Diffusion temperature measurements

A steady-state method is disadvantageous in measurements on a mixture because for a long time the temperature gradient is likely to generate separation of the mixture due to thermal diffusion. Accurate measurement itself seems to be still one of the most pressing concerns for thermal diffusion of high-temperature melts. 

Fig. 20. Hydrogen diffusion coefficient, measured at 240°C, for 0.1% phosphorus doped a-Si H, as a function of the substrate temperature for which the samples were grown (Street and Tsai, 1988). 

Applications to fluorescent or fluorescently labeled proteins and nucleic acids, and to fluorescent lipid probes in phospholipid bilayers, have been reported. In the latter case, the diffusion coefficients measured above the chain melting temperature were found to be 10 7 cm2 s 1, which is in agreement with values obtained by other techniques. 

One of the earliest detailed diagnostic efforts on sooting of diffusion flames was that of Wagner et al. [86-88], who made laser scattering and extinction measurements, profile determinations of velocity by LDV, and temperature measurements by thermocouples on a Wolfhard-Parker burner using ethene as the fuel. Their results show quite clearly that soot particles are generated near the reaction zone and are convected farther toward the center of the fuel stream as they travel up the flame. The particle number densities and generation rates decline with distance from the flame zone. The soot formation rate appeared to... 

Membrane deterioration may be merely caused by decrease of acetyl content(C ) in the active surface layer as a result of hydrolysis or oxidation, not by structure change. Analysis was carried out based on solution-diffusion model proposed by Lonsdale etal( ), using their measured values of solute diffusivity and partition coefficient in homogeneous membrnaes of various degree of acetyl content and also using those values of asymmetric membranes heat treated at various temperatures measured by Glueckauf(x) ... 

Coppalle, A., and D. Joyeux. 1994. Temperature and soot volume fraction in turbulent diffusion flames Measurements of mean and fluctuating values. Combustion Flame 96 275-85. 

Metal Oxide-Polymer Thermistors. The variation of electrical properties with temperature heretofore described can be used to tremendous advantage. These so-called thermoelectric effects are commonly used in the operation of electronic temperature measuring devices such as thermocouples, thermistors, and resistance-temperature detectors (RTDs). A thermocouple consists of two dissimilar metals joined at one end. As one end of the thermocouple is heated or cooled, electrons diffuse toward... 

There are two possible directions for both the atoms in both the first and second atomic jumps. If the jumping direction is completely random and the two atoms have the same probability of performing a jump, then these atomic jumps are said to be uncorrelated. A correlation factor, /, has been introduced for the two atomic jumps, which is defined as the extra probability that the atom making the first jump will also make the second jump in the forward direction. The rest of the probability, (1 — /), is then shared equally for either of the two atoms jumping in either of the two directions. Two experimental displacement distributions measured at 299 K and 309 K fit best with a Monte Carlo simulation with / = 0.1 and /=0.36, respectively. The correlation factor increases with diffusion temperature as can be expected. It is interesting to note that when/= 1, only a and steps can occur. 

Which assumptions are necessary for determining vertical turbulent diffusion coefficients from repeated vertical temperature measurements made at a single location in the middle of a lake ... 

Therefore, any result that follows from considerations of the form of Fick s second law applies to evolution of heat as well as concentration. However, the thermal and mass diffusion equations differ physically. The mass diffusion equation, dc/dt = V DVc, is a partial-differential equation for the density of an extensive quantity, and in the thermal case, dT/dt = V kVT is a partial-differential equation for an intensive quantity. The difference arises because for mass diffusion, the driving force is converted from a gradient in a potential V/u to a gradient in concentration Vc, which is easier to measure. For thermal diffusion, the time-dependent temperature arises because the enthalpy density is inferred from a temperature measurement. 

There is an international standard, ISO 691455 which covers both the continuous and intermittent procedures plus the simplified intermittent method. Strip test pieces are used, 1 mm thick to minimise oxygen diffusion effects. Measurement at a series of temperatures is recommended and results are presented in graphical form but no consideration is given to interpretation. British Standards did not accept this revision of ISO 6914 and BS 903 Part A5256 is identical to the 1985 ISO method. The revision was not accepted in the UK because mistakes in handling comments resulted in inconsistencies. As an example, the title is now stress relaxation but a note says that this term is avoided ... 

Figure 10. Temperature measurements in flat Ht-air diffusion flame. The exit of the flat flame burner is shown schematically (O), radiation-corrected thermocouple measurements (A) Ht CARS temperatures (A), Ot CARS temperatures.

Rambach, G. D., Dibble, R. W., Hollenbach, R. E., "Velocity and Temperature Measurements in Turbulent Diffusion Flames," paper no. 79-51 Fall Meeting of Western States Section of the Combusion Institute, Berkeley, CA, 1979. 

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