| Literature DB >> 30137725 |
Shujun Lian1, Nana Niu1.
Abstract
For inequality constrained optimization problem, we first propose a new smoothing method to the lower order exact penalty function, and then show that an approximate global solution of the original problem can be obtained by solving a global solution of a smooth lower order exact penalty problem. We propose an algorithm based on the smoothed lower order exact penalty function. The global convergence of the algorithm is proved under some mild conditions. Some numerical experiments show the efficiency of the proposed method.Entities:
Keywords: Exact penalty function; Inequality constrained optimization; Lower order penalty function; Smoothing method
Year: 2018 PMID: 30137725 PMCID: PMC5996064 DOI: 10.1186/s13660-018-1723-x
Source DB: PubMed Journal: J Inequal Appl ISSN: 1025-5834 Impact factor: 2.491
Figure 1The behavior of and
Numerical results for Example 4.1 with
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| 0 | (0.185009,0.804369,2.015460,−0.952409) | 1 | 0.01 | −4.797079 | −0.00109 | −2.028111 | −44.225926 |
| 1 | (0.169902,0.835670,2.008151,−0.965196) | 2 | 0.0001 | −9.748052 | −9.337847 | −1.883271 | −44.231252 |
Numerical results for Example 4.1 with
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| 0 | (0.169693,0.835634,2.008291,−0.965082) | 1 | 0.01 | −9.502428 | −8.676884 | −1.883244 | −44.231403 |
Numerical results for Example 4.1 with
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| 0 | (0.169691,0.835633,2.008294,−0.965080) | 1 | 0.01 | −9.502279 | −8.676796 | −1.883249 | −44.231403 |
Numerical results for Example 4.2 with
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| 0 | (3.4217,2.7082) | 2 | 0.001 | 4.1300 | −0.0053 | −15.2492 |
| 1 | (0.8022,1.1978) | 20 | 0.000001 | 0.0000 | −0.4066 | −7.1999 |
Numerical results for Example 4.2 with
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| 0 | (4.0607,3.0227) | 2 | 0.001 | 5.0834 | −0.0153 | −16.0434 |
| 1 | (0.8027,1.1971) | 20 | 0.000001 | −0.0003 | −0.4086 | −7.1992 |
Numerical results for Example 4.2 with
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| 0 | (2.6356,2.3168) | 2 | 0.001 | 2.9523 | −0.0020 | −13.7027 |
| 1 | (0.8005,1.1995) | 20 | 0.000001 | 0.0000 | −0.4015 | −7.2000 |
Numerical results for Example 4.3 with
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| 0 | (2.329795,3.133729) | 5 | 10−2 | −0.047009 | −0.043471 | −5.463524 |
| 1 | (2.329238,3.173320) | 10 | 10−4 | −0.002868 | −0.006501 | −5.502557 |
| 2 | (2.329452,3.177637) | 20 | 10−6 | −0.000302 | −0.001176 | −5.507089 |
| 3 | (2.329626,3.177558) | 40 | 10−8 | −0.001802 | −0.000436 | −5.507185 |
Numerical results for Example 4.3 with
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| 0 | (2.330261,3.061875) | 5 | 10−1 | −0.1226776 | −0.1131323 | −5.392137 |
| 1 | (2.329664,3.161611) | 15 | 10−2 | −0.018055 | −0.016207 | −5.491275 |
| 2 | (2.329639,3.171941) | 45 | 10−3 | −0.007524 | −0.005993 | −5.501580 |
| 3 | (2.329560,3.177804) | 135 | 10−4 | −0.001013 | −0.000503 | −5.507363 |
| 4 | (2.329593,3.177793) | 405 | 10−5 | −0.001297 | −0.000357 | −5.507386 |
| 5 | (2.329622,3.177781) | 1215 | 10−6 | −0.001544 | −0.000234 | −5.507403 |
Numerical results for Example 4.3 with
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| 0 | (2.330460,3.179900) | 2 | 10−5 | −0.006287 | 0.005832 | −5.510360 |
| 1 | (2.329672,3.179735) | 20 | 10−8 | −0.000001 | 0.001957 | −5.509408 |
| 2 | (2.329672,3.179735) | 200 | 10−11 | −0.000000 | 0.001957 | −5.509407 |
| 3 | (2.329541,3.178391) | 2000 | 10−14 | −0.000000 | −0.000000 | −5.507933 |