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		<title>Lisa Hacker: Redirected page to Appendix: Log-Likelihood Equations</title>
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		<updated>2015-06-25T19:27:28Z</updated>

		<summary type="html">&lt;p&gt;Redirected page to &lt;a href=&quot;/index.php/Appendix:_Log-Likelihood_Equations&quot; title=&quot;Appendix: Log-Likelihood Equations&quot;&gt;Appendix: Log-Likelihood Equations&lt;/a&gt;&lt;/p&gt;
&lt;a href=&quot;https://www.reliawiki.com/index.php?title=Weibull_Log-Likelihood_Functions_and_their_Partials&amp;amp;diff=58686&amp;amp;oldid=10597&quot;&gt;Show changes&lt;/a&gt;</summary>
		<author><name>Lisa Hacker</name></author>
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		<id>https://www.reliawiki.com/index.php?title=Weibull_Log-Likelihood_Functions_and_their_Partials&amp;diff=10597&amp;oldid=prev</id>
		<title>Pantelis: Created page with &#039;===Weibull Log-Likelihood Functions and their Partials===  ====The Two-Parameter Weibull==== This log-likelihood function is composed of three summation portions:  ::&lt;math&gt;\begin…&#039;</title>
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		<updated>2011-10-29T13:14:45Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;#039;===Weibull Log-Likelihood Functions and their Partials===  ====The Two-Parameter Weibull==== This log-likelihood function is composed of three summation portions:  ::&amp;lt;math&amp;gt;\begin…&amp;#039;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;===Weibull Log-Likelihood Functions and their Partials===&lt;br /&gt;
&lt;br /&gt;
====The Two-Parameter Weibull====&lt;br /&gt;
This log-likelihood function is composed of three summation portions:&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
  &amp;amp; \ln (L)= &amp;amp; \Lambda =\underset{i=1}{\overset{{{F}_{e}}}{\mathop \sum }}\,{{N}_{i}}\ln \left[ \frac{\beta }{\eta }{{\left( \frac{{{T}_{i}}}{\eta } \right)}^{\beta -1}}{{e}^{-{{\left( \tfrac{{{T}_{i}}}{\eta } \right)}^{\beta }}}} \right]-\underset{i=1}{\overset{S}{\mathop \sum }}\,N_{i}^{\prime }{{\left( \frac{T_{i}^{\prime }}{\eta } \right)}^{\beta }} \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; \text{  }+\underset{i=1}{\overset{FI}{\mathop \sum }}\,N_{i}^{\prime \prime }\ln \left[ {{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right)}^{\beta }}}} \right]   &lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:where:&lt;br /&gt;
::•	&amp;lt;math&amp;gt;{{F}_{e}}&amp;lt;/math&amp;gt; is the number of groups of times-to-failure data points&lt;br /&gt;
::•	&amp;lt;math&amp;gt;{{N}_{i}}&amp;lt;/math&amp;gt; is the number of times-to-failure in the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; time-to-failure data group&lt;br /&gt;
::•	&amp;lt;math&amp;gt;\beta &amp;lt;/math&amp;gt; is the Weibull shape parameter (unknown a priori, the first of two parameters to be found)&lt;br /&gt;
::•	&amp;lt;math&amp;gt;\eta &amp;lt;/math&amp;gt; is the Weibull scale parameter (unknown a priori, the second of two parameters to be found)&lt;br /&gt;
::•	&amp;lt;math&amp;gt;{{T}_{i}}&amp;lt;/math&amp;gt; is the time of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; group of time-to-failure data&lt;br /&gt;
::•	&amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; is the number of groups of suspension data points&lt;br /&gt;
::•	&amp;lt;math&amp;gt;N_{i}^{\prime }&amp;lt;/math&amp;gt; is the number of suspensions in &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; group of suspension data points&lt;br /&gt;
::•	&amp;lt;math&amp;gt;T_{i}^{\prime }&amp;lt;/math&amp;gt; is the time of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; suspension data group&lt;br /&gt;
::•	&amp;lt;math&amp;gt;FI&amp;lt;/math&amp;gt; is the number of interval failure data groups&lt;br /&gt;
::•	&amp;lt;math&amp;gt;N_{i}^{\prime \prime }&amp;lt;/math&amp;gt; is the number of intervals in &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; group of data intervals&lt;br /&gt;
::•	&amp;lt;math&amp;gt;T_{Li}^{\prime \prime }&amp;lt;/math&amp;gt; is the beginning of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt;  interval&lt;br /&gt;
::•	and &amp;lt;math&amp;gt;T_{Ri}^{\prime \prime }&amp;lt;/math&amp;gt; is the ending of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; interval &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
For the purposes of MLE, left censored data will be considered to be intervals with &amp;lt;math&amp;gt;T_{Li}^{\prime \prime }=0.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The solution will be found by solving for a pair of parameters &amp;lt;math&amp;gt;\left( \widehat{\beta },\widehat{\eta } \right)&amp;lt;/math&amp;gt; so that &amp;lt;math&amp;gt;\tfrac{\partial \Lambda }{\partial \beta }=0&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\tfrac{\partial \Lambda }{\partial \eta }=0.&amp;lt;/math&amp;gt; It should be noted that other methods can also be used, such as direct maximization of the likelihood function, without having to compute the derivatives.&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
  &amp;amp; \frac{\partial \Lambda }{\partial \beta }= &amp;amp; \frac{1}{\beta }\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}+\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}\ln \left( \frac{{{T}_{i}}}{\eta } \right) \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; -\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}{{\left( \frac{{{T}_{i}}}{\eta } \right)}^{\beta }}\ln \left( \frac{{{T}_{i}}}{\eta } \right)-\underset{i=1}{\overset{S}{\mathop{\sum }}}\,N_{i}^{\prime }{{\left( \frac{T_{i}^{\prime }}{\eta } \right)}^{\beta }}\ln \left( \frac{T_{i}^{\prime }}{\eta } \right) \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{FI}{\mathop{\sum }}}\,N_{i}^{\prime \prime }\frac{-{{\left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right)}^{\beta }}\ln \left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right){{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right)}^{\beta }}}}+{{\left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right)}^{\beta }}\ln \left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right){{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right)}^{\beta }}}}}{{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right)}^{\beta }}}}}  &lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
  &amp;amp; \frac{\partial \Lambda }{\partial \eta }= &amp;amp; \frac{-\beta }{\eta }\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}+\frac{\beta }{\eta }\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}{{\left( \frac{{{T}_{i}}}{\eta } \right)}^{\beta }} \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\frac{\beta }{\eta }\underset{i=1}{\overset{S}{\mathop{\sum }}}\,N_{i}^{\prime }{{\left( \frac{T_{i}^{\prime }}{\eta } \right)}^{\beta }} \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{FI}{\mathop{\sum }}}\,N_{i}^{\prime \prime }\frac{\left( \tfrac{\beta }{\eta } \right){{\left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right)}^{\beta }}{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right)}^{\beta }}}}-\left( \tfrac{\beta }{\eta } \right){{\left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right)}^{\beta }}{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right)}^{\beta }}}}}{{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }}{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }}{\eta } \right)}^{\beta }}}}}  &lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;br&amp;gt;&lt;br /&gt;
&lt;br /&gt;
====  The Three-Parameter Weibull====&lt;br /&gt;
This log-likelihood function is again composed of three summation portions:&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
  &amp;amp; \ln (L)= &amp;amp; \Lambda =\underset{i=1}{\overset{{{F}_{e}}}{\mathop \sum }}\,{{N}_{i}}\ln \left[ \frac{\beta }{\eta }{{\left( \frac{{{T}_{i}}-\gamma }{\eta } \right)}^{\beta -1}}{{e}^{-{{\left( \tfrac{{{T}_{i}}-\gamma }{\eta } \right)}^{\beta }}}} \right]-\underset{i=1}{\overset{S}{\mathop \sum }}\,N_{i}^{\prime }{{\left( \frac{T_{i}^{\prime }-\gamma }{\eta } \right)}^{\beta }} \\ &lt;br /&gt;
 &amp;amp;  &amp;amp;  \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{FI}{\mathop \sum }}\,N_{i}^{\prime \prime }\ln \left[ {{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}} \right]  &lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:where,&lt;br /&gt;
::•	&amp;lt;math&amp;gt;{{F}_{e}}&amp;lt;/math&amp;gt; is the number of groups of times-to-failure data points&lt;br /&gt;
::•	&amp;lt;math&amp;gt;{{N}_{i}}&amp;lt;/math&amp;gt; is the number of times-to-failure in the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; time-to-failure data group&lt;br /&gt;
::•	&amp;lt;math&amp;gt;\beta &amp;lt;/math&amp;gt; is the Weibull shape parameter (unknown a priori, the first of three parameters to be found)&lt;br /&gt;
::•	&amp;lt;math&amp;gt;\eta &amp;lt;/math&amp;gt; is the Weibull scale parameter (unknown a priori, the second of three parameters to be found)&lt;br /&gt;
::•	&amp;lt;math&amp;gt;{{T}_{i}}&amp;lt;/math&amp;gt; is the time of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; group of time-to-failure data&lt;br /&gt;
::•	&amp;lt;math&amp;gt;\gamma &amp;lt;/math&amp;gt; is the Weibull location parameter (unknown a priori, the third of three parameters to be found)&lt;br /&gt;
::•	&amp;lt;math&amp;gt;S&amp;lt;/math&amp;gt; is the number of groups of suspension data points&lt;br /&gt;
::•	&amp;lt;math&amp;gt;N_{i}^{\prime }&amp;lt;/math&amp;gt; is the number of suspensions in &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; group of suspension data points&lt;br /&gt;
::•	&amp;lt;math&amp;gt;T_{i}^{\prime }&amp;lt;/math&amp;gt; is the time of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; suspension data group&lt;br /&gt;
::•	&amp;lt;math&amp;gt;FI&amp;lt;/math&amp;gt; is the number of interval data groups&lt;br /&gt;
::•	&amp;lt;math&amp;gt;N_{i}^{\prime \prime }&amp;lt;/math&amp;gt; is the number of intervals in the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; group of data intervals&lt;br /&gt;
::•	&amp;lt;math&amp;gt;T_{Li}^{\prime \prime }&amp;lt;/math&amp;gt; is the beginning of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; interval&lt;br /&gt;
::•	and &amp;lt;math&amp;gt;T_{Ri}^{\prime \prime }&amp;lt;/math&amp;gt; is the ending of the &amp;lt;math&amp;gt;{{i}^{th}}&amp;lt;/math&amp;gt; interval&lt;br /&gt;
&lt;br /&gt;
The solution is found by solving for &amp;lt;math&amp;gt;\left( \widehat{\beta },\widehat{\eta },\widehat{\gamma } \right)&amp;lt;/math&amp;gt; so that &amp;lt;math&amp;gt;\tfrac{\partial \Lambda }{\partial \beta }=0,&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\tfrac{\partial \Lambda }{\partial \eta }=0,&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\tfrac{\partial \Lambda }{\partial \gamma }=0.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
  &amp;amp; \frac{\partial \Lambda }{\partial \beta }= &amp;amp; \frac{1}{\beta }\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}+\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}\ln \left( \frac{{{T}_{i}}-\gamma }{\eta } \right)-\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}{{\left( \frac{{{T}_{i}}-\gamma }{\eta } \right)}^{\beta }}\ln \left( \frac{{{T}_{i}}-\gamma }{\eta } \right) \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; -\underset{i=1}{\overset{S}{\mathop{\sum }}}\,N_{i}^{\prime }{{\left( \frac{T_{i}^{\prime }-\gamma }{\eta } \right)}^{\beta }}\ln \left( \frac{T_{i}^{\prime }-\gamma }{\eta } \right) \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{FI}{\mathop{\sum }}}\,N_{i}^{\prime \prime }\frac{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}\ln \left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right){{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}{{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}} \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{FI}{\mathop{\sum }}}\,N_{i}^{\prime \prime }\frac{{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}\ln \left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right){{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}{{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}  &lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
  &amp;amp; \frac{\partial \Lambda }{\partial \eta }= &amp;amp; \frac{-\beta }{\eta }\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}+\frac{\beta }{\eta }\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}{{\left( \frac{{{T}_{i}}-\gamma }{\eta } \right)}^{\beta }}+\underset{i=1}{\overset{S}{\mathop{\sum }}}\,N_{i}^{\prime }{{\left( \frac{T_{i}^{\prime }-\gamma }{\eta } \right)}^{\beta }}\left( \frac{\beta }{\eta } \right) \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{FI}{\mathop{\sum }}}\,N_{i}^{\prime \prime }\frac{\tfrac{\beta }{\eta }{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}\ln \left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right){{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}{{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}} \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; -\underset{i=1}{\overset{FI}{\mathop{\sum }}}\,N_{i}^{\prime \prime }\frac{\tfrac{\beta }{\eta }{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}\ln \left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right){{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}{{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}  &lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
::&amp;lt;math&amp;gt;\begin{align}&lt;br /&gt;
  &amp;amp; \frac{\partial \Lambda }{\partial \gamma }= &amp;amp; \left( 1-\beta  \right)\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,\left( \frac{{{N}_{i}}}{{{T}_{i}}-\gamma } \right)+\underset{i=1}{\overset{{{F}_{e}}}{\mathop{\sum }}}\,{{N}_{i}}{{\left( \frac{{{T}_{i}}-\gamma }{\eta } \right)}^{\beta }}\left( \frac{\beta }{{{T}_{i}}-\gamma } \right) \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{S}{\mathop{\sum }}}\,N_{i}^{\prime }{{\left( \frac{T_{i}^{\prime }-\gamma }{\eta } \right)}^{\beta }}\left( \frac{\beta }{T_{i}^{\prime }-\gamma } \right) \\ &lt;br /&gt;
 &amp;amp;  &amp;amp; +\underset{i=1}{\overset{FI}{\mathop{\sum }}}\,N_{i}^{\prime \prime }\frac{\tfrac{\beta }{T_{Li}^{\prime \prime }-\gamma }{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}-\tfrac{\beta }{T_{Ri}^{\prime \prime }-\gamma }{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}{{{e}^{-{{\left( \tfrac{T_{Li}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}-{{e}^{-{{\left( \tfrac{T_{Ri}^{\prime \prime }-\gamma }{\eta } \right)}^{\beta }}}}}  &lt;br /&gt;
\end{align}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
It should be pointed out that the solution to the three-parameter Weibull via MLE is not always stable and can collapse if &amp;lt;math&amp;gt;\beta \sim 1.&amp;lt;/math&amp;gt; In estimating the true MLE of the three-parameter Weibull distribution, two difficulties arise. The first is a problem of non-regularity and the second is the parameter divergence problem [14].&lt;br /&gt;
&lt;br /&gt;
Non-regularity occurs when &amp;lt;math&amp;gt;\beta \le 2.&amp;lt;/math&amp;gt; In general, there are no MLE solutions in the region of &amp;lt;math&amp;gt;0&amp;lt;\beta &amp;lt;1.&amp;lt;/math&amp;gt; When &amp;lt;math&amp;gt;1&amp;lt;\beta &amp;lt;2,&amp;lt;/math&amp;gt; MLE solutions exist but are not asymptotically normal [14]. In the case of non-regularity, the solution is treated anomalously.&lt;br /&gt;
&lt;br /&gt;
Weibull++ attempts to find a solution in all of the regions using a variety of methods, but the user should be forewarned that not all possible data can be addressed. Thus, some solutions using MLE for the three-parameter Weibull will fail when the algorithm has reached predefined limits or fails to converge. In these cases, the user can change to the non-true MLE approach (in Weibull++ User Setup), where &amp;lt;math&amp;gt;\gamma &amp;lt;/math&amp;gt; is estimated using non-linear regression. Once &amp;lt;math&amp;gt;\gamma &amp;lt;/math&amp;gt; is obtained, the MLE estimates of &amp;lt;math&amp;gt;\widehat{\beta }&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\widehat{\eta }&amp;lt;/math&amp;gt; are computed using the transformation &amp;lt;math&amp;gt;T_{i}^{\prime }=({{T}_{i}}-\gamma ).&amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Pantelis</name></author>
	</entry>
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