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g and molecular weight cited in ref 36.
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22944457079
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For the PS component, no junction effect is included as we assume that there is no significant difference in the segmental dynamics between a free end group and an end group connected to a (much faster) PI chain. For the PI component, we assume that there are four repeat units near the junction point for which the segmental dynamics are significantly slowed by the connected PS chain. In the Lodge/McLeish model we replace eq 13 with eqs 7 and 8 in ref 32.
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22944454051
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For PB/PVE, an "object" solution of entangled PB in oligomeric PVE and a "mirror" solution of entangled PVE in oligomeric PB were studied (ref 21), and the friction coefficients of the entangled component in each type of blend were extracted. Thus, the terminal activation energies of PB and PVE in Figure 7 are not from the same blend.
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22944479814
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note
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In Figure 7 from left to right, the five systems have thermodynamic interaction parameters (Χ) of -0.004, 0.002, -0.0002. 0.094, and -0.002 (refs 25 and 31).
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22944436685
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note
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0 = 170 K, B = 393 K.
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