Magnetic susceptibility elements

NOTE Extensive listing of magnetic susceptibilities of elements and organic and inorganic compounds can be found in G, Foex, Tables de constantes et donnes numeiiques, Massou et Cie, Paris, 1957,... 

The disappearance of the paramagnetism of palladium-silver alloys (rich in Pd) when the ratio (H + Ag)/Pd = 0.6 (24) illustrates that the effect of both these alloying" elements in palladium is additive and each one contributes essentially in the same way to the change of magnetic susceptibility of palladium. 

Silvery-white metal body-centered cubic crystals ductile soft and very hght (the fourth lightest metaUic element) Mobs hardness 0.3 density 1.522 g/cm3 at 18°C melts at 39.3°C density of the liquid metal 1.472 g/mL at 39°C vaporizes at 689°C producing a blue vapor vapor pressure 1 torr at 294°C and 10 torr at 387°C electrical resistivity 11.6 microhm-cm at 0°C and 13.1 mirohm-cm at 25°C viscosity 0.484 centipoise at 100°C magnetic susceptibility 0.09x10 cgs units at 18°C thermal neutron absorption cross section 0.73 barns reacts violently with water... 

The Physical Properties are listed next. Under this loose term a wide range of properties, including mechanical, electrical and magnetic properties of elements are presented. Such properties include color, odor, taste, refractive index, crystal structure, allotropic forms (if any), hardness, density, melting point, boiling point, vapor pressure, critical constants (temperature, pressure and vol-ume/density), electrical resistivity, viscosity, surface tension. Young s modulus, shear modulus, Poisson s ratio, magnetic susceptibility and the thermal neutron cross section data for many elements. Also, solubilities in water, acids, alkalies, and salt solutions (in certain cases) are presented in this section. 

According to P. Pascal,0 fluorine is diamagnetic the specific magnetic susceptibility is —3447 X10 j and the atomic susceptibilitv calculated from the additive law of mixtures for organic compounds is —63X10-1. Ionic fluorine is univalent and negative. The decomposition voltage required to separate this element from its compounds is 1 75 volts.7 The ionic velocity (transport number) 8 of fluorine ions at 18° is 46 6, and 52-5 at 25° with a temp, coeff. of 0 0238. 

The SH formalism is fully justified for this ZFS case and offers simple formulae for the components of the magnetic susceptibility (Table 18). Here, D should not be too small since in such a case the perpendicular component of the susceptibility diverges. For small D one is left with the matrix elements of the SH, a numerical finding of its eigenvalues, and consequently the magnetic functions. The results of the modeling are presented in Fig. 102. 

Gadolinium and dysprosium, both elements of the lanthanide family, differ in the electronic occupancy of their f-shells. As a result, they are very similar chemically but very different magnetically. The relaxivity 1/Tx of Dy-DTPA is as low as 0.1 1/mol s However, dysprosium has a pronounced ability to influence transiently the residual magnetic susceptibility of tissues as it passes through. This effect of Dy-DTPA seems to be ideal for cerebral perfusion imaging and may be useful for the quantitation of partial occlusions and reperfusion. 

Nine derivatives of 1, [RSb9W2i086]16 (R = La-Gd, Dy, Yb), have been isolated and characterized by elemental analysis, magnetic susceptibility, and infrared spectra. The four-line 183W-NMR spectrum of the lanthanum derivative is consistent with the D3h symmetry of the parent structure, but the emission spectrum of the europium derivative suggests a lower symmetry in the solid state (Liu et al., 1992). No structural determinations of these derivatives have yet been reported. 

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