By S. Eichhorn, J.W. S. Hearle, M. Jaffe, T. Kikutani
Because of their complexity and variety, figuring out the constitution of fabric fibers is of key value. This authoritative assortment presents a finished overview of the constitution of an intensive variety of fabric fibers. After an introductory set of chapters on fiber constitution and techniques to signify fibers, the publication is classed into 3 major fiber teams. the second one a part of the booklet contains chapters that evaluation the constitution of usual cellulosic and protein fibers, together with cotton, silk, and wool. half 3 covers the constitution of synthetic polymer fibers, for instance polyester, polyamides, elastomeric fibers, and high-modulus, high-tenacity polymer fibers. The concluding a part of the publication discusses the constitution of a number of different cloth fibers similar to glass, carbon and optical fibers. Edited by means of prime gurus at the topic and with a workforce of foreign authors, the guide of cloth Fiber constitution is a vital reference for fabric technologists, fiber scientists, cloth engineers, and people in academia.
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Extra resources for Handbook of Textile Fibre Structure, Volume 1: Fundamentals and Manufactured Polymer Fibres (Woodhead Publishing in Textiles)
Example text
When [α] has spherical symmetry. This analysis is for an isotropic system of scattering molecules. e. where there is uniaxial orientation, such as for a fibre. To understand this type of symmetry and the effect on the orientation it is necessary to introduce the concept of the orientation distribution function where N(f, q, y) sin q dq dy df is the fraction of scattering units having orientation within the general solid angle sin q dq dy df using the angles as defined in Fig. 3. 3 Definitions of the Euler angles (θ, φ, ψ) the molecular and Raman tensor axes (x, y, z) and the specimen axes (X, Y, Z).
For 25 years, this was the conventional view. Although a verbal statement was easy, the detailed views varied greatly, often reflecting the personality or artistic skill of the author as much as the scientific evidence, as shown by the two examples in Fig. 2. One feature that is common to all the drawings from this period is that the molecules run continuously along the oriented fibre structures with no folding back. 1 Micellar model as drawn by Seifriz (1929) and Meyer (1930). 2 Fringed micelle structure as drawn by (a) Frey-Wyssling (1938, 1953) and (b) Mark (1940).
In this sense, infrared spectroscopy is not sensitive to symmetric vibrations such as –C–C–. Therefore, for polymeric materials, the main-chain or backbone structure is often not detected using this technique, and it is usually the side-chain motions of atoms that give rise to absorptions. Infrared spectroscopy often also relies on the preparation of a thin sample of material, since it typically works in transmission, apart from when used in an ATR (Attenuated Reflectance) 24 Handbook of textile fibre structure mode.