系统工程与电子技术 ›› 2023, Vol. 45 ›› Issue (6): 1893-1901.doi: 10.12305/j.issn.1001-506X.2023.06.34
• 可靠性 • 上一篇
李犟, 吴和成, 朱晨
收稿日期:
2022-06-28
出版日期:
2023-05-25
发布日期:
2023-06-01
通讯作者:
李犟
作者简介:
李犟(1997—), 男, 博士研究生, 主要研究方向为可靠性理论Jiang LI, Hecheng WU, Chen ZHU
Received:
2022-06-28
Online:
2023-05-25
Published:
2023-06-01
Contact:
Jiang LI
摘要:
退化模型是评估长寿命产品可靠性的有效方法, 但已有参数退化模型忽略了退化量分布未知、最优退化量分布和退化量有界性等问题, 导致模型可靠性评估精度不足, 适用范围有限。针对已有方法的不足, 提出一种评估长寿命产品可靠性的半参数退化模型。首先, 通过考虑边界的非参数对数变换核密度估计方法拟合产品在各检测时刻的退化量分布; 然后, 基于退化量分布与寿命分布的关系, 利用最小二乘法与遗传算法估计产品寿命分布参数; 最后, GaAs激光器与合金钢的实例应用表明, 所构建模型能够更好地拟合退化数据, 可靠性评估精度更高。
中图分类号:
李犟, 吴和成, 朱晨. 基于半参数退化模型的长寿命产品可靠性评估[J]. 系统工程与电子技术, 2023, 45(6): 1893-1901.
Jiang LI, Hecheng WU, Chen ZHU. Reliability assessment of long-life products based on semi-parametric degradation model[J]. Systems Engineering and Electronics, 2023, 45(6): 1893-1901.
表1
GaAs激光器相对差异度结果"
t/h | logKDE | KDE | AKDE | 正态分布 | 对数正态分布 | 威布尔分布 | Gamma分布 |
250 | 0.344 | 0.587 | 0.504 | 0.515 | 0.392 | 0.557 | 0.409 |
500 | 0.273 | 0.469 | 0.456 | 0.435 | 0.288 | 0.453 | 0.340 |
750 | 0.336 | 0.459 | 0.432 | 0.488 | 0.355 | 0.524 | 0.397 |
1 000 | 0.436 | 0.619 | 0.564 | 0.746 | 0.615 | 0.772 | 0.659 |
1 250 | 0.325 | 0.500 | 0.490 | 0.486 | 0.354 | 0.525 | 0.395 |
1 500 | 0.375 | 0.489 | 0.479 | 0.585 | 0.482 | 0.610 | 0.526 |
1 750 | 0.344 | 0.546 | 0.539 | 0.525 | 0.403 | 0.571 | 0.443 |
2 000 | 0.360 | 0.490 | 0.455 | 0.558 | 0.435 | 0.589 | 0.477 |
2 250 | 0.268 | 0.448 | 0.427 | 0.437 | 0.375 | 0.418 | 0.415 |
2 500 | 0.269 | 0.426 | 0.405 | 0.539 | 0.438 | 0.547 | 0.481 |
2 750 | 0.327 | 0.500 | 0.443 | 0.634 | 0.526 | 0.656 | 0.567 |
3 000 | 0.344 | 0.515 | 0.460 | 0.648 | 0.538 | 0.671 | 0.580 |
3 250 | 0.341 | 0.525 | 0.478 | 0.681 | 0.575 | 0.701 | 0.617 |
3 500 | 0.257 | 0.501 | 0.479 | 0.597 | 0.480 | 0.622 | 0.522 |
3 750 | 0.316 | 0.502 | 0.463 | 0.650 | 0.541 | 0.668 | 0.583 |
4 000 | 0.370 | 0.580 | 0.504 | 0.728 | 0.608 | 0.755 | 0.649 |
表2
合金钢相对差异度结果"
旋转/次 | logKDE | KDE | AKDE | 正态分布 | 对数正态分布 | 威布尔分布 | Gamma分布 |
1×104 | 0.958 | 0.958 | 0.957 | 1.194 | 1.194 | 1.174 | 1.218 |
2×104 | 0.532 | 0.548 | 0.529 | 0.576 | 0.596 | 0.599 | 0.614 |
3×104 | 0.638 | 0.578 | 0.581 | 0.828 | 0.837 | 0.837 | 0.862 |
4×104 | 0.398 | 0.502 | 0.493 | 0.491 | 0.459 | 0.541 | 0.496 |
5×104 | 0.307 | 0.559 | 0.550 | 0.382 | 0.406 | 0.396 | 0.422 |
6×104 | 0.311 | 0.565 | 0.554 | 0.322 | 0.340 | 0.361 | 0.358 |
7×104 | 0.306 | 0.484 | 0.474 | 0.434 | 0.365 | 0.488 | 0.406 |
8×104 | 0.241 | 0.505 | 0.494 | 0.393 | 0.344 | 0.440 | 0.363 |
9×104 | 0.222 | 0.532 | 0.521 | 0.311 | 0.330 | 0.346 | 0.347 |
10×104 | 0.209 | 0.538 | 0.527 | 0.343 | 0.291 | 0.383 | 0.333 |
11×104 | 0.260 | 0.558 | 0.548 | 0.310 | 0.293 | 0.356 | 0.311 |
12×104 | 0.234 | 0.518 | 0.508 | 0.387 | 0.288 | 0.413 | 0.340 |
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