Ultrasonically induced birefringence in polystyrene-toluene solution was measured as a function of intensities. The birefringence signal was observed by the "nonbiased" and "biased" detection techniques. The values of birefringence obtained by the nonbiased detection technique were proportional to the ultrasonic amplitude, that is, the square root of the ultrasonic intensity and their intensity dependence was in accordance with those obtained by Jerrard (Ultrasonics 2 (1964) 74). The birefringence signal was successfully observed by the biased detection technique and its value was proportional to the square of the ultrasonic amplitude, that is, the ultrasonic intensity. In polymer solutions, two types of birefringence were induced; one was due to linear and the other was due to nonlinear origins.