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CONTROL STRATEGIES FOR A CLASS OF

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Navy needs next generation torpedoes and high speed underwater ... No Phugoid mode (Similar to F-16 aircraft) EOM: Aircraft = Supercavitating Torpedo ... – PowerPoint PPT presentation

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Title: CONTROL STRATEGIES FOR A CLASS OF


1
CONTROL STRATEGIES FOR A CLASS OF
SUPERCAVITATING VEHICLES ANUKUL
GOEL 8/23/2002 Masters Thesis Defense
Advisors Dr. Andrew J. Kurdila
Dr. Rick Lind Committee Dr. Norman Fitz-Coy
2
OUTLINE
  • Introduction and Motivation
  • Equations of Motion
  • Control Objectives
  • LQR Control Synthesis
  • Nonlinear Simulation
  • Conclusion

3
INTRODUCTION
  • Motivation
  • Navy needs next generation torpedoes and high
    speed underwater
  • vehicles such as SUPERCAVITATING VEHICLES
  • Limited research available in public domain for
    modeling and
  • control of supercavitating vehicles.
  • This project was to model and control and
    prototypical
  • supercavitating torpedo.
  • My contributions to the project
  • Equation of motion (Anand and Anukul)
  • Linear equations of motion (Anand and Anukul)
  • Control Synthesis (Anukul)
  • Nonlinear Simulations (Anukul)

4
CAVITATION
  • At High Velocity
  • Fluid Velocity Increases
  • Fluid Pressure Drops below
  • Vapor Pressure
  • Fluid Vaporizes

Tip Vortex Cavitation
Supercavitation
5
ISSUES WITH SUPERCAVITATION
Advantages
Disadvantages
  • High Frequency Motions
  • Prediction of Cavity
  • Control and Maneuvering
  • Maintaining the Cavity
  • Low Skin Friction Drag
  • High Velocities

6
VEHICLE MODEL CONTROL SURFACES
Lc
Le1
De1
Dc
W
Cavitator
  • 2 Elevators
  • 2 Rudders
  • 1 Cavitator

1 DOF Fin
1 DOF Cavitator
7
CAVITATOR/FIN MODEL
Cl for Cavitator
Half angle 150
Cl for Fin
Angle of attack (deg)
Sweepback angle0 deg
Angle of attack (deg)
8
EQUATIONS OF MOTION NONLINEAR
  • Equations of motion are identical for torpedo
    and aircraft.
  • Consider force equation
  • Additional 9 equations for moment, orientation
    and position.
  • Components of forces and moments are unique for
    torpedo.
  • Consider force in body fixed X-axis direction.
  • Similar decomposition for all forces and moments.

9
EQUATIONS OF MOTION LINEAR
10
OPEN-LOOP DYNAMICS
  • Consider root locus of open-loop poles for
    linearizing airspeed
  • Open-loop system is always unstable
  • No Phugoid mode (Similar to F-16 aircraft)

11
CONTROL OBJECTIVE
  • Track a pitch or roll rate command up to 30
    deg/s
  • and
  • maintain an overshoot less than 15.
  • have rise time less 0.5s.
  • have a steady-state error less than 5.
  • Avoid actuator saturation

Control Surface Limits
12
ASSUMPTIONS FOR CONTROL SYNTHESIS
  • The cavity model is fixed cavity. Thus there is
    no variation of immersion
  • and the torpedo is symmetrically situated in
    the cavity.
  • Longitudinal controls are cavitator and
    horizontal fins only
  • Lateral controls are 2 vertical fins (rudders).
  • It is assumed that 9 states (velocities, angular
    rates and orientation ) are
  • available for feedback for tracking
    controller.
  • It is assumed that control surface deflection of
    small order (0.1 deg for
  • longitudinal and 0.01 for lateral) are
    achievable.
  • Propulsive force is assumed to be constant during
    flight, the constant value
  • being obtained during trim optimization.

13
LQR SYNTHESIS
  • Find Controller K such that u-Kx minimizes
  • x is the state
  • u is the control from K
  • Q and R are weighting matrices
  • In case of longitudinal feedback 4 states and
    tracking error
  • In case of lateral feedback 5 states and
    tracking error

14
LQR LONGITUDINAL
  • More weighting on cavitator to ensure more use
    of elevator
  • Weighting of zero on all states to allow for
    their variation

Cavitator Deflection
Linear Response
Cavitator (deg)
q (deg/s)
Time (s)
Time (s)
15
LQR LATERAL
Linear Response
Rudder Deflection
Rudder (deg)
Roll rate (deg/s)
Time (s)
Time (s)
16
NONLINEAR SIMULATION
de1 (deg)
  • Command 15 deg/s doublet
  • of pitch rate

de1 rate (deg/s)
  • Rise Time 0.17s
  • Overshoot 11.53
  • Minimal lateral response
  • Unstable for commands gt 30 deg/s

Time (s)
17
NONLINEAR SIMULATION
dr1 (deg)
p (deg/s)
Time (s)
  • Command 15 deg/s doublet
  • of roll rate

q (deg/s)
  • Rise Time 0.5s
  • Overshoot 0
  • Coupled motion
  • Unstable for commandsgt50 deg/s

Time (s)
18
ROBUSTNESS GAIN/PHASE MARGINS
x
19
ROBUSTNESS GAIN/PHASE MARGINS
Longitudinal (Inner and Outer loop) Gain Margin
inf Phase Margin 57deg
Magnitude (dB)
Phase(deg)
Frequency (rad/sec)
Magnitude (dB)
Lateral (Inner and Outer loop) Gain Margin
50.36 dB Phase Margin inf
Phase(deg)
Frequency (rad/sec)
20
ROBUSTNESSPERTURBED RESPONSE
  • 20 Perturbation given in values of cl, cd,
    immersion.
  • Small variation in A, B matrices.
  • Stable eigenvalues remain stable for variation
    with velocity.
  • Closed-loop response was acceptable with nominal
    controller.
  • Tracking objectives are met
  • Small variations in airspeed

21
  • 10 uncertainty in coefficients of lift and drag
    of cavitator
  • introduced into system during synthesis.
  • Good Lateral performance obtained.
  • Good Longitudinal controller not obtained
    possibly as the
  • controller tries to stabilize the uncertain
    poles.

22
  • Higher overshoot and
  • rise time.
  • Saturation for commands
  • higher than 20 deg/s.

p (deg/s)
Time (s)
  • Rise time 0.025s
  • Overshoot 0
  • Saturation for commands
  • higher than 40deg/s

p (deg/s)
Time (s)
23
CONCLUSIONS
  • A model for supercavitating torpedo has been
    achieved
  • A LQR controller has been obtained than gives
    good
  • performance for pitch and roll rate
    tracking.
  • A controller for lateral dynamics has been
    obtained
  • that shows good performance.
  • The controller for longitudinal is yet to be
    obtained.
  • The model for cavity is assumed to be fixed.
    Dynamic
  • model for cavity is yet to be obtained.
  • The Pitch and Roll rate controllers are for
    inner-loop
  • model. An outer-loop controller can be
    obtained for
  • guidance and navigation

FUTURE WORK
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