Researches Into the Theory of Probability

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Oharlier.
4:o. The quantifies X and lo are so determined that B^ = B^ = 0, whereas c is chosen arbitrarily.
The method 3:o may seem to be the best one, but has the inconvenience of giving to CO very small values and to X very large ones, when v, is vanishing. Hence it is not applicable when the curve differs little from the uormal-form. The following method seems to have a general applicability and has also the advantage of a certain similarity with the process used for the curves of type A.
We
... begin with choosing a determinate value for the quantity c. In many cases it will he found convenient to identify c with the abscissa of the discontinuous end of the frequency curve.
When the value of the quantity c is determined (and it must be borne in mind that this determination is to a certain degree arbitrary) we dispose of X and w in such a manner that the coefficients B^ and B^ vanish. According to (14) we thus get the equations of condition f24] = Xcofio" — iJ./', ' = X^a)^lV'-(2X+l)o)[i./' + (x,".


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