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Transformation superconducting

This doughnut has the hole stuffed with expensive items such as a transformer, superconducting coils and a lithium blanket on the exterior it has the start up injectors. An expression for Vc (empirically derived from many Tokamak conceptual designs, e.g. from those considered in Schmitter s lecture) is Vc = 7U (2 P)2 10a = 4 A (10 tz A a )... [Pg.536]

Fig. 3. A block diagram schematic representation of a Fourier transform nmr spectrometer, ie, a superconducting magnetic resonance system. Fig. 3. A block diagram schematic representation of a Fourier transform nmr spectrometer, ie, a superconducting magnetic resonance system.
Uranium metal is weaMy paramagnetic, with a magnetic susceptibility of 1.740 X 10 A/g at 20°C, and 1.804 x 10 A/g (A = 10 emu) at 350°C (51). Uranium is a relatively poor electrical conductor. Superconductivity has been observed in a-uranium, with the value of the superconducting temperature, being pressure-dependent. This was shown to be a result of the fact that there are actually three transformations within a-uranium (37,52). [Pg.320]

Pure barium is a silvery-white metal, although contamination with nitrogen produces a yellowish color. The metal is relatively soft and ductile and may be worked readily. It is fairly volatile (though less so than magnesium), and this property is used to advantage in commercial production. Barium has a bcc crystal stmcture at atmospheric pressure, but undergoes soHd-state phase transformations at high pressures (2,3). Because of such transformations, barium exhibits pressure-induced superconductivity at sufftciendy low temperatures (4,5). [Pg.471]

Under pressure black phosphorus transforms first to a modification that corresponds to gray arsenic. At an even higher pressure this is converted to the a-polonium structure. Then follows a hexagonal-primitive structure, which has also been observed for silicon under pressure (p. 122), but that hardly ever occurs otherwise. Above 262 GPa phosphorus is body-centered cubic this modification becomes superconducting below 22 K.. [Pg.112]

Fig. 8.3. Schematic of the SRM-768 device containing five superconducting samples, as well as the transformer coils for measuring the transition temperatures of die samples [27-28]. Fig. 8.3. Schematic of the SRM-768 device containing five superconducting samples, as well as the transformer coils for measuring the transition temperatures of die samples [27-28].
One device is made up of samples of superconducting materials put inside a transformer a low-frequency small current in the primary creates a weak magnetic field. [Pg.200]

In fact, with few exceptions [24], the resistance of TES is very low and the matching to a conventional FET amplifier is impossible. A SQUID amplifier (see Section 14.5) coupled to the TES by a superconducting transformer is the natural solution as schematically shown in Fig. 15.4. [Pg.329]

Gemini Superconducting Fourier transform NMR systems, VXR series 5, Varian Instruments, Sugar Lane, Texas, USA... [Pg.90]

The first chemical transformations carried out with Cjq were reductions. After the pronounced electrophilicity of the fullerenes was recognized, electron transfer reactions with electropositive metals, organometallic compounds, strong organic donor molecules as well as electrochemical and photochemical reductions have been used to prepare fulleride salts respectively fulleride anions. Functionalized fulleride anions and salts have been mostly prepared by reactions with carbanions or by removing the proton from hydrofullerenes. Some of these systems, either functionalized or derived from pristine Cjq, exhibit extraordinary solid-state properties such as superconductivity and molecular ferromagnetism. Fullerides are promising candidates for nonlinear optical materials and may be used for enhanced photoluminescence material. [Pg.49]

The neutral insulator TMTSF, which shows field-effect conduction with /Th — 0.2 cm s (Nam et al, 2003), when transformed into a Bechgaard salt also becomes superconducting, but at lower temperatures. In this case the perfect segregation of organic and inorganic molecular planes leads to confined electronic systems, which in the normal state are quasi ID. Organic superconductors based on the BEDT-TTF molecule represent the case of pure 2D electronic systems. [Pg.280]

Non-metals, such as silicon, can also become superconducting when pressure is applied. At 120-130 kbar pressure, silicon exhibits a Tc of 6.7 to 7.1 K. Sulfur has also recently been converted into the superconducting state at 200 kbar with a transition temperature of 5.7 K. In 1989, hydrogen was obtained in the condensed state and under 2.5 megabars pressure, it becomes opaque. This observation indicates that the element is possibly transforming into a metal. Several... [Pg.10]


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See also in sourсe #XX -- [ Pg.320 ]




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Transformer Superconducting Transformers

Transformer Superconducting Transformers

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