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Probabilistic Performance Analysis of Fault Diagnosis Schemes

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• Sample time: T s = 0.05s<br />

• Time horizon: N = 72,000 (i.e., N T s = 1hour)<br />

• Flight path angle: 0.5 ◦ (constant)<br />

• Airspeed: V = 45 m/s (constant)<br />

• Initial Altitude: h(0) = 200m<br />

• Noise standard deviations: σ t = 2.5Pa, σ s = 2.5Pa<br />

• Bias fault magnitudes: b t = −0.04kPa, b s = 0.05kPa<br />

• Continuous failure time models: λ t = λ s = 0.001hr −1 = 2.78 × 10 −7 s −1<br />

• Discrete failure time models: q t = q s = 1.389 × 10 −7<br />

• Filter pole: a = 0.003 (before discretization)<br />

• Threshold: ε = 2m<br />

The resulting performance metrics are plotted in Figures 6.3(a) and 6.3(b). Note that, in this<br />

case, the component failure rates are so small that the plots <strong>of</strong> {P fn,k } and {P tp,k } are barely<br />

distinguishable from zero.<br />

Next, we plot the roc curves as the threshold ε varies from 0.1 m to 50 m. The curves<br />

shown in Figure 6.4 correspond to times ranging from 1 minute to 1 hour. Note that, in<br />

Figure 6.3(b), the probability <strong>of</strong> detection {P d,k } dips at about 7 minutes. Hence, some <strong>of</strong> the<br />

roc curves in Figure 6.4 cross over one another. However, the general trend is that the roc<br />

curves pass closer to the ideal point (0,1) as time increases.<br />

For our third numerical experiment, we observe that the probability <strong>of</strong> detection, plotted<br />

in Figure 6.3(b), converges to a steady-state value. To better understand the effects <strong>of</strong><br />

changing the washout filter pole a and the noise standard deviation σ, we compute the<br />

steady-state values <strong>of</strong> {P d,k } as a and σ vary. In Table 6.1, these steady-state values are<br />

tabulated for a ranging from 0.0005 to 0.004 and σ ranging from 2Pa to 10Pa. Note that the<br />

value <strong>of</strong> a listed in Table 6.1 corresponds to the continuous-time washout filter W before<br />

discretization. Also, the same standard deviation σ is used for both noise signals, {v t,k }<br />

and {v s,k }. All other parameters remain the same as in the previous experiments.<br />

In our fourth experiment, we seek to find the worst-case flight path, with respect to<br />

the probability <strong>of</strong> false alarm. For these optimizations, we use the values a = 0.003 and<br />

σ t = σ s = 2.5Pa, as in the first two experiments. We assume that there is no disturbance w<br />

or model uncertainty ∆ affecting the system. The class <strong>of</strong> uncertain inputs considered is<br />

B 2 (u ◦ ,γ) = { ũ + u ◦ : ‖ũ‖ 2 < γ } ,<br />

where u ◦ = (V,h) is the flight path described in the first experiment. Since we only consider<br />

additive input faults, the conditional variance <strong>of</strong> the residual, {Σ k } does not depend on the<br />

fault parameter sequence θ or the uncertain input. Hence, we can fulfill Assumptions 1–3 <strong>of</strong><br />

105

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