Final Exam TTK 4190 Guidance and Control

Size: px
Start display at page:

Download "Final Exam TTK 4190 Guidance and Control"

Transcription

1 Page 1 of 8 Contact person during the exam: University lecturer Morten Breivik, Department of Engineering Cybernetics, Gløshaugen Phone: 73 5( ) Cell: Final Exam TTK 4190 Guidance and Control Wednesday May 23rd 2007 Hours: Aids: Language: A All printed and handwritten materials are allowed. Calculators approved by NTNU can be used. English. No. of pages: 8. The exams will be graded by June 13th The percentages represent the relative weight each problem is attributed at the evaluation.

2 Page 2 of 8 1 Multiple Choice (15%) Only one alternative is correct. 1. (2%) Which dimensionless expression holds true? (a) Kq 0 = 1 K 1 2 ρl3 U q (b) Kq 0 = 1 1 K 2 ρl3 U 2 q (c) Kq 0 = 1 K 1 2 ρl4 U q 2. (3%) Consider a floating cube where all the sides have length L. Assume that the water density is ρ while the cube density is ρ c. The hydrodynamically added mass in heave is Zẇ = m where m isthecubemass(uniformly distributed). What is the undamped resonance frequency in heave for the floating cube? (a) ω z = q 1 2 ( ρ c ρ ) g L (b) ω z = q 1 2 ( ρ ρ c ) g L 2 (c) ω z = q 1 2 ( ρ ρ c ) g L 3. (4%) Given the nonlinear system ψ = r (1) (I z Nṙ)ṙ + H(r)r = Kδ + d (2) d = 0, (3) where d is a disturbance, H(r) represents the nonlinear maneuvering characteristics, and the rudder angle δ is the control input. Considering e = ψ ψ d and r d = ψ d, which of the suggested controllers delivers the best overall performance? h R i (a) δ = 1 t (I K z Nṙ)(ṙ d K p e K d ė K i e(τ)dτ)+h(r)r o h R i (b) δ = 1 t (I K z Nṙ)(ṙ K p e K d ė K i e(τ)dτ)+h(r)r o h R i (c) δ = 1 t (I K z Nṙ)(ṙ d K p e K d ė K i e(τ)dτ) o 1

3 Page 3 of 8 4. (4%) Employing the following sliding mode controller δ = 1 Z t (I z Nṙ)(ṙ d 2λė λ 2 e)+h(r)(r d 2λe λ 2 K where Z t s = ė +2λe + λ 2 e(τ)dτ, λ>0,andk>0, 0 what is the resulting error dynamics of the nonlinear system (1)-(2)? (a) (I z Nṙ)ṡ + H(r)s + K s = d (b) (I z Nṙ)ṡ +[H(r)+K]sgn(s) =d (c) (I z Nṙ)ṡ + H(r)s + Ksgn(s) =d 5. (2%) Which statement is true (regarding the control design paradigms Maneuvering and Trajectory Tracking)? (a) Maneuvering and Trajectory Tracking are equally flexible. (b) Maneuvering is more flexible than Trajectory Tracking. (c) Trajectory Tracking is more flexible than Maneuvering. 2 Guidance System (20%) 0 e(τ)dτ) Ksgn(s), Consider Figure 1, where a kinematic model of a marine surface vessel is represented by the position vector p =[x, y] > and the velocity vector ṗ =[ẋ, ẏ] > (in NED coordinates). Also, consider a straight line segment (track) represented by its orientation angle α (with respect to the NED frame) and an arbitrary point p l =[x l,y l ] > somewhere along the track. 1. (2%) Show that the cross-track error e (see Figure 1) can be calculated by e = (x x l )sinα +(y y l )cosα. 2. (5%) Consider the Control Lyapunov Function (CLF) for the cross-track error V = 1 2 e2, (4) and show that U V = p e e2 (5) when employing the velocity vector guidance law 2

4 Page 4 of 8 p χ p X N e Δ α p l Y N Figure 1: An ideal, kinematic guidance consideration. µ χ = α +tan 1 e, (6) 4 where 4 > 0 (the so-called lookahead distance), and ṗ = U with U> 0 (Hint: Consider the trigonometry of Figure 1). What global and local stability properties do(4)and(5)givefor the origin of the cross-track error? 3. (5%) How can you combine this guidance concept with a heading (and speed) autopilot in order to achieve track following? How will such a track following concept depend on the lookahead distance 4 (Hint: Relate 4 to what you do when you drive a car along a road)? 4. (3%) What is the relationship between the guidance approach of Figure 1 and the modified LOS guidance scheme? 5. (5%) A ship guided by the LOS (or the modified LOS algorithm) will drift off track when subjected to a constant environmental disturbance. Why? What can be done to minimize the cross-track error in such a situation? Moreover, how can perfect track following be achieved in such a situation (Hint: Distinguish between the course and the heading of a ship)? 3

5 Page 5 of 8 3 Ship Roll Control (20%) Consider the 1 degree-of-freedom (DOF) roll dynamics of a ship φ = p (7) (I x Kṗ)ṗ K p p p p K p p + W GM T sin φ = τ K, (8) where K p p < 0, K p < 0, andgm T > 0. The control objective is to track a bounded, continuous and readily available roll reference trajectory φ d, φ d, φ d. The ship is equipped with two identical fins located symmetrically on each side of the hull such that τ K = K α α,wherek α 0 and α is the effective fin angle. 1. (5%) Derive a feedback linearizing control law for α that fulfills the control objective. Will your controller be able to track the desired roll motion at all ship speeds? Justify your answer. 2. (5%) Derive a backstepping control law for α that fulfills the control objective and takes advantage of useful model properties. 3. (2%) Compare the feedback linearizing and backstepping controller expressions. 4. (3%) The hydraulic machinery that rotate the fins do not respond perfectly to the controller commands. Hence, augment the dynamic model (7)-(8) with the findynamics α = 1 T (α c α), (9) where α c represents the commanded control input and T > 0. Derive a backstepping control law for α c that fulfills the control objective (Hint: Augment your existing backstepping design). 5. (5%) Linearize the open-loop roll kinetics (8) (i.e., τ K =0) about the equillibrium point φ, =[0, 0] > and show the resulting mass-damper-spring h φi > (MDS) model. Subsequently, for a ship with the model data (I x Kṗ) = [kgm 2 ], K p = [kgm 2 /s], W = [kgm/s 2 ], and GM T =1[m], find the relative damping ratio and natural frequency associated with the MDS roll model. Based on this MDS roll model, does the vessel need a ship roll stabilization system? Justify your answer. 4

6 Page 6 of 8 4 Weather Optimal Control (10%) 1. (3%) What is the motivation behind weather optimal position control (WOPC) for marine vessels? What kind of vessels should have WOPC capability? In what situations will the employment of WOPC be an advantage/disadvantage? 2. (2%) What are the basic two rules that make the weather optimal heading control (WOHC) concept work? Justify your answer. 3. (2%) Which variable most significantly influences the rate of convergence toward the weather optimal heading and why? 4. (2%) State the full control law expression τ for the WOPC scheme and explain the purpose of each term. 5. (1%) Why is the WOPC stability result only local? Justify your answer. Figure 2: The principle of weather optimal control. 5 Vessel Motion Control (35%) The standard 3 DOF maneuvering model of a marine surface vessel is given by η = R(ψ)ν (10) M ν + C(ν)ν + D(ν)ν = τ, (11) where M = M > > 0, C(ν) = C > (ν), andd(ν) 0. Here,τ represents the control input vector (i.e., environmental disturbances are not considered). 1. (2%) Explain why you can simplify equation (11) when designing a dynamic positioning (DP) system. Write down the resulting DP model. 5

7 Page 7 of 8 2. (16%) Consider the CLF V = 1 2 (z> 1 z 1 + z > 2 Mz 2 ), (12) where z 2 = ν α (13) and α is a stabilizing function yet to be designed. Furthermore, we can consider either z 1 = η η d, (14) or z 1 = R > (ψ)(η η d ) (15) when deriving a motion control law by backstepping. Here, η d represents the desired trajectory to be tracked, and you can assume that η d, η d,and η d are all bounded, continuous and readily available. (a) (5%) Using the DP model, derive two backstepping controllers by respectively employing (14) and (15) such that the time derivative of (12) becomes V = z > 1 K 1 z 1 z > 2 K 2 z 2 (16) where K 1 = K > 1 > 0 and K 2 = K > 2 > 0. (b) (5%) What is the main qualitative difference between the controller based on (14) and the controller based on (15)? Which controller would you have chosen for implementation and why? (c) (2%) On the basis of (12) and (16), what is the stability property of the origin of the error system state z = z > 1, z > > 2? (d) (2%) Why is (12) referred to as the pseudo-kinetic energy of the error system? (e) (2%) How can you redesign your backstepping controllers to take advantage of hydrodynamic damping? How does such a redesign affect (16) and the stability property of the error system origin? 3. (9%) Now consider the complete maneuvering kinetics of (11) (representing a vessel travelling at moderate speeds). (a) (3%) Derive a backstepping controller by using (12), (13) and (15) such that the time derivative of (12) becomes V = z > 1 K 1 z 1 z > 2 (D(ν)+K 2 )z 2. 6

8 Page 8 of 8 (b) (2%) Explain the role of each term in your control law. (c) (4%) Derive the associated error system dynamics (i.e., the z-dynamics) and elaborate on the resulting model structure. 4. (3%) Consider the control input vector τ =[τ X,τ Y,τ N ] >,representingthe surge, sway and yaw control inputs, respectively. A marine surface vessel travelling at high speeds cannot independently control its sway DOF (usually because τ Y = f(τ N ) for some function f( )). Why is this so and how does this fact influence (the feasibility of) the recently developed backstepping controllers? 5. (5%)Why is it useful(and necessary)to distinguish between autopilot (AP) and dynamic positioning (DP) motion control systems? What are the main differences between AP and DP control system design? 7

Final Exam TTK4190 Guidance and Control

Final Exam TTK4190 Guidance and Control Trondheim Department of engineering Cybernetics Contact person: Professor Thor I. Fossen Phone: 73 59 43 61 Cell: 91 89 73 61 Email: tif@itk.ntnu.no Final Exam TTK4190 Guidance and Control Friday May 15,

More information

Exam - TTK 4190 Guidance & Control Eksamen - TTK 4190 Fartøysstyring

Exam - TTK 4190 Guidance & Control Eksamen - TTK 4190 Fartøysstyring Page 1 of 6 Norges teknisk- naturvitenskapelige universitet Institutt for teknisk kybernetikk Faglig kontakt / contact person: Navn: Morten Pedersen, Universitetslektor Tlf.: 41602135 Exam - TTK 4190 Guidance

More information

Problem 1: Ship Path-Following Control System (35%)

Problem 1: Ship Path-Following Control System (35%) Problem 1: Ship Path-Following Control System (35%) Consider the kinematic equations: Figure 1: NTNU s research vessel, R/V Gunnerus, and Nomoto model: T ṙ + r = Kδ (1) with T = 22.0 s and K = 0.1 s 1.

More information

Comparing Combinations of Linear and Nonlinear Feedback Terms for Motion Control of Marine Surface Vessels

Comparing Combinations of Linear and Nonlinear Feedback Terms for Motion Control of Marine Surface Vessels Comparing Combinations of Linear and Nonlinear Feedback Terms for Motion Control of Marine Surface Vessels Mikkel Eske Nørgaard Sørensen Morten Breivik Centre for Autonomous Marine Operations and Systems,

More information

A Ship Heading and Speed Control Concept Inherently Satisfying Actuator Constraints

A Ship Heading and Speed Control Concept Inherently Satisfying Actuator Constraints A Ship Heading and Speed Control Concept Inherently Satisfying Actuator Constraints Mikkel Eske Nørgaard Sørensen, Morten Breivik and Bjørn-Olav H. Eriksen Abstract Satisfying actuator constraints is often

More information

Computer Problem 1: SIE Guidance, Navigation, and Control

Computer Problem 1: SIE Guidance, Navigation, and Control Computer Problem 1: SIE 39 - Guidance, Navigation, and Control Roger Skjetne March 12, 23 1 Problem 1 (DSRV) We have the model: m Zẇ Z q ẇ Mẇ I y M q q + ẋ U cos θ + w sin θ ż U sin θ + w cos θ θ q Zw

More information

A Time-Varying Lookahead Distance Guidance Law for Path Following

A Time-Varying Lookahead Distance Guidance Law for Path Following A Time-Varying Lookahead Distance Guidance Law for Path Following Anastasios M. Lekkas Thor I. Fossen Centre for Ships and Ocean Structures Norwegian University of Science and Technology, NO-7491, Trondheim,

More information

Minimization of Cross-track and Along-track Errors for Path Tracking of Marine Underactuated Vehicles

Minimization of Cross-track and Along-track Errors for Path Tracking of Marine Underactuated Vehicles Minimization of Cross-track and Along-track Errors for Path Tracking of Marine Underactuated Vehicles Anastasios M. Lekkas and Thor I. Fossen Abstract This paper deals with developing a guidance scheme

More information

Comparing Nonlinear Adaptive Motion Controllers for Marine Surface Vessels

Comparing Nonlinear Adaptive Motion Controllers for Marine Surface Vessels Comparing Nonlinear Adaptive Motion Controllers for Marine Surface Vessels Mikkel Eske Nørgaard Sørensen Morten Breivik Centre for Autonomous Marine Operations and Systems, Department of Engineering Cybernetics,

More information

Nonlinear Tracking Control of Underactuated Surface Vessel

Nonlinear Tracking Control of Underactuated Surface Vessel American Control Conference June -. Portland OR USA FrB. Nonlinear Tracking Control of Underactuated Surface Vessel Wenjie Dong and Yi Guo Abstract We consider in this paper the tracking control problem

More information

Breu, Frequency Detuning of Parametric Roll

Breu, Frequency Detuning of Parametric Roll Frequency Detuning of Parametric Roll Conference on CeSOS Highlights and AMOS Visions, May 29, 2013 Dominik Breu Department of Engineering Cybernetics, NTNU, Trondheim, Norway Centre for Ships and Ocean

More information

Path Following of Underactuated Marine Surface Vessels in the Presence of Unknown Ocean Currents

Path Following of Underactuated Marine Surface Vessels in the Presence of Unknown Ocean Currents Path Following of Underactuated Marine Surface Vessels in the Presence of Unknown Ocean Currents Signe Moe 1, Walter Caharija 1, Kristin Y Pettersen 1 and Ingrid Schjølberg Abstract Unmanned marine crafts

More information

Handling Roll Constraints for Path Following of Marine Surface Vessels using Coordinated Rudder and Propulsion Control

Handling Roll Constraints for Path Following of Marine Surface Vessels using Coordinated Rudder and Propulsion Control 2010 American Control Conference Marriott Waterfront, Baltimore, MD, USA June 30-July 02, 2010 FrB15.5 Handling Roll Constraints for Path Following of Marine Surface Vessels using Coordinated Rudder and

More information

COPYRIGHTED MATERIAL. Index

COPYRIGHTED MATERIAL. Index Index 3 DOF maneuvering model, 113 4 DOF maneuvering model, 158 6 DOF equations of motion, 167 Abkowitz s model, 138 absolute damping factor, 366 acceleration feedback, 365, 369 accelerometer, 329 Adams

More information

Path Following for Marine Surface Vessels with Rudder and Roll Constraints: an MPC Approach

Path Following for Marine Surface Vessels with Rudder and Roll Constraints: an MPC Approach 2009 American Control Conference Hyatt Regency Riverfront, St. Louis, MO, USA June 10-12, 2009 ThC11.6 Path Following for Marine Surface Vessels with Rudder and Roll Constraints: an MPC Approach Zhen Li,

More information

Seakeeping Models in the Frequency Domain

Seakeeping Models in the Frequency Domain Seakeeping Models in the Frequency Domain (Module 6) Dr Tristan Perez Centre for Complex Dynamic Systems and Control (CDSC) Prof. Thor I Fossen Department of Engineering Cybernetics 18/09/2007 One-day

More information

Model Reference Adaptive Control of Underwater Robotic Vehicle in Plane Motion

Model Reference Adaptive Control of Underwater Robotic Vehicle in Plane Motion Proceedings of the 11th WSEAS International Conference on SSTEMS Agios ikolaos Crete Island Greece July 23-25 27 38 Model Reference Adaptive Control of Underwater Robotic Vehicle in Plane Motion j.garus@amw.gdynia.pl

More information

A numerical DP MODULE to help design and operation for projects including DP components

A numerical DP MODULE to help design and operation for projects including DP components DYNAMIC POSITIONING CONFERENCE November 15-16, 25 Control Systems I A numerical DP MODULE to help design and operation for projects including DP components C. Le Cunff PRINCIPIA (La Ciotat, France) Return

More information

A Discussion About Seakeeping and Manoeuvring Models For Surface Vessels

A Discussion About Seakeeping and Manoeuvring Models For Surface Vessels A Discussion About Seakeeping and Manoeuvring Models For Surface Vessels Tristan Perez, Thor I. Fossen and Asgeir Sørensen Technical Report (MSS-TR-001) Marine System Simulator (MSS) Group (http://www.cesos.ntnu.no/mss/)

More information

TTK4190 Guidance and Control Exam Suggested Solution Spring 2011

TTK4190 Guidance and Control Exam Suggested Solution Spring 2011 TTK4190 Guidance and Control Exam Suggested Solution Spring 011 Problem 1 A) The weight and buoyancy of the vehicle can be found as follows: W = mg = 15 9.81 = 16.3 N (1) B = 106 4 ( ) 0.6 3 3 π 9.81 =

More information

Design of a Heading Autopilot for Mariner Class Ship with Wave Filtering Based on Passive Observer

Design of a Heading Autopilot for Mariner Class Ship with Wave Filtering Based on Passive Observer Design of a Heading Autopilot for Mariner Class Ship with Wave Filtering Based on Passive Observer 1 Mridul Pande, K K Mangrulkar 1, Aerospace Engg Dept DIAT (DU), Pune Email: 1 mridul_pande000@yahoo.com

More information

THE EFFECT OF MEMORY IN PASSIVE NONLINEAR OBSERVER DESIGN FOR A DP SYSTEM

THE EFFECT OF MEMORY IN PASSIVE NONLINEAR OBSERVER DESIGN FOR A DP SYSTEM DYNAMIC POSIIONING CONFERENCE October 1-13, 1 DESIGN SESSION HE EFFEC OF MEMORY IN PASSIVE NONLINEAR OBSERVER DESIGN FOR A DP SYSEM By A. Hajivand & S. H. Mousavizadegan (AU, ehran, Iran) ABSRAC he behavior

More information

Output Feedback Control for Maneuvering Systems Using Observer Backstepping

Output Feedback Control for Maneuvering Systems Using Observer Backstepping Output Feedback Control for Maneuvering Systems Using Observer Backstepping Ivar-André F. Ihle 1 RogerSkjetne and Thor I. Fossen 13 Abstract An output feedback design for maneuvering systems is proposed

More information

HOW TO INCORPORATE WIND, WAVES AND OCEAN CURRENTS IN THE MARINE CRAFT EQUATIONS OF MOTION. Thor I. Fossen

HOW TO INCORPORATE WIND, WAVES AND OCEAN CURRENTS IN THE MARINE CRAFT EQUATIONS OF MOTION. Thor I. Fossen HOW TO INCORPORATE WIND, WAVES AND OCEAN CURRENTS IN THE MARINE CRAFT EQUATIONS OF MOTION Thor I. Fossen Department of Engineering Cybernetics, Noregian University of Science and Technology, NO-7491 Trondheim,

More information

Guidance-Based Path Following for Autonomous Underwater Vehicles

Guidance-Based Path Following for Autonomous Underwater Vehicles Guidance-Based Path Following for Autonomous Underwater Vehicles Morten Breivik,1 Centre for Ships and Ocean Structures (CESOS) Norwegian University of Science and Technology (NTNU) NO-7491 Trondheim,

More information

Robot Control Basics CS 685

Robot Control Basics CS 685 Robot Control Basics CS 685 Control basics Use some concepts from control theory to understand and learn how to control robots Control Theory general field studies control and understanding of behavior

More information

Hydrodynamic Forces on Floating Bodies

Hydrodynamic Forces on Floating Bodies Hydrodynamic Forces on Floating Bodies 13.42 Lecture Notes; c A.H. Techet 1. Forces on Large Structures For discussion in this section we will be considering bodies that are quite large compared to the

More information

Geometric Formation Control for Autonomous Underwater Vehicles

Geometric Formation Control for Autonomous Underwater Vehicles 010 IEEE International Conference on Robotics and Automation Anchorage Convention District May 3-8, 010, Anchorage, Alaska, USA Geometric Formation Control for Autonomous Underwater Vehicles Huizhen Yang

More information

Nonlinear Observer Design for Dynamic Positioning

Nonlinear Observer Design for Dynamic Positioning Author s Name, Company Title of the Paper DYNAMIC POSITIONING CONFERENCE November 15-16, 2005 Control Systems I J.G. Snijders, J.W. van der Woude Delft University of Technology (The Netherlands) J. Westhuis

More information

Simultaneous Roll Damping and Course Keeping via Sliding Mode Control for a Marine Vessel in Seaway

Simultaneous Roll Damping and Course Keeping via Sliding Mode Control for a Marine Vessel in Seaway Milano (Italy) August 8 - September, 11 Simultaneous Roll Damping and Course Keeping via Sliding Mode Control for a Marine Vessel in Seaway C. Carletti A. Gasparri S. Longhi G. Ulivi Dipartimento di Ingegneria

More information

Improving the combined operation of Dynamic Positioning and motion compensation from a control engineering perspective I.M.

Improving the combined operation of Dynamic Positioning and motion compensation from a control engineering perspective I.M. Improving the combined operation of Dynamic Positioning and motion compensation from a control engineering perspective Delft Center for Systems and Control Improving the combined operation of Dynamic

More information

Chapter 10. Path Following. Beard & McLain, Small Unmanned Aircraft, Princeton University Press, 2012, Chapter 10, Slide 1

Chapter 10. Path Following. Beard & McLain, Small Unmanned Aircraft, Princeton University Press, 2012, Chapter 10, Slide 1 Chapter 10 Path Following Beard & McLain, Small Unmanned Aircraft, Princeton University Press, 2012, Chapter 10, Slide 1 Control Architecture destination, obstacles map path planner waypoints status path

More information

Sample Lab Report For PHYS221/222

Sample Lab Report For PHYS221/222 This document is intended to provide guidance on how to write a lab report using the 100 point lab report format that is given on this website. There is no such thing as a perfect lab report and there

More information

SEAKEEPING AND MANEUVERING Prof. Dr. S. Beji 2

SEAKEEPING AND MANEUVERING Prof. Dr. S. Beji 2 SEAKEEPING AND MANEUVERING Prof. Dr. S. Beji 2 Ship Motions Ship motions in a seaway are very complicated but can be broken down into 6-degrees of freedom motions relative to 3 mutually perpendicular axes

More information

Nonlinear Formation Control of Marine Craft

Nonlinear Formation Control of Marine Craft Nonlinear Formation Control of Marine Craft Roger Skjetne, Sonja Moi, and Thor I. Fossen Abstract This paper investigates formation control of a fleet of ships. The control objective for each ship is to

More information

Übersetzungshilfe / Translation aid (English) To be returned at the end of the exam!

Übersetzungshilfe / Translation aid (English) To be returned at the end of the exam! Prüfung Regelungstechnik I (Control Systems I) Prof. Dr. Lino Guzzella 5. 2. 2 Übersetzungshilfe / Translation aid (English) To be returned at the end of the exam! Do not mark up this translation aid -

More information

Autonomous Helicopter Landing A Nonlinear Output Regulation Perspective

Autonomous Helicopter Landing A Nonlinear Output Regulation Perspective Autonomous Helicopter Landing A Nonlinear Output Regulation Perspective Andrea Serrani Department of Electrical and Computer Engineering Collaborative Center for Control Sciences The Ohio State University

More information

Trajectory Tracking of a Near-Surface Torpedo using Numerical Methods

Trajectory Tracking of a Near-Surface Torpedo using Numerical Methods ISSN (Print) : 2347-671 An ISO 3297: 27 Certified Organization Vol.4, Special Issue 12, September 215 Trajectory Tracking of a Near-Surface Torpedo using Numerical Methods Anties K. Martin, Anubhav C.A.,

More information

Hierarchical Control of Marine Vehicles for Autonomous. Maneuvering in Offshore Operations

Hierarchical Control of Marine Vehicles for Autonomous. Maneuvering in Offshore Operations Hierarchical Control of Marine Vehicles for Autonomous Maneuvering in Offshore Operations Guoyuan Li, Wei Li, Karl Henning Halse, Hans Petter Hildre, and Houxiang Zhang February 3, 15 Abstract This paper

More information

Trajectory tracking & Path-following control

Trajectory tracking & Path-following control Cooperative Control of Multiple Robotic Vehicles: Theory and Practice Trajectory tracking & Path-following control EECI Graduate School on Control Supélec, Feb. 21-25, 2011 A word about T Tracking and

More information

DIFFERENTIAL KINEMATICS. Geometric Jacobian. Analytical Jacobian. Kinematic singularities. Kinematic redundancy. Inverse differential kinematics

DIFFERENTIAL KINEMATICS. Geometric Jacobian. Analytical Jacobian. Kinematic singularities. Kinematic redundancy. Inverse differential kinematics DIFFERENTIAL KINEMATICS relationship between joint velocities and end-effector velocities Geometric Jacobian Analytical Jacobian Kinematic singularities Kinematic redundancy Inverse differential kinematics

More information

EN Nonlinear Control and Planning in Robotics Lecture 10: Lyapunov Redesign and Robust Backstepping April 6, 2015

EN Nonlinear Control and Planning in Robotics Lecture 10: Lyapunov Redesign and Robust Backstepping April 6, 2015 EN530.678 Nonlinear Control and Planning in Robotics Lecture 10: Lyapunov Redesign and Robust Backstepping April 6, 2015 Prof: Marin Kobilarov 1 Uncertainty and Lyapunov Redesign Consider the system [1]

More information

TTK4150 Nonlinear Control Systems Solution 6 Part 2

TTK4150 Nonlinear Control Systems Solution 6 Part 2 TTK4150 Nonlinear Control Systems Solution 6 Part 2 Department of Engineering Cybernetics Norwegian University of Science and Technology Fall 2003 Solution 1 Thesystemisgivenby φ = R (φ) ω and J 1 ω 1

More information

Global stabilization of an underactuated autonomous underwater vehicle via logic-based switching 1

Global stabilization of an underactuated autonomous underwater vehicle via logic-based switching 1 Proc. of CDC - 4st IEEE Conference on Decision and Control, Las Vegas, NV, December Global stabilization of an underactuated autonomous underwater vehicle via logic-based switching António Pedro Aguiar

More information

Final Exam April 30, 2013

Final Exam April 30, 2013 Final Exam Instructions: You have 120 minutes to complete this exam. This is a closed-book, closed-notes exam. You are allowed to use a calculator during the exam. Usage of mobile phones and other electronic

More information

Optimization techniques for autonomous underwater vehicles: a practical point of view

Optimization techniques for autonomous underwater vehicles: a practical point of view Optimization techniques for autonomous underwater vehicles: a practical point of view M. Chyba, T. Haberkorn Department of Mathematics University of Hawaii, Honolulu, HI 96822 Email: mchyba@math.hawaii.edu,

More information

Underactuated Dynamic Positioning of a Ship Experimental Results

Underactuated Dynamic Positioning of a Ship Experimental Results 856 IEEE TRANSACTIONS ON CONTROL SYSTEMS TECHNOLOGY, VOL. 8, NO. 5, SEPTEMBER 2000 Underactuated Dynamic Positioning of a Ship Experimental Results Kristin Y. Pettersen and Thor I. Fossen Abstract The

More information

( ) Physics 201, Final Exam, Fall 2006 PRACTICE EXAMINATION Answer Key. The next three problems refer to the following situation:

( ) Physics 201, Final Exam, Fall 2006 PRACTICE EXAMINATION Answer Key. The next three problems refer to the following situation: Physics 201, Final Exam, Fall 2006 PRACTICE EXAMINATION Answer Key The next three problems refer to the following situation: Two masses, m 1 and m 2, m 1 > m 2, are suspended by a massless rope over a

More information

Robotics. Dynamics. Marc Toussaint U Stuttgart

Robotics. Dynamics. Marc Toussaint U Stuttgart Robotics Dynamics 1D point mass, damping & oscillation, PID, dynamics of mechanical systems, Euler-Lagrange equation, Newton-Euler recursion, general robot dynamics, joint space control, reference trajectory

More information

DEVELOPMENT AND MATHEMATICAL MODELLING OF PLANNING TRAJECTORY OF UNMANNED SURFACE VEHICLE

DEVELOPMENT AND MATHEMATICAL MODELLING OF PLANNING TRAJECTORY OF UNMANNED SURFACE VEHICLE DEVELOPMENT AND MATHEMATICAL MODELLING OF PLANNING TRAJECTORY OF UNMANNED SURFACE VEHICLE PROMIT CHOUDHURY 1, SRISHA DEO 2 1 B. Tech 4 th Year, Mechanical, SRM University, Tamil Nadu, India, promit17@gmail.com

More information

IAA-CU A Simulator for Robust Attitude Control of Cubesat Deploying Satellites

IAA-CU A Simulator for Robust Attitude Control of Cubesat Deploying Satellites A Simulator for Robust Attitude Control of Cubesat Deploying Satellites Giovanni Mattei, George Georgiou, Angelo Pignatelli, Salvatore Monaco Abstract The paper deals with the development and testing of

More information

The Pursuit Guidance Law

The Pursuit Guidance Law Chapter 7 The Pursuit Guidance Law Module 6: Lecture 15 Pure Pursuit Guidance Law Keywords. Pure pursuit; Capture Region As discussed earlier, pursuit guidance law is one of the most logical guidance laws

More information

A MULTI-BODY ALGORITHM FOR WAVE ENERGY CONVERTERS EMPLOYING NONLINEAR JOINT REPRESENTATION

A MULTI-BODY ALGORITHM FOR WAVE ENERGY CONVERTERS EMPLOYING NONLINEAR JOINT REPRESENTATION Proceedings of the ASME 2014 33rd International Conference on Ocean, Offshore and Arctic Engineering OMAE2014 June 8-13, 2014, San Francisco, California, USA OMAE2014-23864 A MULTI-BODY ALGORITHM FOR WAVE

More information

Chapter 9. Nonlinear Design Models. Beard & McLain, Small Unmanned Aircraft, Princeton University Press, 2012, Chapter 9, Slide 1

Chapter 9. Nonlinear Design Models. Beard & McLain, Small Unmanned Aircraft, Princeton University Press, 2012, Chapter 9, Slide 1 Chapter 9 Nonlinear Design Models Beard & McLain, Small Unmanned Aircraft, Princeton University Press, 2012, Chapter 9, Slide 1 Architecture Destination, obstacles Waypoints Path Definition Airspeed, Altitude,

More information

WAMIT-MOSES Hydrodynamic Analysis Comparison Study. JRME, July 2000

WAMIT-MOSES Hydrodynamic Analysis Comparison Study. JRME, July 2000 - Hydrodynamic Analysis Comparison Study - Hydrodynamic Analysis Comparison Study JRME, Prepared by Hull Engineering Department J. Ray McDermott Engineering, LLC 1 - Hydrodynamic Analysis Comparison Study

More information

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

ELEC4631 s Lecture 2: Dynamic Control Systems 7 March Overview of dynamic control systems

ELEC4631 s Lecture 2: Dynamic Control Systems 7 March Overview of dynamic control systems ELEC4631 s Lecture 2: Dynamic Control Systems 7 March 2011 Overview of dynamic control systems Goals of Controller design Autonomous dynamic systems Linear Multi-input multi-output (MIMO) systems Bat flight

More information

Modeling of Resonators

Modeling of Resonators . 23 Modeling of Resonators 23 1 Chapter 23: MODELING OF RESONATORS 23 2 23.1 A GENERIC RESONATOR A second example where simplified discrete modeling has been found valuable is in the assessment of the

More information

Nonlinear Landing Control for Quadrotor UAVs

Nonlinear Landing Control for Quadrotor UAVs Nonlinear Landing Control for Quadrotor UAVs Holger Voos University of Applied Sciences Ravensburg-Weingarten, Mobile Robotics Lab, D-88241 Weingarten Abstract. Quadrotor UAVs are one of the most preferred

More information

Neural Network Model Reference Adaptive Control of a Surface Vessel

Neural Network Model Reference Adaptive Control of a Surface Vessel Neural Network Model Reference Adaptive Control of a Surface Vessel Alexander Leonessa and Tannen S. VanZwieten Abstract A neural network model reference adaptive controller for trajectory tracking of

More information

Backstepping based approach for the combined longitudinal-lateral vehicle control

Backstepping based approach for the combined longitudinal-lateral vehicle control Intelligent Vehicles Symposium Alcalá de Henares, Spain, June 3-7, Backstepping based approach for the combined longitudinal-lateral vehicle control Lamri Nehaoua and Lydie Nouvelière Abstract This paper

More information

Marine Vehicle Path Following Using Inner-Outer Loop Control

Marine Vehicle Path Following Using Inner-Outer Loop Control Marine Vehicle Path Following sing Inner-Outer Loop Control P. Maurya,, A. Pedro Aguiar, A. Pascoal National Institute of Oceanography, Marine Instrumentation Division Dona Paula Goa-434, India E-mail:

More information

THRUST OPTIMIZATION OF AN UNDERWATER VEHICLE S PROPULSION SYSTEM

THRUST OPTIMIZATION OF AN UNDERWATER VEHICLE S PROPULSION SYSTEM THRUST OPTIMIZATION OF AN UNDERWATER VEHICLE S PROPULSION SYSTEM Senior lecturer Vasile DOBREF Lecturer Octavian TARABUTA Mircea cel Batran Naval Academy, Constanta, Romania Keywords: underwater vehicle,

More information

Department of Aerospace Engineering and Mechanics University of Minnesota Written Preliminary Examination: Control Systems Friday, April 9, 2010

Department of Aerospace Engineering and Mechanics University of Minnesota Written Preliminary Examination: Control Systems Friday, April 9, 2010 Department of Aerospace Engineering and Mechanics University of Minnesota Written Preliminary Examination: Control Systems Friday, April 9, 2010 Problem 1: Control of Short Period Dynamics Consider the

More information

( ) Chapter 3: Free Vibration of the Breakwater. 3.1 Introduction

( ) Chapter 3: Free Vibration of the Breakwater. 3.1 Introduction Chapter : Free Vibration of the Breakwater. Introduction Before conducting forcing analyses on the breakwater, a free vibration study is necessary. This chapter will describe the analysis conducted to

More information

Physics 351 Friday, April 24, 2015

Physics 351 Friday, April 24, 2015 Physics 351 Friday, April 24, 2015 HW13 median report time = 5 hours. You ve solved 145 homework problems this term (not counting XC). Whew! This weekend, you ll read Feynman s two lectures (Feynman Lectures

More information

Path Following with Roll Constraints for Marine Surface Vessels in Wave Fields

Path Following with Roll Constraints for Marine Surface Vessels in Wave Fields Path Following with Roll Constraints for Marine Surface Vessels in Wave Fields by Zhen Li A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy (Naval

More information

AAPT UNITED STATES PHYSICS TEAM AIP F = ma Contest 25 QUESTIONS - 75 MINUTES INSTRUCTIONS

AAPT UNITED STATES PHYSICS TEAM AIP F = ma Contest 25 QUESTIONS - 75 MINUTES INSTRUCTIONS 2014 F = ma Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2014 2014 F = ma Contest 25 QUESTIONS - 75 MINUTES INSTRUCTIONS DO NOT OPEN THIS TEST UNTIL YOU ARE TOLD TO BEGIN Use g = 10 N/kg throughout this

More information

WE propose the tracking trajectory control of a tricycle

WE propose the tracking trajectory control of a tricycle Proceedings of the International MultiConference of Engineers and Computer Scientists 7 Vol I, IMECS 7, March - 7, 7, Hong Kong Trajectory Tracking Controller Design for A Tricycle Robot Using Piecewise

More information

Lecture «Robot Dynamics»: Dynamics 2

Lecture «Robot Dynamics»: Dynamics 2 Lecture «Robot Dynamics»: Dynamics 2 151-0851-00 V lecture: CAB G11 Tuesday 10:15 12:00, every week exercise: HG E1.2 Wednesday 8:15 10:00, according to schedule (about every 2nd week) office hour: LEE

More information

Trajectory-tracking control of a planar 3-RRR parallel manipulator

Trajectory-tracking control of a planar 3-RRR parallel manipulator Trajectory-tracking control of a planar 3-RRR parallel manipulator Chaman Nasa and Sandipan Bandyopadhyay Department of Engineering Design Indian Institute of Technology Madras Chennai, India Abstract

More information

/ m U) β - r dr/dt=(n β / C) β+ (N r /C) r [8+8] (c) Effective angle of attack. [4+6+6]

/ m U) β - r dr/dt=(n β / C) β+ (N r /C) r [8+8] (c) Effective angle of attack. [4+6+6] Code No: R05322101 Set No. 1 1. (a) Explain the following terms with examples i. Stability ii. Equilibrium. (b) Comment upon the requirements of stability of a i. Military fighter aircraft ii. Commercial

More information

Quaternion-Based Tracking Control Law Design For Tracking Mode

Quaternion-Based Tracking Control Law Design For Tracking Mode A. M. Elbeltagy Egyptian Armed forces Conference on small satellites. 2016 Logan, Utah, USA Paper objectives Introduction Presentation Agenda Spacecraft combined nonlinear model Proposed RW nonlinear attitude

More information

Formation Control for Underactuated Autonomous Underwater Vehicles Using the Approach Angle

Formation Control for Underactuated Autonomous Underwater Vehicles Using the Approach Angle Original Article International Journal of Fuzzy Logic and Intelligent Systems Vol. 3, No. 3, September 03, pp. 54-63 http://dx.doi.org/0.539/ijfis.03.3.3.54 ISSNPrint 598-645 ISSNOnline 093-744X Formation

More information

Dynamic Positioning for Unmanned Surface Vehicles

Dynamic Positioning for Unmanned Surface Vehicles Dynamic Positioning for Unmanned Surface Vehicles Håvard Halvorsen Master of Science in Engineering Cybernetics Submission date: June 2008 Supervisor: Morten Breivik, ITK Co-supervisor: Vegard Evjen Hovstein,

More information

Robotics. Dynamics. University of Stuttgart Winter 2018/19

Robotics. Dynamics. University of Stuttgart Winter 2018/19 Robotics Dynamics 1D point mass, damping & oscillation, PID, dynamics of mechanical systems, Euler-Lagrange equation, Newton-Euler, joint space control, reference trajectory following, optimal operational

More information

MEROS Project. Technical Advances in Modeling and Control. Dr. Lotfi CHIKH February (33)

MEROS Project. Technical Advances in Modeling and Control. Dr. Lotfi CHIKH February (33) MEROS Project Technical Advances in Modeling and Control Dr. Lotfi CHIKH February 2013 lotfi.chikh@tecnalia.com + (33) 467 130 125 1 Contents 1 Introduction 3 2 Dynamic model of the ROV: the mathematical

More information

Aircraft Stability & Control

Aircraft Stability & Control Aircraft Stability & Control Textbook Automatic control of Aircraft and missiles 2 nd Edition by John H Blakelock References Aircraft Dynamics and Automatic Control - McRuler & Ashkenas Aerodynamics, Aeronautics

More information

MARINE vessels, AUVs and UAVs rely heavily on guidance

MARINE vessels, AUVs and UAVs rely heavily on guidance IEEE TRANSACTIONS ON CONTROL SYSTEMS TECHNOLOGY, VOL. XX, NO. Y, MONTH 3 Line-of-Sight Path Following for Dubins Paths with Adaptive Sideslip Compensation of Drift Forces Thor I. Fossen, Kristin Y. Pettersen,

More information

CLF-based Tracking Control for UAV Kinematic Models with Saturation Constraints

CLF-based Tracking Control for UAV Kinematic Models with Saturation Constraints CDC3-IEEE45 CLF-based Tracking Control for UAV Kinematic Models with Saturation Constraints Wei Ren Randal W. Beard Department of Electrical and Computer Engineering Brigham Young University Provo, Utah

More information

A GLOBAL SLIDING MODE CONTROL WITH PRE-DETERMINED CONVERGENCE TIME DESIGN FOR REUSABLE LAUNCH VEHICLES IN REENTRY PHASE

A GLOBAL SLIDING MODE CONTROL WITH PRE-DETERMINED CONVERGENCE TIME DESIGN FOR REUSABLE LAUNCH VEHICLES IN REENTRY PHASE IAA-AAS-DyCoSS-4 -- A GLOBAL SLIDING MODE CONTROL WITH PRE-DETERMINED CONVERGENCE TIME DESIGN FOR REUSABLE LAUNCH VEHICLES IN REENTRY PHASE L. Wang, Y. Z. Sheng, X. D. Liu, and P. L. Lu INTRODUCTION This

More information

CONTROL DESIGN FOR SLOW SPEED POSITIONING

CONTROL DESIGN FOR SLOW SPEED POSITIONING CONTROL DESIGN FOR SLOW SPEED POSITIONING Anna Witkowska Gdansk University of Technology, Electrical and Control Engineering Department, Gdansk, Poland E-mail: awitkowska@ely.pg.gda.pl KEYWORDS Backstepping,

More information

1. Froude Krylov Excitation Force

1. Froude Krylov Excitation Force .016 Hydrodynamics eading #8.016 Hydrodynamics Prof. A.H. Techet 1. Froude Krylov Ecitation Force Ultimately, if we assume the body to be sufficiently small as not to affect the pressure field due to an

More information

Non Linear Submarine Modelling and Motion Control with Model in Loop

Non Linear Submarine Modelling and Motion Control with Model in Loop ISSN (Print) : 2347-671 (An ISO 3297: 27 Certified Organization) Vol. 5, Special Issue 9, May 216 Non Linear Submarine Modelling and Motion Control with Model in Loop Ashitha 1, Ravi Kumar S. T 2, Dr.

More information

Nonlinear dynamic model identification methodology for real robotic surface vessels

Nonlinear dynamic model identification methodology for real robotic surface vessels International Journal of Control, 2013 Vol. 86, No. 12, 2315 2324, http://dx.doi.org/10.1080/00207179.2013.813646 Nonlinear dynamic model identification methodology for real robotic surface vessels Yaswanth

More information

Hydrodynamic analysis and modelling of ships

Hydrodynamic analysis and modelling of ships Hydrodynamic analysis and modelling of ships Wave loading Harry B. Bingham Section for Coastal, Maritime & Structural Eng. Department of Mechanical Engineering Technical University of Denmark DANSIS møde

More information

1 Trajectory Generation

1 Trajectory Generation CS 685 notes, J. Košecká 1 Trajectory Generation The material for these notes has been adopted from: John J. Craig: Robotics: Mechanics and Control. This example assumes that we have a starting position

More information

Bank-to-Turn Control for a Small UAV using Backstepping and Parameter Adaptation

Bank-to-Turn Control for a Small UAV using Backstepping and Parameter Adaptation Bank-to-Turn Control for a Small UA using Backstepping and Parameter Adaptation Dongwon Jung and Panagiotis Tsiotras Georgia Institute of Technology, Atlanta, GA 333 USA (e-mail: dongwon.jung, tsiotras@gatech.edu)

More information

Robotics & Automation. Lecture 25. Dynamics of Constrained Systems, Dynamic Control. John T. Wen. April 26, 2007

Robotics & Automation. Lecture 25. Dynamics of Constrained Systems, Dynamic Control. John T. Wen. April 26, 2007 Robotics & Automation Lecture 25 Dynamics of Constrained Systems, Dynamic Control John T. Wen April 26, 2007 Last Time Order N Forward Dynamics (3-sweep algorithm) Factorization perspective: causal-anticausal

More information

Lecture «Robot Dynamics»: Dynamics and Control

Lecture «Robot Dynamics»: Dynamics and Control Lecture «Robot Dynamics»: Dynamics and Control 151-0851-00 V lecture: CAB G11 Tuesday 10:15 12:00, every week exercise: HG E1.2 Wednesday 8:15 10:00, according to schedule (about every 2nd week) Marco

More information

Path following of a model ship using model predictive control with experimental verification

Path following of a model ship using model predictive control with experimental verification 2 American Control Conference Marriott Waterfront, Baltimore, MD, USA June 3-July 2, 2 FrA5.6 Path following of a model ship using model predictive control with experimental verification Reza Ghaemi, Soryeok

More information

Linearize a non-linear system at an appropriately chosen point to derive an LTI system with A, B,C, D matrices

Linearize a non-linear system at an appropriately chosen point to derive an LTI system with A, B,C, D matrices Dr. J. Tani, Prof. Dr. E. Frazzoli 151-0591-00 Control Systems I (HS 2018) Exercise Set 2 Topic: Modeling, Linearization Discussion: 5. 10. 2018 Learning objectives: The student can mousavis@ethz.ch, 4th

More information

Robust Nonlinear Design of Three Axes Missile Autopilot via Feedback Linearization

Robust Nonlinear Design of Three Axes Missile Autopilot via Feedback Linearization Robust Nonlinear Design of Three Axes Missile Autopilot via Feedback Linearization Abhijit Das, Ranajit Das and Siddhartha Mukhopadhyay, Amit Patra 1 1 Abstract The nonlinearity and coupling of the missile

More information

Nonlinear Observer-Based Ship Control and Disturbance Compensation

Nonlinear Observer-Based Ship Control and Disturbance Compensation Preprints, 10th IFAC Conference on Control Applications in Marine Systems September 13-16, 2016. Trondheim, Norway Nonlinear Observer-Based Ship Control and Disturbance Compensation Harald Aschemann Stefan

More information

NONLINEAR CONTROLLER DESIGN FOR ACTIVE SUSPENSION SYSTEMS USING THE IMMERSION AND INVARIANCE METHOD

NONLINEAR CONTROLLER DESIGN FOR ACTIVE SUSPENSION SYSTEMS USING THE IMMERSION AND INVARIANCE METHOD NONLINEAR CONTROLLER DESIGN FOR ACTIVE SUSPENSION SYSTEMS USING THE IMMERSION AND INVARIANCE METHOD Ponesit Santhanapipatkul Watcharapong Khovidhungij Abstract: We present a controller design based on

More information

Control of Mobile Robots Prof. Luca Bascetta

Control of Mobile Robots Prof. Luca Bascetta Control of Mobile Robots Prof. Luca Bascetta EXERCISE 1 1. Consider a wheel rolling without slipping on the horizontal plane, keeping the sagittal plane in the vertical direction. Write the expression

More information

NONLINEAR BACKSTEPPING DESIGN OF ANTI-LOCK BRAKING SYSTEMS WITH ASSISTANCE OF ACTIVE SUSPENSIONS

NONLINEAR BACKSTEPPING DESIGN OF ANTI-LOCK BRAKING SYSTEMS WITH ASSISTANCE OF ACTIVE SUSPENSIONS NONLINEA BACKSTEPPING DESIGN OF ANTI-LOCK BAKING SYSTEMS WITH ASSISTANCE OF ACTIVE SUSPENSIONS Wei-En Ting and Jung-Shan Lin 1 Department of Electrical Engineering National Chi Nan University 31 University

More information

Research Article A Nonlinear Robust Controller Design for Ship Dynamic Positioning Based on L 2 -Gain Disturbance Rejection

Research Article A Nonlinear Robust Controller Design for Ship Dynamic Positioning Based on L 2 -Gain Disturbance Rejection Control Science and Engineering Volume 26, Article ID 927565, 7 pages http://dx.doi.org/.55/26/927565 Research Article A Nonlinear Robust Controller Design for Ship Dynamic Positioning Based on L 2 -Gain

More information

Active Yaw Stabilization for Smooth, Highly Maneuverable Underwater Vehicles

Active Yaw Stabilization for Smooth, Highly Maneuverable Underwater Vehicles Active Yaw Stabilization for Smooth, Highly Maneuverable Underwater Vehicles The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation

More information

OPTIMAL CONSTRAINED CONTROL ALLOCATION IN MARINE SURFACE VESSELS WITH RUDDERS. Tor A. Johansen Λ Thomas P. Fuglseth Λ Petter Tøndel Λ Thor I.

OPTIMAL CONSTRAINED CONTROL ALLOCATION IN MARINE SURFACE VESSELS WITH RUDDERS. Tor A. Johansen Λ Thomas P. Fuglseth Λ Petter Tøndel Λ Thor I. OPTIMAL CONSTRAINED CONTROL ALLOCATION IN MARINE SURFACE VESSELS WITH RUDDERS Tor A. Johansen Λ Thomas P. Fuglseth Λ Petter Tøndel Λ Thor I. Fossen Λ Λ Department of Engineering Cybernetics, Norwegian

More information