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Amorphous water quenching

Now take another batch of sulphur flowers, but this time heat it well past its melting point. The liquid sulphur gets darker in colour and becomes more and more viscous. Just before the liquid becomes completely unpourable it is decanted into a dish of cold water, quenching it. When we test the properties of this quenched sulphur we find that we have produced a tough and rubbery substance. We have, in fact, produced an amorphous form of sulphur with radically altered properties. [Pg.97]

In conclusion, the deformation behavior of poly(hexamethylene sebacate), HMS, can be altered from ductile to brittle by variation of crystallization conditions without significant variation of percent crystallinity. Banded and nonbanded spherulitic morphology samples crystallized at 52°C and 60°C fail at a strain of 0.01 in./in. whereas ice-water-quenched HMS does not fail at a strain of 1.40 in./in. The change in deformation behavior is attributed primarily to an increased population of tie molecules and/or tie fibrils with decreasing crystallization temperature which is related to variation of lamellar and spherulitic dimensions. This ductile-brittle transformation is not caused by volume or enthalpy relaxation as reported for glassy amorphous polymers. Nor is a series of molecular weights, temperatures, strain rates, etc. required to observe this transition. Also, the quenched HMS is transformed from the normal creamy white opaque appearance of HMS to a translucent appearance after deformation. [Pg.126]

Thin (less than 1/8 in. thick) Kel-F sheetstockcan be developed to any degree of crystallinity. The most amorphous material results from a cold water quench of a sample previously heated to a temperature above its melting point (412 F). The most crystalline material results from a gradual oven-cooling of a sample previously exposed for aprolonged time at a temperature between 385 and 410"F. This temperature allows for crystallite growth in the polymer. [Pg.630]

Fig. 131. Change in aa a function of water quenching temperature (Jq) for an amorphous LajsAljjNijo alloy embrittled upon annealing for 1.8 ks at 4S0 K. Fig. 131. Change in aa a function of water quenching temperature (Jq) for an amorphous LajsAljjNijo alloy embrittled upon annealing for 1.8 ks at 4S0 K.
Fig, 132. Tensile fracture surface appearance of an amorphous LajsAljsNijo alloy (a) melt-spun (b) annealed for 1.8 ks at 450 K (c) water-quenched from SlOK after annealing for l.Sks at 4S0K.. [Pg.207]

Fig. 133. The temperature dependence of apparent specific heat of an amorphous LasjAljjNijo alloy subjected to water quenching fiom different temperatures between 450 and 540 K. after annealing for 1.8 ks at 4501C. The data of C, and are also shown for comparison. Fig. 133. The temperature dependence of apparent specific heat of an amorphous LasjAljjNijo alloy subjected to water quenching fiom different temperatures between 450 and 540 K. after annealing for 1.8 ks at 4501C. The data of C, and are also shown for comparison.
Transitions. Samples containing 50 mol % tetrafluoroethylene with ca 92% alternation were quenched in ice water or cooled slowly from the melt to minimise or maximize crystallinity, respectively (19). Internal motions were studied by dynamic mechanical and dielectric measurements, and by nuclear magnetic resonance. The dynamic mechanical behavior showed that the CC relaxation occurs at 110°C in the quenched sample in the slowly cooled sample it is shifted to 135°C. The P relaxation appears near —25°C. The y relaxation at — 120°C in the quenched sample is reduced in peak height in the slowly cooled sample and shifted to a slightly higher temperature. The CC and y relaxations reflect motions in the amorphous regions, whereas the P relaxation occurs in the crystalline regions. The y relaxation at — 120°C in dynamic mechanical measurements at 1 H2 appears at —35°C in dielectric measurements at 10 H2. The temperature of the CC relaxation varies from 145°C at 100 H2 to 170°C at 10 H2. In the mechanical measurement, it is 110°C. There is no evidence for relaxation in the dielectric data. [Pg.366]

Extrusion Resins. Extmsion of VDC—VC copolymers is the main fabrication technique for filaments, films, rods, and tubing or pipe, and involves the same concerns for thermal degradation, streamlined flow, and noncatalytic materials of constmction as described for injection-molding resins (84,122). The plastic leaves the extmsion die in a completely amorphous condition and is maintained in this state by quenching in a water bath to about 10°C, thereby inhibiting recrystallization. In this state, the plastic is soft, weak, and pHable. If it is allowed to remain at room temperature, it hardens gradually and recrystallizes partially at a slow rate with a random crystal arrangement. Heat treatment can be used to recrystallize at controlled rates. [Pg.441]


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See also in sourсe #XX -- [ Pg.190 , Pg.203 , Pg.204 , Pg.205 , Pg.206 , Pg.207 , Pg.208 ]




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