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Temperature gradient microscop

Fig. 6.2. The solidification of salol can be followed very easily on a temperature-gradient microscope stage. This can be made up from standard laboratory equipment and is mounted on an ordinary transmission light microscope. Fig. 6.2. The solidification of salol can be followed very easily on a temperature-gradient microscope stage. This can be made up from standard laboratory equipment and is mounted on an ordinary transmission light microscope.
The photographs presented here were taken on a temperature gradient microscope stage ( ) shown schematically in Fig. 2. The sample contained in a thin glass cell can be moved at a controlled rate across the gap between a hot and a cold plate. The temperatures of the two plates can be adjusted to give the desired temperature gradient, with the transformation occurring between the two temperatures. [Pg.232]

Fig. 2. Schematic drawing of temperature gradient microscope stage. Fig. 2. Schematic drawing of temperature gradient microscope stage.
Fig. 3a. Planar interface growth in carbon tetrabromide LjkTE = 0.8) growing from the melt between glass cover slide approximately 25 apart. Photograph taken using a temperature gradient microscope stage (150 x). Fig. 3a. Planar interface growth in carbon tetrabromide LjkTE = 0.8) growing from the melt between glass cover slide approximately 25 apart. Photograph taken using a temperature gradient microscope stage (150 x).
The description of the microscopic chromatographic process at realistic temperature conditions at the surfaces (real temperature gradient) is possible. [Pg.216]

The accuracy of SDV was assessed by Morikita et. al. [184] who showed that the maximum difference between the arithmetic means of irregular particles by SDV and microscopic measurements was about 10%. Hishida et al. [185] recorded a maximum difference of 4% owing to beam wandering due to temperature gradients and concluded that the maximum error with increasing flame size cannot exceed 15%. [Pg.507]

The smaller aerosol particles can be captured from the air for subsequent counting and size measurement by means of so-called thermal precipitators. In these instruments, metal wires are heated to produce a temperature gradient. Aerosol particles move away from the wire in the direction of a cold surface, since the impact of more energetic gas molecules from the heated side gives them a net motion in that direction. The particles captured are studied with an electron microscope. Another possible way to measure Aitken particles is by charging them electrically under well-defined conditions. The charged particles are passed through an electric field and are captured as a result of their electrical mobility (see equation [4.6]). Since size and electrical mobility are related, the size distribution of particles can be deduced. These devices are called electrical mobility analyzers. [Pg.94]

As the consequence of this, the metabolic waste products are initially distributed evenly in the bulk medium but accumulated with time in batch culture systems. Furthermore, as a part of normal culture operations, the vessels are taken out from the incubator for microscopic observations, which can cause movement of the bulk medium and formation of temperature gradients, consequently contributing to forced and natural convection, respectively. In industrial-scale bioreactors, the applied perfusion creates forced convection, which is the primary mode of mass transfer. The common feature of all the conventional systems, laboratory- or industrial scale, is that due to the long distances and the large medium volume in comparison with the cell volume, the significance of convection is pronounced. Consequently, mass transfer in such systems takes place in all directions (x-, y- and z-direction) with a comparable magnitude, as is schematically shown in Fig. 2a. [Pg.429]

Here h s 2. positive constant, and the minus sign in the equation indicates that the heat flow is in the opposite direction to the temperature difference that is, the flow of heat is from a region of high temperature to a region of low temperature. Similarly, on a microscopic scale, the heat flux in the x-coordinate direction, denoted by (wiih-units of J/m s), is linearly related to the temperature gradient in that direction ... [Pg.22]

Microscopic hot spots, for example temperature gradients between the metal particles and the support, which cannot be detected and measured because they are close to micro scale, i.e. have molecular dimensions, are dose to selective heating of active sites. Unfortunately, microwave radiation effects at the molecular level are not well understood. [Pg.637]


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