Bishop M F
Department of Physics, Virginia Commonwealth University, Richmond 23284-2000.
Biophys J. 1989 Nov;56(5):911-25. doi: 10.1016/S0006-3495(89)82737-7.
We show that the commonly used Rayleigh-Debye method for calculating light scattering can lead to significant errors when used for describing scattering from dilute solutions of long rigid polymers, errors that can be overcome by use of the easily applied Shifrin approximation. In order to show the extent of the discrepancies between the two methods, we have performed calculations at normal incidence both for polarized and unpolarized incident light with the scattering intensity determined as a function of polarization angle and of scattering angle, assuming that the incident light is in a spectral region where the absorption of hemoglobin is small. When the Shifrin method is used, the calculated intensities using either polarized or unpolarized scattered light give information about the alignment of polymers, a feature that is lost in the Rayleigh-Debye approximation because the effect of the asymmetric shape of the scatterer on the incoming polarized electric field is ignored. Using sickle hemoglobin polymers as an example, we have calculated the intensity of light scattering using both approaches and found that, for totally aligned polymers within parallel planes, the difference can be as large as 25%, when the incident electric field is perpendicular to the polymers, for near forward or near backward scattering (0 degrees or 180 degrees scattering angle), but becomes zero as the scattering angle approaches 90 degrees. For randomly oriented polymers within a plane, or for incident unpolarized light for either totally oriented or randomly oriented polymers, the difference between the two results for near forward or near backward scattering is approximately 15%.
我们表明,常用的用于计算光散射的瑞利 - 德拜方法在用于描述长刚性聚合物稀溶液的散射时会导致显著误差,而使用易于应用的希夫林近似可以克服这些误差。为了展示这两种方法之间差异的程度,我们在垂直入射的情况下,针对偏振和非偏振入射光进行了计算,散射强度被确定为偏振角和散射角的函数,假设入射光处于血红蛋白吸收较小的光谱区域。当使用希夫林方法时,使用偏振或非偏振散射光计算出的强度会给出有关聚合物排列的信息,而这一特征在瑞利 - 德拜近似中会丢失,因为散射体不对称形状对入射偏振电场的影响被忽略了。以镰状血红蛋白聚合物为例,我们使用两种方法计算了光散射强度,发现对于平行平面内完全排列的聚合物,当入射电场垂直于聚合物时,在近前向或近后向散射(0度或180度散射角)时,差异可高达25%,但随着散射角接近90度差异变为零。对于平面内随机取向的聚合物,或者对于完全取向或随机取向聚合物的非偏振入射光,近前向或近后向散射时两种结果之间的差异约为15%。