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Behavior Under Tensile Stress

In technical terms, the behavior of a material imder tensile stress is of primary importance, leading to early experimental and theoretical investigation. The investigation of stress-strain behavior is particularly important. It is analyzed in tensile tests in which a test object is elongated to the point of breakage (or tearing) at a certain rate. The maximal tensile stress level reached is the material s tensile strength. [Pg.84]

the AUC (area under curve) of the different materials represents their resilience. Cast iron and ceramics are very brittle steel, copper, and aluminum, as well as the thermoplastics PA and PP, are highly deformable and can therefore absorb large amounts of energy, for example from (impact) load application. It must be remembered here that the deformation behavior of plastics is highly dependent on time and temperature factors (see Fig. 15). Simplified explanations of deformation terminology follow. [Pg.86]

Purely energy elastic bodies are deformed in response to force application with absolutely no time delay by a certain amount that is independent of the [Pg.86]

Calculation of tensiles or elongations at short time loading in between and beside the linear elastic region above. [Pg.87]

Example short time loading, i.e. snap element [Pg.87]


On the other hand, neck behavior under tensile stress is described by elastic theory at small elongations as... [Pg.187]

Figure 1. Behavior of adhesive-paper systems under tensile stress... Figure 1. Behavior of adhesive-paper systems under tensile stress...
The tensile modulus E is not a constant when o varies, and it also depends on temperature T. For these reasons, curves showing the dependence of a vs. e at constant temperatures or of E vs. T are used for the understanding of polymer behavior under mechanical stress. The value of E (in dyn cm or N m ) is usually given at polymer break. [Pg.30]

Mechanical characteristics are an important consideration in the design of NbsSn conductors. The behavior during bending and under tensile stress is compared below for a tape clad on both sides with copper and a tape clad with stainless steel and copper. The NbsSn/Nb substrate ( lO mNb and 10 fim NbsSn) was prepared by liquid diffusion followed by an etching process to reduce ac losses [" ]. The copper and stainless steel cladding were bonded by soldering with an Ag-Sn eutectic. The thickness of the copper was 24 /xm for the... [Pg.455]

At room temperature, carbon fibers exhibit an approximately linear elastic behavior under tensile loading up to failure. However, some non-linearity in the stress-strain curve was recently reported. The slope increases slightly as the fiber is strained [44-46]. After mechanical properties, the most important properties are those which characterize the electrical transport behavior of carbon fibers. [Pg.250]

The effect of temperature on PSF tensile stress—strain behavior is depicted in Figure 4. The resin continues to exhibit useful mechanical properties at temperatures up to 160°C under prolonged or repeated thermal exposure. PES and PPSF extend this temperature limit to about 180°C. The dependence of flexural moduli on temperature for polysulfones is shown in Figure 5 with comparison to other engineering thermoplastics. [Pg.466]

In the identification of different polymorphs in polymers the FTIR technique presents, with respect to the diffraction techniques, the advantage of easier and more rapid measurements. In particular, the high speed of the measurements allows to study the polymorphic behavior under dynamic conditions. As an example let us recall the study of the transition from the a toward the P form of PBT induced by tensile stresses, evaluated by quantitative analysis of the infrared spectra [83],... [Pg.207]

The two network precursors and solvent (if present) were combined with 20 ppm catalyst and reacted under argon at 75°C to produce the desired networks. The sol fractions, ws, and equilibrium swelling ratio In benzene, V2m, of these networks were determined according to established procedures ( 1, 4. Equilibrium tensile stress-strain Isotherms were obtained at 25 C on dumbbell shaped specimens according to procedures described elsewhere (1, 4). The data were well correlated by linear regression to the empirical Mooney-Rivlin (6 ) relationship. The tensile behavior of the networks formed In solution was measured both on networks with the solvent present and on networks from which the oligomeric PEMS had been extracted. [Pg.332]

FFs that are parameterized for high-pressure conditions can still lead to behavior that differs from that observed in experiments. For instance, it is common practice to treat the interatomic interactions with Lennard-Jones (LJ) potentials. Although this method is convenient from a computational standpoint, it is known that LJ potentials do not reproduce experimentally observed behavior such as necking, where a material attempts to minimize surface area and will break under large tensile stresses. Many other examples exist where particular types of FFs cannot reproduce properties of materials, and once again, we emphasize that one should ensure that the FF used in the simulation is sufficiently accurate. [Pg.99]


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