Template:Aw characteristics: Difference between revisions

From ReliaWiki
Jump to navigation Jump to search
No edit summary
Line 2: Line 2:
The characteristics of the 2-parameter Weibull distribution can be exemplified by examining the two parameters, beta,  <math>\beta ,</math>  and eta,  <math>\eta ,</math>  and the effect they have on the  <math>pdf,</math>  reliability and failure rate functions.  
The characteristics of the 2-parameter Weibull distribution can be exemplified by examining the two parameters, beta,  <math>\beta ,</math>  and eta,  <math>\eta ,</math>  and the effect they have on the  <math>pdf,</math>  reliability and failure rate functions.  


==== Looking at <span class="texhtml">β</span> ====
==== Looking at <span class="texhtml">β</span> ====


Beta (<span class="texhtml">β</span>) is called the shape parameter or slope of the Weibull distribution. Changing the value of <span class="texhtml">β</span> forces a change in the shape of the <span class="texhtml">''p''''d''''f''</span> as shown in the next figure. In addition, when the <span class="texhtml">''c''''d''''f''</span> is plotted on Weibull probability paper, a change in beta is a change in the slope of the distribution on Weibull probability paper. <br> '''Effects of <span class="texhtml">β</span> on the ''pdf'''''  
Beta (<span class="texhtml">β</span>) is called the shape parameter or slope of the Weibull distribution. Changing the value of <span class="texhtml">β</span> forces a change in the shape of the <span class="texhtml">''p''''d''''f''</span> as shown in the next figure. In addition, when the <span class="texhtml">''c''''d''''f''</span> is plotted on Weibull probability paper, a change in beta is a change in the slope of the distribution on Weibull probability paper.  
 
<br> '''Effects of <span class="texhtml">β</span> on the ''pdf'''''  


<br> [[Image:ALTA4.3.gif|thumb|center|400px]] <br>  
<br> [[Image:ALTA4.3.gif|thumb|center|400px]] <br>  
Line 51: Line 53:
'''Effects of <span class="texhtml">β</span> on the Failure Rate Function'''  
'''Effects of <span class="texhtml">β</span> on the Failure Rate Function'''  


 
<br> [[Image:ALTA4.6.gif|thumb|center|400px]] <br>  
[[Image:ALTA4.6.gif|thumb|center|400px]] <br>  


:*The Weibull failure rate for <span class="texhtml">0 &lt; β &lt; 1</span> is unbounded at <span class="texhtml">''T'' = 0</span> . The failure rate, <span class="texhtml">λ(''T''),</span> decreases thereafter monotonically and is convex, approaching the value of zero as <math>T\to \infty </math> or <math>\lambda (\infty )=0</math> . This behavior makes it suitable for representing the failure rate of units exhibiting early-type failures, for which the failure rate decreases with age. When such behavior is encountered, one or more of the following conclusions can be drawn:  
:*The Weibull failure rate for <span class="texhtml">0 &lt; β &lt; 1</span> is unbounded at <span class="texhtml">''T'' = 0</span> . The failure rate, <span class="texhtml">λ(''T''),</span> decreases thereafter monotonically and is convex, approaching the value of zero as <math>T\to \infty </math> or <math>\lambda (\infty )=0</math> . This behavior makes it suitable for representing the failure rate of units exhibiting early-type failures, for which the failure rate decreases with age. When such behavior is encountered, one or more of the following conclusions can be drawn:  

Revision as of 23:37, 6 March 2012

Characteristics

The characteristics of the 2-parameter Weibull distribution can be exemplified by examining the two parameters, beta, [math]\displaystyle{ \beta , }[/math] and eta, [math]\displaystyle{ \eta , }[/math] and the effect they have on the [math]\displaystyle{ pdf, }[/math] reliability and failure rate functions.

Looking at β

Beta (β) is called the shape parameter or slope of the Weibull distribution. Changing the value of β forces a change in the shape of the p'd'f as shown in the next figure. In addition, when the c'd'f is plotted on Weibull probability paper, a change in beta is a change in the slope of the distribution on Weibull probability paper.


Effects of β on the pdf


ALTA4.3.gif


  • For 0 < β < 1 , the failure rate decreases with time and:
  • As [math]\displaystyle{ T\to 0, }[/math] [math]\displaystyle{ f(T)\to \infty . }[/math]
  • As [math]\displaystyle{ T\to \infty }[/math] , [math]\displaystyle{ f(T)\to 0 }[/math] .
  • f(T) decreases monotonically and is convex as T increases.
  • The mode is non-existent.
  • For β = 1, it becomes the exponential distribution, as a special case,


or:


[math]\displaystyle{ f(T)=\frac{1}{\eta }{{e}^{-\tfrac{T}{\eta }}};\text{ }\eta \gt 0,T\ge 0 }[/math]


where [math]\displaystyle{ \tfrac{1}{\eta }=\lambda = }[/math] chance, useful life, or failure rate.


  • For β > 1 , f(T), the Weibull assumes wear-out type shapes (i.e. the failure rate increases with time) and:
  • f(T) = 0 at T = 0 .
  • f(T) increases as [math]\displaystyle{ T\to \tilde{T} }[/math] (mode) and decreases thereafter.
  • For β = 2 it becomes the Rayleigh distribution as a special case. For β < 2.6 the Weibull p'd'f is positively skewed (has a right tail), for 2.6 < β < 3.7 its coefficient of skewness approaches zero (no tail); consequently, it may approximate the normal p'd'f , and for β > 3.7 it is negatively skewed (left tail).
  • The parameter β is a pure number, i.e. it is dimensionless.


Effects of β on the Reliability Function and the cdf


ALTA4.4.gif


ALTA4.5.gif


  • R(T) decreases sharply and monotonically for 0 < β < 1 , it is convex, and decreases less sharply for the same β .
  • For β = 1 and the same η , R(T) decreases monotonically but less sharply than for 0 < β < 1 , and is convex.
  • For β > 1 , R(T) decreases as T increases but less sharply than before, and as wear-out sets in, it decreases sharply and goes through an inflection point.


Effects of β on the Failure Rate Function


ALTA4.6.gif


  • The Weibull failure rate for 0 < β < 1 is unbounded at T = 0 . The failure rate, λ(T), decreases thereafter monotonically and is convex, approaching the value of zero as [math]\displaystyle{ T\to \infty }[/math] or [math]\displaystyle{ \lambda (\infty )=0 }[/math] . This behavior makes it suitable for representing the failure rate of units exhibiting early-type failures, for which the failure rate decreases with age. When such behavior is encountered, one or more of the following conclusions can be drawn:
  • Burn-in testing and/or environmental stress screening are not well implemented.
  • There are problems in the production line.
  • Inadequate quality control.
  • Packaging and transit problems.
  • For β = 1 , λ(T) yields a constant value of [math]\displaystyle{ \tfrac{1}{\eta } }[/math] , or:
[math]\displaystyle{ \lambda (T)=\lambda =\frac{1}{\eta } }[/math]

This makes it suitable for representing the failure rate of chance-type failures and the useful life period failure rate of units.

  • For β > 1 , λ(T) increases as T increases and becomes suitable for representing the failure rate of units exhibiting wear-out type failures. For 1 < β < 2 the λ(T) curve is concave, consequently the failure rate increases at a decreasing rate as T increases.
  • For β = 2 , or for the Rayleigh distribution case, the failure rate function is given by:
[math]\displaystyle{ \lambda (T)=\frac{2}{\eta }\left( \frac{T}{\eta } \right) }[/math]


Hence there emerges a straight line relationship between λ(T) and T , starting at a value of λ(T) = 0 at T = 0 and increasing thereafter with a slope of [math]\displaystyle{ \tfrac{2}{{{\eta }^{2}}} }[/math] . Consequently, the failure rate increases at a constant rate as T increases. Furthermore, if η = 1 the slope becomes equal to 2, and λ(T) becomes a straight line which passes through the origin with a slope of 2.

  • When β > 2 the λ(T) curve is convex, with its slope increasing as T increases. Consequently, the failure rate increases at an increasing rate as T increases, indicating wear-out life.


Looking at [math]\displaystyle{ \eta }[/math]

Eta, [math]\displaystyle{ \eta , }[/math] is called the scale parameter of the Weibull distribution. The parameter [math]\displaystyle{ \eta }[/math] has the same units as [math]\displaystyle{ T }[/math] , such as hours, miles, cycles, actuations, etc.

ALTA4.7.gif


• A change in the scale parameter [math]\displaystyle{ \eta }[/math] has the same effect on the distribution as a change of the abscissa scale.
o If [math]\displaystyle{ \eta }[/math] is increased while [math]\displaystyle{ \beta }[/math] is kept the same, the distribution gets stretched out to the right and its height decreases, while maintaining its shape and location.
o If [math]\displaystyle{ \eta }[/math] is decreased while [math]\displaystyle{ \beta }[/math] is kept the same, the distribution gets pushed in toward the left (i.e. toward its beginning, or 0) and its height increases.