Pulse distortion is due to nonlinear wave number functions of the frequency. For the case of smooth nonlinear wave numbers, a sequence of approximations to the propagation operator which carries the incident pulse to the distorted output pulse is set forth. When applied to the actual incident pulse, they allow the study of the development of the distortion with (a) increasing travel length in the propagation medium and (b) also with respect to the properties of the propagation medium. Of special interest are Gaussian incident pulses for which the distorted pulse form is more concisely representable.