Physics for Geologists, Second edition
Physics for Geologists, Second edition
Physics for Geologists, Second edition
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134 Some dangers of mathematical statistics<br />
Table 13.1 Experimental data<br />
Figure 13.2 Plot of data in Table 13.1 with the linear regression line. The sys-<br />
tematic differences are evident although statistical analysis indicates<br />
a very significant linear relationship and implies a random error<br />
about the regression line.<br />
In this case, if you compute the regression of the natural logarithms,<br />
you obtain In y = 2.0 Inx - 0.69, and the correlation coefficient is 1.00<br />
(Figure 13.3). Restoring the natural logarithms (Iny = mlnx + Inb to<br />
y = bxm), this suggests that the true relationship is y = x2/2, which indeed<br />
it is. The result of the test of significance, that it is extremely unlikely that<br />
the association of points arose by chance, must not be interpreted as con-<br />
firmation that it is linear. The test of significance indicates that it is most<br />
unlikely that the association arose by chance, and indeed, the association<br />
did not arise by chance.<br />
The point is, and a very important point it is, that any gentle curve, and<br />
any short part of a curve, will give good linear correlation. You must do the<br />
thinking, because statistics does not think <strong>for</strong> you. In particular, you must<br />
consider the boundary conditions. Take another example.<br />
You determine the acoustic or sonic velocity (V) and fractional porosity<br />
(f) in sandstones of different porosity so that you may determine the poros-<br />
ity by measuring the acoustic velocity. It is much easier to measure acoustic<br />
velocity than porosity in a borehole. You can measure both with considerable<br />
accuracy when you have a sample, so how would you set about the task of<br />
Copyright 2002 by Richard E. Chapman