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{{ | {{Template:RGA_BOOK|Appendix D|Crow Extended Confidence Bounds}} | ||
In this appendix, we will present the two methods used in the RGA software to estimate the confidence bounds for the [[Crow Extended]] model when applied to developmental testing data. The Fisher Matrix approach is based on the Fisher Information Matrix and is commonly employed in the reliability field. The Crow bounds were developed by Dr. Larry Crow. | In this appendix, we will present the two methods used in the RGA software to estimate the confidence bounds for the [[Crow Extended|Crow extended]] model when applied to developmental testing data. The Fisher Matrix approach is based on the Fisher Information Matrix and is commonly employed in the reliability field. The Crow bounds were developed by Dr. Larry Crow. | ||
===Bounds on Demonstrated Failure Intensity=== | ===Bounds on Demonstrated Failure Intensity=== <!-- THIS SECTION HEADER IS LINKED FROM: Crow Extended and several sections on this page. IF YOU RENAME THE SECTION, YOU MUST UPDATE THE LINK(S). --> | ||
====Fisher Matrix Bounds==== | ====Fisher Matrix Bounds==== | ||
If there are no BC failure modes, the demonstrated failure intensity is | If there are no BC failure modes, the demonstrated failure intensity is | ||
:<math>{{\widehat{\lambda }}_{D}}(T)=\tfrac{{{N}_{A}}+{{N}_{BD}}}{T}\,\!</math>. | |||
: | Thus: | ||
< | :<math>Var({{\hat{\lambda }}_{D}}(t))=\frac{{{N}_{A}}}{{{T}^{2}}}+\frac{{{N}_{BD}}}{{{T}^{2}}}=\frac{{{\lambda }_{D}}(t)}{T}\,\!</math> | ||
: | and: | ||
:<math>\sqrt{T}\left( \frac{{{{\hat{\lambda }}}_{D}}(T)-{{\lambda }_{D}}(T)}{\sqrt{{{\lambda }_{D}}(T)}} \right)\sim N(0,1)\,\!</math> | |||
:<math>{{\lambda }_{D}}(T)={{\hat{\lambda }}_{D}}(T)+\frac{{{C}^{2}}}{2}\pm \sqrt{{{{\hat{\lambda }}}_{D}}(T){{C}^{2}}+\frac{{{C}^{4}}}{4}}\,\!</math> | |||
where | where <math>C=\tfrac{{{z}_{1-\alpha /2}}}{\sqrt{T}}\,\!</math>. | ||
If there are BC failure modes, the demonstrated failure intensity, <math>{{\widehat{\lambda }}_{D}}(T)={{\widehat{\lambda }}_{CA}}\,\!</math>, is actually the instantaneous failure intensity based on all of the data. <math>{{\lambda }_{CA}}(T)\,\!</math> must be positive; thus, <math>\ln {{\lambda }_{CA}}(T)\,\!</math> is approximately treated as being normally distributed. | |||
:<math>\frac{\ln {{{\hat{\lambda }}}_{CA}}(T)-\ln {{\lambda }_{CA}}(T)}{\sqrt{Var(\ln {{{\hat{\lambda }}}_{CA}}(T)})}\sim N(0,1)\,\!</math> | |||
The approximate confidence bounds on the instantaneous failure intensity are then estimated from: | The approximate confidence bounds on the instantaneous failure intensity are then estimated from: | ||
:<math>CB={{\hat{\lambda }}_{CA}}(T){{e}^{\pm {{z}_{\alpha }}\sqrt{Var({{{\hat{\lambda }}}_{CA}}(T))}/{{{\hat{\lambda }}}_{CA}}(T)}}\,\!</math> | |||
where <math>{{\lambda }_{CA}}(t)=\lambda \beta {{T}^{\beta -1}}\,\!</math>. | |||
:<math>\begin{align} | |||
Var({{{\hat{\lambda }}}_{CA}}(T))= & {{\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \beta } \right)}^{2}}Var(\hat{\beta })+{{\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \lambda } \right)}^{2}}Var(\hat{\lambda }) \\ | |||
& +2\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \beta } \right)\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \lambda } \right)cov(\hat{\beta },\hat{\lambda }) | |||
\end{align}\,\!</math> | |||
The variance calculation is the same as described in the [[Crow-AMSAA Confidence Bounds]] appendix. | |||
====Crow Bounds==== | ====Crow Bounds==== | ||
If there are no BC failure modes then: | If there are no BC failure modes then: | ||
:<math>\begin{align} | |||
{{[{{\lambda }_{D}}(T)]}_{l}}= & {{\widehat{\lambda }}_{D}}(T)\frac{\chi _{(2N,1-\alpha /2)}^{2}}{2N} \\ | |||
{{[{{\lambda }_{D}}(T)]}_{u}}= & {{\widehat{\lambda }}_{D}}(T)\frac{\chi _{(2N,\alpha /2)}^{2}}{2N} | |||
\end{align}\,\!</math> | |||
where <math>{{\widehat{\lambda }}_{D}}(T)={{\widehat{\lambda }}_{CA}}\,\!</math>. | |||
If there are BC modes then the confidence bounds on the demonstrated failure intensity are calculated as presented in the [[Crow-AMSAA Confidence Bounds]] appendix. | |||
If there are BC modes then the confidence bounds on the demonstrated failure intensity are calculated as presented in | |||
===Bounds on Demonstrated MTBF=== <!-- THIS SECTION HEADER IS LINKED FROM: Crow Extended. IF YOU RENAME THE SECTION, YOU MUST UPDATE THE LINK(S). --> | |||
===Bounds on Demonstrated MTBF=== | |||
====Fisher Matrix Bounds==== | ====Fisher Matrix Bounds==== | ||
:<math>\begin{align} | |||
& MTB{{F}_{{{D}_{L}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{U}}} \\ | & MTB{{F}_{{{D}_{L}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{U}}} \\ | ||
& MTB{{F}_{{{D}_{U}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{L}}} | & MTB{{F}_{{{D}_{U}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{L}}} | ||
\end{align}</math> | \end{align}\,\!</math> | ||
where <math>{{[{{\lambda }_{D}}(T)]}_{L}}\,\!</math> and <math>{{[{{\lambda }_{D}}(T)]}_{U}}\,\!</math> can be obtained from the equation given above for [[Crow_Extended_Confidence_Bounds#Bounds_on_Demonstrated_Failure_Intensity|Bounds on Demonstrated Failure Intensity]]. | |||
====Crow Bounds==== | ====Crow Bounds==== | ||
:<math>\begin{align} | |||
MTB{{F}_{{{D}_{L}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{U}}} \\ | |||
MTB{{F}_{{{D}_{U}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{L}}} | |||
\end{align}</math> | \end{align}\,\!</math> | ||
where <math>{{[{{\lambda }_{D}}(T)]}_{L}}\,\!</math> and <math>{{[{{\lambda }_{D}}(T)]}_{U}}\,\!</math> can be obtained from the equation given above for [[Crow_Extended_Confidence_Bounds#Bounds_on_Demonstrated_Failure_Intensity|Bounds on Demonstrated Failure Intensity]]. | |||
===Bounds on Projected Failure Intensity===<!-- THIS SECTION HEADER IS LINKED FROM: Crow Extended. IF YOU RENAME THE SECTION, YOU MUST UPDATE THE LINK(S). --> | |||
===Bounds on Projected Failure Intensity=== | |||
====Fisher Matrix Bounds==== | ====Fisher Matrix Bounds==== | ||
The projected failure intensity | The projected failure intensity <math>{{\lambda }_{P}}(T)\,\!</math> must be positive; thus, <math>\ln {{\lambda }_{P}}(T)\,\!</math> is approximately treated as being normally distributed as well: | ||
:<math>\frac{\ln {{{\hat{\lambda }}}_{P}}(T)-\ln {{\lambda }_{P}}(t)}{\sqrt{Var(\ln {{{\hat{\lambda }}}_{P}}(T)})}\sim N(0,1)\,\!</math> | |||
:<math>CB={{\hat{\lambda }}_{P}}(T){{e}^{\pm {{z}_{\alpha }}\sqrt{Var({{{\hat{\lambda }}}_{P}}(T))}/{{{\hat{\lambda }}}_{P}}(T)}}\,\!</math> | |||
where: | |||
: | :* <math>{{\hat{\lambda }}_{P}}(T)=\tfrac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T}+\overline{d}\tfrac{M}{T}\bar{\beta }\,\!</math> when there are no BC modes. | ||
:* <math>{{\hat{\lambda }}_{P}}(T)={{\widehat{\lambda }}_{EM}}={{\widehat{\lambda }}_{CA}}-{{\widehat{\lambda }}_{BD}}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T}+\overline{d}\widehat{h}(T|BD)\,\!</math> when there are BC modes. | |||
:* <math>{{N}_{i}}\,\!</math> is the total failure number of the <math>{{i}^{th}}\,\!</math> distinct BD mode. | |||
You can then get: | You can then get: | ||
:<math>Var({{\lambda }_{P}}(T))\approx Var({{\hat{\gamma }}_{GP}})+\mu _{d}^{2}Var(h(T))\approx \frac{{{{\hat{r}}}_{GP}}}{T}+\mu _{d}^{2}Var(h(T))\,\!</math> | |||
where: | |||
:<math>\begin{align} | |||
\hat{h}(T)= & \frac{M}{T}\bar{\beta } \\ | |||
Var(\hat{h}(T))= & {{(\frac{M}{T})}^{2}}Var(\bar{\beta })={{(\frac{M}{T})}^{2}}{{(\frac{M}{M-1})}^{2}}Var(\hat{\beta })=\frac{{{M}^{4}}}{{{T}^{2}}{{(M-1)}^{2}}}Var(\hat{\beta }) | |||
\end{align}</math> | \end{align}\,\!</math> | ||
The | The <math>Var(\hat{\beta })\,\!</math> can be obtained from Fisher Matrix based on <math>M\,\!</math> distinct BD modes. | ||
====Crow Bounds==== | ====Crow Bounds==== | ||
:<math>\begin{align} | |||
{{[{{\lambda }_{P}}(T)]}_{L}}= & {{{\hat{\lambda }}}_{P}}(T)+\frac{{{C}^{2}}}{2}-\sqrt{{{{\hat{\lambda }}}_{P}}(T)\cdot {{C}^{2}}+\frac{{{C}^{4}}}{4}} \\ | |||
{{[{{\lambda }_{P}}(T)]}_{U}}= & {{{\hat{\lambda }}}_{P}}(T)+\frac{{{C}^{2}}}{2}+\sqrt{{{{\hat{\lambda }}}_{P}}(T)\cdot \ \,{{C}^{2}}+\frac{{{C}^{4}}}{4}} | |||
\end{align}</math> | \end{align}\,\!</math> | ||
where <math>C=\tfrac{{{z}_{1-\alpha /2}}}{\sqrt{T}}\,\!</math>. | |||
===Bounds on Projected MTBF===<!-- THIS SECTION HEADER IS LINKED FROM: Crow Extended. IF YOU RENAME THE SECTION, YOU MUST UPDATE THE LINK(S). --> | |||
====Fisher Matrix Bounds==== | |||
:<math>\begin{align} | |||
MTB{{F}_{{{P}_{L}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{U}}} \\ | |||
MTB{{F}_{{{P}_{U}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{L}}} | |||
\end{align}\,\!</math> | |||
<math>{{[{{\lambda }_{P}}(T)]}_{U}}\,\!</math> and <math>{{[{{\lambda }_{P}}(T)]}_{L}}\,\!</math> can be obtained from the equation given above for [[Crow_Extended_Confidence_Bounds#Bounds_on_Projected_Failure_Intensity|Bounds on Projected Failure Intensity]]. | |||
===Bounds on Projected | ====Crow Bounds==== | ||
:<math>\begin{align} | |||
MTB{{F}_{{{P}_{L}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{U}}} \\ | |||
MTB{{F}_{{{P}_{U}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{L}}} | |||
\end{align}\,\!</math> | |||
<math>{{[{{\lambda }_{P}}(T)]}_{U}}\,\!</math> and <math>{{[{{\lambda }_{P}}(T)]}_{L}}\,\!</math> can be obtained from the equation given above for [[Crow_Extended_Confidence_Bounds#Bounds_on_Projected_Failure_Intensity|Bounds on Projected Failure Intensity]]. | |||
===Bounds on Growth Potential Failure Intensity===<!-- THIS SECTION HEADER IS LINKED FROM: Crow Extended and another section on this page. IF YOU RENAME THE SECTION, YOU MUST UPDATE THE LINK(S). --> | |||
====Fisher Matrix Bounds==== | ====Fisher Matrix Bounds==== | ||
If there are no BC failure modes, the growth potential failure intensity is | |||
<math> | :<math>{{\widehat{r}}_{GP}}(T)=\tfrac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T}\,\!</math>. | ||
= | |||
\ | |||
Then: | |||
: | :<math>\begin{align} | ||
Var({{\widehat{r}}_{GP}})= & \frac{1}{T}\left[ \frac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop \sum }}\,{{(1-{{d}_{i}})}^{2}}\frac{{{N}_{i}}}{T} \right] \\ | |||
\le & \frac{1}{T}\left[ \frac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop \sum }}\,(1-{{d}_{i}})\frac{{{N}_{i}}}{T} \right] \\ | |||
= & \frac{{{r}_{GP}}}{T} | |||
\end{align}\,\!</math> | |||
If there are BC failure modes, the growth potential failure intensity is | |||
:<math>{{\widehat{r}}_{GP}}(T)={{\widehat{\lambda }}_{CA}}-{{\widehat{\lambda }}_{BD}}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T},\,\!</math> <math>Var({{\widehat{r}}_{GP}})\approx \tfrac{{{r}_{GP}}}{T}\,\!</math>. | |||
: | Therefore: | ||
:<math>\sqrt{T}\left( \frac{{{{\hat{r}}}_{GP}}-{{r}_{GP}}}{\sqrt{{{r}_{GP}}}} \right)\sim N(0,1)\,\!</math> | |||
The confidence bounds on the growth potential failure intensity are as follows: | The confidence bounds on the growth potential failure intensity are as follows: | ||
:<math>\begin{align} | |||
{{r}_{L}}= & {{{\hat{r}}}_{GP}}+\frac{{{C}^{2}}}{2}-\sqrt{{{{\hat{r}}}_{GP}}\,{{C}^{2}}+\frac{{{C}^{4}}}{4}} \\ | |||
{{r}_{U}}= & {{{\hat{r}}}_{GP}}+\frac{{{C}^{2}}}{2}+\sqrt{{{{\hat{r}}}_{GP}}\,{{C}^{2}}+\frac{{{C}^{4}}}{4}} | |||
\end{align}</math> | \end{align}\,\!</math> | ||
where | where <math>C=\tfrac{{{z}_{1-\alpha /2}}}{\sqrt{T}}\,\!</math>. | ||
====Crow Bounds==== | ====Crow Bounds==== | ||
The Crow bounds for the growth potential failure intensity are the same as the Fisher Matrix bounds. | The Crow bounds for the growth potential failure intensity are the same as the Fisher Matrix bounds. | ||
===Bounds on Growth Potential MTBF===<!-- THIS SECTION HEADER IS LINKED FROM: Crow Extended. IF YOU RENAME THE SECTION, YOU MUST UPDATE THE LINK(S). --> | |||
====Fisher Matrix Bounds==== | |||
:<math>\begin{align} | |||
MTB{{F}_{G{{P}_{L}}}}= & \frac{1}{{{r}_{U}}} \\ | |||
MTB{{F}_{G{{P}_{U}}}}= & \frac{1}{{{r}_{L}}} | |||
\end{align}\,\!</math> | |||
where <math>{{r}_{U}}\,\!</math> and <math>{{r}_{L}}\,\!</math> can be obtained from the equation given above for [[Crow_Extended_Confidence_Bounds#Bounds_on_Growth_Potential_Failure_Intensity|Bounds on Growth Potential Failure Intensity]]. | |||
====Crow Bounds==== | ====Crow Bounds==== | ||
The Crow bounds for the growth potential MTBF are the same as the Fisher Matrix bounds. | The Crow bounds for the growth potential MTBF are the same as the Fisher Matrix bounds. |
Latest revision as of 20:41, 18 September 2023
In this appendix, we will present the two methods used in the RGA software to estimate the confidence bounds for the Crow extended model when applied to developmental testing data. The Fisher Matrix approach is based on the Fisher Information Matrix and is commonly employed in the reliability field. The Crow bounds were developed by Dr. Larry Crow.
Bounds on Demonstrated Failure Intensity
Fisher Matrix Bounds
If there are no BC failure modes, the demonstrated failure intensity is
- [math]\displaystyle{ {{\widehat{\lambda }}_{D}}(T)=\tfrac{{{N}_{A}}+{{N}_{BD}}}{T}\,\! }[/math].
Thus:
- [math]\displaystyle{ Var({{\hat{\lambda }}_{D}}(t))=\frac{{{N}_{A}}}{{{T}^{2}}}+\frac{{{N}_{BD}}}{{{T}^{2}}}=\frac{{{\lambda }_{D}}(t)}{T}\,\! }[/math]
and:
- [math]\displaystyle{ \sqrt{T}\left( \frac{{{{\hat{\lambda }}}_{D}}(T)-{{\lambda }_{D}}(T)}{\sqrt{{{\lambda }_{D}}(T)}} \right)\sim N(0,1)\,\! }[/math]
- [math]\displaystyle{ {{\lambda }_{D}}(T)={{\hat{\lambda }}_{D}}(T)+\frac{{{C}^{2}}}{2}\pm \sqrt{{{{\hat{\lambda }}}_{D}}(T){{C}^{2}}+\frac{{{C}^{4}}}{4}}\,\! }[/math]
where [math]\displaystyle{ C=\tfrac{{{z}_{1-\alpha /2}}}{\sqrt{T}}\,\! }[/math].
If there are BC failure modes, the demonstrated failure intensity, [math]\displaystyle{ {{\widehat{\lambda }}_{D}}(T)={{\widehat{\lambda }}_{CA}}\,\! }[/math], is actually the instantaneous failure intensity based on all of the data. [math]\displaystyle{ {{\lambda }_{CA}}(T)\,\! }[/math] must be positive; thus, [math]\displaystyle{ \ln {{\lambda }_{CA}}(T)\,\! }[/math] is approximately treated as being normally distributed.
- [math]\displaystyle{ \frac{\ln {{{\hat{\lambda }}}_{CA}}(T)-\ln {{\lambda }_{CA}}(T)}{\sqrt{Var(\ln {{{\hat{\lambda }}}_{CA}}(T)})}\sim N(0,1)\,\! }[/math]
The approximate confidence bounds on the instantaneous failure intensity are then estimated from:
- [math]\displaystyle{ CB={{\hat{\lambda }}_{CA}}(T){{e}^{\pm {{z}_{\alpha }}\sqrt{Var({{{\hat{\lambda }}}_{CA}}(T))}/{{{\hat{\lambda }}}_{CA}}(T)}}\,\! }[/math]
where [math]\displaystyle{ {{\lambda }_{CA}}(t)=\lambda \beta {{T}^{\beta -1}}\,\! }[/math].
- [math]\displaystyle{ \begin{align} Var({{{\hat{\lambda }}}_{CA}}(T))= & {{\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \beta } \right)}^{2}}Var(\hat{\beta })+{{\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \lambda } \right)}^{2}}Var(\hat{\lambda }) \\ & +2\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \beta } \right)\left( \frac{\partial {{\lambda }_{CA}}(T)}{\partial \lambda } \right)cov(\hat{\beta },\hat{\lambda }) \end{align}\,\! }[/math]
The variance calculation is the same as described in the Crow-AMSAA Confidence Bounds appendix.
Crow Bounds
If there are no BC failure modes then:
- [math]\displaystyle{ \begin{align} {{[{{\lambda }_{D}}(T)]}_{l}}= & {{\widehat{\lambda }}_{D}}(T)\frac{\chi _{(2N,1-\alpha /2)}^{2}}{2N} \\ {{[{{\lambda }_{D}}(T)]}_{u}}= & {{\widehat{\lambda }}_{D}}(T)\frac{\chi _{(2N,\alpha /2)}^{2}}{2N} \end{align}\,\! }[/math]
where [math]\displaystyle{ {{\widehat{\lambda }}_{D}}(T)={{\widehat{\lambda }}_{CA}}\,\! }[/math].
If there are BC modes then the confidence bounds on the demonstrated failure intensity are calculated as presented in the Crow-AMSAA Confidence Bounds appendix.
Bounds on Demonstrated MTBF
Fisher Matrix Bounds
- [math]\displaystyle{ \begin{align} & MTB{{F}_{{{D}_{L}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{U}}} \\ & MTB{{F}_{{{D}_{U}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{L}}} \end{align}\,\! }[/math]
where [math]\displaystyle{ {{[{{\lambda }_{D}}(T)]}_{L}}\,\! }[/math] and [math]\displaystyle{ {{[{{\lambda }_{D}}(T)]}_{U}}\,\! }[/math] can be obtained from the equation given above for Bounds on Demonstrated Failure Intensity.
Crow Bounds
- [math]\displaystyle{ \begin{align} MTB{{F}_{{{D}_{L}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{U}}} \\ MTB{{F}_{{{D}_{U}}}}= & \frac{1}{{{[{{\lambda }_{D}}(T)]}_{L}}} \end{align}\,\! }[/math]
where [math]\displaystyle{ {{[{{\lambda }_{D}}(T)]}_{L}}\,\! }[/math] and [math]\displaystyle{ {{[{{\lambda }_{D}}(T)]}_{U}}\,\! }[/math] can be obtained from the equation given above for Bounds on Demonstrated Failure Intensity.
Bounds on Projected Failure Intensity
Fisher Matrix Bounds
The projected failure intensity [math]\displaystyle{ {{\lambda }_{P}}(T)\,\! }[/math] must be positive; thus, [math]\displaystyle{ \ln {{\lambda }_{P}}(T)\,\! }[/math] is approximately treated as being normally distributed as well:
- [math]\displaystyle{ \frac{\ln {{{\hat{\lambda }}}_{P}}(T)-\ln {{\lambda }_{P}}(t)}{\sqrt{Var(\ln {{{\hat{\lambda }}}_{P}}(T)})}\sim N(0,1)\,\! }[/math]
- [math]\displaystyle{ CB={{\hat{\lambda }}_{P}}(T){{e}^{\pm {{z}_{\alpha }}\sqrt{Var({{{\hat{\lambda }}}_{P}}(T))}/{{{\hat{\lambda }}}_{P}}(T)}}\,\! }[/math]
where:
- [math]\displaystyle{ {{\hat{\lambda }}_{P}}(T)=\tfrac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T}+\overline{d}\tfrac{M}{T}\bar{\beta }\,\! }[/math] when there are no BC modes.
- [math]\displaystyle{ {{\hat{\lambda }}_{P}}(T)={{\widehat{\lambda }}_{EM}}={{\widehat{\lambda }}_{CA}}-{{\widehat{\lambda }}_{BD}}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T}+\overline{d}\widehat{h}(T|BD)\,\! }[/math] when there are BC modes.
- [math]\displaystyle{ {{N}_{i}}\,\! }[/math] is the total failure number of the [math]\displaystyle{ {{i}^{th}}\,\! }[/math] distinct BD mode.
You can then get:
- [math]\displaystyle{ Var({{\lambda }_{P}}(T))\approx Var({{\hat{\gamma }}_{GP}})+\mu _{d}^{2}Var(h(T))\approx \frac{{{{\hat{r}}}_{GP}}}{T}+\mu _{d}^{2}Var(h(T))\,\! }[/math]
where:
- [math]\displaystyle{ \begin{align} \hat{h}(T)= & \frac{M}{T}\bar{\beta } \\ Var(\hat{h}(T))= & {{(\frac{M}{T})}^{2}}Var(\bar{\beta })={{(\frac{M}{T})}^{2}}{{(\frac{M}{M-1})}^{2}}Var(\hat{\beta })=\frac{{{M}^{4}}}{{{T}^{2}}{{(M-1)}^{2}}}Var(\hat{\beta }) \end{align}\,\! }[/math]
The [math]\displaystyle{ Var(\hat{\beta })\,\! }[/math] can be obtained from Fisher Matrix based on [math]\displaystyle{ M\,\! }[/math] distinct BD modes.
Crow Bounds
- [math]\displaystyle{ \begin{align} {{[{{\lambda }_{P}}(T)]}_{L}}= & {{{\hat{\lambda }}}_{P}}(T)+\frac{{{C}^{2}}}{2}-\sqrt{{{{\hat{\lambda }}}_{P}}(T)\cdot {{C}^{2}}+\frac{{{C}^{4}}}{4}} \\ {{[{{\lambda }_{P}}(T)]}_{U}}= & {{{\hat{\lambda }}}_{P}}(T)+\frac{{{C}^{2}}}{2}+\sqrt{{{{\hat{\lambda }}}_{P}}(T)\cdot \ \,{{C}^{2}}+\frac{{{C}^{4}}}{4}} \end{align}\,\! }[/math]
where [math]\displaystyle{ C=\tfrac{{{z}_{1-\alpha /2}}}{\sqrt{T}}\,\! }[/math].
Bounds on Projected MTBF
Fisher Matrix Bounds
- [math]\displaystyle{ \begin{align} MTB{{F}_{{{P}_{L}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{U}}} \\ MTB{{F}_{{{P}_{U}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{L}}} \end{align}\,\! }[/math]
[math]\displaystyle{ {{[{{\lambda }_{P}}(T)]}_{U}}\,\! }[/math] and [math]\displaystyle{ {{[{{\lambda }_{P}}(T)]}_{L}}\,\! }[/math] can be obtained from the equation given above for Bounds on Projected Failure Intensity.
Crow Bounds
- [math]\displaystyle{ \begin{align} MTB{{F}_{{{P}_{L}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{U}}} \\ MTB{{F}_{{{P}_{U}}}}= & \frac{1}{{{[{{\lambda }_{P}}(T)]}_{L}}} \end{align}\,\! }[/math]
[math]\displaystyle{ {{[{{\lambda }_{P}}(T)]}_{U}}\,\! }[/math] and [math]\displaystyle{ {{[{{\lambda }_{P}}(T)]}_{L}}\,\! }[/math] can be obtained from the equation given above for Bounds on Projected Failure Intensity.
Bounds on Growth Potential Failure Intensity
Fisher Matrix Bounds
If there are no BC failure modes, the growth potential failure intensity is
- [math]\displaystyle{ {{\widehat{r}}_{GP}}(T)=\tfrac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T}\,\! }[/math].
Then:
- [math]\displaystyle{ \begin{align} Var({{\widehat{r}}_{GP}})= & \frac{1}{T}\left[ \frac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop \sum }}\,{{(1-{{d}_{i}})}^{2}}\frac{{{N}_{i}}}{T} \right] \\ \le & \frac{1}{T}\left[ \frac{{{N}_{A}}}{T}+\underset{i=1}{\overset{M}{\mathop \sum }}\,(1-{{d}_{i}})\frac{{{N}_{i}}}{T} \right] \\ = & \frac{{{r}_{GP}}}{T} \end{align}\,\! }[/math]
If there are BC failure modes, the growth potential failure intensity is
- [math]\displaystyle{ {{\widehat{r}}_{GP}}(T)={{\widehat{\lambda }}_{CA}}-{{\widehat{\lambda }}_{BD}}+\underset{i=1}{\overset{M}{\mathop{\sum }}}\,(1-{{d}_{i}})\tfrac{{{N}_{i}}}{T},\,\! }[/math] [math]\displaystyle{ Var({{\widehat{r}}_{GP}})\approx \tfrac{{{r}_{GP}}}{T}\,\! }[/math].
Therefore:
- [math]\displaystyle{ \sqrt{T}\left( \frac{{{{\hat{r}}}_{GP}}-{{r}_{GP}}}{\sqrt{{{r}_{GP}}}} \right)\sim N(0,1)\,\! }[/math]
The confidence bounds on the growth potential failure intensity are as follows:
- [math]\displaystyle{ \begin{align} {{r}_{L}}= & {{{\hat{r}}}_{GP}}+\frac{{{C}^{2}}}{2}-\sqrt{{{{\hat{r}}}_{GP}}\,{{C}^{2}}+\frac{{{C}^{4}}}{4}} \\ {{r}_{U}}= & {{{\hat{r}}}_{GP}}+\frac{{{C}^{2}}}{2}+\sqrt{{{{\hat{r}}}_{GP}}\,{{C}^{2}}+\frac{{{C}^{4}}}{4}} \end{align}\,\! }[/math]
where [math]\displaystyle{ C=\tfrac{{{z}_{1-\alpha /2}}}{\sqrt{T}}\,\! }[/math].
Crow Bounds
The Crow bounds for the growth potential failure intensity are the same as the Fisher Matrix bounds.
Bounds on Growth Potential MTBF
Fisher Matrix Bounds
- [math]\displaystyle{ \begin{align} MTB{{F}_{G{{P}_{L}}}}= & \frac{1}{{{r}_{U}}} \\ MTB{{F}_{G{{P}_{U}}}}= & \frac{1}{{{r}_{L}}} \end{align}\,\! }[/math]
where [math]\displaystyle{ {{r}_{U}}\,\! }[/math] and [math]\displaystyle{ {{r}_{L}}\,\! }[/math] can be obtained from the equation given above for Bounds on Growth Potential Failure Intensity.
Crow Bounds
The Crow bounds for the growth potential MTBF are the same as the Fisher Matrix bounds.