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Chapter 5 Robust Performance Tailoring with Tuning - SSL - MIT

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Multiple Model<br />

The multiple model RPT optimization is run on the SCI sample problem using both<br />

SA, SQP and MC SQP algorithms. The optimization performance metrics and re-<br />

sulting designs are listed in Table 3.4. The optimal costs listed in the table are much<br />

Table 3.4: Algorithm performance: multiple model, βi =1/npv.<br />

J ∗ iter fevals time x ∗ [m] x ∗ [kg]<br />

Alg. [µm] # # [min] d1 d2 m1 m2<br />

SA 273.51 64 2059 12.79 0.0440 0.0515 0.8464 19.5131<br />

SQP 271.78 20 48 3.83 0.0432 0.0529 0.0 22.613<br />

MC SQP 271.78 238 545 41.06 0.0432 0.0529 0.0 22.613<br />

lower than those of the AO designs (Table 3.3), since the multiple model objective<br />

is the weighted sum of the performance values at each of the uncertainty vertices,<br />

and not the worst-case performance. In the results presented here the weighting βi<br />

is the same at each vertex and equals 1/npv, so that the cost is the average of the<br />

performance values at the uncertainty vertices.<br />

The SQP and SA designs are nearly equivalent as the SA cost is only 0.6% higher<br />

than SQP. The individual runs in the MC SQP algorithm result in a few different<br />

optimal solutions <strong>with</strong> slight variations in the diameter of the inner array segments<br />

and the design mass values. All designs, however, are at the maximum mass con-<br />

straint, and the best design is found <strong>with</strong> either MC SQP or the combination of SA<br />

and SQP. As seen previously <strong>with</strong> AO, using SA in conjunction <strong>with</strong> SQP finds the<br />

global optimum much more quickly (16.62 minutes) than performing ten randomly<br />

started MC SQP searches (41.06 minutes). The optimal cross-sectional diameters are<br />

similar to those in the anti-optimization designs, in that the diameters of the inner<br />

truss segments are larger than those of the outer segments. However, the MM design<br />

has 22 kg of design mass on the positive-x arm of the interferometer while the AO<br />

design has no lumped mass at all.<br />

90

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