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Surface tractions defined

Where a melt-crystallized polymer has been processed by drawing, rolling or other means to produce an aligned structure in which lamellae as well as polymer chains have discernible order, a pseudocrystalline unit cell is present. Provided that this unit cell contains elements of the crystals as well as the boundaries between crystals and that it is entirely typical of the material as a whole then it could be considered as a RVE within the meaning defined above. The lamella crystal itself sometimes considered as embedded in an amorphous matrix would not seem to be an acceptable RVE for reasons similar to those advanced against the Takayanagi model, namely that its modulus is dependent upon the surface tractions. The boundaries between lamella crystals in the matrix must be included in an acceptable RVE. [Pg.97]

In Eq. 14, u/x) is the / -th component of the velocity vector at the evaluation point x, f is the Stokeslet density function, and the real part of f corresponds to the real part of the surface traction if there is a single moving object that rigidly moves in the fluid i, is the i-th component of the relative position vector between the evaluation point and the field point, i.e., x = yi — x,, and X is the frequency parameter which is defined as... [Pg.189]

Viscosity, defined as the resistance of a liquid to flow under an applied stress, is not only a property of bulk liquids but of interfacial systems as well. The viscosity of an insoluble monolayer in a fluid-like state may be measured quantitatively by the viscous traction method (Manheimer and Schechter, 1970), wave-damping (Langmuir and Schaefer, 1937), dynamic light scattering (Sauer et al, 1988) or surface canal viscometry (Harkins and Kirkwood, 1938 Washburn and Wakeham, 1938). Of these, the last is the most sensitive and experimentally feasible, and allows for the determination of Newtonian versus non-Newtonian shear flow. [Pg.57]

The average force per unit area is Af,-/AS. This quantity attains a limiting nonzero value as AS approaches zero at point P (Cauchy s stress principle). This limiting quantity is called the stress vector, or traction vector T. But T depends on the orientation of the area element, that is, the direction of the surface defined by normal n. Thus it would appear that there are an infinite number of unrelated ways of expressing the state of stress at point P. [Pg.37]

Interfacial Viscosity. In a clean system in which two pure liquids produce an interface, the viscosity of the interface should be the same as the bulk solution viscosity. However, surfactant or impurity adsorption at an interface can cause a resistance to fiow to occur that can be measured as the interfacial shear viscosity. This viscosity is defined as the ratio between the shear stress and the shear rate in the plane of the interface (12), Methods used to make these measurements include a viscous traction surface viscometer (J2), droplet-droplet coalescence (J3), the rotating ring viscometer (14), and surface laser light scattering (9). [Pg.269]

F is the surface surrounding the domain Q. F refers to the subdomain of F where the i component of the displacement is known and Fj- to the subdomain of F where the i component of the traction force is known. In order to ensure the uniqueness of the solution, additional conditions are required on the boundary conditions Vf, mes(Fo > 0. Otherwise, the solution is defined within a rigid body motion. [Pg.819]

Recall the matrix equations of the BEE and how the boundary conditions are imposed on the system. The imposition of such boundary conditions requires, at aU points of the defined boimd-ary, the definition of one and only one of the couples (m , O or at least a combination of the two. When the motion of a particle in the fluid is considered neither the velocity components, nor the traction components, nor a combination of the two is known at a given element m. Rather, it is known that since the particle moves freely (e.g., free of forces), the net force over the surface will be zero. Also, the motion is a rigid body motion therefore, all points on the particle surface wiU have a velocity that can be expressed as Ui = u - + corii. [Pg.208]

Static coefficient of friction (SCOF) relates to the traction between a person s foot or shoe sole and the walking surface. We can define SCOE as the relative force that resists the tendency of the shoe or foot to slide along a walkway surface. ADA reconunends a minimum of 0.6 on level walking surfaces and 0.8 on ramps. OSHA requires an SCOF 0.5 in all areas. Slip resistance relates to a combination of factors including type of surface, and care and maintenance procedures with the presence of foreign materials between the foot/shoe sole and the walking surface. The AIA s Academy of Architecture for Healthcare states that floor materials shall be readily cleanable and appropriate for each location. Install water-resistant floors in all food preparation areas and in locations containing baths or showers. [Pg.97]

The stress acting on an exposed surface is also the only non-zero principal stress, because the exposed surface is assumed self-supporting and traction-free (i.e., no shear stresses acting on the surface). The flow factor is determined by the geometry of the hopper and the properties of the bulk material. Another function used by Jenike is the flow function . This flow function is the ratio of the consolidating pressure CTi to the unconfined yield strength as defined in Section 6.1.2 ... [Pg.267]

Fig. 6.2. A long straight dislocation in an elastic solid is parallel to a traction-free surface and at a distance tf from it. The dislocation is formed by an offset of one side of the shaded plane with respect to the other side defined by the Burgers vector bi. Fig. 6.2. A long straight dislocation in an elastic solid is parallel to a traction-free surface and at a distance tf from it. The dislocation is formed by an offset of one side of the shaded plane with respect to the other side defined by the Burgers vector bi.

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See also in sourсe #XX -- [ Pg.39 ]




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