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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 />

45

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