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Fourier Transform mechanical

For the continuous mode, we utilized a dynamic rheological technique, Fourier transform mechanical spectroscopy (FTMS) (77,75), which provided a powerful method for monitoring, simultaneously, the evolving dynamic moduli at several frequencies during the course of photo-cross-linking. In this technique, an oscillatory strain, y, was applied to the sample, such that... [Pg.154]

Fourier Transform Mechanical Analysis and Phenomenological Representation of Viscoelastic Material Behavior... [Pg.92]

Spectral analysis techniques to study the behavior of pol3rmers subjected to dynamic mechanical loads and/or deformation is called Fourier Transform Mechanical Analysis (FTMA). FTMA measures the complex moduli over a range of frequencies in one test by exciting the sample by a random signal (band limited white noise) (13.14). FTMA overcomes or circumvents problems inherent in other test methods because it measures dynamic mechanical properties over a wide range of frequency with minimal temperature and moisture changes within the sample. [Pg.94]

Fourier transform mechanical analysis (FTMA) measures isothermal viscoelastic properties of pol)nmers over a wider range of frequencies in a shorter period of time than is possible with other techniques. [Pg.109]

Infrared spectroscopy instrumentation is almost as widely varying as the applications. Mid-infrared instrumentation today consists almost exclusively of Fourier transform instruments. Although dispersive mid-IR instruments are still used, only a few manufacturers still produce these instruments. Dispersive mid-IR instruments have found a niche in the process monitoring field. Near-infrared instrumentation, on the other hand, is still dominated by dispersive instruments. Recently, some manufacturers have begun to offer near-IR instruments with Fourier transform mechanics and optics. [Pg.522]

This criterion for gel-point detection, and the non-equilibrium nature of systems imdergoing gelation, requires that data be obtained rapidly over a wide range of frequeney, prompting the development of a frequeney multiplexing technique known as Fourier Transform Mechanical Spectroscopy, FTMS, which allows the measurement of G at several frequencies simultaneously, rather than eonseeutively, as in a conventional test [Holly et al., 1988]. [Pg.60]

Holy, E.E., Venktaraman, S.K., Chambon, E., and Winter, H.H. (1988) Fourier transform mechanical spectroscopy of viscoelastic materials with transient structure. J. Non-Newton. [Pg.41]

Besides the intrinsic usefulness of Fourier series and Fourier transforms for chemists (e.g., in FTIR spectroscopy), we have developed these ideas to illustrate a point that is important in quantum chemistry. Much of quantum chemistry is involved with basis sets and expansions. This has nothing in particular to do with quantum mechanics. Any time one is dealing with linear differential equations like those that govern light (e.g. spectroscopy) or matter (e.g. molecules), the solution can be written as linear combinations of complete sets of solutions. [Pg.555]

Gc/k instmments are all of the gc/fdr variety that utilize an interferometer and requke a Fourier transform of the signal as opposed to employing a monochrometer and mechanical scanning. At least 3 scan/second are needed across the capillary gc peaks which are from 3 to 6 seconds wide. [Pg.402]

Interferometry is difficult in the uv because of much greater demands on optical alignment and mechanical stabiUty imposed by the shorter wavelength of the radiation (148). In principle any fts interferometer can be operated in the uv when the proper choice of source, beam spHtter, and detector is made, but in practice good performance at wavelengths much shorter than the visible has proved difficult to obtain. Some manufacturers have claimed operating limits of 185 nm, and Fourier transform laboratory instmments have reached 140 nm (145). [Pg.316]

Siesler, H. W. Rheo-Optical Fourier-Transform Infrared Spectroscopy Vibrational Spectra and Mechanical Properties of Polymers. Vol. 65, pp. 1-78. [Pg.215]

An amine-terminated poly ether (ATPE) is prepared as follows. Charge poly(tetramethylene oxide) diol (PolyTHF 1000, BASF, 75.96 g, 0.0759 m) to a 500-mL three-neck round-bottom flask fitted with a thermocouple, a mechanical stirrer, and a vacuum port. Add tert-butylacetoacetate (24.04 g, 0.1582 m) and apply vacuum. Heat at 175° C for 4 h, Fourier transform infrared (FTIR) analysis should indicate complete loss of the polyol OH absorption at 3300 cm. The room temperature viscosity of the product should be about 520 mPa-s. React this acetoacetylated product (85.5 g, 0.0649 m) with cyclohexylamine (14.5 g, 0.1465 m) at 110° C under vacuum for several hours. Cool the resultant cyclohexylaminocrotonate poly ether product to room temperature (1790 mPa-s at room temperature). [Pg.255]

This is a nonpolar rubber with very little unsamration. Nanoclays as well as nanotubes have been used to prepare nanocomposites of ethylene-propylene-diene monomer (EPDM) rubber. The work mostly covers the preparation and characterization of these nanocomposites. Different processing conditions, morphology, and mechanical properties have been smdied [61-64]. Acharya et al. [61] have prepared and characterized the EPDM-based organo-nanoclay composites by X-ray diffracto-gram (XRD), Fourier transform infrared spectroscopy (FTIR), scanning electron microscopy... [Pg.35]

Figure 3.3 The mechanics of obtaining a two-dimensional NMR spectrum. As the l value is varied, the magnetization vectors are caught during detection at their various positions on the x /-plane. The value of the detection time l-i is kept constant. The first set of Fourier transformations across is followed by transposition of the data, which aligns the peaks behind one another, and a second set of Fourier transformations across t then affords the 2D plot. Figure 3.3 The mechanics of obtaining a two-dimensional NMR spectrum. As the l value is varied, the magnetization vectors are caught during detection at their various positions on the x /-plane. The value of the detection time l-i is kept constant. The first set of Fourier transformations across is followed by transposition of the data, which aligns the peaks behind one another, and a second set of Fourier transformations across t then affords the 2D plot.
It is only since 1980 that in situ spectroscopic techniques have been developed to obtain identification of the adsorbed intermediates and hence of reliable reaction mechanisms. These new infrared spectroscopic in situ techniques, such as electrochemically modulated infrared reflectance spectroscopy (EMIRS), which uses a dispersive spectrometer, Fourier transform infrared reflectance spectroscopy, or a subtractively normalized interfacial Fourier transform infrared reflectance spectroscopy (SNIFTIRS), have provided definitive proof for the presence of strongly adsorbed species (mainly adsorbed carbon monoxide) acting as catalytic poisons. " " Even though this chapter is not devoted to the description of in situ infrared techniques, it is useful to briefly note the advantages and limitations of such spectroscopic methods. [Pg.76]

In the present study, we synthesized in zeolite cavities Co-Mo binary sulfide clusters by using Co and Mo carbonyls and characterized the clusters by extended X-ray absorption fine structure (EXAFS), X-ray photoelectron spectroscopy (XPS), Fourier transform infrared spectroscopy (FTIR), and high resolution electron microscopy (HREM). The mechanism of catalytic synergy generation in HDS is discussed. [Pg.503]

At present, most workers hold a more realistic view of the promises and difficulties of work in electrocatalysis. Starting in the 1980s, new lines of research into the state of catalyst surfaces and into the adsorption of reactants and foreign species on these surfaces have been developed. Techniques have been developed that can be used for studies at the atomic and molecular level. These techniques include the tunneling microscope, versions of Fourier transform infrared spectroscopy and of photoelectron spectroscopy, differential electrochemical mass spectroscopy, and others. The broad application of these techniques has considerably improved our understanding of the mechanism of catalytic effects in electrochemical reactions. [Pg.553]

Since the integral is over time t, the resulting transform no longer depends on t, but instead is a function of the variable s which is introduced in the operand. Hence, the Laplace transform maps the function X(f) from the time domain into the s-domain. For this reason we will use the symbol when referring to Lap X t). To some extent, the variable s can be compared with the one which appears in the Fourier transform of periodic functions of time t (Section 40.3). While the Fourier domain can be associated with frequency, there is no obvious physical analogy for the Laplace domain. The Laplace transform plays an important role in the study of linear systems that often arise in mechanical, electrical and chemical kinetic systems. In particular, their interest lies in the transformation of linear differential equations with respect to time t into equations that only involve simple functions of s, such as polynomials, rational functions, etc. The latter are solved easily and the results can be transformed back to the original time domain. [Pg.478]

Chen YX, Ye S, Heinen M, Jusys Z, Osawa M, Behm RJ. 2006b. Application of in-situ attenuated total refiection—Fourier transform infimed spectroscopy for the understanding of complex reaction mechanism and kinetics Formic acid oxidation on a Pt film electrode at elevated temperatures. J Phys Chem B 110 9534-9544. [Pg.200]


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