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Melting temperature, change with

In reality, the temperature distribution is dynamic in other words, melt temperature changes with time. These changes can be significant, but short-term (0-10 seconds) temperature changes cannot be measured with a conventional melt temperature sensor because the thermal mass of the probe is too large. Infrared melt temperature measurement allows detection of rapid (millisecond range) melt temperature fluctuation [114-118]. [Pg.627]

Under certain pressure and temperature conditions, a system can contain two or more phases in equilibrium. An example is the temperature and pressure where solid and liquid are in equilibrium. We refer to this condition as (solid + liquid) equilibrium, and the temperature as the melting temperature. This temperature changes with pressure and with composition. The melting temperature when the... [Pg.231]

Fig. 5. Temperature dependence of the entropy difference between various supercooled liquids and their stable crystals, A5. is the entropy change upon melting, and is the melting temperature. (Reprinted with permission from W. Kauzmann. The nature of the glassy state and the behavior of liquids at low temperatures. Chem. Rev. (1948) 43 219. Copyright 1948, American Chemical Society.)... Fig. 5. Temperature dependence of the entropy difference between various supercooled liquids and their stable crystals, A5. is the entropy change upon melting, and is the melting temperature. (Reprinted with permission from W. Kauzmann. The nature of the glassy state and the behavior of liquids at low temperatures. Chem. Rev. (1948) 43 219. Copyright 1948, American Chemical Society.)...
Fig. 4. In-sample temperature change with elapsed time after the commencement of heating hydrated phosphatidylethanolamine (a, b) and water (c) samples contained in 1 mm diameter capillaries using a temperature-regulated coaxial air stream. The thermal lag in (a) and (b) is due to the diversion of heat away from raising sample temperature and into chain melting which accounts for most of the enthalpy of the transition at 66 °C. T-jumps were from 30 °C to 92 °C (a, c) and 125 °C (b). The inset shows the calculated temperature profile across the capillary diameter in (a) as a function of time in seconds following the T-jump. Adapted from Ref. [31]... Fig. 4. In-sample temperature change with elapsed time after the commencement of heating hydrated phosphatidylethanolamine (a, b) and water (c) samples contained in 1 mm diameter capillaries using a temperature-regulated coaxial air stream. The thermal lag in (a) and (b) is due to the diversion of heat away from raising sample temperature and into chain melting which accounts for most of the enthalpy of the transition at 66 °C. T-jumps were from 30 °C to 92 °C (a, c) and 125 °C (b). The inset shows the calculated temperature profile across the capillary diameter in (a) as a function of time in seconds following the T-jump. Adapted from Ref. [31]...
The main causes of reduced output are increased flow restriction, commonly a result of clogged screens and screw wear. As screens perform their function properly and capture contaminants in the melt stream, they create an increased restriction to flow through the system. This increased restriction will result in higher head pressure. Additionally, there will be more recirculation of melt in the screw channel and less throughput. As discussed above in the section on high melt temperature, changing the screens should alleviate this problem. It is possible that other sources of flow restriction could exist, such as screens with an incorrect mesh size or a valve in the extruder head. [Pg.124]

The elements of an infrared melt temperature sensor are a sapphire window, an optical fiber, and a radiation sensor with associated signal-conditioning electronics as shown in Fig. 4.17. IR melt temperature probes are commercially available [85, 86] and fit in standard pressure transducer mounting holes. Because the sapphire window is flush with the barrel or die, the sensor does not protrude into the polymer melt. As a result, the sensor is less susceptible to damage, there is no chance of dead spots behind the sensor, and the melt velocities are not altered around the sensor. When melt velocities are changed, the melt temperatures will change as well. Therefore, the melt temperatures measured with an IR sensor are less affected by the actual measurement than with an immersion sensor. [Pg.106]

The effect of barrel temperature on melting performance can be predicted in a quantitative way. Figure 7.42 shows how the melting rate changes with barrel temperature for two values of the Nahme number as expressed by Eq. 7.f43. Low Nahme numbers indicate little viscous dissipation, while high Nahme numbers correspond to high levels of viscous dissipation. [Pg.324]

Figure 7.89 shows how the melt temperature changes over distance for several values of the temperature coefficient (a). For very low values of a, the melt temperature Increases linearly with distance. This corresponds to the temperature profile for a temperature independent fluid. [Pg.393]

It should be noted that there are several simplifying assumptions in the analysis. We have assumed that the melt temperatures are uniform across the depth of the channel. In reality this is not the case in fact, large melt temperature changes can occur across the depth of the channel. We can assume that the melt temperature calculated with this analysis corresponds to a bulk average melt temperature. We have also assumed that the fully developed melt temperature is reached before the end of the extruder. This is a reasonable assumption for small diameter extruders however, this may not be a good assumption for large diameter extruders as discussed in the previous section. [Pg.411]

Short-term melt temperature changes can be measured with fast-response thermocouples. A number of studies using a fast-response thermocouple mesh were conducted at Polymer IRC, School of Engineering, Design, and Technology at the University of Bradford, England [121-125]. In these studies, dynamic melt temperatures... [Pg.627]

Here AVm is the difference in the molar volumes of the two phases. The temperature T in this equation is the transition temperature, the boiling point, melting point, etc. This equation tells us how the transition temperature changes with pressure. For a transition from a solid to a liquid in which there is an increase in the molar volume (AT > 0), the freezing point will increase (dr > 0) when the pressure is increased dp > 0) if there is a decrease in the molar volume, the opposite will happen. [Pg.179]

The consequences for the incorporation of chlorine atoms at precise intervals along polyethylene s backbone are much more severe (Boz et al, 2007b). There is a marked decrease in melting temperature compared with both ADMET PE and the precise fluorine family. There is also a change in crystal structure, from orthorhombic to triclinic. Solid-state data show that... [Pg.324]


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