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Lateral magnetization

The X-ray apparatus main circuit scheme is shown in Figure 1. The scheme operation is the following before the power winding 1 connection to a supply main in a lateral magnetic circuit composed by uncontrollable yoke 2, controllable yoke 3 and rods 4, the controllable yoke... [Pg.430]

The field electron microscope permits determination of the distribution of emission and thereby of the covering of the monocrystal with foreign molecules at room temperature. By a method analogous to that shown in Fig, 5, the work function can be measured too. In the anode, covered by a luminous substance, a small opening is made in front of a collector (Fig. 7). By a lateral magnetic field or by adjustment of the cathode, a certain point of the monocrystal is focused on the opening. [Pg.311]

In any case, all contributions M Q. t) = M k i m iyjZkf) to the complex lateral magnetization M are subject to a time development according to the corresponding Larmor frequency ... [Pg.213]

At the end of the mixing period at a given time f p, the magnetization vector in the single-transition operator system is transformed into the lateral magnetization vector of the S-system. The corresponding complex value for the rotating... [Pg.219]

It is a probe whose the coil support is a small circular sticks with a straiglit section. The aim of our study is to assimilate the resulting magnetic field to a material point, hi order to minimize the lateral field, we have chosen the construction of conical coil where the lateral field at a contact point in respect to a straight configuration is decreased with an exponential factor. The results obtained from the curves are as follow ... [Pg.292]

In essence the TCMC method consists in the main transformer magnetic flow redistribution between magnetic circuits of the middle one, which composed by uncontrollable lateral yoke and a number of rods leaned on controllable middle yoke and lateral one, composed by the same uncontrollable yoke and rods leaned on lateral yoke. [Pg.430]

Prepare a paste out of 65g Sodium Azide (lm NaN ) and 65mL of water in a beaker. Add 400mL of either Chloroform or Benzene to this paste (depending on what you have available, but be consistent later on) and stir well. Dump this mixture into a round bottom flask situated in an ice/salt bath, drop in a stirrer magnet, attach a Claisen adapter, addition funnel, and thermometer. Let this mixture cool to OC. [Pg.267]

Once the primary electron beam is created, it must be demagnified with condenser lenses and then focused onto the sample with objective lenses. These electron lenses are electromagnetic in nature and use electric and magnetic fields to steer the electrons. Such lenses are subject to severe spherical and chromatic aberrations. Therefore, a point primary beam source is blurred into a primary beam disk to an extent dependent on the energy and energy spread of the primary electrons. In addition, these lenses are also subject to astigmatism. AH three of these effects ultimately limit the primary beam spot size and hence, the lateral resolution achievable with sem. [Pg.271]

Coreless furnaces derive their name from the fact that the coil encircles the metal charge but, in contrast to the channel inductor described later, the cod does not encircle a magnetic core. Figure 8 shows a cross section of a typical medium sized furnace. The cod provides support for the refractory that contains the metal being heated and, therefore, it must be designed to accept the mechanical loads as well as the conducted thermal power from the load. [Pg.129]

The spectroscopic techniques that have been most frequently used to investigate biomolecular dynamics are those that are commonly available in laboratories, such as nuclear magnetic resonance (NMR), fluorescence, and Mossbauer spectroscopy. In a later chapter the use of NMR, a powerful probe of local motions in macromolecules, is described. Here we examine scattering of X-ray and neutron radiation. Neutrons and X-rays share the property of being found in expensive sources not commonly available in the laboratory. Neutrons are produced by a nuclear reactor or spallation source. X-ray experiments are routinely performed using intense synclirotron radiation, although in favorable cases laboratory sources may also be used. [Pg.238]


See other pages where Lateral magnetization is mentioned: [Pg.431]    [Pg.431]    [Pg.310]    [Pg.53]    [Pg.210]    [Pg.210]    [Pg.210]    [Pg.211]    [Pg.213]    [Pg.217]    [Pg.407]    [Pg.289]    [Pg.594]    [Pg.52]    [Pg.497]    [Pg.148]    [Pg.1931]    [Pg.431]    [Pg.431]    [Pg.310]    [Pg.53]    [Pg.210]    [Pg.210]    [Pg.210]    [Pg.211]    [Pg.213]    [Pg.217]    [Pg.407]    [Pg.289]    [Pg.594]    [Pg.52]    [Pg.497]    [Pg.148]    [Pg.1931]    [Pg.365]    [Pg.633]    [Pg.1298]    [Pg.1529]    [Pg.1539]    [Pg.2093]    [Pg.105]    [Pg.516]    [Pg.517]    [Pg.44]    [Pg.379]    [Pg.540]    [Pg.127]    [Pg.381]    [Pg.426]    [Pg.506]    [Pg.371]    [Pg.268]    [Pg.2150]    [Pg.848]    [Pg.67]    [Pg.58]   


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