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Polyethylene temperature rise

Sometimes technological problems forbid the size of an operation to exceed a certain value. For instance, in the batch polymerization of polyethylene and polystyrene, it is important to maintain the temperature below a critical value, because otherwise the material will be damaged. Since this is an exothermic reaction, it means the energy must be removed as fast as it is formed. If it is not, the temperature will begin to rise, which will increase the rate of polymerization. This will result in an acceleration of the temperature rise and the result will be a discolored batch. This requirement establishes a limit on the size of the reactor. The practical significance is demonstrated in the polystyrene case-study example following Chapter 5. [Pg.64]

Small areas Ventilate to remove vapor. Because the boiling point of some cyanide agents is near normal room temperature (70°F), agent vapors may condense on cooler surfaces and pose a percutaneous hazard. Liquids can then revolatilize when the temperature rises. If deemed necessary, wash the area with copious amounts of soap and water. Collect and place the rinseate and place in containers lined with high-density polyethylene. [Pg.237]

Neat thermoplastic polyethylenes have low moduli that involve high strains for moderate loading. Consequently, creep moduli are also low, the more so as the temperature rises, as we can see in Figures 4.3 ((a) and (b)) where creep moduli are displayed as a function of time, load and temperature. [Pg.224]

Figure 3. Thermoluminescence in polyethylene. The spectrum comprises both fluorescent (F) and phosphorescent (P) components. Contribution of P falls as the temperature rises owing to competitive, non-radiative processes. Polyethylene alkathene 20, no 02, dose 0.8 Mrad, heating rate 2.7°/min. Temperature in °K. Intensities not to same scale. Figure 3. Thermoluminescence in polyethylene. The spectrum comprises both fluorescent (F) and phosphorescent (P) components. Contribution of P falls as the temperature rises owing to competitive, non-radiative processes. Polyethylene alkathene 20, no 02, dose 0.8 Mrad, heating rate 2.7°/min. Temperature in °K. Intensities not to same scale.
Whereas in the example just described the sample amount was about 50 mg, a similar procedure developed by another group 129) started with 4 g polyethylene copolymer. The sample was applied as a dilute solution in xylene and precipitated by very slow cooling (1.5 K/h) onto the Chromosorb P packing of a 500 x 127 mm column. The first separation was temperature-rising elution fractionation at a flow-rate of 20 ml/min and a Unear temperature increase by 8 K/h. The MMD of the fractions was measured by SEC at 145 °C in o-dichlorobenzene at 0.7 ml/min flow rate. The column set included a pair of bimodal columns 100 A and 1000 A plus a 4000 A column. The apparatus was equipped with an IR detector. The experimental data is computed to show the distribution of short-chain branching and of molar mass simultaneously. [Pg.205]

B. If the process were adiabatic, what would be the temperature rise The heat capacity of polyethylene is 2 kJ/kg °C. [Pg.143]

Alternatively physical separation may be realized by encapsulating the softener in a high-melting matrix such as paraffin wax, high-molecular-weight polyethylene glycol, or fatty acid triglycerides. The softener is released in the liquor as the temperature rises at the end of the wash, when the soil has already been removed. [Pg.518]

Samples to be irradiated in the electron accelerator were placed in a pyrex dish which was then covered and sealed with polyethylene film. The apparatus was continuously flushed with nitrogen during irradiation. Provision was made for monitoring the temperature rise during irradiation by drilling a small hole into the side of the sodium chloride plate and inserting a chromel alumel thermocouple which was connected to a digital voltmeter located outside the irradiation area. Temperature rise was monitored in this manner with the thermocouple in several different positions. [Pg.138]

As indicated in the introduction there is a distinct correlation between the commercial growth of linear low density polyethylene and the resurgence of interest in the temperature rising elution fractionation technique. It is clear, however, from the wide variety of examples noted in this review that the scope of TREF extends well beyond the LLDPE area. Since the TREF technique is becoming available to many more research workers it is anticipated that there will be continued growth and development which will lead to greater sophistication in the way the technique is utilized, particularly in the polyolefin area. The power of TREF for blend analysis and cross-fractionation is certain to be exploited in the coming years. [Pg.46]

E.C. Kelusky, C.T. Elston, R.E. Murray, Characterizing polyethylene-based blends with temperature rising elution fractionation (TREF) techniques. Polym. Eng. Sci. 27(20), 1562-1571 (1987)... [Pg.1723]

H. Mahdavi, M.E. Nook, Characterization and microstructure study of low-density polyethylene by Fourier transform infiared spectroscopy and temperature rising elution riactionation. J. Appl. Polym. Sci. 109, 3492-3501 (2008)... [Pg.1725]

B. Monrabal, P. del Hierro, Characterization of polypropylene-polyethylene blends by temperature rising elution and crystallization analysis fractionation. Anal. Bioanal. Chem. 399, 1557-1561 (2011)... [Pg.1726]


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