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Complex compliance tensile

Compliance n The degree to which a material deforms under stress the reciprocal of the modulus. Thus, in each mode of stress, the material is characterized by three moduli and their reciprocals, three compliances. However, when the stress is varying, the real and imaginary parts of the complex compliances are not equal to the reciprocals of their counterparts in the Complex Modulus. Tensile compliance the reciprocal of Young s modulus shear compliance the reciprocal of shear modulus. [Pg.161]

A full description of the relation between (Tzz t) and ezz t) is provided by the complex dynamic tensile compliance jD, defined as... [Pg.194]

We note that, in principle, the main physical discussions related to filler networking in this paper do not change if a sinusoidal tensile or uniaxial compres-sional stress (amplitude 0) is imposed on the rubber material. In some examples the complex dynamic modulus is then denoted with E = E + iE" and the compliance with C = C - iC". All theoretical considerations use the shearing modulus G. ... [Pg.3]

Differentiate and substitute this equation into Equation 13-85 and obtain the following expression for the complex tensile compliance D, defined as the difference in strain at times t2 and tx divided by the difference in stress at these two times ... [Pg.471]

Finally, the complex tensile compliance, and the complete tensile... [Pg.256]

The viscoelastic properties of the crystalline zones are significantly different from those of the amorphous phase, and consequently semicrystalline polymers may be considered to be made up of two phases each with its own viscoelastic properties. The best known model to study the viscoelastic behavior of polymers was developed for copolymers as ABS (acrylonitrile-butadiene-styrene triblock copolymer). In this system, spheres of rubber are immersed in a glassy matrix. Two cases can be considered. If the stress is uniform in a polyphase, the contribution of the phases to the complex tensile compliance should be additive. However, if the strain is uniform, then the contribution of the polyphases to the complex modulus is additive. The... [Pg.496]

For orthorhombic symmetry on the other hand, tensile creep and lateral compliance measurements on specimens cut from oriented sheet will yield only 6 of the 9 required creep functions those not accessible by this method being Suit), Sssit) and S66(t)- The two shear compliances 555(1) and Seeit) can be obtained by torsional creep experiments, but these need to be carefully designed and involve complex experimental procedures. The only possibility for measurement of Su(t) on sheet appears to be by compressive creep techniques, however, one would expect substantial experimental difficulties largely associated with strain measurement and specimen geometry. There appears to be no reported evaluation of the full characterisation of creep for the case of orthorhombic synunetry. [Pg.333]

By employing the complex tensile compliance D in an analogous manner to J (see text), D and D" can be used to obtain the in-phase and (90°) out-of-phase components of e, thus... [Pg.132]

Special specimen preparation as with tensile testing. However, the extraction of intrinsic mechanical parameters from creep indentation data is analytically complex [3, 4]. Confined compression or unconfined compression tests require preparation of cylindrical cored specimens of tissue and underlying bone. With unconfined compression, the free draining tissue edges and low aspect ratio, layered nature of the test specimen may introduce error. Compression of a laterally confined specimen by a porous plunger produces uniaxial deformation and fluid flow. Confined compression creep data has been analyzed to yield an aggregate equilibrium compressive modulus and permeability coefficient [5] and uniaxial creep compliance [6]. [Pg.42]

In some cases, the inverse values of the complex modulae named compliances are used these are similar to the transient modulae and compliances such as seen in Eq. (24.9). The complex tensile compliance D is thus defined as... [Pg.439]

Figure 3. Dipole centered in a sphere (represented by the arrow) surrounded by an environment with properties that depend on the model. In the case of the Debye model, the environment has a viscosity tj independent of time. In the DiMarzio-Bishop model the viscosity is a complex time-dependent viscosity = lit). In the Havriliak-Havriliak model the cavity is not spherical and the environment is taken to be represented by a complex tensile compliance D( Figure 3. Dipole centered in a sphere (represented by the arrow) surrounded by an environment with properties that depend on the model. In the case of the Debye model, the environment has a viscosity tj independent of time. In the DiMarzio-Bishop model the viscosity is a complex time-dependent viscosity = lit). In the Havriliak-Havriliak model the cavity is not spherical and the environment is taken to be represented by a complex tensile compliance D(<a = 1 It).
The viscoelastic properties of materials in other modes of deformation may also be described in terms of a complex modulus or a compliance. In the case of dynamic tensile tests, the complex modulus is given by... [Pg.542]


See other pages where Complex compliance tensile is mentioned: [Pg.183]    [Pg.227]    [Pg.774]    [Pg.194]    [Pg.230]    [Pg.216]    [Pg.24]    [Pg.593]    [Pg.42]    [Pg.990]    [Pg.285]    [Pg.57]    [Pg.161]    [Pg.131]    [Pg.1058]    [Pg.115]    [Pg.862]    [Pg.506]    [Pg.255]   
See also in sourсe #XX -- [ Pg.24 ]




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