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本文由粘滞系数的时间关联函数表达式,得到了实验观察到的现象:在液晶N相→SA相转变点附近(T→T(sA)),体粘滞系数的反常发散比切变粘滞系数反常发散要大得多。说明了Brochard等人的理论中,不能解释此实验的原因。Near the N→SA transition point, recent observations show that the anomalous increase in the volume viscosity is much greater than that of the shear viscosity. This is explained in terms of the time correlation function for viscosity. The reason for the disagreement between the experimental results and the Brochard's theory is also given.







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