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Surface resistivity skin effect

The ac resistance increase due to skin effect given above should be considered as a minimum. When wires are placed next to one another and placed in layers within a transformer, the near field magnetic effects between wires further crowd the current density into even smaller areas within the wire s cross-section. For instance, when wires are wound next to one another, the current is pushed away from the points of contact along the surfaces of the wires to areas orthogonal to the winding plane. When layers are placed on top of one another the inner layers show much greater degradation in apparent resistance than do the outermost layers. [Pg.253]

Equation (5.4) is valid as long as the skin depth is large in comparison to the mean free path of the electrons in the metal. This holds true in the microwave range at room temperature, for cryogenic temperature the surface resistance lies above the values predicted by Equation (5.4) and exhibits a f2 3 rather than a f1 2 frequency dependence (anomalous skin effect [7]). [Pg.101]

A good example to explain this impetus is the shark skin effect. The scales of predatory fishes have fine longitudinal grooves that cause less cross-flow in the displaced water. This principle has been adapted to aeroplane surfaces to help to reduce fuel consumption by 1 %. Similar shark skin swimsuit surfaces allow competitive swimmers to enjoy the advantages of lower resistance to movement through the water. [Pg.204]

Within a certain range of frequencies and resistivities we can neglect the interaction between currents in the borehole, while in the formation the skin effect manifests itself in the same manner as in a uniform medium but the current density in the borehole and surface charges are directly proportional to frequency. For these conditions the field can be presented in the form ... [Pg.299]

Table 10.4 presents the results of calculation of function A/ij, = Qhj,(Li) — Qhx L2), proportional to the electromotive force in three-coil probe by exact and approximate formulae 10.33 and 10.49. As follows from the table, the EMF in the receiver coil of the probe does not practically depend on the resistivity of the borehole even beyond the range of small parameters. It means that, as in the case of the vertical magnetic dipole, there are conditions when induced currents in the borehole and surface charges do not influence the character of the skin effect in the formation, which manifest itself in the... [Pg.556]

When surface-barriers or a surface-resistance or skin effect to sorbate gases occurs, the overall characteristic functions can be indicated by [3,43,44]... [Pg.247]

The behavior of electromagnetic waves in normal metals at ordinary temperatures and microwave frequencies is quite adequately described by the classical treatment based on MaxwelPs equations and Ohm s law. At low temperatures this is no longer true even though MaxwelPs equations are still valid, Ohm s law is inadequate to describe the relation between high frequency electric currents and fields in metals. According to classical theory, the surface resistance R is inversely proportional to the square root of the dc conductivity cr. Consequently, as the temperature is lowered and o- increases, the classical theory predicts that R cc. This is not borne out in practice, as will be seen by referring to Fig, 1. The ordinate is IR the observed surface conductance, and the abscissa is proportional to c T. Initially the behavior is classical and as the temperature is lowered. As the dc conductivity becomes larger, however, I does not increase proportionately and in the low temperature limit it becomes independent of a (and temperature). This phenomenon is known as the anomalous skin effect. The experimental data shown are due to Chambers [1]. The solid curve is the curve predicted from the theory of Reuter and Sondheimer [2],... [Pg.156]

At high frequencies, the surface of the insulator may have a different resistivity from the bulk of the material owing to impurities absorbed on the surface, external contamination, or water moisture hence, electric current is conducted chiefly near the surface of the conductor (i.e., skin effect). The depth, S, at which the current density falls to 1/e of its value at the surface is called the skin depth. The skin depth and the surface resistance are dependent upon the AC frequency. The surface resistivity, R, expressed in 2, is the DC sheet resistivity of a conductor having a thickness of one skin depth ... [Pg.528]

At dc, current in a conductor flows with uniform density over the cross-section of the conductor. At high frequencies, the current is displaced to the conductor surface. The effective cross-section of the conductor decreases and the conductor resistance increases because of the skin effect. [Pg.312]

Resistance to puncture is another type of loading. It is of particular interest in applications involving sheet and film as well as thin-walled tubing or molding and other membrane type loaded structures. Hie surface skins of sandwich panels are another area where it is important. A localized force is applied by a relatively sharp object perpendicular to the plane of the sheet of material being stressed. If the material is thick compared to the area of application of the stress, it is effectively a localized compression stress with some shear effects as the material is deformed below the surface of the sheet. [Pg.93]

In the body of a liquid, intermolecular forces pull the molecules in all directions. At the surface of the liquid, the molecules pull down into the body of the liquid and from the sides. There are no molecules above the surface to pull in that direction. The effect of this unequal attraction is that the liquid tries to minimize its surface area. The minimum surface area for a given quantity of matter is a sphere. In a large pool of liquid, where sphere formation is not possible, the surface behaves as if it had a thin stretched elastic membrane or skin over it. The surface tension is the resistance of a liquid to an increase in its surface area. It requires force to break the attractive forces at the surface. The greater the intermolecular force, the greater the surface tension. Polar liquids, especially those that utilize hydrogen bonding, have a much higher surface tension than nonpolar liquids. [Pg.161]

By acupuncture.—Schnydeb, some few years ago, obtained a patent for a quick process of tanning, effected by exposing a more extended surface of hide to the tan-liquor than is ordinarily done. Ills method is to puncture the hides with steel points either by hand or machinery, with an instrument having from one to three hundred points to the square inch, and afterwards to expose the skins so indented to the action of the tan-juice, with ot without pressure, as may be most convenient. Either the flesh or hair side may be operated upon with the steel points and, notwithstanding that such perforations permit the liquor to. enter into the interior portions of the skis, still, as the tanning approaches completion, they close up, and the leather Is as capable of resisting moisture as that made from hides which have not been subjected to the same operation. [Pg.520]


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See also in sourсe #XX -- [ Pg.528 ]




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Resistance effects

Resistant effects

Skin resistance

Skin surface resistance

Surface resistance

Surface resistivity

Surface skin effect

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