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Young’s modulus elasticity

We have written Eq. (5.4) with variables grouped as they are in order to define two very important quantities. The first quantity in parentheses is called the modulus—or in this case, the tensile modulus, E, since a tensile force is being applied. The tensile modulus is sometimes called Young s modulus, elastic modulus, or modulus of elasticity, since it describes the elastic, or recoverable, response to the applied force, as represented by the springs. The second set of parentheses in Eq. (5.4) represents the tensile strain, which is indicated by the Greek lowercase epsilon, e. The strain is defined as the displacement, r — rp, relative to the initial position, rp, so that it is an indication of relative displacement and not absolute displacement. This allows comparisons to be made between tensile test performed at a variety of length scales. Equation (5.4) thus becomes... [Pg.383]

As with other ceramic composites, the combination of a- and/or P-sialon with reinforcement agents results in sialon composites. This simple and obvious statement encompasses many factors which must be taken into account for successfully fabricating composites with a designed microstructure and improved properties (Prewo, 1989). For sialon matrix composites, the most important factors are physical compatibility including Young s modulus, elastic strain (Kerans and Parthasarathy, 1991) and thermal expansion coefficient (Sambell etal., 1972a, b), and chemical compatibility between sialon matrix... [Pg.493]

Pad porosity is inversely related to its density. Many physical properties of the polyurethan pad are strongly dependent upon its porosity (or density). The hardness and Young s modulus (elastic or storage modulus) of porous pads have a clear linear correlation with the density (or porosity) of the pads [1]. It is obvious that nonporous (noncell) pads have much smaller variability in density and other physical properties compared to porous pads. Nonporous pads have much higher strength, modulus, hardness, and elongation than porous pads. [Pg.128]

DEFINE Young s Modulus (Elastic Modulus) as it relates to stress. [Pg.49]

Young s Modulus (Elastic Modulus) is the ratio of stress to strain, or the gradient of the stress-strain graph. It is measured using the following equation ... [Pg.66]

SF2.1. Withstanding the pressure exerted by the liquid contained in the bottle Rigidity Toughness Young s modulus Elastic limit... [Pg.125]

SF5.1. Withstanding the handling and transport (in a truck, a car, etc.) Rigidity Toughness Shock resistance Young s modulus Elastic limit Shock resistance... [Pg.125]

Figure 5.17 shows stress-strain curves of neat PVAc and its nanocomposites in different PEDOT-PSS contents at 30 1°C. The slope of the stress-strain curve in the elastic deformation region is the modulus of elasticity (Young s modulus—elastic modulus). It represents the stiffness of the material resistance to elastic strain. [Pg.153]

Large-scale atomic/ molecular massively parallel simulator (LAMMPS) code 0.788 for armchair 1.176 for zigzag Effects of chirality and Van der Waals interaction on Young s modulus, elastic compressive modulus, bending, tensile, compressive stiffness, and critical axial force of DWCNTs... [Pg.245]

E = Young s modulus (elastic modulus or E-modulus) for each fiber... [Pg.82]

It should be mentioned that (1/pc) = M(E)/YI, where M(E) is the local induced bending moment and is a function of the imposed electric field E, Y is the Young s modulus (elastic stiffness) of the strip, which is a function of the hydration H of the IPMNC, and I is the... [Pg.147]

The modulus of elasticity is also called Young s modulus, elastic modulus, or just modulus. E was defined by Thomas Young in 1807 although others used the concept that included the Roman Empire and Chinese-BC. It is expressed in terms such as MPa or GPa (psi or Msi). A plastic with a proportional limit and not loaded past its proportional limit will return to its original shape once the load is removed. [Pg.79]

Young s modulus/ elastic modulus/ modulus of elasticity Elastizitatsmodul, Zugmodul, Youngscher Modul... [Pg.557]

The Young s modulus (elastic modulus) of a material is the stress versus strain for the material under elastic (reversible) deformation. Often, it is impossible to separate the film from the substrate without altering its properties, so the measurements must be made on the substrate, This often influences the properties being measured. [Pg.419]

Keywords polyamide (PA), polyethyleneterephthalate (PET), tensile properties, stress, strain, tensile strength, break. Young s modulus, elasticity, system compliance, grips, ASTM, ISO, design, test... [Pg.55]

Restored parameters for the evaluation of PDSM, may be different PMF of material tensor of stresses or its invariants, spatial gradients of elastic features (in particular. Young s modulus E and shear modulus G), strong, technological ( hardness HRC, plasticity ), physical (density) and others. [Pg.250]

The ratio of stress to strain in the initial linear portion of the stress—strain curve indicates the abiUty of a material to resist deformation and return to its original form. This modulus of elasticity, or Young s modulus, is related to many of the mechanical performance characteristics of textile products. The modulus of elasticity can be affected by drawing, ie, elongating the fiber environment, ie, wet or dry, temperature or other procedures. Values for commercial acetate and triacetate fibers are generally in the 2.2—4.0 N/tex (25—45 gf/den) range. [Pg.292]

Elasticity. Glasses, like other britde materials, deform elastically until they break in direct proportion to the appHed stress. The Young s modulus E is the constant of proportionaUty between the appHed stress and the resulting strain. It is about 70 GPa (10 psi) [(0.07 MPa stress per )Tm/m strain = (0.07 MPa-m) / Tm)] for a typical glass. [Pg.299]

Magnesium alloys have a Young s modulus of elasticity of approximately 45 GPa (6.5 x 10 psi). The modulus of rigidity or modulus of shear is 17 GPa (2.4 X 10 psi) and Poisson s ratio is 0.35. Poisson s ratio is the ratio of transverse contracting strain to the elongation strain when a rod is stretched by forces at its ends parallel to the rod s axis. [Pg.328]

Fig. 7. Relations between elastic constants and ultrasonic wave velocities, (a) Young s modulus (b) shear modulus (c) Poisson s ratio and (d) bulk... Fig. 7. Relations between elastic constants and ultrasonic wave velocities, (a) Young s modulus (b) shear modulus (c) Poisson s ratio and (d) bulk...
Moduli and Poisson s Ratio. The Young s modulus of vitreous sihca at 25°C is 73 GPa (<1.06 x 10 psi), the shear modulus is 31 GPa (<4.5 X 10 psi), and the Poisson s ratio is 0.17. Minor differences in values can arise owing to density variations. The elastic modulus decreases with increasing density and Poisson s ratio increases (26). [Pg.506]

It is important to differentiate between brittie and plastic deformations within materials. With brittie materials, the behavior is predominantiy elastic until the yield point is reached, at which breakage occurs. When fracture occurs as a result of a time-dependent strain, the material behaves in an inelastic manner. Most materials tend to be inelastic. Figure 1 shows a typical stress—strain diagram. The section A—B is the elastic region where the material obeys Hooke s law, and the slope of the line is Young s modulus. C is the yield point, where plastic deformation begins. The difference in strain between the yield point C and the ultimate yield point D gives a measure of the brittieness of the material, ie, the less difference in strain, the more brittie the material. [Pg.138]

Elastic behavior is commonly quantified by the Young s modulus E, the proportionality constant between the appHed tensile stress O, and the tensile strain (A length/original length). [Pg.317]

P = pressure of liquid Vl = volume of hquid Ey = Young s modulus of elasticity V = Poisson s ratio... [Pg.2282]


See other pages where Young’s modulus elasticity is mentioned: [Pg.228]    [Pg.43]    [Pg.126]    [Pg.60]    [Pg.132]    [Pg.228]    [Pg.43]    [Pg.126]    [Pg.60]    [Pg.132]    [Pg.270]    [Pg.411]    [Pg.248]    [Pg.175]    [Pg.194]    [Pg.500]    [Pg.210]    [Pg.290]    [Pg.317]    [Pg.317]    [Pg.222]    [Pg.2279]    [Pg.78]    [Pg.297]    [Pg.239]    [Pg.370]    [Pg.48]   


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Comparison of Young s modulus from forceindentation curves using Hertz elastic and

Comparison of Young s modulus from forceindentation curves using Hertz elastic and JKR model

Elasticity modulus

Young modulus

Young’s

Young’s modulus of elasticity

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