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Of contacting surfaces

Fig.5 shows the relation of the echo height F/B and the retio of contact surface area Sa /So. The Sa is the contact surface area, and the So is the contact surface area of the V defectless. The F/B decreased with an increase in the Sa /So, as the ultrasonic wave from the incidence S45C side On the other hand, the F/B as the ultrasonic wave from the incidence Ti side has decreased with an increase in the Sa /So... [Pg.851]

Fig.5 Relation of reflective echo height F/B and retio of contact surface area Sa /So... Fig.5 Relation of reflective echo height F/B and retio of contact surface area Sa /So...
Fig.7 shows the relation of the F/B, the temperature T and the time t as the retio of contact surface area Sa /So=50%. O mark is the B echo on the bottom of the upper specimen A mark is the F echo on the bonding interface. The B echo has changed in the changing temperature T. Therefore, the really reflective echo height F/B on... [Pg.851]

Fretting corrosion (36,37) can lead to high contact resistance of base metal contacts, such as tin plate in electronic connectors. Small cycHcal displacements of the connector halves occur because of external vibration or differential thermal expansion and contraction of the mating contacts. The wear debris that is formed remains in the contact zone. The accumulation of oxide debris in the contact region leads to increased contact resistance. Solutions to this problem are stmctures that do not permit movement of contact surfaces with respect to one another, the use of gold as a contact finish, and the appHcation of thick coatings of contact lubricants and greases, which reduce the rate of wear and restrict access of air to the contact surfaces. [Pg.32]

The shape of the so called master curve, however, depends strongly on the compound formulation and the type of contact surface in the friction process. Its detailed study gives an insight into the processes responsible for the frictional behavior. [Pg.757]

Surface deformation increases the van der Waals forces as a result of the increasing area of contact [Krupp, 1967 Dahneke, 1972]. Thus, for deformable materials, the equations of the van der Waals force, which are valid for rigid materials, should be modified to account for the effect of the increased area of contact. Surface absorption also affects the van der Waals forces. The thickness of the adsorbed layer may increase the distance of separation between the interacting materials, thereby decreasing the van der Waals force [Krupp, 1967]. Moreover, if the thickness of the adsorbed layer is greater than the separation distance, the dielectric properties of the adsorbed layer will dominate the base material in the van der Waals interaction [Langbein, 1969]. [Pg.103]

The width is related to the amount of contact surface the titanium has with the glass. [Pg.39]

The main statements of the kinetics of solid-phase reactions which bind the interaction rate with the diffusion of one of components, at first over the surface of another component, and then in the bulk through product layer, are not suitable for mechanochemical reactions, since mechanical activation of a mixture involves continuous renewal of contact surfaces. On this grounds, it was assumed that the interaction rate is limited by the rate of chemical reaction at contact. [Pg.43]

The availability, size, and surfaces or composition of the required equipment should be specifically identified so that the scale-up effort may be representative of a production run. A preliminary compatibility screen of contact surfaces should be completed before the selection of scale-up equipment. The location of the equipment in reference to other requirements, such as services or the packaging area, may be a factor in the selection of equipment. A cleaning-validation study should be conducted to ensure that no residues of active ingredient or cleaning agent remain after cleaning and that the equipment is suitable for production use again. Alternative equipment may be considered and used however, experience will dictate its suitability. [Pg.3722]

The scattering of Tn and, accordingly, Th-Tn values, especially for runs with 530-550°C, do not corresponds to normal distribution. The difference Th-Tn used instead Tn to minimize influence of contact surface of samples with silver plate and inter laboratory shift. Distribution of Th and Th-Tn demonstrate ... [Pg.314]

The concept of adhesive interaction of contacting surfaces is already familiar to us from previous discussion of the adhesive mechanism of friction (Chapters 8 and 12). If the two bodies participating in the adhesive junction are in motion relative to each other, in particular tangential motion, the junction is ruptured shortly after it is established. Rupture of the junction at a location other than the original interface results in transfer of material from one body to the other. According to the broad definition of wear of Section 13.1, each body has been worn—one by loss of material, the other by gain—but there has been no net loss or gain in the system as a whole. [Pg.365]

It is well known that contact metal-polymers for many systems can be interpreted as Schottky barriers [55-57] or heterojunction [58, 59]. To test the influence of gold contact on the chitin dielectric spectra, a nonsymmetrical contact array was prepared in the following manner a circular chitin film was covered on one side with a piece of gold sheet with a small circular orifice in the center during gold-sputtering. The other side of the film was totally gold-sputtered. This way a top surface available for electrode contact is circa 0.008 cm. The bottom surface area is circa 0.75 cm. Because of contact surface area differences, the current depends on the properties of the top electrode. [Pg.26]

TRIBOLOGY - The science concerned with the design, friction, lubrication and wear of contacting surfaces that move relative to each other (as in bearings, cams, or gears). [Pg.150]


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See also in sourсe #XX -- [ Pg.150 ]




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Bulk Crystallization of Polymers in Contact with a Foreign Surface

Calculation of Surface Tension and Contact Angle

Chemical and Physical Properties of Polymeric Contact Surfaces

Complexity of solid surfaces and effects on contact angle

Contact Angle (0) of Liquids on Solid Surfaces

Contact Angles and Calculation of Solid Surface Energies

Contact angle and wettability of solid surfaces

Determination of Solid Surface Tension by Contact Angle

Equilibration of Surface State Electrons on Contact

Fraction of segments in close contact with the surface

Nature of the Contact between Two Solid Surfaces

Painting of the Surfaces in Contact

Surface Topography and the Mechanics of Asperity Contact

Surface contact

The Contact and Friction of Clean Surfaces

Van der Waals contact surfaces of purines and pyrimidines

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