| The POWER Procedure |
TableNotation:
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Success |
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2 |
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The hypotheses are
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where
is constrained to be
for all but the unconditional Pearson chi-square test.
Internal calculations are performed in terms of
,
, and
. An input set consisting of
,
, and
is transformed as follows:
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An input set consisting of
,
, and
is transformed as follows:
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Note that the transformation of either
or
to
is not unique. The chosen parameterization fixes the null value
at the input value of
.
The usual Pearson chi-square test is unconditional. The test statistic
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is assumed to have a null distribution of
.
Sample size for the one-sided cases is given by equation (4) in Fleiss, Tytun, and Ury (1980). One-sided power is computed as suggested by Diegert and Diegert (1981) by inverting the sample size formula. Power for the two-sided case is computed by adding the lower-sided and upper-sided powers each with
, and sample size for the two-sided case is obtained by numerically inverting the power formula. A custom null value
for the proportion difference
is also supported.
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For the one-sided cases, a closed-form inversion of the power equation yield an approximate total sample size
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For the two-sided case, the solution for
is obtained by numerically inverting the power equation.
The usual likelihood ratio chi-square test is unconditional. The test statistic
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is assumed to have a null distribution of
and an alternative distribution of
, where
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The approximate power is
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For the one-sided cases, a closed-form inversion of the power equation yield an approximate total sample size
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For the two-sided case, the solution for
is obtained by numerically inverting the power equation.
Fisher’s exact test is conditional on the observed total number of successes
. Power and sample size computations for the METHOD=WALTERS option are based on a test with similar power properties, the continuity-adjusted arcsine test. The test statistic
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is assumed to have a null distribution of
and an alternative distribution of
, where
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The approximate power for the one-sided balanced case is given by Walters (1979) and is easily extended to the unbalanced and two-sided cases:
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