Comprehensive System Identification of Ducted Fan UAVs - Cal Poly

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Although part of a larger control surface and augmentation experiment, thevehicle was tested in a baseline configuration similar to that seen in Figure 1.3. From thetests, pitching moment information was extracted with varying wind speeds. Figure 3.8shows the results of that test.21.510.5M (ft-lbf)0-50 -40 -30 -20 -10 0 10 20 30 40 50-0.5-1-1.5-2u (fps)Figure 3.8 – Techsburg OAV Pitching Moment to AirspeedAs Figure 3.8 shows, there is a unique pitching moment created when the vehicleexperiences some wind velocity across the duct. This is illustrated by the slope of thetangent line depicted as a dotted line. In this case, the dimensional derivative about thehover condition is 0.011. This is a corrective moment for velocities below some criticalvelocity. A negative pitching moment is then created above this critical speed. In the caseof OAV as tested, this occurs at roughly 10 fps.- 34 -
3.2.2 Allied Aerospace MAVFlight test was performed on the MAV vehicle in a similar manner as wasdescribed in the previous section for the OAV. Table 3.7 below shows the physicalproperties for the vehicle as it was tested.Table 3.7 – MAV Physical PropertiesPhysical QuantityValueMass (slugs) 0.233C.G. (below duct lip - inches) 2.25Propeller Speed (rad/sec) 1884.0I xx (slug-ft^2) 0.021I yy (slug-ft^2) 0.021I zz (slug-ft^2) 0.021I prop (slug-ft^2) 0.00012** value obtained from Allied Aerospace that contains the inertia of all of the rotating components.Frequency responses for on and off-axis are presented as Figure 3.9. These include theremoval of off-axis control contributions by using the CIFER tool MISOSA.- 35 -
Page 1 and 2: Comprehensive System Identification
Page 3 and 4: APROVAL PAGETITLE:AUTHOR:Comprehens
Page 5 and 6: ACKNOWLEDGMENTSThe author would lik
Page 7 and 8: 3.4.4 Magnetometer Identification..
Page 9 and 10: LIST OF FIGURESFigure 1.1 - Land Wa
Page 11 and 12: Figure 3.48 - Magnetometer Depictio
Page 13 and 14: CHAPTER 1 - INTRODUCTION AND MOTIVA
Page 15 and 16: The vehicles examined within the sc
Page 17 and 18: tunnel testing to study the charact
Page 19 and 20: Figure 1.8 - Helicopter Body Axes S
Page 21 and 22: GPSRate GyrosAccelerometersIMUInner
Page 23 and 24: CHAPTER 2 - METHODS AND TECHNIQUES2
Page 25 and 26: 2.2.1 Flight Test TechniquesThere a
Page 27 and 28: manufacturer specifications are mod
Page 29 and 30: 3.2 Bare-Airframe IDThe bare-airfra
Page 31 and 32: Table 3.2 - OAV Frequency Range of
Page 33 and 34: ⎧ p⎫⎪ ⎪y = ⎨q⎬⎪ r ⎪
Page 35 and 36: Table 3.4 - OAV DERIVID Identified
Page 37 and 38: The identified state-space model yi
Page 39 and 40: Better sensors, at higher sampling
Page 41 and 42: Figure 3.3 - Yaw response frequency
Page 43 and 44: Figure 3.4 shows that even though t
Page 45: It can be seen that the Aerovironme
Page 49 and 50: 30MAGNITUDE(DB)-10-50250PHASE(DEG)5
Page 51 and 52: A 0th/2nd order transfer function i
Page 53 and 54: Figure 3.12 shows the same for the
Page 55 and 56: Techsburg) the pitching moment resp
Page 57 and 58: Table 3.11 shows that all of the di
Page 59 and 60: Figure 3.14 shows how increasing th
Page 61 and 62: the duct, the effects of the man ne
Page 63 and 64: ft-lbMu PLATFORM= 5.11ftsecThis dim
Page 65 and 66: apparent that the size of the duct
Page 67 and 68: adequate way to characterize the di
Page 69 and 70: actuators varied in size, weight, c
Page 71 and 72: It is noticeable from the figure th
Page 73 and 74: Table 3.17 - Actuator Calibration F
Page 75 and 76: Figure 2.1 shows an example frequen
Page 77 and 78: The test matrix is provided as Tabl
Page 79 and 80: frequency response curves shown in
Page 81 and 82: Table 3.22 shows that for the first
Page 83 and 84: The time delays all seemed to be ar
Page 85 and 86: 400035003000250020001500y = -13429x
Page 87 and 88: higher data rates, and tighter tole
Page 89 and 90: esponse and the response obtained f
Page 91 and 92: The time histories show that the ou
Page 93 and 94: Figure 3.31 - Magnitude Comparison
Page 95 and 96: Performing the frequency response a
Page 97 and 98:
Results from STI utilizing the exac
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The fact that the rate saturated du
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Table 3.23 for the maximum rates an
Page 103 and 104:
Verification of the identified mode
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from testing (3.22), it was found t
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3.4.1 Accelerometer IdentificationM
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Figure 3.43 shows that gyros were m
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5 meter circle centered about the t
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Figure 3.46 shows the modeled fluct
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Figure 3.49 - Pressure Altimeter Mo
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Figure 4.1 - Simulink MAV ModelFigu
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Figure 4.3 - Simulink Sweep Generat
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cause a pitching moment to be exert
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Figure 4.6 - Cross Control Decoupli
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⎡ Lp Lq Lr Lu Lv Lw0 0 0⎤⎢MpM
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It can be seen right away that the
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Figure 4.8 shows that the coherence
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CHAPTER 5 - CONCLUSIONSThe need for
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6. Mettler, B., Tischler, M. B., an
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Appendix AOAV Proposal VehicleIdent
Page 137 and 138:
DS8417 - 5V- 125 -
Page 139 and 140:
HS512MG - 5V- 127 -
Page 141 and 142:
DS368 - 5V- 129 -
Page 143 and 144:
94091 - 5V- 131 -
Page 145 and 146:
CS-10BB - 5V- 133 -
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Appendix CActuator Generated Transf
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DS8417 - 100% - 5V- 137 -
Page 151 and 152:
DS8417 - 100% - 6V- 139 -
Page 153 and 154:
HS512MG - 100% - 5V- 141 -
Page 155 and 156:
HS512MG - 100% - 6V- 143 -
Page 157 and 158:
DS368 - 100% - 5V- 145 -
Page 159 and 160:
DS368 - 100% - 6V- 147 -
Page 161 and 162:
94091 - 80% - 5V- 149 -
Page 163 and 164:
94091 - 80% - 6V- 151 -
Page 165 and 166:
CS-10BB - 100% - 5V- 153 -
Page 167 and 168:
CS-10BB - 100% - 6V- 155 -
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Appendix DActuator Time Domain Veri
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94091 5V94091 6V- 159 -
Page 173 and 174:
DS368 5VDS368 6V- 161 -
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Comprehensive System Identification of Ducted Fan UAVs - Cal Poly

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