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Temperature the reciprocal

Studies of dimensiosolvatic effects have continued with an attempt to quantify them for solvolyses of 2-bromoadamantane in water-alcohol mixtures. Product selectivities S = fc(ether)/fc(alcohol) were measured at various concentrations of water in an alcohol and at various temperatures. The reciprocals of the averages of S values for 1.0 0.8 alcohol-water mixtures at all the experimental temperatures (120-150 °C) were proposed as measures D of dimensiosolvatic effects when a solvent molecule intervenes into contact ion pair to form solvent-separated ion pair. The scale runs from Z) = 1.0 (by definition) to D = 10.0 for r-butyl alcohol and is essentially a measure of the bulkiness of solvent molecules. [Pg.339]

Figure 5.11. Illustration of modulus versus time for a creep or stress relaxation experiment on a typical amorphous polymer (T = constant). Note the similarity to the plot of DMA storage modulus versus temperature. The reciprocal of creep compliance, l//(f), would be used to generate the modulus curve derived from the creep response. Figure 5.11. Illustration of modulus versus time for a creep or stress relaxation experiment on a typical amorphous polymer (T = constant). Note the similarity to the plot of DMA storage modulus versus temperature. The reciprocal of creep compliance, l//(f), would be used to generate the modulus curve derived from the creep response.
The temperature dependence of the magnetic susceptibility for the compounds RCo2Si2 (R = Pr, Nd, Gd, Tb, Dy and Ho) and RCo2Gc2 (R = Pr, Nd, Tb, Dy and Ho) shows characteristic maxima connected with the Neel temperatures. Above the Neel temperatures, the reciprocal magnetic susceptibility obeys the Curie-Weiss law. [Pg.154]

In Refs. [48, 49, 59] as the index, characterizing dependence of relaxation properties on temperature, the reciprocal of relative stress decay at definite duration of its relaxation P was used ... [Pg.31]

Conductivity. The standard unit of conductance is electrolytic conductivity (formerly called specific conductance) k, which is defined as the reciprocal of the resistance of a 1-m cube of liquid at a specified temperature m— ]. See Table 8.33 and the definition of the cell constant. [Pg.995]

The relaxation and creep experiments that were described in the preceding sections are known as transient experiments. They begin, run their course, and end. A different experimental approach, called a dynamic experiment, involves stresses and strains that vary periodically. Our concern will be with sinusoidal oscillations of frequency v in cycles per second (Hz) or co in radians per second. Remember that there are 2ir radians in a full cycle, so co = 2nv. The reciprocal of CO gives the period of the oscillation and defines the time scale of the experiment. In connection with the relaxation and creep experiments, we observed that the maximum viscoelastic effect was observed when the time scale of the experiment is close to r. At a fixed temperature and for a specific sample, r or the spectrum of r values is fixed. If it does not correspond to the time scale of a transient experiment, we will lose a considerable amount of information about the viscoelastic response of the system. In a dynamic experiment it may... [Pg.173]

More precise coefficients are available (33). At room temperature, cii 1.12 eV and cii 1.4 x 10 ° /cm. Both hole and electron mobilities decrease as the number of carriers increase, but near room temperature and for concentrations less than about 10 there is Htde change, and the values are ca 1400cm /(V-s) for electrons and ca 475cm /(V-s) for holes. These numbers give a calculated electrical resistivity, the reciprocal of conductivity, for pure sihcon of ca 230, 000 Hem. As can be seen from equation 6, the carrier concentration increases exponentially with temperature, and at 700°C the resistivity has dropped to ca 0.1 Hem. [Pg.530]

A guarded hot-plate method, ASTM D1518, is used to measure the rate of heat transfer over time from a warm metal plate. The fabric is placed on the constant temperature plate and covered by a second metal plate. After the temperature of the second plate has been allowed to equiUbrate, the thermal transmittance is calculated based on the temperature difference between the two plates and the energy required to maintain the temperature of the bottom plate. The units for thermal transmittance are W/m -K. Thermal resistance is the reciprocal of thermal conductivity (or transmittance). Thermal resistance is often reported as a do value, defined as the insulation required to keep a resting person comfortable at 21°C with air movement of 0.1 m/s. Thermal resistance in m -K/W can be converted to do by multiplying by 0.1548 (121). [Pg.461]

H2O/100 kg of adsorbent. At equilibrium and at a given adsorbed water content, the dew point that can be obtained in the treated fluid is a function only of the adsorbent temperature. The slopes of the isosteres indicate that the capacity of molecular sieves is less temperature sensitive than that of siUca gel or activated alumina. In another type of isostere plot, the natural logarithm of the vapor pressure of water in equiUbrium with the desiccant is plotted against the reciprocal of absolute temperature. The slopes of these isosteres are proportional to the isosteric heats of adsorption of water on the desiccant (see... [Pg.515]

From Water Density at Atmospheric Pressure and Temperatures from 0 to 100°C, Tables of Standard Handbook Data, Standartov, Moscow, 1978. To conserve space, only a few tables of density values are given. The reader is reminded that density values may he found as the reciprocal of the specific volume values tabulated in the Thermodynamic Properties Tables subsection. [Pg.135]

No tables of the coefficients of thermal expansion of gases are given in this edition. The coefficient at constant pressure, l/t)(3 0/3T)p for an ideal gas is merely the reciprocal of the absolute temperature. For a real gas or liquid, both it and the coefficient at constant volume, 1/p (3p/3T),, should be calculated either from the equation of state or from tabulated PVT data. [Pg.172]

The regression constants A, B, and D are determined from the nonlinear regression of available data, while C is usually taken as the critical temperature. The hquid density decreases approximately linearly from the triple point to the normal boiling point and then nonhnearly to the critical density (the reciprocal of the critical volume). A few compounds such as water cannot be fit with this equation over the entire range of temperature. Liquid density data to be regressed should be at atmospheric pressure up to the normal boihng point, above which saturated liquid data should be used. Constants for 1500 compounds are given in the DIPPR compilation. [Pg.399]

Refrigeration capacity and power P curves for the reciprocating compressor are shown in Fig. 11-92. They are functions of temperatures of evaporation and condensation ... [Pg.1115]

As predicted by the Arrhenius equation (Sec. 4), a plot of microbial death rate versus the reciprocal or the temperature is usually linear with a slope that is a measure of the susceptibility of microorganisms to heat. Correlations other than the Arrhenius equation are used, particularly in the food processing industry. A common temperature relationship of the thermal resistance is decimal reduction time (DRT), defined as the time required to reduce the microbial population by one-tenth. Over short temperature internals (e.g., 5.5°C) DRT is useful, but extrapolation over a wide temperature internal gives serious errors. [Pg.2142]

By plotting the natural logarithm (In) of against the reciprocal of the absolute temperature (1/T) at constant stress, as shown in Fig. 17.6, we find that ... [Pg.174]

If Equation 3.12 is borrowed from the reciprocating compressor chapter and used for an uncooled section, the pressure ratio per section may be calculated assuming an approximate equal-work division. For the first trial, assume the limit of temperature may be achieved in two sections. [Pg.176]

It is reasonable to assume that the glass transition temperature Tg drops linearly with increase in chain-end concentration, that is with an increase in the reciprocal of the molecular weight. This will give an equation of the form... [Pg.63]

Figure 13.6 shows the influence of temperature on specific volume (reciprocal specific gravity). The exaet form of the eurve is somewhat dependent on the crystallinity and the rate of temperature change. A small transition is observed at about 19°C and a first order transition (melting) at about 327°C. Above this temperature the material does not exhibit true flow but is rubbery. A melt viseosity of 10 -10 poises has been measured at about 350°C. A slow rate of decomposition may be detected at the melting point and this increases with a further inerease in temperature. Processing temperatures, exeept possibly in the case of extrusion, are, however, rarely above 380°C. [Pg.369]

As the nanotube diameter increases, more wave vectors become allowed for the circumferential direction, the nanotubes become more two-dimensional and the semiconducting band gap disappears, as is illustrated in Fig. 19 which shows the semiconducting band gap to be proportional to the reciprocal diameter l/dt. At a nanotube diameter of dt 3 nm (Fig. 19), the bandgap becomes comparable to thermal energies at room temperature, showing that small diameter nanotubes are needed to observe these quantum effects. Calculation of the electronic structure for two concentric nanotubes shows that pairs of concentric metal-semiconductor or semiconductor-metal nanotubes are stable [178]. [Pg.71]

Figure 7 Graph of Intercept and Slope from [Log(V r(T))/Number of CH2 Groups Curves] for a Series of -Alkanes/ the Reciprocal of the Absolute Temperature... Figure 7 Graph of Intercept and Slope from [Log(V r(T))/Number of CH2 Groups Curves] for a Series of -Alkanes/ the Reciprocal of the Absolute Temperature...

See other pages where Temperature the reciprocal is mentioned: [Pg.759]    [Pg.319]    [Pg.357]    [Pg.138]    [Pg.67]    [Pg.805]    [Pg.829]    [Pg.2598]    [Pg.54]    [Pg.31]    [Pg.310]    [Pg.759]    [Pg.319]    [Pg.357]    [Pg.138]    [Pg.67]    [Pg.805]    [Pg.829]    [Pg.2598]    [Pg.54]    [Pg.31]    [Pg.310]    [Pg.148]    [Pg.201]    [Pg.206]    [Pg.17]    [Pg.65]    [Pg.509]    [Pg.95]    [Pg.523]    [Pg.233]    [Pg.103]    [Pg.1131]    [Pg.1143]    [Pg.409]    [Pg.650]    [Pg.52]    [Pg.58]    [Pg.59]    [Pg.82]   
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Reciprocal temperature

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