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Three-element standard solid

What is commonly called the three-element standard, or simply the standard solid (or Zener s solid), is a combination of either a Kelvin-Voigt element in series with a spring or, alternatively, a Maxwell element in parallel with a spring (see Fig. 10.6). The strain response of the first model to the stress input CT = cjoH(t) can be written as [Pg.400]

From this equation and taking into account that a = Goeii a = G1E2 + ti 2 [Pg.400]

For a stress history ct = CToFT(0 the Laplace transform of Eq. (10.27) gives [Pg.401]

The Laplace inverse of Eq. (10.32) gives the response of the model to the step strain input  [Pg.401]

The relaxation moduli in the time and frequency domains are given by [Pg.403]


By applying a Laplace transform to a three-element standard solid, the transitory response can also be obtained. In this case, Eq. (PIO.1.7) can be written as... [Pg.415]

Another model, attributed to Zener, consists of three elements connected in series and parallel, as illustrated in Figure 3.15, and known as the standard linear solid. Following the procedure already given, we derive the governing equation of this model ... [Pg.296]

Figure 4.12 Three-element models (a) is known as the standard linear solid (SLS)... Figure 4.12 Three-element models (a) is known as the standard linear solid (SLS)...
The empirical approach [7] was by far the most fruitful first attempt. The idea was to fit a few Fourier coefficients or form factors of the potential. This approach assumed that the pseudopotential could be represented accurately with around three Fourier form factors for each element and that the potential contained both the electron-core and electron-electron interactions. The form factors were generally fit to optical properties. This approach, called the Empirical Pseudopotential Method (EPM), gave [7] extremely accurate energy band structures and wave functions, and applications were made to a large number of solids, especially semiconductors. [8] In fact, it is probably fair to say that the electronic band structure problem and optical properties in the visible and UV for the standard semiconductors was solved in the 1960s and 1970s by the EPM. Before the EPM, even the electronic structure of Si, which was and is the prototype semiconductor, was only partially known. [Pg.251]

An analytical procedure for the determination of about 20 trace elements in coal samples after microwave digestion is described by Wang et al.15 It was found that high temperature digestion with HN03 alone (250 °C, 7.5 MPa) led to an extensive decomposition of the organic matrix and clay in coal, whereby solid carbon remained in the final solution after evaporation. Most of the trace elements were quantitatively dissolved in three standard coals. A lost of Hg was observed during the evaporation step. [Pg.390]

SOURCES of data Values of V d) were chosen to bring the total cohesive energy into agreement wiih experiment for the homopolar solid, and held fixed in the compounds isoelcctronic with them. The theoretical is predicted by using Eq. (7-3) and the values from the first three columns. Experimental values were obtained by adding the heal of formation (the energy required to separate the compound into elements in the standard state), from Wagman ct al. (1968), to the heat of atomization of the elements, from Kittcl (1967, p. 98). A correction of about 0.01 cV/bond should be made to compensate for the different temperatures at which the heat was measured. [Pg.176]

By way of illustrations we display in Fig. 1.17.2a plot of the molar heat capacity of oxygen under standard conditions. The plot of Cp vs. In T is then used to determine the entropy of oxygen from the area under the curves. Note that the element in the solid state exists in three distinct allotropic modifications, with transition temperatures close to 23.6 and 43.8 K the melting point occurs at 54.4 K, and the boiling point is at 90.1 K. All the enthalpies of transition at the various phase transformations are accurately known. An extrapolation procedure was employed below 14 K, which in 1929 was about the lower limit that could conveniently be reached in calorimetric measurements. [Pg.85]

The existence of reference materials and appropriate calibration procedures are two essential issues to be considered in quantifying the components of a sample. Quantitation has been substantially improved by the commercial availability of an increasing number of certified solid reference materials, especially for low concentration levels. Recently [42], NIST archival leaf standards were used as matrix-matched standards for reliable quantitative elemental analysis of Spanish moss samples. LA-ICP-MS was used with mixing standards in order to produce at least three data points for each calibration curve the results thus obtained were compared with those provided by microwave digestion ICP-MS/AES. Standard addition was also examined and found to be an effective method in the absence of matrix-matched standards. [Pg.446]

Very few of the elements listed on the Periodic Table of Elements exist as liquids at standard temperature and pressure. On the other hand, approximately three-fourths of our planet is covered with the liquid known as water, so you should be very familiar with the properties of liquids. Unlike solids, liquids do not have definite shape. If you pour a liquid from a cylindrical bottle into a square container, it changes shape to match the container. This is possible because the motion of the individual particles within the liquid is much less restricted than in a solid. The particles are not locked into fixed positions, and they push past each other, allowing the liquid sample to flow. Some liquids, such as water, flow readily, whereas other liquids, such as molasses, are said to be viscous and flow slowly. The viscosity of a liquid is its relative resistance to flow. Regardless of how fluid a liquid is, the space that a liquid occupies is more fixed, and it will not expand to occupy an entire vessel the way a gas will. [Pg.22]

Boron, atomic number 5, occurs naturally as two isotopes, and B, with natural abundances of 19.9% and 80.1%, respectively, (a) In what ways do the two isotopes differ from each other Does the electronic configuration of differ from that of B (b) Draw the orbital diagram for an atom of B. Which electrons are the valence electrons (c) Indicate three major ways in which the Is electrons in boron differ from its 2s electrons, (d) Elemental boron reacts with fluorine to form BF3, a gas. Write a balanced chemical equation for the reaction of solid boron with fluorine gas. (e) AHf for Bp3(g) is —1135.6 kl/mol Calculate the standard enthalpy change in the reaction of boron with fluorine, (f) When BCI3, also a gas at room temperature, comes into contact with water, the two react to form hydrochloric acid and boric add, H3BO3, a very weak acid in water. Write a balanced net ionic equation for this reaction. [Pg.237]


See other pages where Three-element standard solid is mentioned: [Pg.394]    [Pg.400]    [Pg.394]    [Pg.400]    [Pg.25]    [Pg.113]    [Pg.110]    [Pg.118]    [Pg.166]    [Pg.120]    [Pg.190]    [Pg.195]    [Pg.22]    [Pg.1082]    [Pg.141]    [Pg.78]    [Pg.84]    [Pg.74]    [Pg.31]    [Pg.411]    [Pg.168]    [Pg.195]    [Pg.456]    [Pg.74]    [Pg.12]    [Pg.675]    [Pg.667]    [Pg.68]    [Pg.39]    [Pg.827]    [Pg.718]    [Pg.408]    [Pg.19]    [Pg.246]    [Pg.438]    [Pg.420]   
See also in sourсe #XX -- [ Pg.400 ]




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Standards solid

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