Kimura Y, Fujiwara M, Ikegami A
Biophys J. 1984 Mar;45(3):615-25. doi: 10.1016/S0006-3495(84)84200-9.
Purple membrane suspension shows two different orientations in electric fields of different frequencies. The orientation at low frequencies (less than or equal to approximately 10 Hz), with the membrane surface perpendicular to the electric field, is due to permanent dipole moment of the membrane and the orientation at high frequencies (greater than or equal to approximately 100 Hz), with the surface parallel to the electric field, is due to induced dipole moment. By quantitative analysis of these orientations, we determined the permanent dipole moment and the polarizability. Both values varied according to the membrane size: the permanent dipole moment ranged from 500 kD to 10 MD and was proportional to the square of the diameter of the membrane. The polarizability ranged from 1 X 10(-13) to 1 X 10(-11)cm3 and was proportional to the third to fourth power of the diameter. Because the permanent dipole moment was proportional to the area of the membrane, we could determine permanent dipole moment per bacteriorhodopsin. By determining the actual membrane size under electron microscopy, we got 98 D/bacteriorhodopsin. We also concluded that the direction of the permanent dipole moment was from the cytoplasmic to the extracellular side. These values, however, were strongly dependent on the ionic strength in the medium, suggesting a screening effect due to counter ions near the membrane surface. We evaluated the screening effect and showed about a four-charge difference between the two sides of the purple membrane. Under illumination, we found that the permanent dipole moment decreased from 98 to 63 D/bacteriorhodopsin. From the best-oriented sample, we also concluded that the angle of retinal against the axis normal to the membrane surface was greater than 68.6 degrees.
紫膜悬浮液在不同频率的电场中呈现出两种不同的取向。低频(小于或等于约10 Hz)时,膜表面垂直于电场,这种取向是由于膜的永久偶极矩;高频(大于或等于约100 Hz)时,膜表面平行于电场,这种取向是由于诱导偶极矩。通过对这些取向进行定量分析,我们确定了永久偶极矩和极化率。这两个值均随膜尺寸而变化:永久偶极矩范围为500 kD至10 MD,且与膜直径的平方成正比。极化率范围为1×10⁻¹³至1×10⁻¹¹ cm³,且与直径的三次方至四次方成正比。由于永久偶极矩与膜面积成正比,我们能够确定每个细菌视紫红质的永久偶极矩。通过在电子显微镜下确定实际膜尺寸,我们得到每个细菌视紫红质为98 D。我们还得出结论,永久偶极矩的方向是从细胞质侧指向细胞外侧。然而,这些值强烈依赖于介质中的离子强度,这表明膜表面附近的反离子具有屏蔽效应。我们评估了屏蔽效应,并表明紫膜两侧存在约四个电荷的差异。在光照下,我们发现每个细菌视紫红质的永久偶极矩从98 D降至63 D。从最佳取向的样品中,我们还得出结论,视黄醛相对于垂直于膜表面的轴的角度大于68.6度。