The theory of the fibrogram has been derived based on the probability of randomly catching and holding a fiber. The amount axis has been shown to be proportional to the relative mass when related to the original specimen. Tangential equations are used to show that theoretically, for a length l or longer, the proportional mass, the mean length by number, the relative number, and the mean length by mass of fibers in the sample can be obtained from the fibrogram, as well as the number and mass arrays. Finally, the theoretical percentage of fiber by number or by mass extending a length l or longer from a clamped random sliver of the sample is obtainable from the fibrogram.The theory of the fibrogram was first published by . Hertel [2]. He considered the abscissa as the length axis and stated that the ordinate for I = 0 is NL where N is the total number of fibers in the sample and L is their mean length by number. This multiple is equivalent to the total length of all the fibers. Since Hertel presented this theory, this axis has been considered as the weight axis [6,7], the number or relative number axis [1, 2, 3, 4], or the probability axis [6,8]. In this work, we show that the ordinate axis can be considered as a proportional mass or mass probability axis, and we examine the fibrogram for additional information pertaining to the length of the sample. ' . Theory . Statistical texts generally write P[x) for the probability that the stochastic variable is less than or equal to the real number x. P[x] is called the cumulative distribution function of the variable. The derivative is called the distribution function of x.The general function that leads to the fibrogram must be defined differently. Consider the probability that the stochastic variable is greater than or equal to the real number l; q[l is then the complement of the cumulative distribution function. Since the fibrogram relates to fiber lengths, constraints must be applied to q[/]. Fibers shorter than 0 and longer than the longest fiber within the sample do not exist. The constraints applied to the probability q[I are that where 1m is the length of the longest fiber(s) in the sample. q[l is then the probability of the existence of a fiber in the sample having a length I or longer. The derivative is the distribution function of l.Since the total number of fibers in the sample is N, where N(l ) is the number of fibers in the sample having a length equal to I or longer. This gives Differentiating Q(1) gives the frequency distribution or