Rossi M L, Martini M
Boll Soc Ital Biol Sper. 1984 May 30;60(5):1005-11.
The functional dependence of the semicircular canal upon its physical dimensions was evaluated by measuring the internal radius (r), the radius of curvature (R) and the cupula radius (rC) of the posterior canal in 10 freshly dissected frog labyrinths. These values have been compared to the same parameters of the cat labyrinth. The coefficients I, B, K in the Steinhausen equation were determined for both animals. The A ratio between cupula deflection and endolymph displacement was also calculated by utilizing the Bernard equation. The A ratio is three times larger in the frog than in the cat. It follows that if the same acceleration produces similar endolymph displacements in the posterior canal of both animals, the cupula deflection will be larger in the frog. The solution of the Steinhausen equation in the presence of a constant acceleration, however, reveals that the same stimulus intensity will result in a larger endolymph displacement in the cat posterior canal; similarly, the endolymph displacement directly depends on the duration of the stimulating period in both animals. Contrary to the Bernard assumption, these effects generate a G ratio (psi frog/psi cat) which is less than the Q ratio (A frog/A cat). Moreover, G decreases on increasing the duration of the stimulating period. For stimuli of short duration the semicircular canal of a small animal is expected to exhibit a higher sensitivity than that of a larger one. However, the definitive primary afferent discharge will be largely controlled by the receptor/generator potential properties.
通过测量10个新鲜解剖的青蛙迷路后壶腹嵴的内半径(r)、曲率半径(R)和壶腹嵴半径(rC),评估了半规管对其物理尺寸的功能依赖性。已将这些值与猫迷路的相同参数进行了比较。确定了两种动物的施泰因豪森方程中的系数I、B、K。还利用伯纳德方程计算了壶腹嵴偏转与内淋巴位移之间的A比值。青蛙的A比值比猫的大三倍。由此可见,如果相同的加速度在两种动物的后壶腹嵴中产生相似的内淋巴位移,那么青蛙的壶腹嵴偏转将更大。然而,在存在恒定加速度的情况下,施泰因豪森方程的解表明,相同的刺激强度将在猫的后壶腹嵴中导致更大的内淋巴位移;同样,内淋巴位移在两种动物中都直接取决于刺激期的持续时间。与伯纳德的假设相反,这些效应产生的G比值(青蛙的ψ/猫的ψ)小于Q比值(青蛙的A/猫的A)。此外,G随着刺激期持续时间的增加而减小。对于短持续时间的刺激,预计小动物的半规管比大动物的半规管表现出更高的敏感性。然而,最终的初级传入放电将在很大程度上由受体/发生器电位特性控制。