A new quantity termed the ''practical peak voltage'' is proposed. This
quantity is derived by equating the low level contrast in an exposure
made with an X-ray tube connected to a generator delivering any arbit
rary wave form, to the contrast produced by the same X-ray tube connec
ted to a constant potential generator. Out of the great number of poss
ible contrast configurations one is selected as being suitable for dia
gnostic radiology. By means of an eigenvalue problem a direct link is
established between the electrical quantity X-ray tube voltage and the
practical peak voltage which was initially defined through the proper
ties of the X-ray field. It is shown that the spread in total X-ray tu
be filtration as encountered in medical diagnostic radiology can influ
ence the result of a measurement of the practical peak voltage only ma
rginally.