436 THE FACTORS OF THE MIND The peculiarities of the index of measurement will be perceived more clearly if we compare the actual frequencies with the normal. From the ordinary table of the probability integral, we can deter- mine precisely what frequencies would be required in theory by a normal distribution having the same mean and the same standard deviation as the present group. These theoretical percentages are printed in Table VI immediately beneath the percentages actually obtained. Since they have been calculated by taking the correla- tions just as they stand, I have labelled them * -/-method.' Evi- dently the fit is far from good. In particular the theoretical distribution, reconstructed in this way, inevitably yields frequencies beyond the values of + POO and — roo. But a coefficient of correlation, of course, cannot go beyond either of these limits, Hence, if our index of measurement is to be expressed in the form of a correlation, true normality is precluded from the outset; and we discover at once an obvious reason for the bunching at the tails, We may, however, remove this limitation by a simple device. We may adopt for our conventional measure, not the correlation coefficient itself, but the number having this coefficient for its hyperbolic tangent. The range of the numbers so derived is un- limited in both directions ; and, as is well known, their sampling distribution conforms almost exactly with the normal curve (cf. [no], p. 451 and refs.). Let us then apply this conversion. We take for our adjusted measure x T_~I 11 i + r . r3 , r5 , r7 , z = tanh x r = \ log, —•— = r-)------1------1------\- ... i —' 357 where r is the correlation (or saturation coefficient) and z the substituted measurement. In terms of z, the mean for the entire group is now *o6 and the standard deviation -62. The size of the standard deviation is alone sufficient to dispose of any notion that the original assessments may have been assigned practically at random: for, in that case, with correlations based on n =» 11 1 I give various equivalent expressions, since different students may prefer to adopt different methods of making the transformation. Full tables of the hyperbolic tangent will be found in Smithsonian Mathematical Tables; Hyperbolic Functions, pp. 86 et seg.; or the calculation may be made from any sixpenny set of mathematical tables that includes * natural, hyperbolic, or Napierian logarithms' or the * exponential function.' Table VB in Fisher's StatisticalMethods for Research Workers (p. 197) may also be used, if available : for such work as the present, however, this involves interpolation ; hence we find it more convenient to employ a specially compiled table giving z values for r instead of vice versa.