Note – When the material is air, μ en ρ MathType@MTEF@5@5@+=feaagCart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHXgaruavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGeaGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaqFn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpeWZqaaeaaciWacmGadaGadeaabaGaaqaaaOqaamaalaaabaGaeqiVd02aaSbaaSqaaiaabwgacaqGUbaabeaaaOqaaiabeg8aYbaaaaa@3AE3@ is proportional to the quotient of exposure by energy fluence in the usual case of constant W.
Note – Lorsque cette substance est l'air, μ en ρ MathType@MTEF@5@5@+=feaagCart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbbjxAHXgaruavP1wzZbItLDhis9wBH5garmWu51MyVXgarqqtubsr4rNCHbGeaGqipG0dh9qqWrVepG0dbbL8F4rqqrVepeea0xe9LqFf0xc9q8qqaqFn0lXdHiVcFbIOFHK8Feea0dXdar=Jb9hs0dXdHuk9fr=xfr=xfrpeWZqaaeaaciWacmGadaGadeaabaGaaqaaaOqaamaalaaabaGaeqiVd02aaSbaaSqaaiaabwgacaqGUbaabeaaaOqaaiabeg8aYbaaaaa@3AE3@ est proportionnel au quotient de l'exposition par la fluence énergétique dans le cas habituel où l'énergie moyenne par paire d'ions W est constante.