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Fiber behavior

Copper and zinc were also bound. The metals were released by hemicellulase and peptidase action. These hemi-cellulose isolates included considerable amounts of digestible protein and consequently do not conform to the concept of fiber as a non-digestible residue. However, close associations of fiber and protein do occur and their implications for fiber behavior must be recognized Mod et al (15) assign a role to fiber bound protein in binding of metals. Thompson and Weber (16) observed that ion exchange properties of dietary fiber depended upon method of preparation. [Pg.146]

Special experiments were carried out for the estimation of ultrathin fibers behavior in ozone atmosphere as in effective oxide-active medium. [Pg.410]

Most materials expand when heated. However, many fibers contract when heated. This fiber behavior is called thermal contract, or negative thermal expansion. [Pg.344]

Rosenbaum, S., Polyacrylonitrile Fiber Behavior. I. Mechanisms of Tensile... [Pg.365]

Rosenbaum, S., Polyacrylonitrile Fiber Behavior. I. Dependence on Structure and Enviromnent , Journal of Applied Polymer Science, 9, 2085-2099, 1965. [Pg.365]

Shaving products Shaw process Shear breeding Shear energy Shearlings Shearometer Shear plane Shear rate Shear stresses Shear test Shear thinning behavior Shear viscosity Sheath-core fiber... [Pg.882]

Acrylonitrile has been grafted onto many polymeric systems. In particular, acrylonitrile grafting has been used to impart hydrophilic behavior to starch (143—145) and polymer fibers (146). Exceptional water absorption capabiUty results from the grafting of acrylonitrile to starch, and the use of 2-acrylamido-2-methylpropanesulfonic acid [15214-89-8] along with acrylonitrile for grafting results in copolymers that can absorb over 5000 times their weight of deionized water (147). [Pg.197]

The resistance to plastic flow can be schematically illustrated by dashpots with characteristic viscosities. The resistance to deformations within the elastic regions can be characterized by elastic springs and spring force constants. In real fibers, in contrast to ideal fibers, the mechanical behavior is best characterized by simultaneous elastic and plastic deformations. Materials that undergo simultaneous elastic and plastic effects are said to be viscoelastic. Several models describing viscoelasticity in terms of springs and dashpots in various series and parallel combinations have been proposed. The concepts of elasticity, plasticity, and viscoelasticity have been the subjects of several excellent reviews (21,22). [Pg.271]

Noncrystalline domains in fibers are not stmctureless, but the stmctural organization of the polymer chains or chain segments is difficult to evaluate, just as it is difficult to evaluate the stmcture of Hquids. No direct methods are available, but various combinations of physicochemical methods such as x-ray diffraction, birefringence, density, mechanical response, and thermal behavior, have been used to deduce physical quantities that can be used to describe the stmcture of the noncrystalline domains. Among these quantities are the amorphous orientation function and the amorphous density, which can be related to some of the important physical properties of fibers. [Pg.272]

The elongation of a stretched fiber is best described as a combination of instantaneous extension and a time-dependent extension or creep. This viscoelastic behavior is common to many textile fibers, including acetate. Conversely, recovery of viscoelastic fibers is typically described as a combination of immediate elastic recovery, delayed recovery, and permanent set or secondary creep. The permanent set is the residual extension that is not recoverable. These three components of recovery for acetate are given in Table 1 (4). The elastic recovery of acetate fibers alone and in blends has also been reported (5). In textile processing strains of more than 10% are avoided in order to produce a fabric of acceptable dimensional or shape stabiUty. [Pg.292]

Electrical Behavior. The resistivity of acetate varies significantly with humidity with typical values ranging from 10 ohm-cm at 45% rh to 10 ohm-cm at 95% rh (16). Because of the high resistivity both acetate and triacetate yams readily develop static charges and an antistatic finish is usually apphed to aid in fiber processing. Both yams have also been used for electrical insulation after lubricants and other finishing agents are removed. [Pg.293]

A common measurement usehil in predicting threadline behavior is fiber tension, frequentiy misnamed spinline stress. It is normally measured after the crystallization point in the threadline when the steady state is reached and the threadline is no longer deformed. Fiber tension increases as take-up velocity increases (38) and molecular weight increases. Tension decreases as temperature increases (41). Crystallinity increases slightiy as fiber tension is increased (38). At low tension, the birefringence increases as tension is increased, leveling off at a spinline tension of 10 MPa (1450 psi) (38). [Pg.317]

F. P. McCuUough and B. C. Goswami, "Novel Fibers and Their Ignition Behavior," Hi-Tech Conference, Clemson University, S.C., July 21,1993. [Pg.74]

Boltzmann s constant, and T is tempeiatuie in kelvin. In general, the creep resistance of metal is improved by the incorporation of ceramic reinforcements. The steady-state creep rate as a function of appHed stress for silver matrix and tungsten fiber—silver matrix composites at 600°C is an example (Fig. 18) (52). The modeling of creep behavior of MMCs is compHcated because in the temperature regime where the metal matrix may be creeping, the ceramic reinforcement is likely to be deforming elastically. [Pg.204]

Because the fibers generally are anisotropic, they tend to be deposited on the wire in layers under shear. There is Htde tendency for fibers to be oriented in an out-of-plane direction, except for small undulations where one fiber crosses or passes beneath another. The layered stmcture results in the different properties measured in the thickness direction as compared to those measured in the in-plane direction. The orthotropic behavior of paper is observed in most paper properties and especially in the electrical and mechanical properties. [Pg.2]


See other pages where Fiber behavior is mentioned: [Pg.269]    [Pg.271]    [Pg.454]    [Pg.177]    [Pg.454]    [Pg.218]    [Pg.201]    [Pg.274]    [Pg.86]    [Pg.86]    [Pg.197]    [Pg.174]    [Pg.269]    [Pg.271]    [Pg.454]    [Pg.177]    [Pg.454]    [Pg.218]    [Pg.201]    [Pg.274]    [Pg.86]    [Pg.86]    [Pg.197]    [Pg.174]    [Pg.271]    [Pg.276]    [Pg.290]    [Pg.291]    [Pg.292]    [Pg.293]    [Pg.293]    [Pg.312]    [Pg.316]    [Pg.318]    [Pg.367]    [Pg.491]    [Pg.416]    [Pg.326]    [Pg.33]    [Pg.136]    [Pg.185]    [Pg.202]    [Pg.202]    [Pg.203]    [Pg.3]    [Pg.5]   
See also in sourсe #XX -- [ Pg.645 ]




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Carbon fiber reinforced polymer structural behavior

Cellulose fibers chemical behavior

Characterizing Fatigue Behavior in Fiber Reinforced Plastics

Continuous fiber composites fatigue behavior

Continuous fiber reinforced composites fatigue behavior

Continuous fiber-reinforced ceramic behavior

Creep behavior of continuous fiber-reinforced ceramics

Deformation Behavior of Fiber-Reinforced Plastic

Fatigue Behavior in Fiber-Reinforced Plastics

Fatigue behavior continuous fiber-reinforced ceramic

Fatigue behavior of continuous fiber reinforced composites under multiaxial loading

Fatigue behavior, continuous fiber

Fiber-reinforced plastics deformation behavior

Glass fiber elastic behavior

Glass fibers viscoelastic behavior

Long-Term Mechanical Behavior of Fiber Reinforced Plastics

Mechanical Behavior of Fiber Reinforced Plastics

Melting behavior of Nylon 6 fibers

Stability and Flow Behavior of Fiber-Containing Drilling Sweeps

Stress-Strain Behavior of Commercial Fibers

Stress-strain behavior fibers

Swelling Behavior, and the Effect of Fiber Shape on Reactivity

Thermal behavior, textile fibers

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