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Online proceedings - EDA Publishing Association

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100%<br />

0.1%<br />

1e-04%<br />

1e-07%<br />

1e-10%<br />

1e-13%<br />

10 -2 10 0 10 2 10 4 10 6<br />

Frequency (Hz)<br />

Fig. 2. Progress of the AMPXT error indicator<br />

0.01%<br />

1e-04%<br />

1e-06%<br />

err for H(s)<br />

1e-08%<br />

err for H (s) E<br />

err for H (s) θ<br />

1e-10%<br />

10 2 10 3 10 4 10 5 10 6<br />

Frequency (Hz)<br />

11-13 <br />

May 2011, Aix-en-Provence, France<br />

<br />

TABLE III<br />

RUNTIMES AND MAXIMUM RELATIVE ERRORS FOR PARAMETER SWEEP<br />

Fig. 3. Maximum relative errors of nominal ROM transfer function and<br />

Maximum relative error for parameter sweep w.r.t. 0.08%<br />

sensitivities according to (16)<br />

dimension of 72. Using the FOM reference solutions, we neighborhood of the nominal value.<br />

computed the exact relative errors of the ROM transfer For PMORinterp, a parameter sweep for the magnitude and<br />

function and its sensitivities w.r.t. and shown in phase of the ROM transfer function is plotted for selected<br />

Figure 3. The plots have a maximum of 0.06% and thus input-output-pairs in Figures 5 and 6. Compared to ,<br />

clearly demonstrate that the error indicator must not be clearly affects a broader portion of the frequency range.<br />

misinterpreted as an error bound, but is sufficient to monitor<br />

V. CONCLUSIONS AND OUTLOOK<br />

the convergence of ROM.<br />

In summary, the computation of 500 frequency samples of In this paper we presented an extension of existing MOR<br />

the transfer function and its sensitivities w.r.t. and takes methods for rapid and accurate computation of the frequency<br />

roughly 51 minutes for the FOM opposed to a total of 75 response and its sensitivities w.r.t. arbitrary parameters for<br />

seconds for generating and evaluating the parametric ROMs large scale finite element models. Optimization tasks with an<br />

with PMORnom. Hence, we obtained a speedup factor of objective function dependent on the transfer function will<br />

40.6.<br />

greatly benefit from the obtained speedup factor of more than<br />

For parameter sweeps, the speedup through model order 40.<br />

reduction is even more extreme. We considered an increment The lack of tools for the generation of parameter dependent<br />

of m for the suspension beam thickness , such that 21 full order models has been overcome with a system<br />

parameter values are obtained in the interval of m.<br />

interpolation approach that proved to be practical. For the<br />

sake of simplicity, we focused on interpolation of a single<br />

This results in a variation of rougly w.r.t the nominal<br />

parameter at a time, but the method can be easily extended to<br />

value of . For the Young’s modulus we considered 21<br />

multivariate polynomial interpolation involving cross terms<br />

parameter values in the interval of<br />

GPa, yielding<br />

for the interpolation polynomial. However, the more<br />

a variation of w.r.t the nominal value of . This sums parameters are involved, the more expensive the<br />

up to 41 distinct transfer function evaluations for 500<br />

10%<br />

frequency points each.<br />

Table III lists the corresponding runtimes, speedup factors, 1%<br />

and the maximum relative transfer function errors as defined<br />

in (16) taken over all 500 frequency points for all 41<br />

0.1%<br />

parameter values. Note that we did not use interpolated 0.01%<br />

parametric FOMs for the computation of the full order transfer<br />

0.001%<br />

functions which would have increased computation time even<br />

130 140 150 160 170 180 190<br />

further. Instead, we generated 41 single FOMs for fixed<br />

E (GPa)<br />

PMORnom<br />

parameter values and the time to generate these FOMs and<br />

PMORinterp<br />

export them to MATLAB ®<br />

0.001%<br />

was not accounted for the time<br />

10%<br />

measurements.<br />

1%<br />

Figure 4 shows a parameter dependent comparison of the<br />

0.1%<br />

maximum transfer function errors obtained with method<br />

PMORnom and PMORinterp over the frequency range of<br />

0.01%<br />

0.001%<br />

interest. Clearly, PMORinterp provides an accurate<br />

2.8 3 3.2<br />

approximation of the transfer function over the whole<br />

θ (µ m)<br />

3.4 3.6 3.8<br />

parameter range while PMORnom is only accurate in the Fig. 4. Maximum relative transfer function errors for parameter sweep<br />

FOM<br />

PMORnom<br />

PMORinterp<br />

Total costs for transfer function parameter sweep for 500<br />

frequency points and 41 parameter values<br />

25.1h<br />

Total costs for generation of param. ROMs w.r.t. and 74.9s<br />

Total costs for parameter sweep w.r.t. and 27.2s<br />

Speedup factor for parameter sweep<br />

885x<br />

Maximum relative error for parameter sweep w.r.t. 1.07%<br />

Maximum relative error for parameter sweep w.r.t. 78.93%<br />

Total costs for generation of parametric ROM w.r.t. 156.2s<br />

Total costs for generation of parametric ROM w.r.t. 371.8s<br />

Total costs for parameter sweep w.r.t. and 27.6s<br />

Speedup factor for parameter sweep<br />

163x<br />

Maximum relative error for parameter sweep w.r.t. 0.84%<br />

70

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