TY - GEN
T1 - The re-entry of disordered phases in a crystalline polymer (poly-4-methyl pentene-1)
AU - Rastogi, S.
AU - Newman, M.
AU - Keller, A.
AU - Hikosaka, M.
PY - 1993
Y1 - 1993
N2 - In situ x-ray expts. are reported on a cryst. polymer, poly(4-methylpentene-1) (I) as a function of pressure (P) and temp. (T) carried out under isothermal and isobaric conditions. At room temp., when the cryst. tetragonal phase (Ct) of I is subjected to pressure, it passes through a range of mesomorphic phases leading to complete amorphization. The melting temp. (Tm) gradually increases with P up to 3Kb where the trend reverses on further increase in P leading to a decrease in Tm. This, combined with the pressure-induced amorphization at room temp. raises the possibility of reentrant of 2 widely sepd. regions of disordered phases (along the T axis) in the P-T phase diagram. This effect, namely a reentrant of disordered phases, i.e. disordering setting in on isobaric cooling, at appropriately elevated P, was in fact obsd. exptl. In the course of the above expts. a new hexagonal crystal (Ch) phase was identified lying between Ct and the low T disordered phase along the T axis of P-T phase diagram. This Ch phase is attainable along 2 routes with basically different characteristics. Also, there is a triple point where the liq., Ct, and Ch phases are in equil. Recently similar observations were reported for inorg. materials such as silicates, phosphates, sulfates, and ice-water (the latter at low T and high P), so that the newly recognized behavior pattern seems to be of wider generality beyond the subject of polymers. [on SciFinder (R)]
AB - In situ x-ray expts. are reported on a cryst. polymer, poly(4-methylpentene-1) (I) as a function of pressure (P) and temp. (T) carried out under isothermal and isobaric conditions. At room temp., when the cryst. tetragonal phase (Ct) of I is subjected to pressure, it passes through a range of mesomorphic phases leading to complete amorphization. The melting temp. (Tm) gradually increases with P up to 3Kb where the trend reverses on further increase in P leading to a decrease in Tm. This, combined with the pressure-induced amorphization at room temp. raises the possibility of reentrant of 2 widely sepd. regions of disordered phases (along the T axis) in the P-T phase diagram. This effect, namely a reentrant of disordered phases, i.e. disordering setting in on isobaric cooling, at appropriately elevated P, was in fact obsd. exptl. In the course of the above expts. a new hexagonal crystal (Ch) phase was identified lying between Ct and the low T disordered phase along the T axis of P-T phase diagram. This Ch phase is attainable along 2 routes with basically different characteristics. Also, there is a triple point where the liq., Ct, and Ch phases are in equil. Recently similar observations were reported for inorg. materials such as silicates, phosphates, sulfates, and ice-water (the latter at low T and high P), so that the newly recognized behavior pattern seems to be of wider generality beyond the subject of polymers. [on SciFinder (R)]
M3 - Conference contribution
SN - 0-7923-2350-5
T3 - NATO ASI Series, Series C: Mathematical and Physical Sciences
SP - 135
EP - 140
BT - Crystallization of polymers : [proceedings of the NATO Advanced Research Workshop on Crystallization of Polymers, Mons, Belgium]
A2 - Dosiére, M.
PB - Kluwer Academic Publishers
CY - Dordrecht
T2 - conference; NATO Advanced Research Workshop on Crystallization of Polymers ; (Mons) : 1992.09.07-11; 1993-09-07; 1993-09-11
Y2 - 7 September 1993 through 11 September 1993
ER -