1 Challenge the future Ship motion compensation platform for high payloads dynamic analysis and...

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1 Challenge the future Ship motion compensation platform for high payloads dynamic analysis and control MSc Project at GustoMSC – Wouter de Zeeuw Prof.dr. D.J. Rixen, Ir. M. Wondergem

Transcript of 1 Challenge the future Ship motion compensation platform for high payloads dynamic analysis and...

Page 1: 1 Challenge the future Ship motion compensation platform for high payloads dynamic analysis and control MSc Project at GustoMSC – Wouter de Zeeuw Prof.dr.

1Challenge the future

Ship motion compensation platform for high payloads dynamic analysis and control

MSc Project at GustoMSC – Wouter de ZeeuwProf.dr. D.J. Rixen, Ir. M. Wondergem

Page 2: 1 Challenge the future Ship motion compensation platform for high payloads dynamic analysis and control MSc Project at GustoMSC – Wouter de Zeeuw Prof.dr.

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Introduction: Pooltable on cruise ship

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Two ship motion compensation platforms:Ampelmann (personnel) Bargemaster (~400 tonnes)

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Feed the components to the site Jack up and install

Offshore windturbine installation with Jack-up units Present method

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Goal: Complete windturbine installation from a floating unit

1000[t]

400[t](concept of competitor)

Motion stabilizing platform to extend operating limits

Fast feeder barges

Jack up unit stays at site

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Small overview

Preliminary 2D model1. Analysis of Ampelmann scalemodel tests2. 3D modeling of new mechanism on ship3. Controlling the system

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Goal: Complete windturbine installation from a floating unit

Preliminary 2D model showed feasibility ...

400[t](concept of competitor)

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Goal: Complete windturbine installation from a floating unit

Preliminary 2D model showed feasibility but dynamic instability

400[t](concept of competitor)

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1. (In-)stability due to the quasistatic control?Similar mass system: Ampelmann scale model tests

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Maximum real part of eigenvalues of system matrix. 1 parameter varied around maximum likelihood estim.

1. Stability of the fitted linear model

All parameters as in fit of first 15 seconds

e.g. cH times 2 (double the hydrodyn. damping) others identical

UNSTABLE

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1. Stability of the fitted linear modelMaximum real part of eigenvalues of system matrix.

1 parameter varied around maximum likelihood estim.

• Adding hydro-damping stabilizes

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1. Stability of the fitted linear modelMaximum real part of eigenvalues of system matrix.

1 parameter varied around maximum likelihood estim.

• The damping on opposite movements is a destabilizing factor, possible unmodeled nonlinearities

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1. Stability of the fitted linear modelMaximum real part of eigenvalues of system matrix.

1 parameter varied around maximum likelihood estim.

• The proportional control has stable and unstable settings

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2. 3D modeling - ship movements

• Accelerations due to planar movements surge, sway and yaw are smaller than due to off planar movements

• Platform should compensate heave, roll and pitch

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2. 3D modeling - platform mechanism

• New mechanism for a 3 degree of freedom platform• Planar movements are constrained by 3 Sarrus type

linkages• Force vs. Reach variable via α

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2. 3D modeling - hydrodynamicsBarge panel model(35x115m)

State-Space approx. of wave radiation terms

External wave field realization

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2. 3D modeling - vessel+platform

• Lagrangian dynamics (body fixed) • Extension of serial robot on ship to parallel robots

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2. 3D modeling - total dynamics

• Nonlinear kinematics• Coriolis terms • Pose dep. mass matrix

• External waveloads• Hydrostatics• Hydrodynamics

• Wave radiation• Added mass/damping

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2. 3D modeling - total dynamics

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3. Controllers - Naïve Quasistatic vs. Model Based

Quasistatic:• Calculate leg length error assuming fixed boat

position• 2 Proportional-Integral-Derivative (PID) controllers

• On mean error• On asymmetric errors

Model Based:• Nonlinear Model Predictive Control

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3. Control - Nonlinear Model Predictive Control

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3. Control - Nonlinear Model Predictive Control

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Visualizations

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Visualizations

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Heave-Roll-Pitch in storm conditionsHead sea, seastate Hs=4m T1=6.5s.

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Energy usage in disturbance rejectionMilder sea

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Conclusions

• The scalemodel roll instability can be reproduced by a linear model with quasistatic control and influential parameters can be recognized.

• The coupled ship - parallel platform dynamics are derived and he new platform can compensate the ship movements.

• MPC is shown to be a successful candidate for control, requires less power than PID in disturbance rejection and is less hard to tune and to stabilize.

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Thank you. Questions?

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#1: Second degree model fit, technique

Fitting technique:

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#1b: Second degree model fit, results

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#2: Kinematics – leg joint velocity Jacobian construction

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#3: Hydrodynamics – rad forces

Retardation forces (vector):

Cummins eqn. in hydrodyn. ref. frame:

State space approx. per radiation component (scalar):

Known values via hydrodynamic code (WAMIT):

Approx. model: (Gauss-Newton iter)

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#4a: Dynamics – Pose dep. mass matrix

(Relative velocity)

(ref. frame transf.)

(notation)

(expand)

The total mass matrix is now (platform) pose dependent

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#4b: Dynamics - Lagrange

(euler angle rates)(body fixed general velocities)