  with collective  pitch  (powered ex-
periment, nacelle angle is 0°, and wind speed 0 m/s). 
 
3. Flight Control System Design   
3.1. Conversion corridor 
Fig.2    Change  of  lift  with  pitch  angle  (unpowered  experi-
ment, nacelle angle is 90° , and wind speed 30 m/s). 
 
Conversion corridor is the sticking point in design-
ing a control system. There are many choices available 
for the conversion corridor as lots of control interfaces 
exist. The problem is how to choose a proper path that 
 
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Song Yanguo et al. / Chinese Journal of Aeronautics 22(2009) 250-256 
No.3 
ensures the safety and control simplicity in conversion. 
The  principle  of  choosing  conversion  corridor  in  this 
example is described as follows: the pitch angle of an 
aircraft  should  make  slow  changes  at  low  speeds. 
When the aircraft’s forward speed gradually increases, 
as all of the control interfaces start working, the pitch 
angle  could  be  kept  fixed  in  the  vicinity  of  a  given 
value.  This  is done for  two purposes:  one is  to  make 
the conversion flight of the aircraft as stable as possi-
ble and the other is to provide guidance for designing 
the  flight  control  system.  The  conversion  characteris-
tics  should  be  optimized  by  the  experience  from 
flight-tests. Figs.6-7 indicate the theoretical trim results. 
Fig.6    Nacelle angles against forward speeds. 
Fig.7    Trim control of conversion. 
 
 
According to the calculated results of the flight dy-
namics  model,  it  is  known  that  the  experimental  air-
craft is dynamically unstable in flight, which illustrates 
obvious changes of the dynamic characteristics in the 
conversion  mode.  As  a  very  critical  controlled-state 
variable  in  the  full  envelope  flight,  the  attitude  angle 
should  be  controlled  and  preserved  to  enable  the  un-
manned  tilt  rotor  aircraft  to  successfully  accomplish 
the full envelope flight. The established and well-tried 
flight dynamic model makes it possible to adopt mod-
ern control theory to conduct the system analysis and 
synthesis. As a design method in the time domain, ei-
genstructure assignment with state feedback can assign 
the  eigen-values  and  eigen-vectors  to  change  the  re-
sponse  of  the  system.  A  description  of  eigenstructure 
assignment is offered in Ref.[11].   
The attitude control system of tilt rotors is made up 
of  the  inner/outer  loop  of  the  feedback  control.  The 
method  is  not  only  good  for  system  decoupling  and 
multi-mode control law design for this aircraft but also 
convenient  for  construction  of  the  flight  control  sys-
tem. 
Fig.8 shows the structure of the inner/outer loop of 
feedback  controller.  In  Fig.8,  rm  is  reference  input,  e 
control error, uf system input, yc,inner inner loop output, 
and  yc,outer  outer  loop  output.  The  objectives  and  the 
technology  of  designing  the  inner  loop  and  the  outer 
loop  are  not  the  same.  The  inner  loop  mainly  adopts 
state  feedback  combining  the  compensable  matrix 
while the outer loop employs output feedback based on 
proportional  and  integral  (PI) control.  The  inner  loop 
makes the system decouple and improves the frequency 
response characteristics and stability and the outer loop 
pays  attention  to  the  control  quality  of  the  controlled 
variables.  The  inner  loop  regards  the  angular  rate  as 
controlled variables and the outer loop aims at the atti-
tude control.   
Fig.8    Structure of inner/outer loop of a feedback controller.
have a relationship as follows. 
 
y
c,inner
y
c,outer
T
w p q r
  
=[
   ]
  
rφ θ
T
w
=[
  
   ]
  
(Output of inner loop)
(Output of outer loop)
 
⎧⎪
⎨
⎪⎩
where  w  is  vertical  velocity;  p,  q,  and  r  are  angular 
velocity components about fuselage x-, y-, and z-axes; 
andφand θ roll angle and pitch angle, respectively. 
The  inner  loop  design  includes  state  feedback  and 
compensable  matrix.  Here,  state  feedback  control  is 
3.2. Inner loop design 
The  design  of  inner  loop  control  views  rate  com-
mand  attitude  hold  (RCAH)  as  the  design  objective 
and the outer loop control is used for design of attitude 
command  attitude  hold  (ACAH).  There  is  a  simple 
integral  relationship  between  the  outer  loop  and  the 
inner loop. When using both loops to design an attitude 
control system, the outputs of the inner and outer loops 
 
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Song Yanguo et al. / Chinese Journal of Aeronautics 22(2009) 250-256 
· 253 · 
based  on  the  eigenstructure  assignment,  the  expected 
closed-loop  eigen-values  and  eigen-vectors  generated 
by  the  implicit  model,  which  is  abstracted  from  Ref. 
[12]. 
The  four  expected  rate  responses  of  the  implicit 
model can be expressed as follows: 
①  The model of vertical velocity response 
w s
( )
w s
( )
c
=
λ
w
λ
+
w
s
                        (1) 
②  The model of roll rate response 
p s
( )
p s
( )
c
=
λ
p
+
λ
p
s
                          (2) 
③  The model of pitch rate response 
             
q s
( )
q s
( )
c
=
λ
q
+
λ
q
s
                          (3) 
④  The model of yaw rate response 
       
=
r s
( )
r s
( )
c
λ
r
+
λ
r
s
                          (4) 
The  coupling  relationship  between  the  forward 
speed and the pitch rate, and that between the side slip 
speed  and  the  roll  rate  remain  unchanged  and  can  be 
expressed by 
u s
( )
q s
( )
c
v s
( )
p s
( )
c
=
=
                      (5) 
                      (6) 
s s
(
λ
q
+
λ
p
+
λ
)
u
λ
)
v
s s
(
Eq.(5) can be rewritten into   
u s
( )
q s
( )
=
u s
( )
q s
( )
c
i
q s
( )
c
q s
( )
=
⎛
⎜
⎝
+
1
λ
q
s
⎛
⎞
i
⎜
⎟
⎠ ⎝
1
λ
+
u
⎞
⎟
⎠
s
    (7) 
In Eqs.(1)-(7), λw, λp, λq, λr, λu, and λv are desired ei-
gen-values  of  transfer  functions;  u  and  v  are  forward 
and sideward velocity; and subscript “c” indicates con-
trol commands. 
By  transforming  the  above  functions  into  the  state 
space model (θ(s)=q(s)/s), can be obtained 
               
                  (8) 
The  differential  equation  of  lateral  velocity  can  be 
+ +
u qλ
u
λθ
q
= −
u
derived in the same way:   
v
= −
+ +
pλ
v
v
λφ
p
                      (9) 
Eqs.(1)-(9)  describe  the  expected  models,  which 
show  the basic  response  type  and  expected  flight  dy-
namical performances of tilt rotor aircraft according to 
control performance requirements. λw, λp, λq, λr, λu, and 
λv can be confirmed based on control quality require-
ments.   
The above expressions can be expressed in the gen-
eral form as follows 
 
c
+
x A x B x
d
x
x
=
d
=
u v w p q r
[
=
w p q r
]
[
c
c
c
c
c
φθ
T
]
⎫
⎪
⎬
⎪
⎭
             (10) 
−
=
−
−
−
A
d
0
λ
v
0
0
0
0
0
0
0
0
0
0
0
λ
r
0
0
0
1
0
λ
p
0
0
1
0
0
λ
p
0
0
0
0
0
0
λ
p
0
0
0
0
0
0
0
1
0
0
0
λ
q
−
0
0
1
where x is state vector of implicit model, xc input vec-
tor  of  implicit  model,  subscript  “d”  indicates  desired 
matrices, and 
−⎡
λ
0
u
⎢
0
0
⎢
⎢
λ
0
w
⎢
0
0
⎢
⎢
0
0
⎢
⎢
0
0
⎢
⎢
0
0
⎢
0
0
⎣
0 0 0 0
⎤
⎡
⎥
⎢
0 0 0 0
⎥
⎢
λ
0 0 0
⎥
⎢
w
⎢
⎥
λ
0
0 0
⎥
⎢
p
= ⎢
⎥
λ
0 0
0
⎢
⎥
q
λ
⎢
⎥
0 0 0
r
⎥
⎢
0 0 0 0
⎢
⎥
⎢
⎥
0 0 0 0
⎦
⎣
⎫
⎤
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎥
⎪
⎦⎬
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎪
⎭
    (11) 
In  the  model,  parameters  λw,  λp,  λq,  and  λr  can  be 
chosen according to the flying quality while parameter 
λu and λv only must be greater than zero to ensure the 
system stability. The expected closed-loop eigen-values 
and  eigen-vectors  can  be  obtained  from  the  implicit 
model. 
According  to  the  expected  eigen-values  and  ei-
gen-vectors,  the  eigenstructure  of  the  original  system 
can be assigned by using eigenstructure assignment to 
acquire the state feedback gain K.   
B
d
3.3. Outer loop design 
After the inner loop design, the system becomes sta-
ble with an inner loop made of four independent loops 
characteristic of [w p q r]T. This paves a way for de-
signing  the  outer  loop  design.  Every  channel  of  the 
outer loop can be designed separately. The structure of 
the outer loop of the longitudinal pitch angular velocity 
is shown by Fig.9, in which Kθ is the proportional gain 
of the pitch controller. 
Fig.9    Structure of outer loop of pitch angle. 
The transfer function of the pitch angle is 
 
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Song Yanguo et al. / Chinese Journal of Aeronautics 22(2009) 250-256 
No.3 
θ
s
( )
θ
s
( )
c
=
λ
K
θ
q
λ
λ
+
s K
θ
q
q
+
2
s
             
(12) 
The  transfer  function  of  the  roll  angle  can  be  ex-
pressed likewise. And the transfer function of the yaw 
angle is 
φ
s
( )
φ
s
( )
c
=
+
2
s
λ
K
φ
p
λ
λ
+
s K
φ
p
p
             
(13) 
where Kφis the proportional gain of the roll controller. 
In  the  above  transfer  functions,  the  parameters  λp 
and  λq  have  already  been  attained  in  the  inner  loop 
design and the parameters Kθ and Kφshould be deter-
mined by flight performance in the outer loop design. 
Figs.10-11  show  the  simulation  results  in  the  conver-
sion mode, when the nacelle angle is 55°. 
Fig.10    Pitch  angle  response  under  unit  step  pitch  angle 
input (nacelle angle is 55° ). 
 
 
Fig.11    Roll angle response under unit step roll angle input 
(nacelle angle is 55° ). 
3.4. Construction of flight control system   
The control system of the experimental tilt rotor in-
cludes a ground station and an airborne flight control 
system (see Fig.12).   
The airborne flight system consists of a flight con-
trol computer, a servo control computer, a sensor sys-
tem,  GPS,  a  digital  transmitter/receiver,  and  servos. 
The  primary  functions  are:  ①  receiving  control  in-
structions from the ground station; ② guaranteeing the 
stability  of  the  longitudinal,  lateral,  directional,  and 
altitudinal  channels  and  accomplishing  closed-loop 
control  of  the  longitudinal,  lateral,  directional,  and 
altitudinal  channels  in  helicopter  mode,  conversion 
mode, and airplane mode;  ③ monitoring the airborne 
Note: VDC—Voltage direct current; TTL—Transistor-transistor logic; RF—Radio frequency; DO—Digital out 
Fig.12    Structure of control system. 
 
 
 
 
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Song Yanguo et al. / Chinese Journal of Aeronautics 22(2009) 250-256 
· 255 · 
system performance; ④ transmitting flight data to the 
ground station so as to replay, edit, and analyze them 
after the experiments; ⑤ controlling rotation speed of 
the  engine;  and  ⑥  estimating  the  flight  state  of  the 
unmanned tilt rotor aircraft. 
The  ground  station  includes  a  joy  stick,  a  ground 
station computer, and a digital transmitter/receiver. The 
joy  stick  serves  the  interface  transmitting  the  opera-
tor’s instructions; the ground station computer mainly 
monitors flight states; and the digital transmitter sends 
and the receiver receives commands and flight data. 
4.  Program  of  Experimental  Research 
In order to validate the proposed technology, a pro-
totype of a small unmanned tilt rotor was chosen to be 
manufactured  for  reducing  the  research  risk,  shorten-
ing  the  research  period,  and  saving  the  research  cost. 
The flight speed of the experimental aircraft in airplane 
mode  was  minimized  enough  to  satisfy  the  require-
ments  for  visual  manipulation  in  initial  flight  tests. 
Technically  ripe  engine,  actuator,  and  others  were 
adopted  to  ensure  the  planned  research  progress  rate 
and  reliability.  Full  use  of  existing  testing  conditions 
was  made  to  verify  every  technological  detail  of  the 
experimental aircraft with the purpose of realizing ver-
tical  taking-off  and  landing,  hovering  in  helicopter 
mode,  and  flying  in  conversion  mode  and  airplane 
mode. 
During the general design of the unmanned tilt rotor, 
a normal high-wing layout was adopted. The flaps and 
ailerons were integrated into the wing and two tilt na-
celles were fitted outboard of the wing. The horizontal 
and  vertical  tails,  elevator,  and  rudder  were  arranged 
on  the  tail.  A  tricycle  landing  gear  was  chosen.  Two 
engines were used to drive two sets of rotors through a 
synchronous  shaft  to  coordinate  the  rotational  speeds 
of both rotors. A digital position control system with a 
worm  gear  and  worm  mechanism  provided  the  re-
quired  moments  for  tilting  the  nacelles.  Fig.13  illus-
trates the aerodynamic configuration of the aircraft. 
The  ongoing  research  program  of  the  experimental 
aircraft  includes  the structure  tests  of  the aircraft,  the 
tests of the rotor and the engine on the ground, simula-
tion of flight control system on the ground, and flight 
(a) Three views 
 
 
(b) Photo 
 
Fig.13    Three views and a photo of experimental aircraft. 
tests  (see  Fig.14).  From  the  successful  flight  tests,  it 
can be concluded that the control trim point shown in 
Fig.7 is reasonable. 
(a) Helicopter and take off 
(b) Conversion 
Fig.14    Flight test photos. 
5. Conclusions 
 
 
This  article  presents  a  flight  control  system  of  a 
small  unmanned  tilt  rotor  aircraft  based  on  an  im-
proved mathematical model that has been validated in 
flight tests. The following conclusions can be drawn: 
(1) The small unmanned tilt rotor aircraft developed 
by authors is fit for attesting to the critical technology 
which  includes  flight  dynamic  modeling  and  flight 
control system design. 
(2)  The  results  of  the  wind  tunnel  test  have  evi-
denced  the  viability  of  the  tilt  rotor  flight  dynamic 
model. Based on this mathematical model, the conver-
sion corridor of the tilt rotor is derived. The flight con-
trol  system  is  analyzed  and  synthesized  by  using  an 
eigenstructure  assignment  control  algorithm  and  the 
inner/outer loop control structure. 
(3)  Flight  tests  of  the  tilt  rotor  aircraft  have  been 
successfully carried out. The results have born out the 
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Song Yanguo et al. / Chinese Journal of Aeronautics 22(2009) 250-256 
No.3 
credibility  of  the aircraft design  and  the  effectiveness 
of the flight control system in controlling the tilt rotor 
in helicopter mode. 
(4) A full envelope flight test is planned to research 
the flight control law. 
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Biography: 
Song Yanguo    Born in 1973, he graduated and earned Ph. D. 
degree  in  flight  dynamics  and  flight  control  from  Nanjing 
University  of  Aeronautics  and  Astronautics  (NUAA)  in 
2003.  He is currently an associate professor at NUAA, with 
academic interest in UAV flight control and UAV design. 
E-mail: songyg@nuaa.edu.cn
 
小型无人倾转旋翼机飞行控制系统设计 
宋彦国 王焕瑾 
(南京航空航天大学航空宇航学院,直升机旋翼动力学国家级重点实验室) 
摘 要:倾转旋翼飞行器是一种独特的新构型飞行器,兼具固定翼飞机和直升机双重飞行模式和优点。但是,这种
飞行器仍有许多关键技术需要解决,飞行控制系统是其中之一。本文介绍了南航所做的小型无人倾转旋翼机飞行控
制系统技术研究的主要内容。研究工作建立在良好的飞行力学数学模型基础上,这一模型经风洞吹风试验进行了验
证。控制律设计采用内外环控制结构和节点配置方法。这一控制律设计通过飞行控制系统的实现和飞行试验进行了
验证。目前,飞行试验仍在进行,已有数据验证了模型的可靠性和直升机模式飞行控制律设计的有效性。下面将继
续进行全飞行包线的飞行试验来进一步研究飞行控制律。 
关键词:垂直/短距起降飞行器;  控制;  飞行器模型;  飞行动力学 
 
Erratum to “Uniform Coverage of Fibres over Open-contoured Free-
form Structure Based on Arc-length Parameter” 
  [Chinese Journal of Aeronautics 21(2008)571-577] 
 
Wang Xiaoping*, An Luling, Zhang Liyan, Zhou Laishui 
Jiangsu Key Laboratory of Precision and Macro-manufacturing Technology, Nanjing University of Aeronautics and Astronautics,   
Nanjing 210016, China 
It is regretted that the author corrections requested at the proof stage were not made accurately. There are some 
incorrect typings in two equations which will lead to inaccurate results if readers perform calculations directly with 
them.   
Actually , the vector “N(s)” in equations (8) and (12) should be changed into “Su×Sv”. 
Readers who still have questions could contact the corresponding author:   
Tel: +86-25-84891678 
E-mail address: levine@nuaa.edu.cn