<p>We consider the <i>k</i>-out-of-<i>n</i> system which is subject to a new version of mixed <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42519_2025_455_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation>-shock models as a combination of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42519_2025_455_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>δ</mi> </math></EquationSource> </InlineEquation>-shock and extreme shock which occur randomly. In this mixed shock model, the system fails: first, when <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42519_2025_455_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\ell \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ℓ</mi> </math></EquationSource> </InlineEquation> interarrival times between two successive shocks with magnitude larger than the critical threshold <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42519_2025_455_Article_IEq6.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>γ</mi> </math></EquationSource> </InlineEquation> are in <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42519_2025_455_Article_IEq7.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="106" /> </InlineMediaObject> <EquationSource Format="TEX">\(\left[ \delta _1, \delta _2\right] , \delta _1 &lt; \delta _2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfenced close="]" open="["> <msub> <mi>δ</mi> <mn>1</mn> </msub> <mo>,</mo> <msub> <mi>δ</mi> <mn>2</mn> </msub> </mfenced> <mo>,</mo> <msub> <mi>δ</mi> <mn>1</mn> </msub> <mo>&lt;</mo> <msub> <mi>δ</mi> <mn>2</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>; second, the first interarrival time between two successive shocks is less than <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="42519_2025_455_Article_IEq8.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\delta _1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>δ</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>. We derive various mathematical properties of the new model, including hazard rate functions, moment properties, mean deviations, mean residual life, expected inactive time, Lorenz, Bonferroni and Zenga curves, stress strength probability and geometric mean. We also discuss maximum likelihood estimation of the parameters of the model.</p>

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Reliability Properties of k-out-of-n System Based on a New Mixed \(\delta \)-shock Model

  • Rasool Roozegar,
  • Saralees Nadarajah,
  • Marjan Entezari

摘要

We consider the k-out-of-n system which is subject to a new version of mixed \(\delta \) δ -shock models as a combination of \(\delta \) δ -shock and extreme shock which occur randomly. In this mixed shock model, the system fails: first, when \(\ell \) interarrival times between two successive shocks with magnitude larger than the critical threshold \(\gamma \) γ are in \(\left[ \delta _1, \delta _2\right] , \delta _1 < \delta _2\) δ 1 , δ 2 , δ 1 < δ 2 ; second, the first interarrival time between two successive shocks is less than \(\delta _1\) δ 1 . We derive various mathematical properties of the new model, including hazard rate functions, moment properties, mean deviations, mean residual life, expected inactive time, Lorenz, Bonferroni and Zenga curves, stress strength probability and geometric mean. We also discuss maximum likelihood estimation of the parameters of the model.