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Fourier cylindrically averaged

The cylindrically averaged Fourier transform of the sevenfold and six-fold triple-stranded structures are shown in Figure 15. The Fourier transform of the six-fold triple-stranded model illustrates the symmetry of the system by the total absence of intensity on layer lines with index i 3 n, where n is an integer. The Fourier transform of the seven-fold triple-stranded structure shows that in destroying this precise symmetry relationship intensity occurs on all layer lines which are orders of the 2.27 nm spacing. This reinforces the concept of an indigenous triple-stranded structure which is perturbed slightly by the interaction of solvent. [Pg.408]

An infrared spectrum is a plot of percent radiation absorbed versus the frequency of the incident radiation given in wavenumbers (cm ) or in wave length ( xm). A variation of this method, diffuse reflectance spectroscopy, is used for samples with poor transmittance, e.g. cubic hematite crystals. Increased resolution and sensitivity as well as more rapid collection of data is provided by Fourier-transform-IR (FTIR), which averages a large number of spectra. Another IR technique makes use of attenuated total reflectance FTIR (ATR-FTIR) often using a cylindrical internal reflectance cell (CIR) (e.g. Tejedor-Tejedor Anderson, 1986). ATR enables wet systems and adsorbing species to be studied in situ. [Pg.141]

A simple and frequently occurring structural element in fibrous materials is the helix. 1 will use the relationship between the dimensions of simple helices and that of their diffraction patterns to illustrate how diffraction can reveal structural information. As a further simplification, 1 will assume that the helix axis is parallel to the fiber axis. As in all diffraction methods, the diffraction pattern is a Fourier transform of the object in the X-ray beam, averaged over all the orientations present in the sample. In the case of fibers, this means that the transform is averaged cylindrically, around the molecular axis parallel to the fiber axis. [Pg.189]

Consider a long cylindrical layer (such as a circular pipe) of inne.r radius r outer radius rz, length L, and average thermal conductivity k (Fig. 3-24). The two surfaces of the cylindrical layer arc maintained at constant temperatures T, and Tz- There is no heat generation in the layer and the thermal conductivity is constant. For one-dimensional heat conduction through the cylindrical layer, we have T r). Then Fourier s law of heat conduction for heat transfer through the cylindrical layer can be expressed as... [Pg.169]

SOLUTION A long cylindrical shaft is allowed to cool slowly. The center temperature and the heat transfer per unit length are to be determined. Assumptions 1 Heat conduction in the shaft is one-dimensional since it is long and it has thermal symmetry about the centerline. 2 The thermal properties of the shaft and the heat transfer coefficient are constant. 3 The Fourier number is t > 0.2 so that the one-term approximate solutions are applicable. Properties The properties of stainless steel 304 at room temperature are k - 14,9 W/m °C, p = 7900 kg/m r. = 477 J/kg X, and a = 3.95 X 10 mVs (Table A-3). More accurate results can be oblained by using properties at average temperature. [Pg.258]


See other pages where Fourier cylindrically averaged is mentioned: [Pg.37]    [Pg.390]    [Pg.217]    [Pg.151]    [Pg.259]    [Pg.90]    [Pg.383]   


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