CIFER®-MATLAB Interfaces: Development and ... - Cal Poly
CIFER®-MATLAB Interfaces: Development and ... - Cal Poly
CIFER®-MATLAB Interfaces: Development and ... - Cal Poly
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Figure 4.14: Roll Angle to Rate Comparison<br />
Figure 4.15: Pitch Angle to Rate Comparison<br />
The next check using the simulation data was performed for Equations 4.6 through 4.8.<br />
Frequency response arithmetic was used to combine the on-axis responses of rates <strong>and</strong> attitudes to<br />
calculate the velocity perturbations in the frequency domain from the appropriate frequency<br />
responses. These were compared to the corresponding velocity perturbation responses that were<br />
initially reconstructed in the FRESPID program using the same math on the time history data.<br />
Equation 4.11 shows an example of how the frequency responses were combined using<br />
arithmetic.<br />
u<br />
δ<br />
ele<br />
=<br />
a<br />
δ<br />
x<br />
ele<br />
1 q<br />
− g<br />
s δ<br />
ele<br />
[4.11]<br />
These comparisons are shown in Figure 4.16 through Figure 4.18 using a forward velocity of 65<br />
knots. Both methods of calculation overlay nearly precisely, which makes sense as both plots are<br />
based on the same data, one created straight from the time domain <strong>and</strong> one built through<br />
frequency response arithmetic. Even in regions of low coherence, both calculations include the<br />
same errors <strong>and</strong> thus arrive at the same answers. The coherence plots vary due to a convention in<br />
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