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Temperature scales, comparison

Fig. 2-2 Comparison of Celsius, Fahrenheit, and Kelvin temperature scales... Fig. 2-2 Comparison of Celsius, Fahrenheit, and Kelvin temperature scales...
The use of data of 4He and 3He vapour pressure which was accurately reported for T > 0.5 K was recommended. Unfortunately it was clear that also for the IPTS-68 errors (order of 10-4 K) existed in this temperature scale in comparison with the thermodynamic temperature. [Pg.194]

Figure 7.9. Variation of (a) the Gibbs energy, (b) ttie enthalpy and (c) the entropy with temperature (scaled to the nearest-nei bour interaction energy J ) for the complex structure A15. Comparison between BWG CVM in the tetrahedron approximation ( ) and the Monte Carlo method (—) (Turchi and Finel 1992). Figure 7.9. Variation of (a) the Gibbs energy, (b) ttie enthalpy and (c) the entropy with temperature (scaled to the nearest-nei bour interaction energy J ) for the complex structure A15. Comparison between BWG CVM in the tetrahedron approximation ( ) and the Monte Carlo method (—) (Turchi and Finel 1992).
Lord Kelvin (1824-1907). The Kelvin temperature scale has an absolute zero. True comparisons can be made using the Kelvin scale. A substance at a temperature of 400 Kelvins contains particles with twice as much kinetic energy as a substance at 200 Kelvins. Absolute zero is the temperature where the random motion of particles in a substance stops. It is the absence of temperature. Absolute zero is equivalent to —273.16°C. How this value is determined is discussed shortly after we discuss our next gas law. The relationship between Kelvin and Celsius temperature is... [Pg.105]

When a hot body and a cold body are brought into physical contact, they lend to achieve the same warmth after a long lime. These two bodies are then said to be at thermal equilibrium with each other. The zeroth law of thermodynamics (R.H. Fowler) states that two bodies individually at equilibrium with a third are at equilibrium with each other. This led lo the comparison of the states of thermal equilibrium of two bodies in lei ms ol a third body called a thermometer. The temperature scale is a measure of state or thermal equilibrium, and tw-o systems at thermal equilibrium must have the same temperature. [Pg.580]

Comparison of this result with Eq. (5.5) yields the simplest possible functional relation for f namely, = T. We conclude that the Kelvin temperature scale,... [Pg.82]

Scientists also normally use the Celsius temperature scale, but we will report temperatures in both degrees Celsius and the traditional US Fahrenheit temperature scale. For convenience, a comparison of some common temperatures is given below. [Pg.28]

Comparison of this result with Eq. (5.5) yields the simplest possible functional relation for V, namely, f T) = T. We conclude that the kelvin temperature scale, based on the properties of ideal gases, is in fact atliennodynamic scale, independent of the characteristics of any particular substance. Substitution of Eq. (5. TjintoEq. (5.2) gives ... [Pg.154]

Figure 9-1 Comparison of Kelvin and Celsius temperature scales... Figure 9-1 Comparison of Kelvin and Celsius temperature scales...
C can be regarded as the absolute zero of temperature. Since there cannot be less than zero volume, there can be no temperature colder than 273 °C. The temperature scale that has been devised using this fact is called the Kelvin, or absolute, temperature scale. A comparison of the Kelvin scale and the Celsius scale is shown in Figure 9-1. It is seen that any temperature in degrees Celsius may be converted to Kelvins by adding 273°. It is customary to use capital T to represent Kelvin temperatures and small t to represent Celsius temperatures. [Pg.77]

Primary standards are those developed and maintained by national standards laboratories such as the National Bureau of Standards. These laboratories develop, maintain, and disseminate standards, such as the International Practical Temperature Scale. The IPTS-68 is disseminated to the users through secondary standards such as calibrated thermometers, fixed point references, and so on (see Table II). Some of these thermometers are calibrated directly against the defining fixed points and others are calibrated over the range of need by a comparison calibration against a standard interpolating thermometer. This ensures that the basis for temperature measurement, the IPTS-68, is the same everywhere throughout the world. [Pg.286]

FIGURE 1.10 Comparison of the three temperature scales Celsius, Fahrenheit, and the absolute (Kelvin) scales. Note that there are 100 divisions, or 100 degrees, between the freezing point and the boiling point of water on the Celsius scale, and there are 180 divisions, or 180 degrees, between the same two temperature limits on the Fahrenheit scale. [Pg.19]

The value of 1/a for nitrogen at 1 atm is 272. Experiments with other gases indicate that the ice point, 0°C, is equivalent to a value of near 273 K. The Kelvin scale is now defined with high accuracy such that the triple point of water (where ice, water and water vapour are all in equilibrium, at 0.01°C) has the temperature 273.1600° on the Kelvin scale. The triple point is more accurately defined than the ice point. On this basis 0°C is 273.15 K. Measurement on this ideal gas scale is best conducted with a constant pressure helium thermometer, although there are small deviations from the absolute scale. A comparison of the four temperature scales discussed above is given in Table 1.1. [Pg.8]

PFB F8BT blend device at 340 K. PL and —APL ferent temperatures. For comparison the PL are plotted or the same scale and reflect their spectrum from an F8BT-only device (open relative intensities, (b) APL spectra (at 10V) circles) is plotted in both parts (a) and (c). from the same device as in (a) at different... [Pg.73]

Initial concepts of temperature came from the physical sensation of the relative hotness or coldness of bodies. This sensation of warmth or cold is so subjective relative to our immediate prior exposure that it is difficult to use for anything but simple qualitative comparison. The need to assign a quantitative value to temperature leads to the definition of a temperature scale. The concept of fixed points of temperature arises from the observation that there exist some systems in nature that always exhibit the same temperatures. The scientific or thermodynamic definition of temperature comes from Kelvin, who defined the ratio of the thermodynamic or absolute temperatures of two systems as being equal to the ratio of the heat added to the heat rejected for a reversible heat engine operated between the systems. This unique temperature scale requires only one fixed point, the triple point of water, for its definition. [Pg.1159]

Sol-gel process is proven to be an attractive fabrication method of multi-component oxide ceramics. In addition to the achieved homogeneity and purity of the products, the sol-gel method also enables a lower phase-formation and sintering temperature in comparison to the conventional sintering of powder With good size scaling possibility, colloidal sol-gel materials are suitable for depositing layers on macroporous substrates to serve as support of polymeric sol-gel derived layers preventing infiltration of the sol. [Pg.165]

Figure 4, Temperatures (a) Comparison of the three temperatures (bottom to top), radiance temperature, self-calibrated temperature (with an uncertainty of 4%, k = 2), Tseifi and the temperature using the measured emittance, T, for the same experiment on cobalt. The beginning and end of the melting transition are marked by vertical dashed lines, (b) Enthalpy of tantalum scaled with two different temperatures self-calibrated temperature (using the melting temperature and assuming a constant emittance in the liquid state) and temperature using directly measured emittance. Differences in the liquid state are due to the non-constant emittance (with respect to melting point). Figure 4, Temperatures (a) Comparison of the three temperatures (bottom to top), radiance temperature, self-calibrated temperature (with an uncertainty of 4%, k = 2), Tseifi and the temperature using the measured emittance, T, for the same experiment on cobalt. The beginning and end of the melting transition are marked by vertical dashed lines, (b) Enthalpy of tantalum scaled with two different temperatures self-calibrated temperature (using the melting temperature and assuming a constant emittance in the liquid state) and temperature using directly measured emittance. Differences in the liquid state are due to the non-constant emittance (with respect to melting point).
FIGURE 1.17 Comparison of the Kelvin, Celsius, and Fahrenheit temperature scales. [Pg.17]


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See also in sourсe #XX -- [ Pg.38 ]




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