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首页> 外文期刊>Polymer: The International Journal for the Science and Technology of Polymers >Elongational flow birefringence of poly(methyl methacrylate)/poly(vinylidene fluoride-co-hexafluoro acetone) blends
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Elongational flow birefringence of poly(methyl methacrylate)/poly(vinylidene fluoride-co-hexafluoro acetone) blends

机译:聚(甲基丙烯酸甲酯)/聚(偏二氟乙烯-共六氟丙酮)共混物的伸长流动双折射

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For blends of a poly(methyl methacrylate) (PMMA) and a poly(vinylidene fluoride-co-hexafluoro acetone) [P(VDF-HFA)], we examined phase behavior and crystalline melting (T_m) and glass transition (T_g) temperatures. In the range 130-160 deg C, which is a miscible one-phase region between their lower critical solution temperature (LCST: T_c = 220 deg C; #phi#_c approx= 0.5) and T_m (approx= 120 deg C) of P(VDF-HFA), simultaneous measurements of transient tensile stress #sigma#(t) and birefringence #DELTA#n(t) were conducted via elongational flow opto-rheometry (EFOR) on the blends under uniaxial elongation at constant Hencky strain rates. The stress optical coefficient C(t)(ident to #DELTA#n(t)/#sigma#(t)) increased monotonically with increasing volume fraction #phi#_(P(VDF-HFA)) of P(VDF-HFA) in the blend. Molten PMMA/P(VDF-HFA) blends in the one-phase region appear to follow the stress optical rule with C(t) obeying the simple additivity: C(t) = C_(P(VDF-HFA))#phi#_(P(VDF-HFA)) + C_(PMMA)#phi#_(PMMA) with the suffices being relevant to each component. The value of C(t) extrapolated to #phi#_(P(VDF-HFA)) = 1 yielded C_(P(VDF-HFA)) = 6.5 * 10~(-9) Pa~(-1). The C(t) vs #phi#_(P(VDF-HFA)) behavior suggested that C(t) can be zero for the (97/3) blend or the addition of only 3% P(VDF-HFA) to PMMA makes the blend non-birefringent. Thus, P(VDF-HFA) can be an optimal modifier when PMMA is used as a high-technology optical material, e.g., optical discs and lenses.
机译:对于聚甲基丙烯酸甲酯(PMMA)和聚偏二氟乙烯-共六氟丙酮[P(VDF-HFA)]的共混物,我们研究了相行为,晶体熔化(T_m)和玻璃化转变(T_g)温度。在130-160摄氏度的范围内,这是它们的下临界溶液温度(LCST:T_c = 220摄氏度;#phi#_c大约= 0.5)和T_m(大约= 120摄氏度)之间的可混溶一相区域。 P(VDF-HFA),瞬态拉伸应力#sigma#(t)和双折射#DEL#n(t)的测量是通过伸长流动光度法(EFOR)在恒定Hencky应变率下在单轴伸长率下进行的。应力光学系数C(t)(与#DEL#n(t)/#sigma#(t)相同)随着P(VDF-HFA)的体积分数#phi #_(P(VDF-HFA))的增加而单调增加。 )。在单相区域中,熔融的PMMA / P(VD​​F-HFA)共混物似乎遵循应力光学法则,其中C(t)遵循简单的可加性:C(t)= C_(P(VDF-HFA))#phi# _(P(VDF-HFA))+ C_(PMMA)#phi #_(PMMA),并且与每个组件都有关。将C(t)的值外推到#phi #_(P(VDF-HFA))= 1得到C_(P(VDF-HFA))= 6.5 * 10〜(-9)Pa〜(-1)。 C(t)与#phi #_(P(VDF-HFA))的行为表明,对于(97/3)混合,或仅向其中添加3%P(VDF-HFA),C(t)可以为零。 PMMA使混合物非双折射。因此,当将PMMA用作高科技光学材料(例如光盘和透镜)时,P(VDF-HFA)可能是最佳的改性剂。

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