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PCHART Statement

Constructing Charts for Proportion Nonconforming (p Charts)

The following notation is used in this section:
pexpected proportion of nonconforming items produced by the process
piproportion of nonconforming items in the i th subgroup
Xinumber of nonconforming items in the i th subgroup
ninumber of items in the i th subgroup
\bar{p}average proportion of nonconforming items taken across subgroups:
\bar{p} = \frac{n_1p_1 +  ...  + n_Np_N}
 {n_1 +  ...  + n_N}
 = \frac{X_1 +  ...  + X_N}
 {n_1 +  ...  + n_N}
Nnumber of subgroups
I_{T}(\alpha,\beta)incomplete beta function:
I_{T}(\alpha,\beta) =
 (\Gamma(\alpha+\beta)/\Gamma(\alpha)\Gamma(\beta))
 \int_{0}^Tt^{\alpha - 1}(1-t)^{\beta-1}dt
for 0<T<1, \alpha\gt, and \beta\gt, where \Gamma(\cdot)is the gamma function

Plotted Points

Each point on a p chart represents the observed proportion (pi=Xi/ni) of nonconforming items in a subgroup. For example, suppose the second subgroup (see Figure 38.10) contains 16 items, of which two are nonconforming. The point plotted for the second subgroup is p2 = 2/16=0.125.

balls.gif (4631 bytes)

Figure 38.10: Proportions Versus Counts

Note that an np chart displays the number (count) of nonconforming items Xi. You can use the NPCHART statement to create np charts; see Chapter 37, "NPCHART Statement."

Central Line

By default, the central line on a p chart indicates an estimate of p that is computed as \bar{p}.If you specify a known value (p0) for p, the central line indicates the value of p0.

Control Limits

You can compute the limits in the following ways:

The lower and upper control limits, LCL and UCL, respectively, are computed as
{LCL} &= &{max} (\bar{p} -
 k\sqrt{\bar{p}(1-\bar{p})/n_i}\;, 0 ) \ {UCL} &= &{min}(\bar{p} +
 k\sqrt{\bar{p}(1-\bar{p})/n_i}\;, 1 )

A lower probability limit for pi can be determined using the fact that
P\{p_i \lt {LCL}\} & = 1 - P\{p_i \geq {LCL}\} \ & = 1 - P\{X_i \geq n_i{LCL}\} ...
 ...bar{p}}(n_i{LCL},n_i+1-n_i{LCL}) \ & = I_{1- \bar{p}}(n_i+1-n_i{LCL},n_i{LCL}) \

Refer to Johnson, Kotz, and Kemp (1992). This assumes that the process is in statistical control and that Xi is binomially distributed. The lower probability limit LCL is then calculated by setting

I_{1- \bar{p}}(n_i+1-n_i{LCL},n_i{LCL}) = \alpha/2
and solving for LCL. Similarly, the upper probability limit for pi can be determined using the fact that
P\{p_i \gt {UCL}\} & = P\{p_i \gt {UCL}\} \ & = P\{X_i \gt n_i{UCL}\} \ & = I_{\bar{p}}(n_i{UCL},n_i+1-n_i{UCL}) \

The upper probability limit UCL is then calculated by setting

I_{\bar{p}}(n_i{UCL},n_i+1-n_i{UCL}) = \alpha/2
and solving for UCL. The probability limits are asymmetric around the central line. Note that both the control limits and probability limits vary with ni.

You can specify parameters for the limits as follows:


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