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Navigation Functionalities for an Autonomous UAV Helicopter

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3.4. THE AUGMENTED RMAX DYNAMIC MODEL 19<br />

3.4 The augmented RMAX dynamic model<br />

The RMAX helicopter model presented in this thesis includes the bare helicopter<br />

dynamics <strong>an</strong>d the YACS control system dynamics. The code of the<br />

YACS is strictly Yamaha proprietary so the approach used to build the relative<br />

mathematical model has been that of black-box model identification.<br />

With the use of this technique, it is possible to estimate the mathematical<br />

model of <strong>an</strong> unknown system (the only hypothesis about the system is that<br />

it has a linear behavior) just by observing its behavior. This is achieved in<br />

practice by sending <strong>an</strong> input signal to the system <strong>an</strong>d measuring its output.<br />

Once the input <strong>an</strong>d output signals are known there are several methods to<br />

identify the mathematical structure of the system.<br />

The YACS model identification is not part of this thesis <strong>an</strong>d details<br />

c<strong>an</strong> be found in [4]. In the following section the tr<strong>an</strong>sfer functions of the<br />

augmented attitude dynamics will be given. These tr<strong>an</strong>sfer functions will<br />

be used to build the augmented RMAX helicopter dynamic model used in<br />

the simulator.<br />

3.4.1 Augmented helicopter attitude dynamics<br />

As previously stated the YACS <strong>an</strong>d helicopter attitude dynamics have been<br />

identified through black-box model identification.<br />

The equations 3.3 represent the four input/output tr<strong>an</strong>sfer functions in<br />

the Laplace domain:<br />

∆Φ =<br />

∆Θ =<br />

∆R =<br />

∆AZ =<br />

2.3(s 2 + 3.87s + 53.3)<br />

(s 2 + 6.29s + 16.2)(s 2 + 8.97s + 168) ∆AIL<br />

0.5(s 2 + 9.76s + 75.5)<br />

(s 2 + 3s + 5.55)(s 2 + 2.06s + 123.5)<br />

9.7(s + 12.25)<br />

(s + 4.17)(s2 + 3.5s + 213.4) ∆RUD<br />

0.0828s(s + 3.37)<br />

(s + 0.95)(s2 ∆T HR<br />

+ 13.1s + 214.1)<br />

∆ELE (3.3)<br />

where ∆Φ <strong>an</strong>d ∆Θ are the roll <strong>an</strong>d pitch <strong>an</strong>gle increments (deg), ∆R

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