(some lines are higher than others) and it is this variance that we have here. For most of us
that variance is not particularly important, but there are studies in which it is.
As I said earlier, mixed model analyses do not require an assumption of compound
symmetry. In fact, that assumption is often incorrect. In Table 14.17 you can see the pat-
tern of correlations among trials. These are averaged over the separate groups, but give you
a clear picture that the structure is not one of compound symmetry.
There are a number of things that we could do to alter the model that we just ran, which
requested a solution based on compound symmetry. We could tell SPSS to solve the problem
without assuming anything about the correlations or covariances. (That is essentially what
the MANOVA approach to repeated measures does.) The problem with this approach is
that the solution has to derive estimates of those correlations and that will take away
degrees of freedom, perhaps needlessly. There is no point in declaring that you are to-
tally ignorant when you are really only partially ignorant. Another approach would be to
assume a specific (but different) form of the covariance matrix. For example, we could
use what is called an autoregressive solution. Such a solution assumes that correlations
between observations decrease as the times move further apart in time. It further assumes
that each correlation depends only on the preceding correlation plus some (perhaps
much) error. If the correlation between adjacent trials is, for example 0.5121 (as it is in
the study we are discussing), then times that are two steps apart are assumed to correlate
.5121^2 and times three steps apart are assumed to correlate .5121^3. This leads to a matrix
Section 14.12 Mixed Models for Repeated-Measures Designs 503
Time
1 2 3 4
Mean dv
300
250
200
150
100
Treatment
Control
Group
Figure 14.5 Means across trials for the two conditions
Table 14.17 Correlations among trials
Estimated RCorrelation Matrix for Subject 1
Row Col1 Col2 Col3 Col4
1 1.0000 0.5121 0.4163 2 0.08840
2 0.5121 1.0000 0.8510 0.3628
3 0.4163 0.8510 1.0000 0.3827
4 2 0.08840 0.3628 0.3827 1.0000