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Surface Indentations

A third type of surface disturbance is like that envisioned by Bous-sinesq (B6). Fluttering surface instabilities of a very local nature may be observed. A small area of the drop surface can dilate and recede in a periodic fashion much like that observed on the front of large air bubbles rising through liquids. Interference from other types of oscillations quickly compel a change in frequency and location of these surface instabilities. [Pg.75]

With all three types of oscillations superimposed, the final result has a random appearance. Since a sphere has the smallest area per unit volume, all oscillatory movements cause an alternate creation and destruction of interfacial area. The rate of mass transfer is thereby enhanced for oscillating drops. Since surface stretch due to oscillations is not uniformly distributed, all such oscillations produce interfacial turbulence (see Section VII, E). [Pg.75]


An important aspect concerning the surface indentation mechanism is the creep effect shown by polymeric materials i.e. the time dependent part of the plastic deformation of the polymer surface under the stress of the indenter14-16. The creep curves are characterized by a decreasing strain rate, which can be described by a time law of the form... [Pg.121]

In these equations, the repulsion of the sample became interrelated with the adhesion force via the contact area. Several models have been developed to include the effect of the adhesion forces [80-83]. Johnson, Kendall, and Roberts derived the following expression for the contact radius and surface indentation ... [Pg.70]

In the active probe approach, SFM acquires both static and dynamic mechanical properties (Sect. 2.2.2). The former includes the shear and Young s modulus (G,E) as well as the surface indentation and contact area (S,a). Dynamic meas-... [Pg.127]

The SFM images (Fig. 43) show, that using a d.c. offset of-10.57 V and an excitation voltage of 4.4 V at 1 kHz, high currents in the ilA range can be measured. For this scenario, ceramics are ideal samples, because the low stiffness of the polymers makes it impossible to use excitation frequencies below the bandwidth limit of the constant-force feedback. The much stiffer ceramics permit one to perform measurements without cross-talk effects. Such cross-talk effects occur with soft polymer samples, due to a surface indentation by the tip, which is at virtual ground and so attracted by the back electrode under potential. [Pg.184]

Practical adhesion mapping can be performed in the so-called force-volume (FV) mode. In this mode, f-d curves are acquired for each pixel. Thus, information is obtained on attractive forces before the tip contacts the surface, indentation in the contact region (see Sect. 4.3), adhesive interactions, and the dissipated energy (as area under the f-d curve, compare Fig. 4.3). [Pg.193]

Kelchner C. L., Plimpton S. J. and Hamilton J. C., Dislocation Nucleation and Defect Structure during Surface Indentation, Phys. Rev. B58, 11 085 (1998). [Pg.763]

Fixed-Position Refill. A process development matrix was obtained with a smooth cylindrical pin and shoulder profile using the fixed-position refill method (Fig. 12.28). The materials used for this study were 3.18 mm (0.13 in.) thick upper and lower sheet 2024-T3 aluminum lap joints. Characteristic measurements were made of surface indentation, effective shear area, void size, and lap-shear strength. [Pg.252]

Surface indentation arises from excessive flash being extruded through the clearance space between the shoulder and clamping ring. [Pg.253]

Figure 3. The muscle calcium binding protein molecule has the general shape of a prolate ellipsoid of revolution (59). The shell, 2.7-A thick, contains those atoms, exclusive of hydrogen, that would be exposed to the solvent were there no surface indentations. The oblate ellipsoid hydrocarbon core consists of side chains of phenylalanine, leucine, isoleucine, and valine. Figure 3. The muscle calcium binding protein molecule has the general shape of a prolate ellipsoid of revolution (59). The shell, 2.7-A thick, contains those atoms, exclusive of hydrogen, that would be exposed to the solvent were there no surface indentations. The oblate ellipsoid hydrocarbon core consists of side chains of phenylalanine, leucine, isoleucine, and valine.
Increasing the thickness of a plastics product does not necessarily make it more resistant to penetration. Discuss this statement with respect to surface indentation by a sharp object. [Pg.498]

Fig. 3 Isolation of nuclei from suspension tissue culture cells. (A) Low-power SEM image of nucleus isolated from K.S62 tissue culture cell, after isolation and Percoll density-gradient purification. This particular nucleus shows surface indentations due to its position in the cell cycle (approaching prophase), but the overall surface morphology of the nuclear envelope is largely free of cytoplasmic contamination, and numerous pore complexes (arrowed) arc apparent. Scale bar, 1.0 /u,m. (B) Detail of A, showing cytoplasmic surface of the nuclear envelope with clearly visible nuclear pore complexes, and a typical density of ribosomes (remember the outer nuclear envelope is the innermost element of the rough endoplasmic reticulum). Scale bar, 125 nm. Fig. 3 Isolation of nuclei from suspension tissue culture cells. (A) Low-power SEM image of nucleus isolated from K.S62 tissue culture cell, after isolation and Percoll density-gradient purification. This particular nucleus shows surface indentations due to its position in the cell cycle (approaching prophase), but the overall surface morphology of the nuclear envelope is largely free of cytoplasmic contamination, and numerous pore complexes (arrowed) arc apparent. Scale bar, 1.0 /u,m. (B) Detail of A, showing cytoplasmic surface of the nuclear envelope with clearly visible nuclear pore complexes, and a typical density of ribosomes (remember the outer nuclear envelope is the innermost element of the rough endoplasmic reticulum). Scale bar, 125 nm.
Figure 3.5 shows a plot of hardness against volume fraction of filler [ISAF (intermediate super abrasion furnace) black] in the vulcanizate base on the rubber compound formulations shown in Table 3.1. Hardness is defined as the resistance to surface indentation as measured under specified conditions. It is a non-destructive test that measures the reversible deformation when an... [Pg.113]

The resistance to compression and surface indentation, usually measured by the depth of penetration of a blunt point under a given load using a particular instrument according to a prescribed procedure. Among the most important methods of testing are Barcol hardness, Brinell hardness, Knoop hardness, Mohs hardness, Rockwell hardness, and Shore hardness. [Pg.2227]

A number of other specialized adhesion testing methods have been tried, but most apply only to a very limited class of materials. These other methods use many other techniques, such as surface indentation probes or acoustic or thermal shock of the coating to get an idea of the film adhesion. In addition to being applicable only to a small class of materials, all of these techniques are plagued by the lack of a direct relation to adhesive strength and limited use and experience with the technique. Reference 16 reviews a few of the more common methods of adhesion testing. [Pg.59]

Fig. 6.39. Images of dislocation nucleation in a bubble raft model of a single crystal subjected to surface indentation. In the case of the smallest surface roughness (a), dislocation nucleation occurs at the peaks of the asperities where they contact the indenter. At the intermediate scale (b), dislocation nucleation occurs at the reentrant corners at the bases of the asparities. Finally, for the largest scale asperity (c), the stress level near the stress concentrations has been reduced geometrically, and dislocations nucleated homogeneously at an interior point where the shear stress is the largest. Each bubble in this raft is 1 mm in diameter and it represents an atom which is approximately 0.3 nm in diameter. Reproduced with permission from Gouldstone et al. (2001). Fig. 6.39. Images of dislocation nucleation in a bubble raft model of a single crystal subjected to surface indentation. In the case of the smallest surface roughness (a), dislocation nucleation occurs at the peaks of the asperities where they contact the indenter. At the intermediate scale (b), dislocation nucleation occurs at the reentrant corners at the bases of the asparities. Finally, for the largest scale asperity (c), the stress level near the stress concentrations has been reduced geometrically, and dislocations nucleated homogeneously at an interior point where the shear stress is the largest. Each bubble in this raft is 1 mm in diameter and it represents an atom which is approximately 0.3 nm in diameter. Reproduced with permission from Gouldstone et al. (2001).
Figure 5.64. Surface topography and molecular organization of a molded flexural test bar of a copolymer was shown by contact mode AFM to have surface indentations (A) and surface fibrils (B). (From Schiraldi et al. [300], (2(X)1) Wiley-Interscience used with permission.)... Figure 5.64. Surface topography and molecular organization of a molded flexural test bar of a copolymer was shown by contact mode AFM to have surface indentations (A) and surface fibrils (B). (From Schiraldi et al. [300], (2(X)1) Wiley-Interscience used with permission.)...
Hardness/Flexural Strength - The analogous resistance to elastomer chain deformation accounts for the increase in rubber hardness obtained in proportion to filler loading, surface area, structure activity/surface treatment, and structural anisometry. Hardness is typically measured as resistance to surface indentation under specific conditions, so the force is supplied as a point of compression rather than an area of tension. Similar filler particle dynamics apply, nevertheless. Flexural strength is likewise related as a measure of a sample s resistance to deformation (flex) imder a compressive force. With a force supplied to an end-supported test sample, the upper surface is under compression and the lower surface is in tension... [Pg.229]

Hardness is probably the most often-measured property of elastomer vuleanizates. It appears in almost every specification and is widely used by rubber goods manufacturers for quality control. However, its practical significance is questionable, because surface indentation rarely bears any relationship to end-use performance. Also, hardness is a very imprecise measurement it is not uncommon to find 5 or more points difference in readings by different people on the same pieee of rubber. Nevertheless, hardness will probably remain as a standard test in the rubber industry beeause it is simple and quick to measure and has been correlated with product quality over many years of experience. [Pg.263]

Surface indentation using a loaded point can be used for adhesion testing in much the same way as the scratch test. Indentations are made with varying load and tip geometries and the area around the indentation is observed for fracture, flaking, and deadhesion of the film from the substrate.An instrument that can be used for performing this test is the common indentation hardness tester. [Pg.459]


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