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8/12/2019 9. Math Modeling and Flight Simulation5_9
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9. MATH MODELING AND
FLIGHT SIMULATION
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GOALS OF FLIGHT SIMULATION
Predict mathematically:
1. Equilibrium flight condition (Trim)
2. Flight mode stability of the aircraft (Stab
Analysis),
3. Time history response of the aircraft due to
pilot inputs, external disturbances.(Maneuver)
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NON REAL TIME GLOBAL MODELS
BASED ON KNOWN AVAILABLE PHYSICS
PRIMARY USES:
COMPONENT DESIGN (Rotor, fuselage, etc)
INTER-RELATIONSHIP AMONG COMPONENTS
DEVELOPMENT OF MORE ADVANCED MODLES LIMITED BY
ACCURATE KNOWLEDGE OF PHYSICS
DEVELOPMENT OF DIGITIAL COMPUTERS
ONE ANALYSIS/PROGRAM APPLICABLE TO SEVERAL
AIRCRAFT MODELS
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REAL TIME MODELS
INDIVIDUAL MODEL FOR EACH AIRCRAFT MODEL
MODEL LOOSELY BASED IN PHYSICS BUT TWEAKED
TO AIRCRAFT FLIES LIKE THE REAL AIRCRAFT TO
TEST PILOTS
PRIMARY USES: PILOT FAMILIARZATION, PILOT
TRAING, CONTROL SYSTEM DESIGN AND
EVALUATION, ACCIDENT INVESTIGATION
MAY NOT BE USEFUL FOR DETAILED DESIGN OF
MECHANICAL COMPONENTS
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MODES OF OPERATION
TRIM
STAB (Linearized Model)
TIME HISTORY
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TRIM
Required Inputs:
1. Complete structural and aerodynamic description of
aircraft using either measured aerodynamic data or analytic functions.
2. Complete description of Control System
3. Flight Condition description (gross weight, cg, speed,atmospheric properties)
Typical Results:
1. Attitude of aircraft (yaw, pitch, roll), Rotor flapping angles
(fore/aft and lateral flapping) for 2 rotors
2. Position of pilots controls
3. Steady state performance (HP, fuel flow,etc) and
Steady state oscillatory rotor and fuselage loads
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TRIM MATHEMATICS
Trimmed Helicopter flight condition is described by 11
independent variables: 3 fuselage angles(yaw, pitch,
roll); 4 pilot controls (collective, f/a cyclic, lateral cyclic,
and pedals) and 4 rigid blade flapping angles (f/a and
lateral) for 2 independent rotors.
These 11 independent variables must satisfy 10 static
equilibrium equations ( 3 forces and 3 moments at and
about cg, fore/aft and lateral flapping moments for 2independent rotors
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TRIM SOLUTION TECHNIQUE
1. Assume fixed value of 1 flight condition
independent variable (usually fuselage
pitch or roll angle) to obtain 10
nonlinear algebraic equations in 10unknowns.
2. Guess values for remaining 10
independent variables and iterate on
them until all 10 static equilibriumequations are satisfied
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STAB ANALYSIS
GOAL: Produce a linearized mathematical model
that is valid over a small region about the equilibrium
flight condition obtained in the Trim process.
METHOD: Calculate the changes in all fuselage
and rotor forces and moments due to small
perturbations in the flight variables- displacements,
velocities, and control inputs.
Produces 10x10 mass, damping, and stiffness
matrices; and a 10x4 control effectiveness matrix
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STAB RESULTS
Stick fixed aircraft stability obtained from Eigen value
solution. System damped natural frequencies and
mode shapes. Time to half (stable roots) or time to
double amplitude (unstable roots)
Single input-Single output transfer functions to show
aircraft response to control inputs. Starting point in
designing automatic flight control system.M
Many System requirements are described in terms
resulting for the Stab Results.
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TIME HISTORY SOLUTION
TASK: Determine time history response of aircraft, performance,
rotor loads, fuselage vibrations, etc following Pilot control input,
change is aircraft configuration change is atmosphere.
SOLUTION: Use 4 cycle Runge_Kutta method to numericallyintegrate NDE nonlinear, coupled differential equations
NDE= Fuselage Rigid Body Degrees of Freedom 6
number of elastic fuselage modes from NASTRAN ??
number of elastic rotor modes from MYKLESSAD ???
5< NDE
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ROTOR MODELS
1. Rotor Disk or Frisbee Model
2. Blade Element Model
3. Aeroelastic Model
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ROTOR DISK or FRISBEE
Linear Model
Rotor Forces as function of (radius, tipspeed,
solidity, average slope of lift curve, collectivepitch, cyclic pitch, rotor inflow, twist)
Neglects: Stall, compressibility effects, mach
number effects, different airfoils, taper,
nonlinear twist, elastic blade deflections andvelocities
Produce quick Back of the Envelope results
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]T+T+T+T[2
a
=C 423T201T
Thrust Coefficient from
Approximate Linearized Integration
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BLADE ELEMENT MODEL
Blade Aerodynamic forces are calculated at 20
radial stations and 24 azimuth locations
Requires solution of Rigid Blade Flapping
Differential Equation
Includes nonlinear aerodynamic effects (stall,
compressibility, nonlinear twist, non uniform
airfoil radial distribution
Neglects effects of blade/fuselage Elastic
displacements and velocities
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BLADE ELEMENT AERODYNAMIC
MODEL
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BLADE ELEMENT AERODYNAMICS
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BLADE FLAPPING DIFFERENTIAL
EQUATION
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BLADE ELEMENT AERO FORCES
CL from Airfoil data tables
CD from Airfoil data tables
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AIRFOIL LIFT AS A FUNCTION
OF MACH AND ALPHA
MACH NUMBERANGLE OF ATTACK 0.3 0.4 0.5 0.68 0.74 0.92 1
(DEGREES) -25 -0.892 -0.892 -0.892 -0.892 -0.892 -0.8922 -0.892
-14 -0.81 -0.81 -0.81 -0.783 -0.76 -0.69 -0.69
-12 -0.816 -0.816 -0.816 -0.786 -0.761 -0.59 -0.59
-10 -0.766 -0.766 -0.766 -0.758 -0.751 -0.48 -0.48
-8 -0.655 -0.67 -0.66 -0.68 -0.69 -0.39 -0.39
-6 -0.51 -0.54 -0.53 -0.625 -0.681 -0.35 -0.35
-4 -0.34 -0.35 -0.34 -0.44 -0.5 -0.3 -0.3
-3 -0.24 -0.25 -0.24 -0.313 -0.35 -0.2 -0.2
-2 -0.14 -0.15 -0.13 -0.161 -0.17 -0.1 -0.1
-1 -0.03 -0.03 0 0.006 0.02 0 00 0.09 0.095 0.12 0.163 0.2 0.1 0.1
1 0.21 0.22 0.24 0.3177 0.35 0.2 0.2
2 0.32 0.33 0.36 0.447 0.47 0.3 0.3
3 0.44 0.45 0.49 0.56 0.56 0.4 0.4
4 0.55 0.57 0.65 0.663 0.64 0.5 0.5
6 0.78 0.79 0.87 0.863 0.78 0.59 0.59
8 0.99 1.02 1.13 1.021 0.91 0.69 0.69
10 1.2 1.24 1.36 1.122 1.03 0.73 0.73
11 1.31 1.35 1.47 1.15 1.09 0.74 0.74
12 1.41 1.435 1.55 1.195 1.14 0.74 0.74
12.5 1.46 1.43 1.43 1.212 1.17 0.738 0.738
13 1.51 1.39 1.42 1.229 1.2 0.735 0.735
13.5 1.54 1.34 1.42 1.251 1.23 0.732 0.732
14 1.535 1.29 1.41 1.269 1.26 0.73 0.73
14.5 1.5 1.26 1.39 1.285 1.29 0.73 0.73
15 1.435 1.24 1.36 1.297 1.32 0.72 0.72
16 1.392 1.19 1.325 1.274 1.295 0.7 0.7
17 1.326 1.15 1.3 1.288 1.316 0.67 0.67
20 1.172 1.172 1.172 1.294 1.3 0.64 0.64
25 0.892 0.892 0.892 1.036 1.16 0.65 0.65
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TYPICAL AIR FOIL LIFT DATA TABLE
-1.5
-1
-0.5
0
0.5
1
1.5
2
-30 -20 -10 0 10 20 30
Angle of Attack (degrees)
LiftC
oefficient(cl)
0.3
0.4
0.5
0.68
0.74
0.92
1
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AEROELASTIC MODEL
REQUIRES AS INPUT FULLY COUPLED
(BEAM/CHORD/TORSION) BLADE MODE SHAPES
AND NATURAL FREQUIENCES)
SOLUTION REQUIRES NUMERICAL INTEGRATIONOF SEVERAL NON-LINEAR SECOND ORDER
COUPLED DIFFERENTIAL EQUATIONS WITH TIME
DEPENDENT COEFFICENTS
PRODUCES ROTOR SHEAR AND MOMENT
DISTRIBUTIONS INCLUDING ELASTIC EFFECTS
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AIRPLANES VS. HELICOPTERS
AIRPLANES
6 DEGREES OF FREEDOM: 3 FORCES AND 3 MOMENTS
7 IND. VARIABLES: YAW PITCH ROLL ANGLES
THROTTLE F/A STICK LAT STICK PEDALS
HELICOPTERS
10 DEGREES OF FREEDOM: 3 FUSE FORCES AND 3 FUS MOMENTS
+ F/A AND LATERAL MOMENTS ON 2 ROTORS
11 IND. VARIABLES: FUSELAGE YAW PITCH AND ROLL ANGLES
COLLECTIVE F/A CYCLIC LAT CYCLIC PEDAL+ F/A AND LATERAL FLAPPING FOR 2 ROTORS
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PROBLEMS ASSOCIATED WITH GLOBAL
SIMULATION PROGRAMS
COPTER
CAMRAD
FLIGHT LAB
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VALIDITY OF IMBEDDED ANALYTICAL
MODELS
INDIVIDUAL COMPONENTS (Induced Velocity, Tip
Vortex, Mechanical Friction) cannot be verified as a
stand alone component
INNERACTION OF MAJOR COMPONENTS ARE
DIFFICULT, IF NOT IMPOSSIBLE, TO MODEL
(Operating environment of Tail Rotor)
MATH MODELS OF PILOT/HUMAN REACTION
ARE SUSPECT
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VALIDITY OF INPUT DATA
STEADY/UNSTEADY AERODYNAMIC
COEFFICIENTS OVER TOTAL OPERATING REGION
(Mach, Angle of Attack)
FINITE ELEMENT MODEL/RESULTS FOR FIXED
COMPONENTS
FULLY COUPLED BEAM/CHORD/TORSION BLADE
NATURAL FREQUENCIES AND MODE SHAPES
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USE OF OUTPUT DATA
MANAGING THE NUMBER OF OUTPUT DATA
INTERPRETATION OF RESULTS (Knowledge ofCoordinate System, Units, etc)
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ADVANCES IN DIGITAL COMPUTERS
1972: IBM 360 MAIN FRAME COMPUTER
BLADE ELEMENT MODEL REQUIRED 15
MINUTES TO MODEL 4 SEC REAL TIME
RATIO: 1 SEC REAL TIME=225 SEC CPUTIME
2002: DESKTOP PC:
1 SEC REAL TIME=.2 SEC CPU TIME
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DESK TOP SIMULATION PROGRAMS
MICROSOFT FLIGHT SIMULATOR 2002
X PLANE
FLY II
STRONG POINTS:
GRPHICS, EYE CANDY, NAVIGATION
AIDS, AIRPORTS, WEATHER
WEAK POINTS:
ACCURATE REPRESENTATION OF
VEHICLE DYNAMICS
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ROTOR MODELING PROBLEMS
AERODYNAMIC MODELS HAVE DIFFICULTY WITH
1 UNSTEADY AERODYNAMICS
2 STALL/ REVERSED FLOW3 TIP VORTEX
4 ROTOR WAKE
INCREASING MODELING DETAIL DOES
NOT NECESSARILY PRODUCE BETTER
ANSWERS *** UNIFORM TEXTURE***