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Shifted temperature scale

Figure 15.1a shows a single-stage evaporator represented on both actual and shifted temperature scales. Note that in shifted temperature scale, the evaporation and condensjftion duties are shown at different temperatures even though they are at the same actual temperature. Figure 15.16 shows a similar plot for a three-stage evaporator. [Pg.355]

The same information can be used for drawing the diagram Grand Composite Curve (Figure 10.1-right). Here the difference between the enthalpy of the hot and cold streams is plotted against a conventional shifted temperature scale. This representation identifies the possibilities of heat recovery by internal process/process exchange, as well as the optimal selection and placement of utilities. [Pg.395]

Firstly, the temperature scale is modified such to accommodate a minimum driving force (Fig. 10.11). Hot streams are represented on the left scale. Cold streams are plotted on the right scale, where the temperature is shifted with AT , say by convenience with 10°C. Both hot and cold streams can be referred to shifted temperature scale, where the hot stream temperatures are moved down with AT , /1, and the cold stream temperatures shifted up with AT, f2. [Pg.402]

With the information issued from the Problem Table, we can draw the Grand Composite Curve (GCC). A composite curve is obtained by plotting the heat content of each temperature interval (x-axis) against shifted temperature scale (y-axis). As mentioned, the shifted temperature scale takes into account a difference of between hot and cold streams. Figure 10.14 presents GCC corresponding to the streams given in Table 10.1 for 7 , =10 °C. The following observations are of interest ... [Pg.405]

Figure 6.2 Temperature-interval diagram (TID) with shifted temperature scales. Figure 6.2 Temperature-interval diagram (TID) with shifted temperature scales.
The volume of a gas would theoretically be zero at a temperature of approximately -273°C or -460°F. Tliis temperature, wliich lias become known as absolute zero, is tlie basis for tlie definition of two absolute temperature scales, tlie Kelvin (K) and Rankine (°R) scales. The former is defined by shifting tlie Celsius scale by 273-Celsius degrees so that 0 K is equal to -273°C. Equation (4.2.3) shows tliis relation. [Pg.112]

Figure I 1.6. Master viscosity curve produced by superposing all data for all systems. Viscosity data taken at 175 °C have been shifted to 150°C by employing the temperature scaling factor aT for pure polystyrene. The master viscosity curve is identical to the viscosity curve for pure polystyrene at 1 atm and 150 °C, which is displayed as the solid line. Data from Kwag (1998). Figure I 1.6. Master viscosity curve produced by superposing all data for all systems. Viscosity data taken at 175 °C have been shifted to 150°C by employing the temperature scaling factor aT for pure polystyrene. The master viscosity curve is identical to the viscosity curve for pure polystyrene at 1 atm and 150 °C, which is displayed as the solid line. Data from Kwag (1998).
TMS cannot be used in aqueous solution because it is not water soluble. For a chemical-shift reference, a water-soluble equivalent (such as sodium d4-3-trimethylsilylpropanoate ((CH3)3SiCD2CD2C02-Na l, TSP )) can be added the single H peak is defined as zero ppm in water. The water peak itself can also be used as a chemical-shift reference, but care must be taken to correct for the temperature dependence of its chemical shift. Referencing of 13C and 15N chemical shifts can be done by using an accurate H reference. If the exact chemical shift is known at the center of the H spectral window (usually the water resonance), the precise radio frequency can be calculated for the zero point of the XH chemical-shift (ppm) scale. For example, on a 600 MHz spectrometer with a reference frequency of 600.13231564 MHz and a water chemical shift of 4.755 ppm ... [Pg.565]

Figure 4. Tan vs. temperature curves at 3.5 Hz for the diblocks and homopolymers. The scale on the ordinate corresponds to the bottom curve only, the other curves have been shifted upwards for clarity. The two arrows along the temperature scale indicate the polybutadiene (—82°C) and polyisoprene (—49°C) transitions. Figure 4. Tan vs. temperature curves at 3.5 Hz for the diblocks and homopolymers. The scale on the ordinate corresponds to the bottom curve only, the other curves have been shifted upwards for clarity. The two arrows along the temperature scale indicate the polybutadiene (—82°C) and polyisoprene (—49°C) transitions.
The intercept of the straight line generated by the two fixed points (that is, the value of t at which V would vanish on that straight line if He could be maintained as an ideal gas down to extremely low temperatures ) is found to be 7b = — 100Vb/( ioo — o) = —273.15°C. This suggests a natural lower limit to temperature, namely, the point where V vanishes. It also suggests a shift of scale whereby the quantity T = lOOL/(Tioo — Vb) is the fundamental entity of interest. Adoption of this method leads an absolute scale for quantifying hotness levels we construct a thermodynamic temperature scale T(K) = r(°C) -I- 273.15, where K stands for kelvins as the temperature unit. This still maintains the desired proportionality between absolute temperature and measured volumes of He at fixed, low pressures. [Pg.7]

The non-SI temperature units require special mention. The two most important temperature scales in the United States are the Fahrenheit scale and the Celsius scale, which employ the Fahrenheit degree (°F) and the Celsius degree (°C), respectively. The size of the Celsius degree is the same as that of the SI temperature unit, the kelvin, but the two scales are shifted relative to each other by 273.15°C ... [Pg.967]

Figure 1.16 Temperature dependence of the water/oil interfacial tension Figure 1.16 Temperature dependence of the water/oil interfacial tension <jab (plotted on log-scale) for some representative water-n-octane-QEj systems. Note that the minimum of the interfacial tension curves <jab decreases substantially by increasing both the hydrophobic chain length / and the size of the hydrophilic head group / of the surfactants. The shift on the temperature scale stems from the shift of the phase behaviour. The full line is again calculated from an analysis of interfacial tensions in terms of the bending energy model [96], (Figure redrawn with data from Ref. [1 7].)...
The propane system shown in Fig. 11.3 is clearly subcritical as the critical temperature of propane is about 96°C. An increase of the C02 fraction ((3) in the mixture of C02 and propane shifts the one-phase region (1), i.e. the bicontinuous microemulsion, to lower temperatures. For pure C02 the bicontinuous microemulsion (1) exists around 35°C, which is higher than the Tc = 31°C of C02. In other words, the C02 solubilised in the microemulsion is supercritical Knowing how to tune the phase behaviour of these systems, one can easily shift phase diagrams on the temperature scale by simply choosing an appropriate surfactant. Other tuning parameters are the oil-to-water fraction and the temperature which maybe adjusted such that, e.g. a C02-in-water droplet microemulsion forms. [Pg.352]

In 1848 Lord Kelvin realized the significance of this phenomenon. He identified -273.15°C as absolute zero, theoretically the lowest attainable temperature. Then he set up an absolute temperature scale, now called the Kelvin temperature scale, with absolute zero as the starting point (see Section 1.6). On the Kelvin scale, one kelvin (K) is eqnal in magnitude to one degree Celsius. The only difference between the absolute temperature scale and the Celsius scale is that the zero position is shifted. Important points on the two scales match up as follows ... [Pg.164]

In (39) the slow time td behaves identically for the two fluids, ordinary water (OW) and heavy water (HW), by shifting the temperature scale by... [Pg.354]

The temperatures of the magnetic ordering and of the resistivity maximum have the tendency to increase with applied pressure. The superconducting transition is, however, shifted down on the temperature scale, and finally the superconductivity is completely suppressed in =1.6 GPa (De Boer et al. 1986, McElfresh et al. 1987). [Pg.451]

For most applications, an alternative is employed. Recall that, in measuring the resistance of a thermistor, a fixed resistor is normally connected in series with the sensor. If a constant-voltage source ( s) is used, the circuit current is inversely proportional to the total resistance. Then the relationship between the measured voltage drop across the fixed resistor and the thermistor temperature can be almost linear over a range of temperature. The linear part of this curve can be shifted along the temperature scale by changing the value of the fixed resistor. [Pg.1179]

In the iSR study of UTe by Aggarwal et al. (1989) the signal was lost in TF as well as in ZF below Tq = 104K. The published data are restricted to the paramagnetic regime, especially to the temperature range close to the second-order Ciuie point. They yield a frequency shift that scales with susceptibility Af/fo = [(T- TcyTcT with w = 1) and a relaxation rate that rises faster than susceptibility (w = 1.3). [Pg.167]

A random system can have several temperature scales, namely Tc N) — Tc) and (T — Tc) in addition to the shift in the transition temperature itself. For a system... [Pg.44]

Fig. 3.33. The optical conductivity of Gd film at two temperatures (Myers, 1976). Note the shift in scales for the two curves. Fig. 3.33. The optical conductivity of Gd film at two temperatures (Myers, 1976). Note the shift in scales for the two curves.
Simple models of the melting point depression going back to Kelvin would predict that shift ATJn of the particle melting temperature scaling as HR, where R is the radius of the particle or A assuming a spherical or other compact... [Pg.540]

The centigrade scale has been replaced by the Celsius scale, which is based on the triple point of water rather than on the less reproducible ice point and steam point. The Celsius scale is the thermodynamic (or ideal-gas) temperature scale shifted by exactly 273.15 kelvins. The temperature unit is the degree Celsius (°C), identical in size to the kelvin. Thus, Celsius temperature t is related to thermodynamic temperature T by... [Pg.41]


See other pages where Shifted temperature scale is mentioned: [Pg.403]    [Pg.403]    [Pg.267]    [Pg.497]    [Pg.113]    [Pg.318]    [Pg.335]    [Pg.5]    [Pg.16]    [Pg.136]    [Pg.15]    [Pg.2674]    [Pg.667]    [Pg.383]    [Pg.62]    [Pg.88]    [Pg.205]    [Pg.2673]    [Pg.274]    [Pg.192]    [Pg.791]    [Pg.554]    [Pg.104]   
See also in sourсe #XX -- [ Pg.400 ]




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