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118      4 Parametric Tests of Hypotheses


           measures the  deviation of the alternative hypothesis from the null hypothesis,
           normalised by the standard deviation, as follows:

                   µ − µ
              E =   B σ  A  .                                               4.1
                s

              For instance, for  n = 24 the protection against  µ A  = 1100 corresponds to a
           standardised effect of (1300 − 1100)/260 = 0.74 and the power graph of Figure 4.6
           indicates a value  of about  0.94 for  E s  =  0.74. The difference  from the previous
           value of 0.98  in  Table 4.2  is due  to  the fact that, as already  mentioned,
           STATISTICA uses the Student’s t distribution.



                        1.0
                            Power
                         .9
                         .8
                         .7
                         .6
                         .5
                         .4
                         .3
                         .2
                         .1
                                                   Standardized Effect (Es)
                        0.0
                          0.0  0.1  0.2  0.3  0.4  0.5  0.6  0.7  0.8  0.9  1.0
           Figure 4.6. Power curve obtained with STATISTICA for the drill example with
           α = 0.05 and n = 24.

              In the work  of Cohen  (Cohen,  1983),  some guidance is provided on how to
           qualify the standardised effect:

              Small effect size:    E s = 0.2.
              Medium effect size:    E s = 0.5.
              Large effect size:    E s = 0.8.

              In the example we have been discussing, we are in presence of a large effect
           size. As the effect size becomes smaller, one needs a larger sample size in order to
           obtain a reasonable  power.  For instance,  imagine that the alternative  hypothesis
           had precisely the same value as the sample mean, i.e., µ A=1260. In this case, the
           standardised effect is very small, E s = 0.148. For this reason, we obtain very small
           values of the power for n = 12 and n = 24 (see the power for µ A =1250 in Tables
           4.1 and 4.2). In order to “resolve” such close values (1260 and 1300) with low
           errors α and β, we need, of course, a much higher sample size. Figure 4.7 shows
           how the  power evolves  with the sample  size in this example, for  the fixed
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