Adaptive Optimal Path Following for High Wind Flights

Size: px
Start display at page:

Download "Adaptive Optimal Path Following for High Wind Flights"

Transcription

1 Milano (Italy) August - September, 11 Aaptive Optimal Path Following for High Win Flights Ashwini Ratnoo P.B. Sujit Mangal Kothari Postoctoral Fellow, Department of Aerospace Engineering, Technion-Israel Institute of Technology, Haifa, 3, Israel. ( ashwini@aeroyne.technion.ac.il) Research Scientist, Department of Electrical an Computer Engineering, University of Porto, Portugal ( sujit@fe.up.pt) Grauate stuent, Department of Engineering, University of Leicester, Unite Kingom-LE1 7RH. ( mk1@le.ac.uk) Abstract: Unmanne aerial vehicle path following is aresse as an infinite horizon regulator problem. Using the linear quaratic regulator technique an optimal guiance law is erive. The state weighting matrix is chosen as a function of the position error an this aaptive nature of the cost function controls the UAV errors tightly. Numerical simulations are carrie out for straight line an circular paths uner various win conitions. Results show consierably lower position errors as compare to an existing guiance law. Path following with wins up to half the vehicle airspee is achieve. Keywors: Guiance systems, Optimal control, Path planning 1. INTRODUCTION Unmanne aerial vehicles (UAVs) have been successfully eploye in various applications that inclue search an rescue, surveillance, patrol an monitoring missions. They have the capability to provie information remotely an act like an extene sensor. With avances in flight control an miniaturization of UAVs, they are foun to play a key role in urban environments. Of particular interest is path following in high wins. Urban environments have unstructure win patterns an with high magnitues causing very high errors in UAV path following. Most of the mission paths can be efine using a set of waypoint an loiters maneuvers, where way-points are straight line segments while loiters are circular orbits. The path following controller has to accurately track the esire path in presence of win isturbances. The path following control law must have low computational complexity to be use in real-time. There is wie boy of literature on eveloping guiance laws for UAVs to follow straight line, curve trajectories an loiter maneuvers in the presence of wins. A piecewiseaffine control law with Lyapunov base controller for the UAV to follow a path is presente by Shehab an Rorigues [5]. The authors i not consier win isturbances in their work. Kaminer et al. [] evelope an optimal control law for multiple UAV trajectory following with coorination. The trajectory is parameterize as a function of time to follow which becomes an issue when UAV is initially locate away from the path. A L 1 aaptive controller for UAV path following taking win isturbances into account is evelope by Cao et al. [7]. Nelson et al. [] evelope a simple an effective path following controller using vector fiels. Vector fiels are evelope for both straight line an circular paths in the presence of wins. Rysyk [] evelope guiance laws for following straight line an circular paths base on helmsman behavior. The guiance law changes the course of the vehicle base on the win magnitue an irection which is estimate online. Lawrence et al. [] evelope a generalize vector fiel metho with lyapunov stability for ifferent maneuvers. Ceccarelli et al. [7] esigne a guiance law for a MAV taking win into consieration for continuous monitoring a target in the camera fiel of view. Breivik an Fossen [7] presente guiance laws for path following in D an 3D using control lyapunov functions. The approach oes not take win into account. Park et al. [7] presente a non-linear guiance law () that generates a reference target point on the path an uses this reference point as a target to maneuver the aircraft along the path. The authors present theoretical results an show results through experiments uner win isturbances. A typical path following comman as a constant gain linear function of position an velocity errors is incapable of placing a har boun on the position error. As the main contribution of the present work, we present an optimal UAV path following guiance law as an infinite horizon linear quaratic regulator (LQR) solution with an aaptive running cost where the state weighting gains are functions of the position error itself. The state weighting matrix is chosen as a function of the current an the maximum allowable position error an this aaptive nature of the cost function controls the UAV errors tightly in presence of wins. The guiance law oes not require path curvature information an is base on position an heaing errors of the UAV. Copyright by the International Feeration of Automatic Control (IFAC) 195

2 Milano (Italy) August - September, 11 The organization of the rest of the paper is as follows: The UAV path following problem is efine in Section followe by the aaptive optimal guiance law erivation in Section 3. Guiance law implementation an UAV kinematics are escribe in Section. Section 5 presents the simulations stuies on the guiance laws with comparative results. Section contains concluing remarks.. PROBLEM FORMULATION 3.1 Infinite horizon LQR Consier the general infinite-horizon nonlinear regulator problem of the form: Minimize J = 1 [x T Qx + Ru (t)]t () t with respect to the state x an control u subject to the linear system ynamics ẋ = Ax + Bu (5) an erive the feeback control u = R 1 B T Px () where P is obtaine from the algebraic Riccati equation A T P + PA PBR 1 B T P + Q = (7) an Q an R > are esign parameters. 3. Trajectory Tracking Problem an LQR Solution Fig. 1. Formulation Geometry Consier a UAV flying with a constant spee v in a plane as shown Fig. 1. The UAV mission is to follow a esire path as shown with the ashe line in Fig. 1. The UAV has a position error of with respect to the esire path an also a velocity error calculate as = v sin(ψ ψ p ) (1) wherev, ψ an ψ p are the UAV spee, heaing angle, an esire path angle, respectively. The path following problem is to formulate a control law u for the UAV to keep the errors, an small in presence of changing esire path geometries an wins. We consier the path following problem with a boun on the allowable error as b () where b is the esire position error ban with respect to the path. Also, u is the lateral acceleration which can be relate to the UAV heaing angle rate ψ, as u = v ψ (3) 3. ADAPTIVE OPTIMAL GUIDANCE LAW The problem of UAV path following is inherently an infinite horizon regulator problem where the guiance objective is to annul the UAV position an velocity errors with respect to a esire path. Contrary to finite time missile guiance applications, the UAV regulator solutions shoul keep the errors close to zero for all times an not just at the termination of the flight. We use aaptive running cost on the error states in an infinite horizon regulator formulation for the UAV path following problem. Linearizing UAV ynamics with respect to the esire heaing as v = = v sin(ψ ψ p ) () v = v( ψ ψ p ) cos(ψ ψ p ) (9) In the absence of path curvature information, we assume ψ p =. Using (3) an substituting for ψ p in (9) with small angle (ψ ψ p ), we have v = v ψ = u (1) Representing () an (1) in the stanar form we have x = [ v ], A = ẋ = Ax + Bu (11) 1, B = 1 (1) Consier the general infinite-horizon linear quaratic regulator problem where we minimize J = 1 [x T Qx + Ru (t)]t (13) t with respect to x an u subject to (11). Here, Q an R are the state weighting matrix an the control weighting matrix, respectively. Also, Q an R are the two esign parameters available to us for obtaining the esire control. We assume R = 1 (1) an Q to be an aaptive matrix with q Q = 1 q (15) We check the conitions for the LQR control solution to be locally asymptotically stable as, 19

3 Milano (Italy) August - September, 11 (1) {A, B} shoul be controllable in the omain of interest. Using (1) we have, {B,A B} = 1 (1) () f(x) = Ax C 1. From (1), we euce Ax = C 1 (17) Y W1 u R θ UAV ψ v ψp W esire straight line path (3) f() =. Using (17), we have f() = (1) O X (a) Straight-line () B. From (1) we have B as a constant non-zero matrix. (5) Q an R >. From (15) an (1) these conitions are met. Solving algebraic Riccati equation Optimal solution for the optimal control problem (13) is given as, u UAV ψ v ψp where P > is efine as, p11 p P = 1 p 1 p u = R 1 B T Px (19) is obtaine by solving the algebraic Riccati equation, () R' Rc esire circular path A T P + PA PBR 1 B T P + Q = (1) Solving for P using (1), (1), (15) an () in (1), we have p11 p 1 p11 p p11 p 1 1 p 1 p p 1 p p 1 p 1 p11 p [ 1 ] 1 q + 1 p 1 p q = () Simplifying an equating iniviual elements, we have, p 1 = q 1 (3) p = q 1 + q () p 11 = q 1 q 1 + q (5) Aaptive feeback control Using (1), (), (3), () an (5) in (19), we have the optimal control solution as, u p11 p = [ 1 ] 1 p 1 p v [ ] = q 1 + +q 1 + q v () We propose an aaptive gain q1 for a running penalty on as, q1 = b b (7) where b is the maximum allowable position error as consiere in (). The aaptive state weight q 1 increases Fig.. Path geometries (b) Circular the penalty as the UAV position error increases an gets closer to the maximum allowable limit. Very close to the maximum allowable limit the UAV uses maximum control to keep itself in the esire error ban. Note that, the weight remains close to unity for UAV flights with negligible error. This way the error is controlle tightly in case there are suen changes in the esire path or win isturbances. Since there are no practical concerns on the gain q associate with v, we chose q = 1 () Using (7) an () in (), we have the aaptive optimal guiance law () as u b = b + b b + 1 v (9). GUIDANCE LAW IMPLEMENTATION UAV trajectory planning involves two stanar geometries, namely, the straight line/way-point guiance an circular/loiter guiance. The guiance law of (9) can be implemente on the two stanar geometries an the relate kinematics are escribe next. 197

4 Milano (Italy) August - September, 11.1 Straight-line following Consier a straight line path forme by the way-points W1-W as shown in Fig. (a). Let R be the isplacement of UAV with respect to point W1 making an angle θ with the reference. The UAV position an velocity errors can be calculate as, Y position (m) Path an = R sin(θ ψ p ) (3) 1 5 Win Direction respectively. = v sin(ψ ψ p ), (31) X position (m) (a) Trajectories. Circular path following Consier a circular path of raius R c as shown in Fig. (b). Let R be the isplacement of the UAV with respect to the center of the circular path. The UAV position an velocity errors can be calculate as, an = R R c (3) 1.3 Effect of win = v sin(ψ ψ p ), (33) Motion of a UAV with respect to groun or stationary esire paths is affecte by win isturbances. In presence of win the groun velocity components, say v gx an v gy, of the UAV are given as v gx = v cos ψ + x (3) v gy = v sin ψ + y (35) where x an y are the components of the win spee along X an Y irection. Note that though is inepenent of win, v in presence win can be expresse as v = v sin(ψ ψ p ) + sin(ψ w ψ p ) (3) where ψ w is the irection of win with reference. Note that kinematics escribe in this section is use to simulate trajectories in the next section. However, in real life scenarios a GPS/INS aie UAV can compute onboar its groun position an groun velocity an then an v can irectly be compute with respect to any path. 5. SIMULATION RESULTS Using the guiance law erive in (9) we simulate various path following scenarios. Simulations are carrie out for straight line an circular paths consiering the two as the basic geometries for a general path planning problem. For comparative stuies we use well known non-linear guiance law ()Park et al. [7] an present the results here. The UAV spee, v, is consiere 5 m/sec with a minimum turn raius r min = 3v = 75 m. Lateral acceleration: u (m/sec ) (b) Position error (c) Lateral accelerations Fig. 3. Straight line following in % win 5.1 Straight line following Consier a straight line path passing through the origin of the X-Y plane with a unity slope as shown by a ashe line in Fig. 3(a) with a ashe black line. We consier win with =.v blowing perpenicular to the esire path with ψ w = 135. The parameters use for are: b = an for - L1 = 15. Trajectories for an are plotte in Fig.3 (a) with blue an re colors, respectively. The trajectory is affecte highly by the cross win. The corresponing position errors are shown Fig. 3(b) where has a maximum UAV position error of m an the transient of the position error settles quickly to the steay state. Whilst has a maximum position error is as high as 9.5 m an the guiance law has much higher settling time. Lateral acceleration profiles for 19

5 Milano (Italy) August - September, 11 1 =.3v =.v =.5v 3 Path Y (m) (a) Position error for X (m) (a) Trajectories 5 =.3v =.v =.5v (b) Position error for Fig.. Position error comparison in 3, an 5 % win following a straight line path the case are plotte in Fig. 3(c). For, as shown in blue color, the aaptive gains of (9) quickly increase as the win inuces the position error. This higher control input quickly reuces the position error an both the errors an the control input go to zero at a fast rate. The lateral acceleration is lower initially resulting in a higher position error cause ue to win. Further, we vary the win spee magnitue an compare the performance of the two guiance laws. The position error for is plotte in Fig. (a) with an approximate maximum of 3, an 9.5 m for a win spee of 3,, 5% of the UAV airspee. The performance, as shown in Fig. (b), eteriorates consierably in presence of high wins an corresponing maximum position errors are 1.5, 19 an 5 m, respectively. 5. Circular path following Next, we consier a circular path of raius 5 m centere at the origin an a UAV initially following the circle with no errors. The win is consiere blowing at a spee 3% of the UAV air spee in a irection perpenicular to the UAV initial heaing. The trajectories are plotte in Fig. 5(a) where the blue an re color paths show an trajectories, respectively. The esire circular path is shown by a ashe curve. Again, the win is less affective against the law where a maximum position error, as plotte in Fig. 5 (b), of. m in observe. The corresponing maximum error for is aroun 1 m. Note that the position errors o not converge to zero as in the straight line following case Lateral acceleration:u (m/sec ) (b) Position error (c) Lateral accelerations Fig. 5. Circular path following in 3% win since the UAV woul require a centripetal acceleration to follow the circular path an nees position an velocity errors to generate it. The corresponing lateral acceleration profiles, as plotte in Fig. 5(c), shows a higher initial control response by the resulting in superior error control. Next, we stuy the effect of win magnitue on circular path following with win spees 5, 35 an 5 % UAV air spee. All other parameters are the same as previously. The position errors for are plotte in Fig. (a) with a maximum of 3.3,. an 1. m for =.5v,.35v, 5v, respectively. The corresponing maximum error values for, as shown in Fig. (b), are 1.9, 1.1 an 5. m, respectively. A consierable position error improvement is gaine using the propose guiance law. 199

6 Milano (Italy) August - September, 11 Error in istance (m) 1 1 =.5v =.35v =.5v (a) Position error for =.5v =.35v =.5v (b) Position error for ference, New York, NY, USA, 7, pp , oi:1.119/acc.7.3 D.R. Nelson, D.B. Barber, T.W. McLain an R.W. Bear Vector Fiel Path Following for Small Unmanne Air Vehicles Proceeings of the American Control Conference, Minneapolis, Minnesota, USA,, pp , oi:1.119/acc..157 R. Rysyk UAV Path Following for Constant Line-of-Sight AIAA Unmanne Unlimite Systems, Technologies an Operations Aerospace, Lan an Sea Conference, San Diego, CA, USA, 3, AIAA-3-. D.A. Lawrence, E.W. Frew an W.J. Pisano Lyapunov Vector Fiels for Autonomous UAV Flight Control AIAA Guiance, Navigation an Control Conference an Exhibit, Hilton Hea, South Carolina, USA, 7, AIAA N. Ceccarelli, J.J. Enright, E.Frazzoli, S.J. Rasmussen an C.J. Schumacher Micro UAV Path Planning for Reconnaissance in Win Proceeings of the American Control Conference, New York City, NY, USA, 7, pp , oi:1.119/acc M. Breivik an T.I. Fossen Principles of Guiance-Base Path Following in D an 3D Proceeings of the IEEE Conference on Decision an Control, Seville, Spain, 5, pp. 7-3, oi:1.119/cdc S. Park, J. Deystt an J.P. How Performance an Lyapunov Stability of a Nonlinear Path-Following Guiance Metho Journal of Guiance, Control, an Dynamics, vol. 3, no., pp , oi:1.51/ Fig.. Position error comparison in 5, 35 an 5 % win following a circular path. CONCLUSIONS An aaptive optimal UAV guiance law is presente for high win flights. Infinite horizon LQR formulation is use to solve the guiance problem after linearizing the error ynamics. An aaptive state weighting matrix is use for tighter control of UAV errors in high isturbances. The guiance law results is consierably low errors as compare to an existing law in the literature. Simulations are carrie out for win spees up to half the UAV airspee for straight line an circular path following. REFERENCES S. Shehab an L. Rorigues Preliminary Results on UAV Path Following Using Piecewise-Affine Control Proceeings of the IEEE Conference on Control Applications, Toronto, Canaa, 5, pp oi:1.119/cca I. Kaminer, O. Yakimenko, A. Pascoal an R. Ghabcheloo Path Generation, Path Following an Coorinate Control for Time Critical Missions of Multiple UAVs Proceeings of the American Control Conference, Minneapolis, Minnesota, USA,, pp , oi:1.119/acc C. Cao an N. Hovakimyan, I. Kaminer, V.V. Patel an V. Dobrokhoov Stabilization of Cascae Systems via L1 Aaptive Controller with Application to a UAV Path Following Problem an Flight Test Results Proceeings of the American Control Con- 199

An Evaluation of UAV Path Following Algorithms

An Evaluation of UAV Path Following Algorithms 213 European Control Conference (ECC) July 17-19, 213, Zürich, Switzerland. An Evaluation of UAV Following Algorithms P.B. Sujit, Srikanth Saripalli, J.B. Sousa Abstract following is the simplest desired

More information

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain Nonlinear Aaptive Ship Course Tracking Control Base on Backstepping an Nussbaum Gain Jialu Du, Chen Guo Abstract A nonlinear aaptive controller combining aaptive Backstepping algorithm with Nussbaum gain

More information

Nested Saturation with Guaranteed Real Poles 1

Nested Saturation with Guaranteed Real Poles 1 Neste Saturation with Guarantee Real Poles Eric N Johnson 2 an Suresh K Kannan 3 School of Aerospace Engineering Georgia Institute of Technology, Atlanta, GA 3332 Abstract The global stabilization of asymptotically

More information

Practical implementation of Differential Flatness concept for quadrotor trajectory control

Practical implementation of Differential Flatness concept for quadrotor trajectory control Practical implementation of Differential Flatness concept for quarotor trajectory control Abhishek Manjunath 1 an Parwiner Singh Mehrok 2 Abstract This report ocuments how the concept of Differential Flatness

More information

Attitude Control System Design of UAV Guo Li1, a, Xiaoliang Lv2, b, Yongqing Zeng3, c

Attitude Control System Design of UAV Guo Li1, a, Xiaoliang Lv2, b, Yongqing Zeng3, c 4th National Conference on Electrical, Electronics an Computer Engineering (NCEECE 205) Attitue Control ystem Design of UAV Guo Li, a, Xiaoliang Lv2, b, Yongqing eng3, c Automation chool, University of

More information

VIRTUAL STRUCTURE BASED SPACECRAFT FORMATION CONTROL WITH FORMATION FEEDBACK

VIRTUAL STRUCTURE BASED SPACECRAFT FORMATION CONTROL WITH FORMATION FEEDBACK AIAA Guiance, Navigation, an Control Conference an Exhibit 5-8 August, Monterey, California AIAA -9 VIRTUAL STRUCTURE BASED SPACECRAT ORMATION CONTROL WITH ORMATION EEDBACK Wei Ren Ranal W. Bear Department

More information

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers

Optimal Variable-Structure Control Tracking of Spacecraft Maneuvers Optimal Variable-Structure Control racking of Spacecraft Maneuvers John L. Crassiis 1 Srinivas R. Vaali F. Lanis Markley 3 Introuction In recent years, much effort has been evote to the close-loop esign

More information

Guidance Control of a Small Unmanned Aerial Vehicle with a Delta Wing

Guidance Control of a Small Unmanned Aerial Vehicle with a Delta Wing Proceeings of Australasian Conference on Robotics an Automation, -4 Dec 13, University of New South Wales, Syney Australia Guiance Control of a Small Unmanne Aerial Vehicle with a Delta Wing Shuichi TAJIMA,

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

FORMATION INPUT-TO-STATE STABILITY. Herbert G. Tanner and George J. Pappas

FORMATION INPUT-TO-STATE STABILITY. Herbert G. Tanner and George J. Pappas Copyright 2002 IFAC 5th Triennial Worl Congress, Barcelona, Spain FORMATION INPUT-TO-STATE STABILITY Herbert G. Tanner an George J. Pappas Department of Electrical Engineering University of Pennsylvania

More information

Analytic Scaling Formulas for Crossed Laser Acceleration in Vacuum

Analytic Scaling Formulas for Crossed Laser Acceleration in Vacuum October 6, 4 ARDB Note Analytic Scaling Formulas for Crosse Laser Acceleration in Vacuum Robert J. Noble Stanfor Linear Accelerator Center, Stanfor University 575 San Hill Roa, Menlo Park, California 945

More information

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity

Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Preprints of the 9th Worl Congress The International Feeration of Automatic Control Cape Town, South Africa. August -9, Exponential Tracking Control of Nonlinear Systems with Actuator Nonlinearity Zhengqiang

More information

Composite Hermite Curves for Time-Based Aircraft Spacing at Meter Fix

Composite Hermite Curves for Time-Based Aircraft Spacing at Meter Fix AIAA Guiance, Navigation an Control Conference an Exhibit 0-3 August 007, Hilton Hea, South Carolina AIAA 007-6869 Composite Hermite Curves for Time-Base Aircraft Spacing at Meter Fix Thierry Miquel *

More information

Solution. ANSWERS - AP Physics Multiple Choice Practice Kinematics. Answer

Solution. ANSWERS - AP Physics Multiple Choice Practice Kinematics. Answer NSWRS - P Physics Multiple hoice Practice Kinematics Solution nswer 1. Total istance = 60 miles, total time = 1.5 hours; average spee = total istance/total time 2. rea boune by the curve is the isplacement

More information

Relative Position Sensing by Fusing Monocular Vision and Inertial Rate Sensors

Relative Position Sensing by Fusing Monocular Vision and Inertial Rate Sensors Proceeings of ICAR 2003 The 11th International Conference on Avance Robotics Coimbra, Portugal, June 30 - July 3, 2003 Relative Position Sensing by Fusing Monocular Vision an Inertial Rate Sensors Anreas

More information

Vectors in two dimensions

Vectors in two dimensions Vectors in two imensions Until now, we have been working in one imension only The main reason for this is to become familiar with the main physical ieas like Newton s secon law, without the aitional complication

More information

VISUAL SERVOING WITH ORIENTATION LIMITS OF A X4-FLYER

VISUAL SERVOING WITH ORIENTATION LIMITS OF A X4-FLYER VISUAL SERVOING WITH ORIENTATION LIMITS OF A X4-FLYER Najib Metni,Tarek Hamel,Isabelle Fantoni Laboratoire Central es Ponts et Chaussées, LCPC-Paris France, najib.metni@lcpc.fr Cemif-Sc FRE-CNRS 2494,

More information

TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS

TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS TRAJECTORY TRACKING FOR FULLY ACTUATED MECHANICAL SYSTEMS Francesco Bullo Richar M. Murray Control an Dynamical Systems California Institute of Technology Pasaena, CA 91125 Fax : + 1-818-796-8914 email

More information

A New Nonlinear H-infinity Feedback Control Approach to the Problem of Autonomous Robot Navigation

A New Nonlinear H-infinity Feedback Control Approach to the Problem of Autonomous Robot Navigation Intell In Syst (15) 1:179 186 DOI 1.17/s493-15-1- ORIGINAL PAPER A New Nonlinear H-infinity Feeback Control Approach to the Problem of Autonomous Robot Navigation G. Rigatos 1 P. Siano Receive: 8 December

More information

Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory

Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory Design A Robust Power System Stabilizer on SMIB Using Lyapunov Theory Yin Li, Stuent Member, IEEE, Lingling Fan, Senior Member, IEEE Abstract This paper proposes a robust power system stabilizer (PSS)

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

A New Backstepping Sliding Mode Guidance Law Considering Control Loop Dynamics

A New Backstepping Sliding Mode Guidance Law Considering Control Loop Dynamics pp. 9-6 A New Backstepping liing Moe Guiance Law Consiering Control Loop Dynamics V. Behnamgol *, A. Vali an A. Mohammai 3, an 3. Department of Control Engineering, Malek Ashtar University of Technology

More information

Math 342 Partial Differential Equations «Viktor Grigoryan

Math 342 Partial Differential Equations «Viktor Grigoryan Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite

More information

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies Laplacian Cooperative Attitue Control of Multiple Rigi Boies Dimos V. Dimarogonas, Panagiotis Tsiotras an Kostas J. Kyriakopoulos Abstract Motivate by the fact that linear controllers can stabilize the

More information

Optimal Control of Spatially Distributed Systems

Optimal Control of Spatially Distributed Systems Optimal Control of Spatially Distribute Systems Naer Motee an Ali Jababaie Abstract In this paper, we stuy the structural properties of optimal control of spatially istribute systems. Such systems consist

More information

Optimal Control of Spatially Distributed Systems

Optimal Control of Spatially Distributed Systems Optimal Control of Spatially Distribute Systems Naer Motee an Ali Jababaie Abstract In this paper, we stuy the structural properties of optimal control of spatially istribute systems. Such systems consist

More information

ELEC3114 Control Systems 1

ELEC3114 Control Systems 1 ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.

More information

From Local to Global Control

From Local to Global Control Proceeings of the 47th IEEE Conference on Decision an Control Cancun, Mexico, Dec. 9-, 8 ThB. From Local to Global Control Stephen P. Banks, M. Tomás-Roríguez. Automatic Control Engineering Department,

More information

ECE 422 Power System Operations & Planning 7 Transient Stability

ECE 422 Power System Operations & Planning 7 Transient Stability ECE 4 Power System Operations & Planning 7 Transient Stability Spring 5 Instructor: Kai Sun References Saaat s Chapter.5 ~. EPRI Tutorial s Chapter 7 Kunur s Chapter 3 Transient Stability The ability of

More information

Switching Time Optimization in Discretized Hybrid Dynamical Systems

Switching Time Optimization in Discretized Hybrid Dynamical Systems Switching Time Optimization in Discretize Hybri Dynamical Systems Kathrin Flaßkamp, To Murphey, an Sina Ober-Blöbaum Abstract Switching time optimization (STO) arises in systems that have a finite set

More information

AN INTRODUCTION TO AIRCRAFT WING FLUTTER Revision A

AN INTRODUCTION TO AIRCRAFT WING FLUTTER Revision A AN INTRODUCTION TO AIRCRAFT WIN FLUTTER Revision A By Tom Irvine Email: tomirvine@aol.com January 8, 000 Introuction Certain aircraft wings have experience violent oscillations uring high spee flight.

More information

Separation Principle for a Class of Nonlinear Feedback Systems Augmented with Observers

Separation Principle for a Class of Nonlinear Feedback Systems Augmented with Observers Proceeings of the 17th Worl Congress The International Feeration of Automatic Control Separation Principle for a Class of Nonlinear Feeback Systems Augmente with Observers A. Shiriaev, R. Johansson A.

More information

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi

BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS. Mauro Boccadoro Magnus Egerstedt Paolo Valigi Yorai Wardi BEYOND THE CONSTRUCTION OF OPTIMAL SWITCHING SURFACES FOR AUTONOMOUS HYBRID SYSTEMS Mauro Boccaoro Magnus Egerstet Paolo Valigi Yorai Wari {boccaoro,valigi}@iei.unipg.it Dipartimento i Ingegneria Elettronica

More information

A Path Planning Method Using Cubic Spiral with Curvature Constraint

A Path Planning Method Using Cubic Spiral with Curvature Constraint A Path Planning Metho Using Cubic Spiral with Curvature Constraint Tzu-Chen Liang an Jing-Sin Liu Institute of Information Science 0, Acaemia Sinica, Nankang, Taipei 5, Taiwan, R.O.C., Email: hartree@iis.sinica.eu.tw

More information

Chapter 2 Lagrangian Modeling

Chapter 2 Lagrangian Modeling Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie

More information

TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM

TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM 265 Asian Journal of Control, Vol. 4, No. 3, pp. 265-273, September 22 TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM Jurachart Jongusuk an Tsutomu Mita

More information

Optimal LQR Control of Structures using Linear Modal Model

Optimal LQR Control of Structures using Linear Modal Model Optimal LQR Control of Structures using Linear Moal Moel I. Halperin,2, G. Agranovich an Y. Ribakov 2 Department of Electrical an Electronics Engineering 2 Department of Civil Engineering Faculty of Engineering,

More information

Quantum Mechanics in Three Dimensions

Quantum Mechanics in Three Dimensions Physics 342 Lecture 20 Quantum Mechanics in Three Dimensions Lecture 20 Physics 342 Quantum Mechanics I Monay, March 24th, 2008 We begin our spherical solutions with the simplest possible case zero potential.

More information

Calculus BC Section II PART A A GRAPHING CALCULATOR IS REQUIRED FOR SOME PROBLEMS OR PARTS OF PROBLEMS

Calculus BC Section II PART A A GRAPHING CALCULATOR IS REQUIRED FOR SOME PROBLEMS OR PARTS OF PROBLEMS Calculus BC Section II PART A A GRAPHING CALCULATOR IS REQUIRED FOR SOME PROBLEMS OR PARTS OF PROBLEMS. An isosceles triangle, whose base is the interval from (0, 0) to (c, 0), has its verte on the graph

More information

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University

More information

Time-Optimal Motion Control of Piezoelectric Actuator: STM Application

Time-Optimal Motion Control of Piezoelectric Actuator: STM Application Time-Optimal Motion Control of Piezoelectric Actuator: STM Application Yongai Xu, Peter H. Mecl Abstract This paper exaes the problem of time-optimal motion control in the context of Scanning Tunneling

More information

Exam 2 Review Solutions

Exam 2 Review Solutions Exam Review Solutions 1. True or False, an explain: (a) There exists a function f with continuous secon partial erivatives such that f x (x, y) = x + y f y = x y False. If the function has continuous secon

More information

Visual Servoing for Underactuated VTOL UAVs : a Linear, Homography-Based Framework

Visual Servoing for Underactuated VTOL UAVs : a Linear, Homography-Based Framework Visual Servoing for Uneractuate VTOL UAVs : a Linear, Homography-Base Framework Henry e Plinval, Pascal Morin, Philippe Mouyon, Tarek Hamel H. e Plinval an P. Mouyon are with ONERA-The French Aerospace

More information

Statics. There are four fundamental quantities which occur in mechanics:

Statics. There are four fundamental quantities which occur in mechanics: Statics Mechanics isabranchofphysicsinwhichwestuythestate of rest or motion of boies subject to the action of forces. It can be ivie into two logical parts: statics, where we investigate the equilibrium

More information

Further Differentiation and Applications

Further Differentiation and Applications Avance Higher Notes (Unit ) Prerequisites: Inverse function property; prouct, quotient an chain rules; inflexion points. Maths Applications: Concavity; ifferentiability. Real-Worl Applications: Particle

More information

Calculus in the AP Physics C Course The Derivative

Calculus in the AP Physics C Course The Derivative Limits an Derivatives Calculus in the AP Physics C Course The Derivative In physics, the ieas of the rate change of a quantity (along with the slope of a tangent line) an the area uner a curve are essential.

More information

Dynamic Load Carrying Capacity of Spatial Cable Suspended Robot: Sliding Mode Control Approach

Dynamic Load Carrying Capacity of Spatial Cable Suspended Robot: Sliding Mode Control Approach Int J Avance Design an Manufacturing echnology, Vol. 5/ No. 3/ June - 212 73 Dynamic Loa Carrying Capacity of Spatial Cable Suspene Robot: Sliing Moe Control Approach M. H. Korayem Department of Mechanical

More information

Invariant Extended Kalman Filter: Theory and application to a velocity-aided estimation problem

Invariant Extended Kalman Filter: Theory and application to a velocity-aided estimation problem Invariant Extene Kalman Filter: Theory an application to a velocity-aie estimation problem S. Bonnabel (Mines ParisTech) Joint work with P. Martin (Mines ParisTech) E. Salaun (Georgia Institute of Technology)

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,

More information

Total Energy Shaping of a Class of Underactuated Port-Hamiltonian Systems using a New Set of Closed-Loop Potential Shape Variables*

Total Energy Shaping of a Class of Underactuated Port-Hamiltonian Systems using a New Set of Closed-Loop Potential Shape Variables* 51st IEEE Conference on Decision an Control December 1-13 212. Maui Hawaii USA Total Energy Shaping of a Class of Uneractuate Port-Hamiltonian Systems using a New Set of Close-Loop Potential Shape Variables*

More information

IN the recent past, the use of vertical take-off and landing

IN the recent past, the use of vertical take-off and landing IEEE TRANSACTIONS ON ROBOTICS, VOL. 27, NO. 1, FEBRUARY 2011 129 Aaptive Position Tracking of VTOL UAVs Anrew Roberts, Stuent Member, IEEE, an Abelhami Tayebi, Senior Member, IEEE Abstract An aaptive position-tracking

More information

A PID-Sliding Mode Control Design for a Coupled Tank

A PID-Sliding Mode Control Design for a Coupled Tank International Conference CRATT 0, Raes, Tunisia 0 A PID-Sliing Moe Control Design for a Couple Tank Ahme RHIF, Zohra Karous, Naceur BenHaj Braiek Avance System Laboratory, Polytechnic School of Tunisia

More information

The total derivative. Chapter Lagrangian and Eulerian approaches

The total derivative. Chapter Lagrangian and Eulerian approaches Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function

More information

FrIP6.1. subject to: V 0 &V 1 The trajectory to the target (x(t)) is generated using the HPFbased, gradient dynamical system:

FrIP6.1. subject to: V 0 &V 1 The trajectory to the target (x(t)) is generated using the HPFbased, gradient dynamical system: Proceeings of the 45th IEEE onference on Decision & ontrol Manchester Gran Hyatt Hotel San Diego, A, USA, December 3-5, 006 Agile, Steay Response of Inertial, onstraine Holonomic Robots Using Nonlinear,

More information

Trajectory Tracking in the Sagittal Plane: Decoupled Lift/Thrust Control via Tunable Impedance Approach in Flapping-Wing MAVs

Trajectory Tracking in the Sagittal Plane: Decoupled Lift/Thrust Control via Tunable Impedance Approach in Flapping-Wing MAVs Trajectory Tracking in the Sagittal Plane: Decouple Lift/Thrust Control via Tunable Impeance Approach in FlappingWing MAVs Hosein Mahjoubi, an Katie Byl Abstract Flappingwing microaerial vehicles (MAVs

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

and from it produce the action integral whose variation we set to zero:

and from it produce the action integral whose variation we set to zero: Lagrange Multipliers Monay, 6 September 01 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine

More information

Chapter 24: Magnetic Fields and Forces Solutions

Chapter 24: Magnetic Fields and Forces Solutions Chapter 24: Magnetic iels an orces Solutions Questions: 4, 13, 16, 18, 31 Exercises & Problems: 3, 6, 7, 15, 21, 23, 31, 47, 60 Q24.4: Green turtles use the earth s magnetic fiel to navigate. They seem

More information

Nonlinear Trajectory Tracking using Vectorial Backstepping Approach

Nonlinear Trajectory Tracking using Vectorial Backstepping Approach International Conference on Control Automation an Systems 8 Oct. -7 8 in COEX Seoul Korea Nonlinear rajectory racking using Vectorial Backstepping Approach Hyochoong Bang Sangjong Lee an Haechang Lee 3

More information

Distributed coordination control for multi-robot networks using Lyapunov-like barrier functions

Distributed coordination control for multi-robot networks using Lyapunov-like barrier functions IEEE TRANSACTIONS ON 1 Distribute coorination control for multi-robot networks using Lyapunov-like barrier functions Dimitra Panagou, Dušan M. Stipanović an Petros G. Voulgaris Abstract This paper aresses

More information

Automatica. Global trajectory tracking control of VTOL-UAVs without linear velocity measurements

Automatica. Global trajectory tracking control of VTOL-UAVs without linear velocity measurements Automatica 46 (200) 053 059 Contents lists available at ScienceDirect Automatica journal homepage: www.elsevier.com/locate/automatica Brief paper Global trajectory tracking control of VTOL-UAVs without

More information

Numerical Integrator. Graphics

Numerical Integrator. Graphics 1 Introuction CS229 Dynamics Hanout The question of the week is how owe write a ynamic simulator for particles, rigi boies, or an articulate character such as a human figure?" In their SIGGRPH course notes,

More information

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v Math Fall 06 Section Monay, September 9, 06 First, some important points from the last class: Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v passing through

More information

PD Controller for Car-Following Models Based on Real Data

PD Controller for Car-Following Models Based on Real Data PD Controller for Car-Following Moels Base on Real Data Xiaopeng Fang, Hung A. Pham an Minoru Kobayashi Department of Mechanical Engineering Iowa State University, Ames, IA 5 Hona R&D The car following

More information

Implicit Lyapunov control of closed quantum systems

Implicit Lyapunov control of closed quantum systems Joint 48th IEEE Conference on Decision an Control an 28th Chinese Control Conference Shanghai, P.R. China, December 16-18, 29 ThAIn1.4 Implicit Lyapunov control of close quantum systems Shouwei Zhao, Hai

More information

12.5. Differentiation of vectors. Introduction. Prerequisites. Learning Outcomes

12.5. Differentiation of vectors. Introduction. Prerequisites. Learning Outcomes Differentiation of vectors 12.5 Introuction The area known as vector calculus is use to moel mathematically a vast range of engineering phenomena incluing electrostatics, electromagnetic fiels, air flow

More information

A new approach to explicit MPC using self-optimizing control

A new approach to explicit MPC using self-optimizing control 28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June -3, 28 WeA3.2 A new approach to explicit MPC using self-optimizing control Henrik Manum, Sriharakumar Narasimhan an Sigur

More information

Moving Charges And Magnetism

Moving Charges And Magnetism AIND SINGH ACADEMY Moving Charges An Magnetism Solution of NCET Exercise Q -.: A circular coil of wire consisting of turns, each of raius 8. cm carries a current of. A. What is the magnitue of the magnetic

More information

Qubit channels that achieve capacity with two states

Qubit channels that achieve capacity with two states Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

Approximate reduction of dynamic systems

Approximate reduction of dynamic systems Systems & Control Letters 57 2008 538 545 www.elsevier.com/locate/sysconle Approximate reuction of ynamic systems Paulo Tabuaa a,, Aaron D. Ames b, Agung Julius c, George J. Pappas c a Department of Electrical

More information

arxiv: v1 [math.oc] 25 Nov 2017

arxiv: v1 [math.oc] 25 Nov 2017 Constraine Geometric Attitue Control on SO(3) Shankar Kulumani* an Taeyoung Lee November 8, 017 arxiv:17199v1 [math.oc] 5 Nov 017 Abstract This paper presents a new geometric aaptive control system with

More information

Shared Control Between Adaptive Autopilots and Human Operators for Anomaly Mitigation

Shared Control Between Adaptive Autopilots and Human Operators for Anomaly Mitigation Share Control Between Aaptive Autopilots an Human Operators for Anomaly Mitigation Benjamin T. Thomsen Anuraha M. Annaswamy Eugene Lavretsky Massachusetts Institute of Technology, Cambrige, MA 02139 The

More information

Impact of DFIG based Wind Energy Conversion System on Fault Studies and Power Swings

Impact of DFIG based Wind Energy Conversion System on Fault Studies and Power Swings Impact of DFIG base Win Energy Conversion System on Fault Stuies an Power Swings Likin Simon Electrical Engineering Department Inian Institute of Technology, Maras Email: ee133@ee.iitm.ac.in K Shanti Swarup

More information

Multivariable Calculus: Chapter 13: Topic Guide and Formulas (pgs ) * line segment notation above a variable indicates vector

Multivariable Calculus: Chapter 13: Topic Guide and Formulas (pgs ) * line segment notation above a variable indicates vector Multivariable Calculus: Chapter 13: Topic Guie an Formulas (pgs 800 851) * line segment notation above a variable inicates vector The 3D Coorinate System: Distance Formula: (x 2 x ) 2 1 + ( y ) ) 2 y 2

More information

Gravitation as the result of the reintegration of migrated electrons and positrons to their atomic nuclei. Osvaldo Domann

Gravitation as the result of the reintegration of migrated electrons and positrons to their atomic nuclei. Osvaldo Domann Gravitation as the result of the reintegration of migrate electrons an positrons to their atomic nuclei. Osvalo Domann oomann@yahoo.com (This paper is an extract of [6] liste in section Bibliography.)

More information

Chapter-2. Steady Stokes flow around deformed sphere. class of oblate axi-symmetric bodies

Chapter-2. Steady Stokes flow around deformed sphere. class of oblate axi-symmetric bodies hapter- Steay Stoes flow aroun eforme sphere. class of oblate axi-symmetric boies. General In physical an biological sciences, an in engineering, there is a wie range of problems of interest lie seimentation

More information

Solutions to Math 41 Second Exam November 4, 2010

Solutions to Math 41 Second Exam November 4, 2010 Solutions to Math 41 Secon Exam November 4, 2010 1. (13 points) Differentiate, using the metho of your choice. (a) p(t) = ln(sec t + tan t) + log 2 (2 + t) (4 points) Using the rule for the erivative of

More information

Situation awareness of power system based on static voltage security region

Situation awareness of power system based on static voltage security region The 6th International Conference on Renewable Power Generation (RPG) 19 20 October 2017 Situation awareness of power system base on static voltage security region Fei Xiao, Zi-Qing Jiang, Qian Ai, Ran

More information

Homework 7 Due 18 November at 6:00 pm

Homework 7 Due 18 November at 6:00 pm Homework 7 Due 18 November at 6:00 pm 1. Maxwell s Equations Quasi-statics o a An air core, N turn, cylinrical solenoi of length an raius a, carries a current I Io cos t. a. Using Ampere s Law, etermine

More information

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE Journal of Soun an Vibration (1996) 191(3), 397 414 THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE E. M. WEINSTEIN Galaxy Scientific Corporation, 2500 English Creek

More information

Feedback-Linearizing Control for Velocity and Attitude Tracking of an ROV with Thruster Dynamics Containing Input Dead Zones

Feedback-Linearizing Control for Velocity and Attitude Tracking of an ROV with Thruster Dynamics Containing Input Dead Zones Feeback-Linearizing Control for Velocity an Attitue Tracking of an ROV with Thruster Dynamics Containing Input Dea Zones Joran Boehm 1, Eric Berkenpas 2, Charles Shepar 3, an Derek A. Paley 4 Abstract

More information

The Principle of Least Action

The Principle of Least Action Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of

More information

Polynomial Inclusion Functions

Polynomial Inclusion Functions Polynomial Inclusion Functions E. e Weert, E. van Kampen, Q. P. Chu, an J. A. Muler Delft University of Technology, Faculty of Aerospace Engineering, Control an Simulation Division E.eWeert@TUDelft.nl

More information

Day 4: Motion Along a Curve Vectors

Day 4: Motion Along a Curve Vectors Day 4: Motion Along a Curve Vectors I give my stuents the following list of terms an formulas to know. Parametric Equations, Vectors, an Calculus Terms an Formulas to Know: If a smooth curve C is given

More information

1. The electron volt is a measure of (A) charge (B) energy (C) impulse (D) momentum (E) velocity

1. The electron volt is a measure of (A) charge (B) energy (C) impulse (D) momentum (E) velocity AP Physics Multiple Choice Practice Electrostatics 1. The electron volt is a measure of (A) charge (B) energy (C) impulse (D) momentum (E) velocity. A soli conucting sphere is given a positive charge Q.

More information

State observers and recursive filters in classical feedback control theory

State observers and recursive filters in classical feedback control theory State observers an recursive filters in classical feeback control theory State-feeback control example: secon-orer system Consier the riven secon-orer system q q q u x q x q x x x x Here u coul represent

More information

G j dq i + G j. q i. = a jt. and

G j dq i + G j. q i. = a jt. and Lagrange Multipliers Wenesay, 8 September 011 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine

More information

Track Initialization from Incomplete Measurements

Track Initialization from Incomplete Measurements Track Initialiation from Incomplete Measurements Christian R. Berger, Martina Daun an Wolfgang Koch Department of Electrical an Computer Engineering, University of Connecticut, Storrs, Connecticut 6269,

More information

Slide10 Haykin Chapter 14: Neurodynamics (3rd Ed. Chapter 13)

Slide10 Haykin Chapter 14: Neurodynamics (3rd Ed. Chapter 13) Slie10 Haykin Chapter 14: Neuroynamics (3r E. Chapter 13) CPSC 636-600 Instructor: Yoonsuck Choe Spring 2012 Neural Networks with Temporal Behavior Inclusion of feeback gives temporal characteristics to

More information

Topic 2.3: The Geometry of Derivatives of Vector Functions

Topic 2.3: The Geometry of Derivatives of Vector Functions BSU Math 275 Notes Topic 2.3: The Geometry of Derivatives of Vector Functions Textbook Sections: 13.2 From the Toolbox (what you nee from previous classes): Be able to compute erivatives scalar-value functions

More information

Experimental Robustness Study of a Second-Order Sliding Mode Controller

Experimental Robustness Study of a Second-Order Sliding Mode Controller Experimental Robustness Stuy of a Secon-Orer Sliing Moe Controller Anré Blom, Bram e Jager Einhoven University of Technology Department of Mechanical Engineering P.O. Box 513, 5600 MB Einhoven, The Netherlans

More information

Efficient Macro-Micro Scale Coupled Modeling of Batteries

Efficient Macro-Micro Scale Coupled Modeling of Batteries A00 Journal of The Electrochemical Society, 15 10 A00-A008 005 0013-651/005/1510/A00/7/$7.00 The Electrochemical Society, Inc. Efficient Macro-Micro Scale Couple Moeling of Batteries Venkat. Subramanian,*,z

More information

Left-invariant extended Kalman filter and attitude estimation

Left-invariant extended Kalman filter and attitude estimation Left-invariant extene Kalman filter an attitue estimation Silvere Bonnabel Abstract We consier a left-invariant ynamics on a Lie group. One way to efine riving an observation noises is to make them preserve

More information

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1

Assignment 1. g i (x 1,..., x n ) dx i = 0. i=1 Assignment 1 Golstein 1.4 The equations of motion for the rolling isk are special cases of general linear ifferential equations of constraint of the form g i (x 1,..., x n x i = 0. i=1 A constraint conition

More information

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing

Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Course Project for CDS 05 - Geometric Mechanics John M. Carson III California Institute of Technology June

More information

Calculus of Variations

Calculus of Variations 16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t

More information

This section outlines the methodology used to calculate the wave load and wave wind load values.

This section outlines the methodology used to calculate the wave load and wave wind load values. COMPUTERS AND STRUCTURES, INC., JUNE 2014 AUTOMATIC WAVE LOADS TECHNICAL NOTE CALCULATION O WAVE LOAD VALUES This section outlines the methoology use to calculate the wave loa an wave win loa values. Overview

More information