UNLABELLED: The phase characteristic of the vestibular system of man was determined for sinusoidal oscillation in yaw in the frequency range from 0.0025 to 0.4 Hz. Three different sets of experimental conditions were used: (1) a dark room with a fixation light; stimulus: sinusoidal rotation; (2) a dark room without a fixation light; stimulus: sinusoidal rotation + noise, and (3) a dark room without a fixation light; stimulus; sinusoidal rotation. RESULTS: the sensation leads the velocity by about 90 degrees at 0.005 Hz. The phase lead decreased for higher frequencies becoming nearly zero at 0.05 Hz and remaining constant in the frequency range 0.05 to 0.4 Hz. A phase lag was not found. At very low frequencies (less than 0.005 Hz), the phase lead was more than 90 degrees. The results can be described in terms of a second-order model with time constants Tau1 = 20 sec and Tau2 = 0.013 sec and an adaptation term with a time constant of Taau = 0.40 sec.
UNLABELLED: The phase characteristic of the vestibular system of man was determined for sinusoidal oscillation in yaw in the frequency range from 0.0025 to 0.4 Hz. Three different sets of experimental conditions were used: (1) a dark room with a fixation light; stimulus: sinusoidal rotation; (2) a dark room without a fixation light; stimulus: sinusoidal rotation + noise, and (3) a dark room without a fixation light; stimulus; sinusoidal rotation. RESULTS: the sensation leads the velocity by about 90 degrees at 0.005 Hz. The phase lead decreased for higher frequencies becoming nearly zero at 0.05 Hz and remaining constant in the frequency range 0.05 to 0.4 Hz. A phase lag was not found. At very low frequencies (less than 0.005 Hz), the phase lead was more than 90 degrees. The results can be described in terms of a second-order model with time constants Tau1 = 20 sec and Tau2 = 0.013 sec and an adaptation term with a time constant of Taau = 0.40 sec.