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Low Strain Rates

Compression tests were conducted at room temperature (23°C) under 35% relative humidity. The effect of polymer crosslinking was investigated by comparing results from native and X-aerogels. The strain recovery behavior on X-aerogel specimens was [Pg.510]

A specimen with density 0.40 g/cm expands at 10% laterally in the elastic regime, but does not expand further until about 60% compressive strain, as the material is mostly [Pg.512]

The working principle of SHPB has been well documented in the literature [26, 73]. Under a valid SHPB experiment, the stress applied in a specimen is calculated from the transmission bar signal through [Pg.518]

When a hollow transmission bar is used, the strain rate on the specimen is determined [74, 75] from the incident bar signal using [Pg.518]

In the case of high strain rates, SHPB experiments were conducted to determine the effects of strain rate, water content, moisture absorption, and low temperature. In each SHPB experiment, five or more specimens were tested to ensure repeatability under the same test conditions. [Pg.518]


Equations (5.21), (5.22) and (5.23) are useful for the high strain rates experienced in injection moulding or extrusion but unfortunately they do not predict the low strain rate situation very well where plastic melts tend towards Newtonian behaviour (ie n -) 1). This is illustrated in Fig. 5.7. [Pg.352]

As in the previous case, this apparatus is usually restricted to relatively low strain rates. [Pg.371]

Certain peculiarity was characteristic of each alloy studied. For example, any hydrogen content embrittled the non-alloyed titanium at room temperature. Other behavior was observed on the Ti-6A1-4.5V alloy at room temperature and low strain rates. The ultimate compressive strain of this alloy without hydrogen was about 8.5% at = 10 s while hydrogen alloying to r = 0.27 increased this value to about 20% and to 10 to 14% at other x. [Pg.430]

Since we are interested in this chapter in analyzing the T- and P-dependences of polymer viscoelasticity, our emphasis is on dielectric relaxation results. We focus on the means to extrapolate data measured at low strain rates and ambient pressures to higher rates and pressures. The usual practice is to invoke the time-temperature superposition principle with a similar approach for extrapolation to elevated pressures [22]. The limitations of conventional t-T superpositioning will be discussed. A newly developed thermodynamic scaling procedure, based on consideration of the intermolecular repulsive potential, is presented. Applications and limitations of this scaling procedure are described. [Pg.658]

Blevins, L. G., and J.P. Gore. 1999. The compnted strnctnre of low-strain rate partially premixed CLl4/air flames Implications for NO formation. Combustion Flame 116 546-66. [Pg.452]

PP bead foams were subjected to oblique impacts (167), in which the material was compressed and sheared. This strain combination could occur when a cycle helmet hit a road surface. The results were compared with simple shear tests at low strain rates and to uniaxial compressive tests at impact strain rates. The observed shear hardening was greatest when there was no imposed density increase and practically zero when the angle of impact was less than 15 degrees. The shear hardening appeared to be a unique function of the main tensile extension ratio and was a polymer contribution, whereas the volumetric hardening was due to the isothermal compression of the cell gas. Eoam material models for FEA needed to be reformulated to consider the physics of the hardening mechanisms, so their... [Pg.18]

The thermal conductivity, thermal expansion, mechanical properties at low strain rates and dynamic mechanical properties of a collection of crosslinked closed cell PE foams manufactured by a high pressure nitrogen solution process were studied as a function of the cell size. The... [Pg.36]

The mechanical properties at low strain rates, dynamic mechanical properties, creep-recovery behaviour, thermal expansion and thermal conductivity of foams manufactured from blends of LDPE with an EVA and with an isoprene-styrene block copolymer were studied as a function of the LDPE content in the blends. The experimental results demonstrated important aspects related to the modification of the foam properties by blending. 16 refs. [Pg.66]

The cross-link density can be determined by equilibrium swelling or from equilibrium stress-strain measurements at low strain rate, elevated temperature, and sometimes in the swollen state3 °... [Pg.103]

The value of Ci is obtained from the plot of o/2(X - A ) vs. 1A and extrapolating to 1A = 0. By comparison with the theory of elasticity, it has been proposed that Cl = 1/2 NRT, where N is cross-link density, R the gas constant, and T the absolute temperature (of the measurement). To assure near-equilibrium response, stress-strain measurements are carried out at low strain rate, elevated temperature, and sometimes in the swollen state. °... [Pg.103]

One of the simplest criteria specific to the internal port cracking failure mode is based on the uniaxial strain capability in simple tension. Since the material properties are known to be strain rate- and temperature-dependent, tests are conducted under various conditions, and a failure strain boundary is generated. Strain at rupture is plotted against a variable such as reduced time, and any strain requirement which falls outside of the boundary will lead to rupture, and any condition inside will be considered safe. Ad hoc criteria have been proposed, such as that of Landel (55) in which the failure strain eL is defined as the ratio of the maximum true stress to the initial modulus, where the true stress is defined as the product of the extension ratio and the engineering stress —i.e., breaks down at low strain rates and higher temperatures. Milloway and Wiegand (68) suggested that motor strain should be less than half of the uniaxial tensile strain at failure at 0.74 min.-1. This criterion was based on 41 small motor tests. [Pg.229]

While the Bingham plastic model is an adequate approximate description of foam rheology, it is by no means exact, especially at low strain rates. More detailed models attempl to relate the rheological properties of foams to the structure and behavior of the bubbles. [Pg.663]

Under conditions where chain mobility is high enough, typically at high temperature and low strain rate, the loss of entanglement in the active layer at the craze-bulk interface can occur by chain disentanglement, resulting in chain disentanglement craze (CDC). [Pg.230]

When polymer thin films are deformed under certain conditions (usually low strain rates and temperatures higher than those at which only CSCs are ob-... [Pg.232]

The changes in crack propagation types (from stable to stick-slip) are associated with the crack blunting mechanism, which is favored by high temperatures and low strain rates, conditions that decrease general trends cannot be extended to very high strain rates because a transition from isothermal to adiabatic conditions may... [Pg.386]

The theory of sqeezing flow rheometry assumes that the sample is nonelastic. Tests on viscoelastic samples should therefore be carried out at low strain rates, to minimize elastic response, and results should be reported as apparent elongational viscosity. [Pg.762]

Relevant and complementary information about the damage process of polymers can be obtained among others by the analysis of the force-displacement curves, by the observation of the fracture surfaces (cf. Sects. 3.2.5 and 5.4) and, as will be shown in Sect. 6.2.2, by the determination of the amount of voids in a sample during and/or after deformation. However, a complete elucidation of the deformation mechanisms is only possible by their direct observation at the sub-micron level. Transmission electron microscopy is often used for this purpose. For convenience, the tests (which require experience and touch) are generally carried out at room temperature and at a low strain rate. [Pg.81]


See other pages where Low Strain Rates is mentioned: [Pg.150]    [Pg.153]    [Pg.181]    [Pg.403]    [Pg.1264]    [Pg.1282]    [Pg.118]    [Pg.98]    [Pg.138]    [Pg.79]    [Pg.284]    [Pg.436]    [Pg.147]    [Pg.36]    [Pg.61]    [Pg.525]    [Pg.33]    [Pg.56]    [Pg.150]    [Pg.153]    [Pg.264]    [Pg.67]    [Pg.118]    [Pg.253]    [Pg.342]    [Pg.85]    [Pg.86]    [Pg.853]    [Pg.718]    [Pg.585]    [Pg.463]   


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Low strain rate deformation

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