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6- vacuum problems with

A big problem with /t-type materials is their laigc instability in oxygen. This is exemplified by CW), the mobility of which can be as high as 0.08 cm" V 1 s l in ultra-high vacuum, but falls by four or five orders of magnitude upon exposure to air [105]. This could be due to problems of contacts, as illustrated by the fact that modifying the surface of the source and drain electrodes with tetrakisdimethylami-noethylene (TDAE) leads to a substantial increase in the mobility [I05. ... [Pg.574]

We may encounter problems in the purification of substances with a high normal boiling point. If purification only requires a small number of theoretical stages. Short Path Distillation (SPD), in which pressures can be as low as 0.001 bar, can prove useful. Many vitamins and pharmaceuticals can be processed without deterioration of quality. It is now common to use mechanical vacuum pumps with proper condensers preceding the pump. [Pg.415]

Vacuum operation. The second consideration, illustrated in Figure 24.32, is that at the evaporator temperature, evaporator pressure below atmospheric pressure should be avoided. An evaporator pressure above atmospheric avoids potential problems with the ingress of air into the cycle, which can cause performance and safety problems. However, special designs can use evaporator pressures below atmospheric. The boiling points of some common refrigerants are given in Table 24.3 at atmospheric pressure. [Pg.532]

An important problem with rupture discs is the flexing of the metal as process pressures change. Flexing could lead to premature failure at pressures below the set pressure. For this reason some rupture disc systems are designed to operate at pressures well below the set pressure. In addition, vacuum service may cause rupture disc failure if the relief system is not specifically designed for this service. [Pg.362]

Surface of the cooled detector would attract contamination from the residual gases of the vacuum. To prevent the detector from being contaminated, the vacuum space of the detector is separated from that of the microscope by a thin window. The window itself is thermally isolated from the cold detector, so it does not attract contamination. An unwanted byproduct of the presence of this window is the absorption of the photons (to be detected) by the window. Softer radiation (of lighter elements) is affected more. This is the second problem with the analysis of light elements with EDS. [Pg.214]

In the Langmuir free-evaporation method, the sample is suspended freely in a vacuum system with no container sunounding it. As very low levels of vapour pressure can be measured it has advantages over the Knudsen method where the lower limit is about 10" atm. (Kubaschewski et al. 1993). It is therefore more usefril in materials with high sublimation energies and therefore inherently low vapour pressiues. It has a further advantages in that there is no container with which to react, but there are more significant problems associated with temperature measurement. [Pg.86]

Mass spectrometry (MS) is highly selective. The ability to further perform tandem mass spectrometry (MS/MS) analysis when a compound is detected to confirm the detection virtually eliminates false positive and negative alarms. But MS/MS analysis must be completely automated for the average GI to be able to perform it. A clever hand-held chemical and biological mass spectrometer has been developed that weighs only 4.3 pounds. The problem with the unit is production of the necessary vacuum, which requires 35 amps at 24 volts. Thus, battery-operated portable mass spectrometry is not yet available. [Pg.81]

A major problem with functional inlet systems is that they are often quite bulky, which makes it difficult to move the cryostat from the sample deposition line to different spectrometers, or from there to stationary sources of radiation. If only one form of spectroscopy is applied in a given study, then the vacuum shroud may be mounted with all parts attached to it in the sample chamber of the corresponding spectrometer. In this case the expander, on which the sample holder is attached, must be rotated within the vacuum shroud to switch the sample from... [Pg.808]

In the received opinion [5], these are the vacuum Faraday law and Ampere-Maxwell law, respectively. The vacuum charges and currents are missing in the received opinion. Nevertheless, solving Eq. (625) numerically is a useful computational problem with boundary conditions stipulated in the vacuum. The potentials and fields are related as usual by... [Pg.199]


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See also in sourсe #XX -- [ Pg.2 , Pg.331 ]




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