FibersVolume 1
Ullmann’s Fibers, Vol. 1c© 2008 Wiley-VCH Verlag GmbH & Co. KGaA, WeinheimISBN: 978-3-527-31772-1
Fibers, 1. Survey 3
Fibers, 1. Survey
Fritz Schultze-Gebhardt, Dusseldorf, Federal Republic of Germany (Chaps. 2 – 7)
Karl-Heinz Herlinger, Institut fur Chemiefasern der Deutschen Institute fur Textil- und FaserforschungStuttgart, Denkendorf, Federal Republic of Germany (Chaps. 2 – 8)
1. Introduction . . . . . . . . . . . . . . . . . 32. History . . . . . . . . . . . . . . . . . . . . 43. Characteristics of Fibers . . . . . . . . . 43.1. Fineness . . . . . . . . . . . . . . . . . . . . 43.2. Tenacity and Modulus of Elasticity . . 53.3. Elongation . . . . . . . . . . . . . . . . . . 54. Spinning . . . . . . . . . . . . . . . . . . . 54.1. Wet Spinning . . . . . . . . . . . . . . . . 54.2. Dry Spinning . . . . . . . . . . . . . . . . 64.3. Melt Spinning . . . . . . . . . . . . . . . . 65. Prerequisites for Fiber Formation . . 65.1. Molecular Mass and Fiber Formation 65.2. Molecular Structure and Fiber
Properties . . . . . . . . . . . . . . . . . . 75.3. Property Requirements for the
Formation of Fiber Structures . . . . . 8
5.4. Crystallization . . . . . . . . . . . . . . . 95.5. Organization of Structural Elements 95.6. Structural Models . . . . . . . . . . . . . 105.7. Molecular Symmetry and Physical
Properties . . . . . . . . . . . . . . . . . . 105.8. Changes in Properties Caused by
Symmetry Defects . . . . . . . . . . . . . 116. Fiber Properties Required by Textiles 126.1. Requirements to Be Met by Textiles . 126.2. Modification of Fiber Properties . . . 126.3. Comfort Properties of Textiles . . . . . 147. Economic Aspects . . . . . . . . . . . . . 148. Tabular Survey of Fibers . . . . . . . . 159. References . . . . . . . . . . . . . . . . . . 36
1. Introduction
The term fibers refers collectively to a wide va-riety of forms of fibrous materials. Standardshave been established to introduce order intothe field. The most frequently employed termsare defined here. Natural fibers that can be spuninto yarn are called staple fibers. The primaryspinning of man-made fibers results in the pro-duction of continuous filaments (endless fibers).Indeed, both monofilaments (threads; spinnerethas one hole) and multifilaments (spinneret hasmany holes) can be produced. A filament yarnconsists of a large number of filaments that canbe given texture by twisting, crimping and/orheat setting.
Theword tow refers to a fiber tapemade fromthousands of filaments. If a tow is cut or torn, itgives rise to staple fibers. Fiber tapes obtainedby cutting or tearing parallel to the fibers areknown as fiber bands.
Conventional standards divide fibers into (1)natural fibers and (2) man-made fibers (alsocalled chemical fibers).
Natural fibers are subdivided into plant andanimal fibers. Man-made fibers are subdivided
into natural materials brought into fiber form bya chemical reaction (regenerate fibers) and fibersmade from synthetic polymers (synthetic fibers).The following classification includes standard-ized abbreviations that are used occasionallythroughout this article:
1. Natural fibers1.1. Plant fibers, e.g.,cottonflaxhempjute
1.2. Animal fibers, e.g.,woolcamel hairangorasilk
2. Man-made fibers2.1. Fibers based on natural polymers, e.g.,viscose rayon (CV)Lyocell (CLY)cellulose acetate (CA)elastodiene (LA)
2.2. Fibers based on synthetic polymers(synthetic fibers), e.g.,polypropylene (PP)
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polyacrylonitrile (PAN)poly(vinyl chloride) (PVC),polyamide 6 (PA 6, nylon 6)polyamide 66 ( PA 6,6; nylon 66)poly(ethylene terephthalate) (PET)poly(ether ether ketone) (PEEK)polyurethane (PUR; spandex)
2. History
Natural Fibers. Natural fibers have beenused by humans for thousands of years. Animalhair and plant fibers were spun into yarn andwoven into textiles. Indeed, the textile industrytoday is still based on this ancient technology.
Man-Made Fibers. The idea of making “ar-tificial” fibers and threads is over 300 yearsold. In fact, the start of the chemical fiberindustry dates from about 1884. The processof regenerating fiber-forming cellulose wasbased on the discovery of solvents such ascopper oxide – ammonia by E. Schweizer in1857. Later, Count Chardonnet succeeded informing derivatives of cellulose which could besolubilized and spun into threads; “Chardonnetsilk” was first made in 1884. A detailed accountof the history of man-made fibers is not given inthis article. The subject was dealt with compe-tently by H. Klare in 1985 [19].
The most important developments in the pro-duction of man-made fibers based on cellulosewere:
1) the cuprammonium process for solubiliza-tion and spinning of cellulose;
2) the formation of spinning solutions of cellu-lose derivatives, such as cellulose nitrate andcellulose acetate;
3) the intermediate derivatization of celluloseto cellulose xanthate which in turn is spuninto cellulose fibers;
4) the development of new solvent sys-tems for cellulose, such as N-methylmor-pholine oxide (NMMO) or dimethylacet-amide – lithium chloride.
In 1927, H. Staudinger used polyoxy-methylene as a model of cellulose to demon-strate that fiber-forming polymers were linearpolymeric molecules.
The production of synthetic fibers was theresult of pioneering work on the formation ofsynthetic polymers and the development of ex-trusion techniques known as wet, dry, and meltspinning.
Nylon 66 was first synthesized by W.H.Carothers in 1935. This was closely followedby the discovery of nylon 6 by P. Schlack in1938. The work of J. R. Whinfield and I. T.Dickson led to the development of polyesterfibers in 1941. Today, polyamides and poly-esters are the largest-volume polymers capableof being melt-spun. The production of syntheticfibers based on familiar polymers such as poly-acrylonitrile, which cannot be melt-spun, wasmade possible by the introduction of new sol-vents, e.g., dimethylformamide (H.Rein, 1942).Discovery of the stereospecific polymerizationof propylene (G. Natta, 1954) led to the in-troduction of polyolefins into the fiber industry.The development of technology and the simul-taneous elucidation of structure and propertiesresulted in “tailor-made” polymers and fibers.Specific properties such as rubber elasticity (O.Bayer, 1947) or extreme tenacity and stiffnesswere realized (high-modulus fibers, P.W.Mor-gan andS. L.Kwolek, 1968). In addition, high-temperature fibers were made from polyhetero-cyclic compounds.
Apart from organic polymers, inorganic sub-stances such as glass, carbon, BN, and SiC werealso spun into fibers.
Future developments are likely to be directedtoward classical mass production, particularlytowards the attaining of optimal processing char-acteristics and clothing comfort. New types ofapplication – above all in the field of industrialfibers and in medical technology – will stimu-late the development of special fibers with veryspecific properties.
3. Characteristics of Fibers
3.1. Fineness
The thickness of fibers and filaments rangesfrom 1 to 100µm. Measuring thickness bymeans of conventional instruments is very diffi-cult. Indeed, even small variations in fiber uni-formity, thickness, and cross-sectional area hin-der microscopic measurement. To make a sta-
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tistically valid statement about the fineness of afiber (fiber density), length and mass are com-puted instead of thickness. The unit tex is usedto express fiber fineness. According to the ISO,
1tex = 1gper1000m
If 1000m of fiber weigh 1 g, the fineness is 1 tex.Another unit commonly used to express finenessis dtex. If themass per length is given in dtex, thenumerical values will be comparable to those inthe formerly used unit denier [46]:
1denier = 1gper9000m
3.2. Tenacity and Modulus of Elasticity
The cross-sectional area of fibers is generallynonuniform and cannot be determined easily.Hence, measurements based on area have lim-ited applicability. For this reason, tenacity is notmeasured in gigapascal (GPa) units (ISO) butis expressed relative to the fineness. Usually, themaximal tensile force (at break) is employed, ex-pressed in centinewtons per tex (cN/tex); otherunits used are cN/dtex (1 cN/dtex = 10 cN/tex) orN/tex (1N/tex = 100 cN/tex). Textile and indus-trial fibers have tenacities ranging from 10 tomore than 300 cN/tex (see Table 4). The mod-ulus of elasticity corresponds to the tangent tothe stress – strain curve at the origin (→Fibers,6. Testing and Analysis, Chap. 3.). It is also ex-pressed relative to the fineness, in cN/tex. Typ-ical moduli range from 50 to 1000 cN/tex fortextile fibers and from 1000 to 40 000 cN/tex forindustrial fibers. (See Table 5.)
3.3. Elongation
The highest possible degree of elongationat break (→Fibers, 6. Testing and Analysis,Chap. 3.) varies greatly with the type of fiber.Industrial fibers, e.g., carbon fibers and high-modulus aramids, have values of 0.1 – 2%; tex-tile fibers and yarns have values of 5 – 70%; andvalues of 300 – 700% are obtained for spandexfibers (see Table 4).
In practical applications, fibers are elongatedonly to a small extent. Maximal elongation is
never attained because otherwise fibers undergopartially irreversible stretching.
Temperature and moisture (weather) affectboth the tenacity and the elongation of fibers tovarying extents, depending on the type of poly-mer. The same applies to dimensional stabilityand wrinkling tendency, properties that are alsoinfluenced by the type of fiber and by the textilestructure.
4. Spinning
Both natural and synthetic fibers are consist-ing of linear polymers. These polymers are con-verted into fibrous form by growth (animal hair,plant fibers) or extrusion (spider, silkworm, spin-ning technology) and are specifically oriented tothe fiber axis. The many mechanisms found innature for the formation of filamentous struc-tures are, by no means completely understood(see e.g. [87]). Only a few processes are avail-able for large-scale production of man-madefibers. Specific production techniques are basedon the deformability of fiber polymers. In prin-ciple, a distinction is made between spinningmethods involving solutions and those involv-ing molten polymer. For a detailed descriptionof spinning, see →Fibers, 3. General Produc-tion Technology.
4.1. Wet Spinning
Polymer solutions are converted into fibers bydiluting a highly concentrated polymer solu-tion in a coagulating bath. The extremely vis-cous polymer solution, e.g., 3.5 – 10 Pa · s (stillhigher values are obtained with viscose rayon)can be extruded, i.e., spun, by forcing it througha spinneret to form threadlike structures. In gen-eral, polymers are soluble only in specific sol-vents. The viscous polymer solution is extrudedinto a coagulating bath where the solvent is di-luted, which results in precipitation of polymerthreads. For instance, polyacrylonitrile is solu-ble in dimethylformamide (DMF). In the coag-ulating bath, DMF is washed out of the viscouspolymer threads with water, and polyacryloni-trile fibers precipitate (Fig. 1).
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Figure 1. Fiber formation by solvent extraction in the spin-ning bathPAN=polyacrylonitrile: DMF= dimethylformamide
The solvent concentration in the fiber de-creases along the length of the coagulating bath.In wet spinning, several physicochemical pro-cesses occur simultaneously, e.g., solvent dif-fusion, polymer precipitation, and formation ofmembrane-like interfaces and system-specificmorphological structures. One of the main pur-poses of developingwet-spunpolymers is to pro-duce specific fiber structures in the coagulatingbath. This is achieved, in principle, by modifica-tion in the coagulating bath, which is describedin more detail under →Fibers, 4. Synthetic Or-ganic, Chap. 5.3.3., wet spinning of polyacry-lonitrile. In a spinning process of this type, thepolymer can also undergo a chemical reaction;e.g., the viscose process involves acid hydroly-sis of cellulose xanthate in the coagulating bath(→ Cellulose, Chap. 3.1.3.).
Tomake the process economical, the polymerconcentration should be kept as high as possi-ble during spinning. In the case of soluble poly-mers, the viscosity of the spinning solution, andthus its basic spinnability, are directly relatedto the concentration and solvation of the poly-mers. However, complicated processes, such asexchange, diffusion, and drying, that occur dur-ing wet and dry spinning result in polymer- andsolvent-dependent limitations on the polymerconcentration.
4.2. Dry Spinning
In dry spinning, the polymer solution is alsoforced through a spinneret. Solvent is then evap-orated in a warm current of air to produce almostsolvent-free filaments. Cellulose acetate, poly-acrylonitrile, and polyurethane are spun by thistechnique (→Fibers, 4. Synthetic Organic).
4.3. Melt Spinning
In melt spinning, the polymer is melted by heat-ing and then passed through a spinneret via aspinning pump. Only polymers that are ther-mally stable under melt conditions can be sub-jected to this extrusion (i.e., spinning) process.The fluid threads emerging from the spinneretsolidify on cooling (usually air cooling) to formfilaments. This technique is applied in spinning,e.g., nylon 6, nylon 66, or poly(ethylene tere-phthalate) (→Fibers, 4. Synthetic Organic).
The difference betweenmelting and spinningtemperatures depends on the viscosity of themelt. Usually, the spinning temperature is about30K higher than the melting temperature Tm.However, if the viscosity is still too high, thespinning temperature must be increased evenfurther. For example, Tm of polypropylene is170 C but the polymer is spun at 260 C. Themelt index, not the viscosity, is generally usedto characterize the melting properties of poly-mers. In fact, the tedious measurement of meltviscosity has now been replaced by simple massdetermination (→Fibers, 6. Testing and Analy-sis).
Hence, melt spinning requires polymers thatare thermally stable and, as far as possible, re-sistant to thermal oxidation at temperatures ap-proximately 30K higher than their melting tem-peratures (PA-6, PA-66, and PET).
Production conditions must be optimally co-ordinated with the properties of the product toachieve the desired melt viscosity, on the onehand, and the required fiber tenacity, on theother. Rapid advances in process technology,however, have made possible not only the pro-cessing of very highly viscousmelts, but also theextrusion of solids.
5. Prerequisites for Fiber Formation
5.1. Molecular Mass and FiberFormation
The spinnability of polymer melts or solutionsdepends on their viscosity at technically feasi-ble spinning conditions. The viscosity η of lin-ear polymers depends, in turn, on the molecularmass Mr:
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Table 1. Polymer type and molecular mass suitable for fiber formation
η=K ·Mαr
where K is a constant that is known for mostcommon polymers.
The fiber-forming tendency of a polymer in-creases with increasing molecular mass. Thevarying forces of interaction between individ-ual structural groups of polymers are directlyrelated to the chemical nature of these linearmolecules. For this reason, optimal conditionsfor fiber formation are very polymer-specific.In principle, the weaker the interaction betweenstructural segments, the higher is the molecularmass required (Table 1) [47].
5.2. Molecular Structure and FiberProperties
The thermochemical and photochemical stabil-ity of a fiber polymer is controlled by its chemi-cal structure. The possibility of chemicallymod-ifying textile properties is determined by thechemical reactivity and polarity of the individ-ual structural units (Table 2). The type of chem-ical bonds and the stereochemistry are impor-tant formolecular geometry, interaction of struc-tural units, and thermal conformational stabil-ity. Low conformational mobility is generallyrelated to high mechanical tenacity, modulus,and torsion modulus. Finally, the molecular or-ganization is influenced by the symmetry of thestructural units and of the entiremolecular chain.
The interaction energy (cohesion energy) con-trols the solubility and compatibility of struc-tural units with each other. These factors finallylead to specific morphological domains, whichfrequently occur in block structures of varyingchemical composition along the polymer chain,e.g., in polyurethane (spandex) fibers. The gen-eral relationship between the structure and prop-erties of polymers suitable for fiber productionis discussed in the literature [47]. In this sectionthe structural elements of technically importantfibers are compared.
Table 2. Structural characteristics of polymers and their importancefor fiber properties
Structural characteristics Importance for fiber properties
Chemical structure thermochemical andphotochemical stability,
(primary structure) textile chemical processes(dyeing, textile finishing)
Molecular organization and general properties,symmetry melting point, shrinkage behaviorType of binding and thermophysical andstereochemistry (secondary thermomechanical propertiesstructure) (moduli, elasticity)Conformation andconformational mobilityMorphological structures,superstructures
diffusion (dyeing), breakingmechanism
Crystallization. The interaction betweenstructural units is of considerable importance forcrystallization. The chemical structure, stereo-chemistry, and symmetry of polymers deter-mine, to a large extent, the structural conforma-
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tion of the polymer under prevailing conditionssuch as temperature (melt or solid), conditionof solution (solvation of molecules), coil struc-ture, and aggregation. Higher orientation orparallelism of the chain molecules increasesorientation of the structure elements. Their in-teraction also depends on the possible molecularconformations.
During spinning, a preliminary orientation ofthe molecules occurs, which is enhanced dur-ing drawing, and stabilized by partial crystal-lization. The individual segments usually crys-tallize independently of each other; hence amor-phous intercrystalline areas exist unavoidably.The course of polymer crystallization, especiallyof fibers, is quite different from the crystalliza-tion characteristics of low molecular mass com-pounds.
5.3. Property Requirements for theFormation of Fiber Structures
Fiber-forming polymers require certain proper-ties that make possible the formation of typicalfiber structures; these are linearity, intermolec-ular forces, and the possibility of crystallizationwhereby, in general, supermolecular structuresresult.
1) Linearity. Only linear polymers can be ex-pected to have optimal fiber-forming prop-erties. Linearity is specifically a prerequisitefor the spinnability of polymer solutions andmelts.
2) Intermolecular Forces. After orientation oflinear polymers during spinning and draw-ing, dispersion forces, e.g., dipole-dipole in-teractions or hydrogen bonds between thepolymer segments contribute to the fixationof the polymer chains.
3) Crystallization. The well-developed organi-zation of the polymer chains usually resultsin crystallization. Polymer-specific crystal-lization results in crystalline domains andamorphous intercrystalline areas.
4) Supermolecular Structure. The crystallitesare oriented so that they lie parallel to thefiber axis, which results in supermolecu-lar structures, e.g., fibrils and fibril bundles(→Fibers, 2. Structure).
These requirements were fulfilled byStaudinger’s model of cellulose as polymericformaldehyde [48]. Even this simple compoundmet all the conditions for fiber formation. It is ameltable linear polymer, capable of crystalliza-tion with formation of fiber fibrils.
The simplest model for intermolecular dis-persion forces (van der Waals forces) is shownin a polyolefin molecule such as polyethylene orpolypropylene:
In poly(ethylene terephthalate), interaction bet-ween the aromatic π-electron systems of thebenzene rings and of the carbonyl groups makesdipole – dipole interaction possible:
Hydrogen bonds act on amide or urea groups inpolyamides, such as nylon 66 or nylon 6, or inpolyurethane, respectively:
The OH groups of poly(vinyl alcohol) and ofcellulose (viscose rayon) are also able to formhydrogen bonds. Very strong dipole – dipole in-teraction occurs between the nitrile groups ofpolyacrylonitrile:
However, this all-trans conformation of poly-acrylonitrile can change into lower energy heli-cal structures [49]:
Fibers, 1. Survey 9
The strong dipole–dipole interaction of poly-acrylonitrile is one of the reasons for the specificsolubility behavior of that polymer.
Weak dispersion forces are effective only in ahighly symmetrical conformation. This high de-gree of symmetry, in turn, is possible only with ahighly symmetrical arrangement of substituents,e.g., along an aliphatic carbon chain. Such ahigh degree of symmetry in linear polymers canbe achieved only by coordination polymeriza-tion, in the presence of organometallic catalysts(Ziegler –Natta), to yield isotactic polymers. Ifthis symmetry (e.g., in polypropylene) is dis-turbed by the presence of other structural units(e.g., carboxylic acid ester groups; acrylic acidcomonomers), both polymer and fiber propertieschange drastically.
5.4. Crystallization
The flexible linear polymer takes on a vari-ety of conformations during fiber formation,seeking the conformation with the lowest freeenergy (i.e., highest molecular organization).However, spinning conditions do not allowpoly-mers to attain this state completely, and fiberpolymers usually undergo only partial crystal-lization. The ratio of crystalline to amorphousregions varies from almost totally amorphous tohighly crystalline, single-phase systems (Fibers,2. Structure).
Linear polymers exist in solution or asmolten polymer in a more or less coiled form(Fig. 2A). In the shearing field during spin-ning, the molecules are partially uncoiled andoriented in the direction of flow (Fig. 2 B). Ahigher degree of orientation is achieved dur-ing the subsequent drawing operation (Fig. 2 C).
In this step, spun fibers are stretched by morethan 200%, resulting in partial crystallizationof polymer molecules (Fig. 2D). In high-speedspinning, the extremely high windup speeds(3000 – 6000m/min; 50 – 100m/s) induce crys-tallization during fiber formation. The resultingpreoriented yarns (POY) have to be stretchedby only 40 – 100% in subsequent steps (tex-turing). Additional polymer-specific increasesin windup speeds lead to fully oriented yarns,which require almost no further stretching.
Wu et al. [77] succeeded to orientate spin-ning PET in a threadline modification process.Theone-steporientation (without separate draw-ing) could be realized by the installation of a liq-uid bath in the spinline. High-performance fila-ments, however, have to be drawn after spinningto reach maximum fiber strength.
Liquid Crystals. Some linear polymers, insolution or molten form, tend to undergoself-organization by forming liquid – crystallinestructures. Soluble linear polymers (lyotropicsystems) form liquid crystals as a result of theirrigid conformation and the formation of poly-electrolytes, e.g., the system poly(p-phenylene-terephthalamide) –H2SO4. Liquid crystals canalso be formed in polymer melts (thermotropicsystems). Examples of suitable systems are thearomatic polyesters of the poly(4-hydroxyben-zoic acid) type or aromatic blocks built up insegments and separated by flexible spacers. Fig-ure 2 E shows the resulting structures of somehigh-modulus aramids; pronounced amorphousintercrystalline areas are not visible.
5.5. Organization of StructuralElements
The arrangement of fibrils and fibril bundles inman-made fibers is controlled by the produc-tion procedure, i.e., by physical and physico-chemical processes. Therefore, resulting struc-tures depend on production parameters, and de-spite the different types of polymers employed,the tertiary structures of all man-made fibers arevery similar.
In contrast, natural fibers have organized,evolved structures which differ considerablyfrom each other, depending on the organism.Structural variations are reflected in different ge-ometric positions of the fibrils with respect to the
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Figure 2. Various conformations of fiber polymersA: Unstirred solution (coil of polymer molecules)B: Molecular orientation in the shearing field during spinningC: Molecular orientation during drawing or liquid crystal formation from the melt or solution (polyelectrolyte molecules)D: Formation of structure on crystallization of flexible polymer chains. Examples are polyethylene, polypropylene, polyamide,and polyester.a) Crystallite; b) Intercrystalline (amorphous) region; l) Long period (10 – 20 nm)E: Formation of structure of lyotropic and thermotropic systems, such as crystallization of rigid polymer chains. Examplesare high-modulus fibers of the aramid type, polyesters, and carbon fibers.
fiber axis (e.g., in cotton fibers) or in differentchemical structures along the fiber cross section(e.g., in animal hair, such as wool). Fibers couldthus be classified into two principal structuralcategories, namely, organized and unorganized,if the structure of each fiber were known.
5.6. Structural Models
The chemical structure of linear polymers de-termines the degree of conformational mobil-ity of the chain segments of these molecules.Both chain mobility and molecular structure,in turn, greatly influence fiber structure. Flex-ible chain molecules may crystallize partially toform structures that conform with the classicalcrystalline – amorphous model (Fig. 3A). Span-dex fibers, on the other hand, have a special do-main structure, because the chemical structure ofthese polymers changes considerably in the vari-ous segments along the polymer chain (Fig. 3 B).
The relatively planar structure of aramids andpolyheterocyclic compounds, their conforma-tional rigidity, and their tendency to form ly-otropic structures in the spinning solution areconsistent with a structural model in which theintercrystalline segments are bridged (Fig. 3 C).
Even more planar molecules form graphite-like structures (Fig. 3D). Structural defects leadto cavities and weakly bent planes of the aro-matic systems; for more details on carbon fibers,see →Fibers, 5. Synthetic Inorganic.
5.7. Molecular Symmetry and PhysicalProperties
The importance ofmolecular symmetry for ther-mophysical properties (melting point, glass tran-sition temperature) can be demonstrated forpolyamides. Figure 4 shows the fluctuation ofmelting points in the series of polyamides PA-3 to PA-13 (nylon 3 to nylon 13). Apparently,polyamides with an even number of carbonatoms and those with an odd number of carbonatoms belong to different structural series [47].This can be explained by the different overallsymmetry and, consequently, the different pos-sibilities for hydrogen-bond formation (Fig. 5).In PA-7, more hydrogen bonds can be formed –at least in the all-trans conformation – than inPA-6. Analogously, all nylon types with an evennumber of carbon atoms have lower meltingpoints than those with an odd number of carbonatoms (Fig. 5).
Fibers, 1. Survey 11
Figure 3. Various structural models of different polymertypesA: Classical structural model of amorphous – crystallinefiber polymers. Examples are polyamide, polyester, and vis-cose rayon. Long period (l) 10 – 30 nm.B: Structural model of spandex fibers (polyurethane).Length of hard segment 2.5 nm; length of soft segment15.0 nmC: Structural model of aramid fibers (p-structures). Noamorphous phases present; stretched molecules due to ly-otropic structures during fiber formationD: Structural model of carbon fibers; graphite structure withdefects (cavities, bent layers; D = position of defect).
5.8. Changes in Properties Caused bySymmetry Defects
The incorporation of comonomers affects notonly chemical structure, but also symmetry and,therefore, other fiber properties. For instance,the tacticity of polypropylene is changed by the
insertion of comonomers, such as vinyl com-pounds. The resulting copolymer has alteredproperties and is no longer suitable for textileproduction. In addition, polar comonomers in-terfere with the isotactic course of the polymer-ization process itself.
Figure 4. Melting points of nylons as a function of chainlength n.
Figure 5.Hydrogen bonding in nylon 6 (A;mp 225 C) andnylon 7 (B; mp 232 C)
Polyacrylonitrile is rarely used for textilefibers without comonomers being incorporatedinto the polymer, because the desired fiber prop-erties (e.g., deformability, dyeability) cannot beachieved with polyacrylonitrile alone. This, ofcourse, changes the solubility of the polymer.
Polyesters of similar chemical structure, butquite different molecular symmetry, also havevery different melting points. For example, the
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highly symmetrical poly(ethylene terephthalate)has a melting point of 265 C, whereas the melt-ing point of poly(m-phenyleneisopthalamide) isonly 102 C [47].
The same situation arises with aramids.Here, too, the highly symmetrical para-linkedpolyamides have higher melting points (in thiscase, decomposition temperatures) than the lesssymmetrical meta-linked polymers (Fig. 6). Thedifferent dipole orientation, oppositely directedor in the same direction (arrows in Fig. 6), andthe total symmetry cause higher fiber tenacityand modulus.
Figure 6. Effect of dipole orientation on the melting point(decomposition temperature) of aramids
6. Fiber Properties Required byTextiles
Despite the fact that a large number of polymerspossess the basic properties required for fiberformation, they are not all suitable for large-scale production of fibers. In textile productionand in commercial applications, polymers mustfulfill a variety of requirements:
1) Chemical Stability. Polymers must be stableunder the influence of heat, light, air, water,and the chemicals commonly used in textilefinishing and care.
2) Thermomechanical Stability. Polymers mustpossess the ability to be solution- or melt-
spun and, at the same time, retain their di-mensional stability during processing, useand care.
The requirements to bemet by fibers and theirparent polymers are, therefore, determined bythe demands on the final products.
6.1. Requirements to Be Met by Textiles
The need for a variety of textile fabrics havingspecific properties should be clear from the di-versity of textile uses. The priorities and orderof importance of properties depend on the appli-cation in question.
For clothing, textile properties like appear-ance, aesthetics, optics, drape, formability (iron-ing, pleating), comfort, heat and moisture trans-port, handle, ease of care, and fastness of alltypes are of considerable importance. In ad-dition, certain chemical requirements, such asdyeability, crease-resistant finishing, anddimen-sional stability, must be met in the productionof textile materials. Finally, processibility to thefinished textile product in partially automatedproduction lines has become increasingly im-portant.
Industrial textiles must also possess specificproperties, depending on their application. Forexample, high tenacity is required for ropes; highmodulus, for fiber reinforcement; heat stability,for protective clothing and insulation; highwaterabsorption, for articles of hygiene; resistance tochemicals and flue gas, for filter materials; andlong-term stability, for geotextiles [45].
In the past, fiber production and the utiliza-tion of specific properties were optimized pri-marily. Today, fibers with desired properties aremade specifically to fulfill the requirements ofthe final product. The correlation between re-quirements and properties of the finished prod-uct and correspondingfiber (polymer) propertiesis given in Table 3.
6.2. Modification of Fiber Properties
The specific properties of the finished productdepend directly on its end use. Since the fiberitself is not the final product, changes in fiberstructure result in changes in the property profile
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Table 3. Correlation of textile properties with fiber properties
Properties of the final product Corresponding fiber properties
Optical properties luster, fiber surfaceAesthetics profile, fiber cross sectionMechanical properties modulus of elasticity, tenacity, elongationComfort
Physiological properties of clothing moisture absorption, moisture transportAntistatics electrical resistanceThermal insulation heat capacity, porosity, heat conduction∗Hand textile structure, bending modulusFeel roughness, modulus of elasticity, finenessEase of care and washability wetting, moisture absorption, glass transition temperature (wet and dry) [78]Dry cleaning polymer (in)solubility, swellingSoiling characteristics zeta potential, adsorption and dissolution of soil components
FastnessMechanical stability tenacity, elongation, moduli, abrasion resistanceDimensional stability melting point, glass transition point (wet and dry)Forming (e.g., pleating) thermoplasticity, glass transition temperature (Tg)Lightfastness chemical structure, sensitizers, stabilizersLightfastness of dyeing polymer – dye interaction, radical lifetime
Specific propertiesFlame resistance chemical structure, combustion mechanismImpermeability to water moisture absorption, wetting propertiesWater vapor permeability surface properties, morphology, yarn structureDyeability glass transition point during dyeingMechanical properties(ropes, material, tire cord) modulus of elasticity, tenacity, elongation, dynamic modulus
Rubber elasticity chemical structure, glass transition temperature, morphological structure,domain structure
∗The thermal insulation of a textile is largely due to the air inside the pores, which is of low thermal conductivity.
of the finished product. Matching the require-ment profile with the property profile is not al-ways possible. the purpose of numerous mod-ification procedures (e.g., of the fiber polymer,productionmethod, processing, and finishing) isto confer special functional properties on the endproduct. Some of these procedures are describedin more detail in the following sections.
Copolymers. Fibers are used predominantlyas raw materials in textile manufacture. specificfabric properties, such as dimensional stability,brightness, color, pattern, or luster, are impartedto textiles during the physical and physicochem-ical processes of textile finishing. These charac-teristics should remain unchanged, particularlyduring use and cleaning. Chemical modificationof the fiber polymer is generally employed toachieve this goal. Chemical treatment involves,above all, the introduction of special structuralgroups into the basic polymer, groups that arecapable of taking part in polar and homopolarinteractions with the chemicals used in textilefinishing. Some examples are
1) introduction of a sulfonic acid group intopoly(ethylene terephthalate) to bind cationicdyes (sulfoisophthalic acid as comonomer);
2) introduction of a sulfonic acid group intopolyacrylonitrile with the help of vinylsul-fonic or styrenesulfonic acid or a similarcomonomer to make possible the use ofcationic dyes;
3) introduction of flexible chain segments intopoly(ethylene terephthalate) to change itsdyeing characteristics. Polymer modifica-tion [copolycondensation with poly(ethyl-ene glycol)] in the production of carrier-freedyeable polyester makes use of this princi-ple.
Polymer Mixtures. Polymers are generallyincompatible. If two different polymers are spuntogether, fibril structures are formed (matrix fib-ril fibers) that are known as biconstituent fibers.If two polymer streams are combined in thespinneret without blending, bicomponent fibersare obtained (→Fibers, 3. General ProductionTechnology).
14 Fibers, 1. Survey
Additives. Many specific fiber characteris-tics can be achieved by use of additives in thespinning solution or the melt. For example, thefollowing effects can be obtained:
1) Delustering: use of titanium dioxide as addi-tive in spinning
2) Spin dyeing: use of pigments as additives inspinning
3) Antistatic properties: use of electrically con-ducting additives in spinning
4) Flame resistance: use of flame retardants asadditives in spinning
The use of additives in spinning produces a verybroad spectrum of properties. For economic rea-sons, this type offibermodification is themethodof choice, if it produces the required effect. Bycomparison, the development of special poly-mers is a much more expensive procedure.
6.3. Comfort Properties of Textiles
Fibers used to produce clothing must possess avariety of properties. The term comfort refers tothose properties responsible for the wash andwear performance of garments. Physiologicalstudies have shown that apart from fiber sub-stance, i.e., the chemical structure of the fiberpolymer, the most important factors that influ-ence textile wearability are fiber, yarn, and tex-tile construction [50]. Along with moisture ab-sorption, moisture transport across the fiber sur-face or through textile spaces is of particular sig-nificance for the moisture balance of textiles.Textiles must retain their appearance and formduringwashing and dry cleaning. In this connec-tion, certain inherent fiber properties are of vitalimportance. The thermomechanical stability oftextiles is controlled by the glass transition tem-perature (Tg) of the fiber polymers. However,this temperature is not a structural property but,rather, is directly related to the fiber system, e.g.,the type of polymer and polymer –water interac-tion. Deformability generally increases with in-creasing moisture absorption because the chain-segment mobility of polymers is increased. Theglass transition temperature of fiber polymerswith a high moisture-absorbing capacity de-creases dramatically with increasing moisturecontent. The resulting structural changes in the
fiber lead to fiber shrinkage or stretching, de-pending on the degree of thermosetting. In otherwords, the textiles lose their shape.
Even in the dry state, dimensional stabil-ity decreases with increasing temperature, fiberscan undergo permanent deformation at dry heat.Suitable fixation and textile finishing, e.g., ther-mofixation (heat setting) of polyester, felting orshrink-resistant finishing of wool, and crease-resistant finishing of cotton, can enhance dimen-sional stability and ease of care. Textiles thatare still not dimensionally stable enough to bewashed with water must be dry-cleaned. Here,soil release is achieved by using organic sol-vents such as perchloroethylene or fluorochloro-hydrocarbons; the temperature must be main-tained below the glass transition points of thefiber – solvent system throughout the process.
Figure 7. Total production of man-made fibers [2]
7. Economic Aspects
The production of natural and man-made fibersis influenced by a number of factors, such as de-mand (state of the economy), availability (pro-duction and trade), prices, and availability of rawmaterials. The per capita consumption variesconsiderably from country to country and de-
Fibers, 1. Survey 15
pends on climate, supply, domestic productionversus imports, standard of living, fashion, stateof the economy, and degree of industrialization.
The balance between the consumption of nat-ural and of man-made fibers is also controlledby these factors, although a certain “awarenessof nature” currently tips the scales in favor ofnatural fibers. The production of natural fibers,e.g., cotton or wool, is determined in terms ofthe profit made per area cultivated. A dramaticincrease in production cannot be expected atpresent. However, new developments in geneticengineering could rapidly improve the yields ob-tained per given area.
The economic importance of individual fibertypes can be deduced from their annual world-wide consumption [51], and Figure 7 shows theworldwide production of man-made fibers.
Both the consumption and the production offibers also depend directly on the level of devel-opment and on per capita income [52]. The con-sumption per person in individual countries dif-fers considerably for a variety of reasons. Somecountries have already reached a high level ofconsumption, and despite their high standard ofliving, the population spends only a fixed per-centage of their available incomeon textiles. Thegrowth of fiber production for industrial use, onthe other hand, is likely to continue. In 1984, 7 kgof fiber was consumed per capita; for the year2000, a total fiber production of 43×106 t is ex-pected if per capita consumption remains at 7 kg,or 48.6×106 t if it increases to 8 kg. The growthrate of 2.8% achieved in the period 1968 – 1984is not expected to continue. Up to 1995 the aver-age growth rate was only 2.3%/a. Nevertheless,a world fiber volume of about 50×106 t is ex-pected in the year 2000 [52], [79].
The limited means of production in EasternEurope also contributed to reduced consump-tion. In the developing countries, lack of spend-ing power, capital, and means of production allcombine to reduce growth of consumption. Re-gional differences in population growthwill leadto an increase in fiber consumption in the devel-oping countries.
8. Tabular Survey of Fibers [6], [53],[54]
A quantitative survey of the most importantproperties of fibers based on polycondensationand polymerization, as well as some inorganicfibers, is shown inTables 4, 5, 6, 7, 8, 9, 10. Prop-erties of these fibers, are compared with those ofnatural and semisynthetic fibers. The propertiesof all textile and industrial fibers are determinedby variables related to production and aftertreat-ment. Hence, in general, only a range of valuescharacteristic of individual fiber classes is givenin this survey. In fact, only the order of magni-tude is indicated for electric resistance of fibersbecause of considerable variations in measuredvalues. No entries have beenmadewhen reliableinformation was unavailable.
The numbers in brackets are plausibleestimated values. Figures for tenacity andmodulus are based on both fiber fineness(1tex = 1g/km) and cross-sectional area of thesample. The following relationship is applica-ble:
Fineness (tex) = 105×Density(gcm−3)
×Crosssection(cm2)
In general, the characteristic stress – strain curveσ (ε) of fibers does not show a constant gradi-ent, even at low elongation. Hence, the modulusof elasticity is usually defined as the differentialquotient dσ (ε)/dε. Experimental determinationat low fiber elongation ε is difficult but can beconducted successfully by extrapolation of thefunction dσ (e) /de for e= 0 [55].
The elastic recovery of a fiber (in percent)can be measured by standard methods [56] andis shown in Table 5 as
(1− er
e
)100
where εr = residual elongation, ε= total elonga-tion.
16 Fibers, 1. SurveyTa
ble4.
Mechanicalp
ropertiesof
fibers(dataatbreak)
Fibername/polymer
Trade
names
Fibertype
aDensity
(),
Elongation
εH
(21
C)
Tenacity
(σH)at21
CRelative
Relative
g/cm
3at65
%“w
et/dry,”
at65
%R.H.
Wet/dry
loop
knot
R.H.b
,%%
σH/,
σH
(relative),
tenacity
tenacity
cN/tex
GPa
%[62],%
[63],%
Natural
fibers
Cotton
st1.50
–1.54
6–15
100–110
25–50
0.35
–0.7
100–110
65–75
60–100
Wool
st1.32
25–50
110–130
10–20
0.15
–0.25
70–90
75–85
80–85
Silk
fi1.25
10–30
120–200
25–50
0.3–0.6
75–95
60–80
80–85
Hem
pst
1.48
2–5
≈100
36–75
0.5–1.1
100–106
Flax
st1.438–1.456
1–4
110–125
30–55
0.43
–0.8
105–120
20–40
Jute
st1.436
1.3
100
20–40
0.3–0.57
99–104
Regeneratecellu
lose
Viscose
rayon,Viscose
Modal
Evlan,F
ibro,
Sarille,...
st/fi
1.52
–1.54
10–30
100–130
16–45
0.25
–0.7
40–80
25–65
25–60
Cuprammonium
rayon
Asahi
Bem
berg,
Bem
berg
st/fi
1.52
10–40
170–200
14–21
0.2–0.32
60–70
60–75
60–85
Cellulose
acetate
Arnel,C
elco,
Dicel
st/fi
1.29
–1.32
20–45
120–150
10–15
0.13
–0.2
50–80
70–95
80–90
Cellulose
triacetate
Estron,Silene,
Tricel
st/fi
1.29
–1.32
20–45
120–150
10–15
0.13
–0.2
50–80
70–95
80–90
NMMOfib
ers[88]
Lyocell,
Tencel,...
st1.5
10–16
110–115
32–48
0.5–0.7
55–70
45–50
≈75
Proteinfib
ers
st1.315
25–60
60–110
11–12
0.14
–0.16
40–65
Alginatefib
er(Ca-Alginate)
fi1.78
511
–18
0.2–0.3
27–30
Polycon
densatefib
ers
Nylon
6(PA6)
Perlon,A
celon,
Amilan,Anso,
Caprolan,
Grilon,...
st1.14
30–70
105–125
30–40
0.35
–0.45
80–90
65–85;
fi1.14
20–45
105–125
40–60
0.45
–0.7
85–90
70–95
80–90;
hd1.14
15–20
105–125
60–90
0.7–1
85–90
70–90
60–70
Nylon
66(PA66)
Nylon,A
ntron,
Cantrece,
Meryl,
Tim
brelle,
Ultron...
st1.14
30–60
105–125
35–40
0.4–0.45
seePA
6seePA
6seePA
6
fi1.14
20–40
105–125
40–60
0.45
–0.7
hd1.14
15–20
105–125
60–90
0.7–1
Fibers, 1. Survey 17Ta
ble4.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aDensity
(),
Elongation
εH
(21
C)
Tenacity
(σH)at21
CRelative
Relative
g/cm
3at65
%“w
et/dry,”
at65
%R.H.
Wet/dry
loop
knot
R.H.b
,%%
σH/,
σH
(relative),
tenacity
tenacity
cN/tex
GPa
%[62],%
[63],%
Aramids
Com
pressive
strength,axial
inGPa,[80],
[81],[82]
Poly(m
-phenyleneisophthalamide)
Nom
ex,C
onex
fi1.38
15–30
60–80
≈95
80–85
Poly(p-phenyleneterephthalam
ide)
(PPT
A)
Kevlar29,
Twaron
fi1.44
3–4
185–195
2.7–2.8
0.35
≈45
≈50
Kevlar49
fi/an
1.45
2–2.5
185–195
2.7–2.8
0.365
50–78
35–50
Kevlar149
fi/an
1.47
1.2–1.9
150–160
2.2–2.4
Kevlar981,
Twaron
fi/hd
2.8–3.5
230–260
3.5–3.8
KevlarHp
fi1.44
3.6
140–150
2.05
Poly(ethyleneterephthalate)
(PET)
Dacron,Diolen,
st1.36
–1.41
25–50
100–105
30–55
0.4–0.75
95–100
75–95
Fortrel,Grilene,st/ap
1.36
–1.41
30–55
100–105
25–40
0.35
–0.55
95–100
75–85
Serene,
Terylene,
fi1.36
–1.41
20–30
100–105
40–60
0.55
–0.85
95–100
70–98
70–80
Trevira,....
fi/hd
1.36
–1.41
8–20
100–105
60–100
0.85
–1.5
95–100
60–90
40–70
Poly(butyleneterephthalate)
(PBT)
Trevira
810,
st/fi
1.25
35–40
40–45
0.5–0.56
Trevira
813
Poly(1,4-dim
ethylenecyclohexane
terephthalate)
(PDCT)[59]
Kodel
st1.22
–1.23
15–35
22–36
0.37
–0.45
≈100
30–95
Polyarylate
Ekonol[60],
Vectran
fi1.40
–1.41
2–5
200–280
2.8–3.9
Com
pressive
strength,axial
[80],[81],[82]
GPa
0.04
–0.075
23–34
Poly(etheretherketone)(PEEK)
Zyex
fi1.27
–1.298
15–60
20–100
0.25
–1.3
55–80
65–68
Polyim
ide(PI)
P84
st/fi
1.41
forst30
–38
andforfi
19–21
27–37
0.38
–0.53
60–65
70–75
Novolak
Kynol,P
hilene,
Novoloid
st1.2–1.3
20–60
13–22
0.17
–0.27
7080
Poly(amideim
ide)
(PAI)
Kermel
st10
–25
25–60
Poly(ether
imide)
(PEI)
st/fi
16–38
15–27
0.2–0.35
Polyurethane
elastomers(spandex)
Dorlastan,
Lycra,...
fi1.1–1.3
400–700
≈100
5–12;
30–70
=σ
H(1+
εH)/
c0.06
–0.15
75–100
18 Fibers, 1. SurveyTa
ble4.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aDensity
(),
Elongation
εH
(21
C)
Tenacity
(σH)at21
CRelative
Relative
g/cm
3at65
%“w
et/dry,”
at65
%R.H.
Wet/dry
loop
knot
R.H.b
,%%
σH/,
σH
(relative),
tenacity
tenacity
cN/tex
GPa
%[62],%
[63],%
Polym
erizatefib
ers
Polyethylene
(HD–PE
)(H
M–HD–PE
:M
r>
106)
Hiralon,
Vegon,...
fi0.95
–0.96
10–45
100
30–70
0.3–0.65
100
60–90
70–90
Spectra1000...
hd0.97
3–6
100
270–370
2.6–3.6
100
≈50
Polypropylene(PP)
Herculon,
Meraklon...
st/fi
0.90
–0.92
15–50
100
25–60
0.22
–0.55
100
85–95
70–90
Polyacrylonitrile
(PAN)
DralonT,...
st/fi
1.17
–1.19
25–40
≈100
35–58
0.42
–0.69
80–100
≈60
≈70
Copolym
erizates
with
PAN
≥85
%Dolan,D
ralon,
st1.17
–1.19
20–60
100–120
18–32
0.2–0.37
75–95
30–80
75–80
Euroacril,
Leacril,...
fi1.17
–1.19
15–40
100–120
35–45
0.42
–0.53
80–100
30–80
≈70
Modacrylics(50–84
%PA
N)
Kanekalon,
SEF,...
st1.3–1.4
25–50
100–110
15–25
0.2–0.35
80–100
50–70
≈80
Poly(vinyl
chloride)(PVC)
atactic
Clevil,
Rhovil,....
st/fi
1.38
–1.40
10–40
100
20–24
0.28
–0.34
100
35–70
syndiotactic[61]
st1.40
35–60
100
25–30
0.35
–0.42
100
60–90
65–85
Poly(vinyl
alcohol)(PVA)
Kuralon,
Mew
lon,
st1.26
–1.31
13–26
120–140
20–55
0.25
–0.7
65–85
35–40
55–65
Solvron,
Vilo
n,...
fi1.26
–1.31
9–22
120–140
55–77
0.7–1
65–85
35–40
55–65
(HM:M
r>
106)
hd1.31
3–4
150–230
2–3
Polytetrafluoro-ethylene(PTFE
)Gore-Tex
Fibers,...
st/fi
2.1–2.3
20–40
100
8–18
0.16
–0.38
100
60–90
75–90
Poly(phenylene
sulfide)(PPS
)Procon,R
ylon
st/fi
1.37
–1.38
25–40
28–47
0.4–0.65
7860
–80
Melam
ineresinfib
erBasofi
l1.4–1.5
15–25
15–40
0.2–0.6
Fibers, 1. Survey 19Ta
ble4.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aDensity
(),
Elongation
εH
(21
C)
Tenacity
(σH)at21
CRelative
Relative
g/cm
3at65
%“w
et/dry,”
at65
%R.H.
Wet/dry
loop
knot
R.H.b
,%%
σH/,
σH
(relative),
tenacity
tenacity
cN/tex
GPa
%[62],%
[63],%
Inorganicfib
ers
Fiber
diam
eter,µ
mCom
pressive
strength,axial,
GPa
Textile
glass
Gevetex,
Fiberglas
2.45
–2.6
2–5
100
70–120
1.7–2.7
15–30
Eglass
E-Fiber,
Enkafort
5–15
2.52
–2.54
2–3.5
100
80–140
2–3.5
0.5
Aluminum
silicate
(e.g.,3Al 2O
3·2
SiO
2·B
2O
3)
Nextel3
1217
2.63
–2.7
651.7
Nextel4
403.1
Nextel4
803.05
1.1
752.3
β-Siliconcarbide
Nicalon
(Nippon
Carbon)
5–20
2.6–3.1
1≈
100
3
FP(D
uPont)
200.4
1.4–1.5
Saffil,Saffimax
(ICI)
3–3.2
2.8–3.3
0.7
30–60
1–2
Silica(SiO
2)
Silica(A
kzo)
9–10
1.8–2.0
1.4–2.0
15–40
0.25
–0.8
Steel(20
%Cr,7%
Ni)
Bekinox
fi7.9
1–2
100
22–29
1.75
–2.25
65–75
60–70
Carbon(pitchbased)
High-modulus
types(H
M)
Tornel,G
rafil,
6–9
2.0–2.06
0.4(-2)
≈100
2(-4)
0.4–0.8
0
High-strength
types(H
S)FiberG
9–12
2.02
0.5–2
≈250
≈5
0.5–1.1
0
Carbon(PANbased)
Magnamite,
High-modulus
types(H
M)
Pyrofil,
6–7
1.8–1.96
0.4–1.2
100–180
1.9–3.5
1.4–1.5
0
High-strength
types(H
S)To
rayca,...
7–9
1.74
–1.82
1.5–2.4
170–380
3–7
1.44
–4
0
ast=staplefib
er,fi
=filam
ent,hd
=highly
draw
n,an
=annealed,ap=antip
illing;
bR.H.=
relativ
ehumidity
;ceffectivebreaking
strength
20 Fibers, 1. SurveyTa
ble5.
Elastom
echanicalp
ropertiesof
fibers
Fibername/polymer
Trade
Fiber
Elasticrecovery,%
:InitialModulus
Torsionmodulus
[64]
Torsion
names
type
a(1–
εr/ε)100for
(elongation
ε→
0)G/,
G,
brittleness
ε=2%
(5%)
E/,
E,
N/tex
GPa
[66],degrees
N/tex
GPa
Natural
fibers
Cotton
st75
453–6
4.5–9
1.6
2.4
53–56
Wool
st95
–99
60–70
1.5–3
2–4
0.8–1
≈1
48–52
Silk
fi95
707–10
9–12.5
1.5–2.3
1.9–2.9
51Hem
pst
6090
Flax
st≈
608–25
12–36
0.95
1.3–1.4
68Jute
st21
–22
30–31
Regeneratecellu
lose
Viscose
rayon,Viscose
Modal
Evlan,F
ibro,
Sarille,..
st/fi
70–100
40–60
2–3(6.5–7.5)
3–4.5(4.2–4.9)
0.5–1
≈1
51–55
Cuprammonium
rayon
Asahi
Bem
berg,
Bem
berg
st/fi
70–95
40–60
2–3
3–4.5
48–57
Cellulose
acetate
Arnel,C
elco,
Dicel,
st/fi
90–95
(40–60)
2–3.5
2.5–4.5
0.6–0.8
≈1
44–50
Cellulose
triacetate
Estron,Silene,
Tricel,...
st/fi
90–95
55–70
2–3.5
2.5–4.5
0.6–0.8
≈1
44–50
NMMOFiber
Lyocell,Tencel,..
st/fi
46
Proteinfib
erst
262
2–3
0.9
≈1
30–40
Alginatefib
er(Ca-Alginat)
fi7
12–13
1.2
≈2
Polycon
densatefib
ers
Nylon
6(PA6)
Perlon,A
celon,
st27
–41
Amilan,Anso,
fi95
–100
95–100
0.5–3
0.6–3.5
≈0.3
≈0.3
33–42
Caprolan,
Grilon,...
hd95
–100
90–95
4–5
4.5–5.5
0.7
0.8
Nylon
66(PA66)
Nylon,A
ntron,
st27
–41
Cantrece,Meryl,fi
95–100
95–100
0.5–3
0.6–3.5
0.45
0.5
40–41
Tim
brelle,
Ultron,...
hd95
–100
90–95
4–5
4.5–6
Fibers, 1. Survey 21Ta
ble5.
(Contin
ued)
Fibername/polymer
Trade
Fiber
Elasticrecovery,%
:InitialModulus
Torsionmodulus
[64]
Torsion
names
type
a(1–
εr/ε)100for
(elongation
ε→
0)G/,
G,
brittleness
ε=2%
(5%)
E/,
E,
N/tex
GPa
[66],degrees
N/tex
GPa
Aramids
Poly(m
-phenyleneisophthalamide)
Nom
ex,C
onex,
fi8–14
11–20
≈50
Poly(p-phenyleneterephthalam
ide)
(PPT
A)
Kevlar29,
Twaron,
fi95
–100
41–53
59–77
Kevlar49,
Twaron,
fi/an
95–100
85124
Kevlar149,
fi/an
96103
150
Kevlar981,
Twaron,
fi/hd
70–83
102–120
KevlarHp
fi50
72
Poly(ethyleneterephthalate)
(PET)
Dacron,Diolen,
st2.5–4
3.4–5.5
30–49
Terylene,
Trevira,
ap2.5–4
3.4–5.5
≈48
Fortrel,Grilene,
fi90
–98
70–90
7–18
10–25
0.65
0.9
41–48
Serene,...
hd7–18
10–25
1.1
1.5
47–48
Poly(butyleneterephtalate)(PBT)
Trevira
810...813
fi100
99–100
4–5
5–6
Poly(1,4-dim
ethylene
cyclohexane
terephthalate)
(PDCT)[59]
Kodel
st85
–95
50–60
2.5–4
3–5
49
Polyarylate
Vectran,E
konol
[61]
fi60
–128
80–180
Poly(ether
etherketone)(PEEK)
Zyex
fi4–12
5–15
Polyim
ide(PI)
P84
st/fi
3.5–5
5–7
Novolak
Kynol,P
hilene,
Novoloid
st2.6–3.6
3.3–4.6
Poly(amideim
ide)
(PAI)
Kermel
st3.5–7.5
Poly(ether
imide)
(PEI)
st2.7–4.2
3.5–5.1
Polyurethane
elastomers(spandex)
Dorlastan,
Lycra,...
fi93
–98
≈0.005–0.01
0.006–0.012
forε=300%
0.004
0.005
22 Fibers, 1. SurveyTa
ble5.
(Contin
ued)
Fibername/polymer
Trade
Fiber
Elasticrecovery,%
:InitialModulus
Torsionmodulus
[64]
Torsion
names
type
a(1–
εr/ε)100for
(elongation
ε→
0)G/,
G,
brittleness
ε=2%
(5%)
E/,
E,
N/tex
GPa
[66],degrees
N/tex
GPa
Polym
erizatefib
ers
Polyethylene
(HD–PE
)(H
M–HD–PE
:Mr
>10
6)
Hiralon,V
egon,
fi95
–100
90–95
0.2–5
0.2–5
0.05
0.05
Spectra1000,...
hd100
51–165
50–160
1.5[65]
1.5[65]
Polypropylene(PP)
Herculon,
Meraklon,...
st/fi
95–100
85–95
0.5–5
0.5–5
Polyacrylonitrile
(PAN)
DralonT,...
st/fi
90–95
50–90
9.5–14
11–17
1.5–1.7
1.8–2
Copolym
erizates
with
PAN
≥85
%Dolan,Dralon
st90
–95
50–90
3–5
3.5–6
45–52
Euroacril,
Leacril,...
fi90
–95
50–90
9–10
10–12
11.2
55–60
Modacrylics(50–84
%PA
N)
Kanekalon,
SEF,..
st95
–99
85–98
1–2.5
1.3–3.5
Poly(vinyl
chloride)(PVC)
atactic
Clevyl,
Rhovyl,...
st/fi
70–90
55–65
2–4
3–5.5
0.6–0.7
0.8–1
27–50
syndiotactic[61]
st90
–95
75–80
2.5–3
3.5–4
Poly(vinyl
alcohol)(PVA)
Kuralon,
Mew
lon
st60
–80
40–60
3–4
4–5
0.9
1.2
Solvron,Vilo
n,...
fi60
–80
40–60
3–4.5
4–6
1.2–1.5
1.6–2
(HM:M
r>
106)
hd30
–60
40–80
Polytetrafluoroethylene
(PTFE
)Gore-TexFibers
st/fi
0.35
–2
0.7–4
0.2–0.3
0.4–0.7
Poly(pheneylenesulfide)(PPS
)Procon,R
yton,...st/fi
2.7–5
3.7–6.8
Fibers, 1. Survey 23Ta
ble5.
(Contin
ued)
Fibername/polymer
Trade
Fiber
Elasticrecovery,%
:InitialModulus
Torsionmodulus
[64]
Torsion
names
type
a(1–
εr/ε)100for
(elongation
ε→
0)G/,
G,
brittleness
ε=2%
(5%)
E/,
E,
N/tex
GPa
[66],degrees
N/tex
GPa
Inorganicfib
ers
Fiber
diam
eter,
Textile
glass
Gevetex,
Fiberglas,...
µm100
28–34
70–90
16
40
85–88
Eglass
E-Fiber,
Enkafort,...
5–15
100
28–34
70–90
16
40
85–88
Aluminum
silicate
(e.g.3
Al 2O
3·2
SiO
2·B
2O
3)
Nextel3
12,
175.5–52
15–140
Nextel4
40,
65200
Nextel4
80[89]
73224
β-Siliconcarbide
Nicalon
(Nippon
Carbon)
5–20
67–100
200–300
FP(D
uPont)
20120–125
350–385
Saffil,Saffimax
(ICI)
3–3.2
33–83
100–250
Silica(SiO
2)
Silica(A
kzo)
9–10
6–30
12–56
Steel(20
%Cr,7%
Ni)
Bekinox
fi100forε=1%
19–25
150–200
7.9–9.5
60–70
Carbon(pitchbased)
High-modulus
types(H
M)
Thornel,G
rafil,
6–9
250–400
500–800
High-strength
types(H
S)FiberG
9–12
124–200
250–400
Carbon(PANbased)
Magnamite
High-modulus
types(H
M)
Pyrofil,
6–7
160–260
300–500
High-strength
types(H
S)To
rayca,...
7–9
110–165
200–300
2.2
4
ast=stablefib
er,fi
=filam
ent,hd
=highly
draw
n,an
=annealed,ap=antip
illing.
24 Fibers, 1. SurveyTa
ble6.
Therm
alpropertiesof
fibers
Fibername/polymer
Trade
names
Fibertype
aFibershrinkage
Specific
Therm
alGlass
transitio
nMeltin
gHeatresistance
inwater
of95
C,%
heatcapa-
conductiv
ity,
temperature,
temperature
inairup
tot,
C
draw
nthermoset
city
[67],
Wm
−1K
−1
C(decom
positio
nJg
−1K
−1
temperature),
C
Natural
fibers
Cotton
st1.3
0.3–0.5
(400)
120
Wool
st1.3–1.6
0.2–0.4
45[90]
120
Silk
fi1.4
0.2–0.4
40–50
(170
–180)
120
Flax
st1.4
0.3
Regeneratecellu
lose
Viscose
rayon,Viscose,M
odal
Evlan,F
ibro,
Sarille,...
st/fi
0.5–10
b1.3–1.5
0.3–0.6
(175
–190)
120
Cuprammonium
rayon
Asahi
Bem
berg,
Bem
berg
st/fi
0.5–10
b1.4
(175
–205)
120
Cellulose
acetate
Arnell,Celco,
Dicel,
st/fi
5–20
1.3–1.5
0.3
255
120
Cellulose
triacetate
Estron,Silene,
Tricel,...
st/fi
5–20
0.7
1.5
0.3
170–180[68]
300
130
Polycon
densatefib
ers
Nylon
6(PA6)
Perlon,A
celon,
st8–15
0.5–1.5
1.5–1.8
80–85
(dry)
215–220
120
Amilan,Anso,
fi8–15
1–5
1.5–1.8
0.2–0.3
≈20
(3.7%
water)
215–220
120
Caprolan,
Grilon,...
hd8–15
1.5–1.8
0.4
90–95
(dry)
215–220
120–150
Nylon
66(PA66)
Nylon,A
ntron,
st8–15
0.5–1.5
1.5
90–95
(dry)
255–260
120
Cantrece,Meryl,fi
8–15
1–5
1.5
0.2–0.3
≈30
(3.7%
water)
255–260
120
Tim
brelle,
Ultron,...
hd8–15
1.5
0.4
255–260
120–150
Fibers, 1. Survey 25Ta
ble6.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aFibershrinkage
Specific
Therm
alGlass
transitio
nMeltin
gHeatresistance
inwater
of95
C,%
heatcapa-
conductiv
ity,
temperature,
temperature
inairup
tot,
C
draw
nthermoset
city
[67],
Wm
−1K
−1
C(decom
positio
nJg
−1K
−1
temperature),
C
Aramids
Poly(m
-phenyleneisophthalamide)
Nom
ex,C
onex
fi1.5
1.2
0.13
280–290
(≈370)
180–200
Poly(p-phenyleneterephthalam
ide)
(PPT
A)
Kevlar29,
Twaron,
fi1.4
0.05
340–360
(≈550)
180–200
Kevlar49,
Kevlar
149,Tw
aron,
fi/an
0.05
340–360
(≈550)
180–200
Kevlar981,
Twaron,
fi/hd
340–360
KevlarHp
fi340–360
Poly(ethyleneterephthalate)
(PET)
Dacron,Diolen,
st0.5–1
80–110
250–260
120–150
Fortrel,Grilene,
ap0.5–1
80–110
250–260
120–150
Serene,T
erylene,
fi5–10
0.5–1.5
0.4–1.9[70]
0.2–0.3
80–110
250–260
120–150
Trevira,...
hd7–8
80–110
250–260
150–160
Poly(butyleneterephtalate)(PBT)
Trevira
810,
Trevira
813
st/fi
68–75
224
120
Poly(1,4-dim
ethylene
cyclohexane
terephthalate)
(PDCT)[59]
Kodel
st0.1–0.5
≈100
285–290
≈200
Polyarylate
Vectran,E
konol
[60]
fi320–290
180–260
Poly(ether
etherketone)(PEEK)
Zyex
fi0.4–0.5
139–153
334–345
200–250
Polyim
ide(PI)
P84
st/fi
315
260
Novolak
Kynol,P
hilene,
Novoloid
st0
Poly(amideim
ide)
(PAI)
Kermel
st(>
380)
250
Poly(ether
imide)
(PEI)
st/fi
4–8
0.7
215–225
160–170
Polyurethane
elastomers(spandex)
Dorlastan,
Lycra,...
fi≈
3–12
0.15
Polyether:≈
−60
[70]
;Po
lyester−
40to
−20
230–290
120
26 Fibers, 1. SurveyTa
ble6.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aFibershrinkage
Specific
Therm
alGlass
transitio
nMeltin
gHeatresistance
inwater
of95
C,%
heatcapa-
conductiv
ity,
temperature,
temperature
inairup
tot,
C
draw
nthermoset
city
[67],
Wm
−1K
−1
C(decom
positio
nJg
−1K
−1
temperature),
C
Polym
erizatefib
ers
Polyethylene
(HD-PE)
Hiralon,V
egon,
fi5–10
1.4–2.0
0.2–0.4
−20
to−
30124–138
70–90
(HM
–HD–PE
:Mr
>10
6)
Spectra1000
hd10
–38
[84],
[85]
−20
to−
30124–138
Polypropylene(PP)
Herculon,
Meraklon
st/fi
0–5
1.6
0.2–0.3
160–175
≈120
Polyacrylonitrile
(PAN)
DralonT
fi/st
14–16
≈1
0.2
≈95
(dry)
≈320
140
Copolym
erizates
with
PAN
≥85
%Dolan,D
ralon
st(20–40
c)
0.5–5
1.2–2.5
0.2
85–95
(dry);
50–60
(wet)
(>250)
140
Euroacril,
Leacril,
fi16
–22
≈1
1.2–1.5
0.2
85–95
(dry);
50–60
(wet)
(>250)
140
Modacrylics(50–84
%PA
N)
Kanekalon,
SEF,...
st0.2–5
85–95
(170)
≈120
Poly(vinyl
chloride)(PVC)
atactic
Clevyl,Rhovyl,
st/fi
20–30
0.8–0.9
0.16
–0.17
70–90
(160
–200)
<65
syndiotactic[61]
st0
90–100
(160
–200)
Poly(vinyl
alcohol)(PVA)
Kuralon,
Mew
lon,
st2–3
75–90
140
Solvron,Vilo
n,fi
75–130
(240
–260)
(water
vapor:
120)
Polytetrafluoroethylene
(PTFE
)Gore-TexFibers
st/fi
21.0–1.1
0.23
127–130
327–342[72]
180
Poly(phenylene
sulfide)(PPS
)Procon,R
yton,...st/fi
16
85–95
270–290
190–200
Melam
ineresinfib
erBasofi
lst
200–220
ast=stablefib
er,fi
=filam
ent,hd
=highly
draw
n,an
=annealed,ap=antip
illing;
bDepending
onfib
ertype;
cHigh-shrinkage(H
S)fib
er.
Fibers, 1. Survey 27Ta
ble7.
Therm
alandelectricalpropertiesof
inorganicfib
ers
Fibername
Trade
name
Fiberdiam
eter,µ
mSp
ecificheatcapacity
[67],Jg−
1K
−1
Therm
alconductiv
ity,
Wm
−K
−1
Heatresistancein
air
upto
, CFire
Lim
iting
Oxygen
Index(LOI),%
Meltin
gtemperature
(Glass
transitio
nTg),
C
Specificelectrical
resistance,Ω
cm
Textile
glass
Gevetex,F
iberglas
5–15
≈0.75
≈0.8
300–400
(600
Tg
700)
1012–10
15
EGlass
E-Fiber,E
nkafort
5–15
≈0.75
≈0.8
300-400
(600
Tg
700)
1012–10
15
Aluminum
silicate
Nextel3
1217
1200
–1300
1800
(e.g.,3Al 2O
3·2
SiO
2·B
2O
3)
Nextel4
401200
–1300
1800
Nextel4
801200
β-Siliconcarbide
Nicalon
(Nippon
Carbon)
5–20
12>
800
2700
FP(D
uPont)
20900
Saffil,Saffimax
(ICI)
3–3.2
1000
Silica(SiO
2)
Silica(A
kzo)
9-10
1000
–1100
1750
Steel(20
%Cr,7%
Ni)
Bekinox
filam
ents
0.46
151400
–1450
Carbon(pitchbased)
0.7
×10
−4
High-modulus
types(H
M)
Thornel,G
rafil,
6–9
300(-500)
High-strength
types(H
S)FiberG,...
9–12
300(-500)
>10
−3
Carbon(PANbased)
High-modulus
types(H
M)
Magnamite,P
yrofi
l,6–7
60–115[73]
300(-500)
>60
3600
≈10
−3
High-strength
types(H
S)To
rayca,...
7–9
0.7
15–20
[73]
300(-500)
>60
≈1.5×
10−
3
28 Fibers, 1. SurveyTa
ble8.
Electricalresistance,ironingtemperature,w
ater
absorptio
nandsolubilityof
fibers
Fibername/polymer
Trade
names
Fibertype
aSp
ecific
Ironing
Water
Water
Solubilityin
selected
solvents
c
electrical
tempera-
absorptio
nretention
resistance,b
ture, C
at21
C,
[74],%
Ωcm
65%
R.H.,d
%
Natural
fibers
Cotton
st10
6–10
8180–220
7–11
40–50
concentrated
H2SO
4,C
uoxam-solution
Wool
st10
8–10
11
160–170
15–17
40–45
conc.inorg.acids,conc.KOH
Silk
fi10
9–10
10
140–165
9–11
40–45
conc.inorg.acids,conc.KOH,conc.HCO
2H
Flax
st215–240
8–10
50–55
concentrated
H2SO
4
Regeneratecellu
lose
Viscose
rayon
Evlan,F
ibro,
Sarille,...
st/fi
106–10
7150–180
12–14
85–120
conc.inorg.acids
Cuprammonium
rayon
Asahi
Bem
berg,
Bem
berg,...
st/fi
≈10
7–10
8150–180
11–12
100–125
conc.inorg.acids
Cellulose
acetate
Arnel,C
elco,D
icel
st/fi
109–10
12
180
6–7
20–28
conc.inorg.acids,acetone,dioxane,phenols
Cellulose
triacetate
Estron,Silene,
Tricel,...
st/fi
≈10
14
220–250
2–5
10–18
conc.inorg.acids,acetone,dioxane,phenols
NMMOFiber
Lyocell,Tencel,...
st/fi
150
65–70
N-m
ethylm
orpholineoxide(N
MMO)
Polycon
densatefib
ers
Nylon
6(PA6)
Perlon,A
celon,
st150
3.5–4.5
10–15
conc.inorg.acids,phenols
Amilan,Anso,
fi10
9–10
11
150
3.5–4.5
10–15
conc.inorg.acids,phenols
Caprolan,Grilon,...
hd150
3.5–4.5
9–11
conc.inorg.acids,phenols
Nylon
66(PA66)
Nylon,A
ntron,
st180–200
3.5–4.5
10–15
conc.inorg.acids,phenols
Cantrece,Meryl,
fi10
9–10
11
180–200
3.5–4.5
10–15
conc.inorg.acids,phenols
Tim
brelle,U
ltron,...
hd180–200
3–4
9–11
conc.inorg.acids,phenols
Aramids
Poly(m
-phenyleneisophthalamide)
Nom
ex,C
onex
fi4.5–5
12–17
polarorg.solventsandsolutes(LiCl,CaC
l 2),conc.
H2SO
4
Poly(p-phenyleneterephthalam
ide)
(PPT
A)
Kevlar29,T
waron,
fi2–3
7conc.H
2SO
4
Kevlar49,K
evlar
149,Tw
aron
fi/an
1015
2–3
7conc.H
2SO
4
Kevlar981,Tw
aron
fi/hd
2–3
7conc.H
2SO
4
KevlarHp
fi2–3
7conc.H
2SO
4
Poly(ethyleneterephthalate)
(PET)
Dacron,Diolen,
st150–200
0.3–0.4
3–5
conc.H
2SO
4,conc.KOH,phenols,tetrachloroethane
Fortrel,Grilene,
fi10
11–10
14
150–200
0.2–0.5
3–5
conc.H
2SO
4,conc.KOH,phenols,tetrachloroethane
Terylene,T
revira,...
hd150–200
0.2–0.4
3–5
conc.H
2SO
4,conc.KOH,phenols,tetrachloroethane
Poly(1,4-dim
ethylene
cyclohexane
terephthalate)
(PDCT)[59]
Kodel
st≈
200
0.2
conc.H
2SO
4,conc.KOH,phenols,tetrachloroethane
Fibers, 1. Survey 29Ta
ble8.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aSp
ecific
Ironing
Water
Water
Solubilityin
selected
solvents
c
electrical
tempera-
absorptio
nretention
resistance,b
ture, C
at21
C,
[74],%
Ωcm
65%
R.H.,d
%
Polyarylate
Ekonol[60],Vectran
fi0
NMP+CaC
l 2Po
ly(ether
etherketone)(PEEK)
Zyex
ficonc.H
2SO
4
Novolak
Kynol,P
hilene,
Novoloid,...
6–8
Poly(amideim
ide)
(PAI)
Kermel
3polarorg.solvents(D
MA,N
MP)
Poly(ether
imide)
(PEI)
st/fi
0.25
–1.25
dichloromethane
Polyurethane
elastomers(spandex)
Dorlastan,L
ycra,...
fi150–180
0.5–1.5
7–11
noncross-linkedfib
ers:DMA,D
MF,HMPA
,conc.
inorg.acids(decom
p.)
Polym
erizatefib
ers
Polyethylene
(HD-PE)
Hiralon,V
egon,
Spectra,...
fi10
13–10
17
00
conc.H
2SO
4,benzene,chlorinated
hydrocarbons
Polypropylene(PP)
Herculon,
Meraklon,...
st/fi
>10
13
130
00
conc.H
2SO
4,toluene,chlorinated
hydrocarbons
Polyacrylonitrile
(PAN)
e.g.,D
ralonT
fi/st
≈10
14
150–180
≈1
4–6
conc.inorg.acids,D
MA,D
MF,DMS,
ethylene
carbonate,conc.Z
nCl 2
orNaSCNsolutio
nsCopolym
erizates
with
PAN
≥85
%Dolan,D
ralon,...
st/fi
108–10
14
150–180
1–1.5
5–12
conc.inorg.acids,D
MA,D
MF,DMS,
ethylene
carbonate,conc.Z
nCl 2
orNaSCNsolutio
nsModacrylics(50–84
%PA
N)
Kanekalon,S
EF,...
st10
12–10
13
0.4–3
10–20
conc.H
2SO
4,D
MF,acetone,phenol,cyclohexanone
Poly(vinyl
chloride)(PVC)
atactic
Clevyl,Rhovyl
st/fi
1012–10
14
0–0.2
4–6
conc.H
2SO
4,chlorinated
hydrocarbons,dioxane,
cyclohexanone,DMF
syndiotactic[61]
st10
12–10
14
04–6
conc.H
2SO
4,chlorinated
hydrocarbons,dioxane,
cyclohexanone,DMF
30 Fibers, 1. SurveyTa
ble8.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aSp
ecific
Ironing
Water
Water
Solubilityin
selected
solvents
c
electrical
tempera-
absorptio
nretention
resistance,b
ture, C
at21
C,
[74],%
Ωcm
65%
R.H.,d
%
Poly(vinyl
alcohol)(PVA)
Kuralon,M
ewlon,...
st/fi
3.5–5
25–35
conc.inorg.acids,phenols,D
MF
Poly(tetraflu
oroethylene)
(PTFE
)Gore-TexFibers,...
st/fi
>10
14
0perfluorinatedsolvents
>300
CPo
ly(phenylene
sulfide)(PPS
)Procon,R
yton,...
st/fi
≈0.03
–0.25
(<0.6)
<200
Cno
solvent
Melam
ineresinfib
erBasofi
lst
9Inorganicfib
ers
Textile
glass
Gevetex,F
iberglas
st/fi
1012–10
15
0.1
0hydrofl
uoricacid
Eglass
E-Fiber,E
nkafort
fi10
12–10
15
0.1
0hydrofl
uoricacid
Aluminum
silicate
Nextel3
12st
≈0
0hydrofl
uoricacid
(e.g.,3Al 2O
3·2
SiO
2·B
2O
3)
Nextel4
40st
≈0
hydrofl
uoricacid
Steel(20
%Cr,7%Ni)
Bekinox
fi0.7×
10−
40
(attacked
byhalogenatedsolvents)
ast=staplefib
er,fi
=filam
ent,hd
=highly
draw
n,an
=annealed,ap=antip
illing;
bof
fiberswith
outadditivesor
specialfi
nishes;
cDMA=dimethylacetamide,DMF=dimethylformam
ide,DMS=dimethylsulfoxide,H
MPA
=hexamethylphosphoramide,NMP=N-m
ethylp
yrrolid
one;
dR.H.=
relativ
ehumidity.
Fibers, 1. Survey 31Ta
ble9.
Resistanceof
fibersc
Fibername/polymer
Trade
names
Fibertype
aHeat(air)
Light/weather
bBiologicalinfl
uencec
Chemicalsc
Fire
upto
t, C
Residual
Micro-
Insects
Residualtenacity,%
limiting
tenacity,%
organism
sAfter
1000
hat20
C/10hat100
Coxygen
[57],[58],
diluteacid
dilutealkali
index
[75],[76]
(LOI),%
Natural
fibers
Cotton
st120
20–30/0–20
−(+)
60–80/0–20
80–100/80
–100
19–20
Wool
st120
0–20/0–20
−−
90–100/selective
selective
25–28
Silk
fi120
0–20/0–20
(+)
(+)
lower
than
wool
selective
Flax
st0–20/0–20
bleached
(+)
moreresistantthan
cotto
nlower
than
cotto
n
Regeneratecellu
lose
Viscose
rayon,Viscose
Modal
Evlan,F
ibro,
Sarille,...
st/fi
120
0–30/0
−−
similarto
cotto
n19
–20
Cuprammonium
rayon
Asahi
Bem
berg,
Bem
berg
st/fi
120
0–30/0
−−
similarto
cotto
n19
–20
Cellulose
acetate(CA)
Arnell,Celco,D
icel,
st/fi
120
20–45/0–25
(+)
−60
–100/selective
0–20/20–60
NaO
H18
–19
Cellulose
triacetate
Estron,Silene,
Tricel,...
st/fi
130
20–45/0–25
(+)
−60
–100/selective
betterthan
CA
18–19
NMMOFiber
Lyocell,Tencel
st/fi
150
similarto
cotto
nsimilarto
cotto
nsimilarto
cotto
n
Polycon
densatefib
ers
Nylon
6(PA6)
Perlon,A
celon,
st120
20–30/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–21.5
Amilan,Anso,
fi120
20–30/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–21.5
Caprolan,Grilon,...
hd120–150
20–30/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–21.5
Nylon
66(PA66)
Nylon,A
ntron,
st120
20–30/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–21.5
Cantrece,Meryl,
fi120
20–30/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–21.5
Tim
brelle,U
ltron,...
hd120–150
20–30/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–21.5
32 Fibers, 1. SurveyTa
ble9.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aHeat(air)
Light/weather
bBiologicalinfl
uencec
Chemicalsc
Fire
upto
t, C
Residual
Micro-
Insects
Residualtenacity,%
limiting
tenacity,%
organism
sAfter
1000
hat20
C/10hat100
Coxygen
[57],[58],
diluteacid
dilutealkali
index
[75],[76]
(LOI),%
Aramids
Poly(m
-phenyleneiso-
phthalam
ide)
Nom
ex,C
onex
fi180–200
/50
+80
–100/80
–100
90–100/90
–100
26–30
Poly(p-phenylene-
terephthalam
ide)
(PPT
A)
Kevlar29,T
waron,
fi180–200
65–80/after
16weeks
(+)
++
+
Kevlar49,T
waron,
Kevlar149,
fi/an
180–200
65–80/after
16weeks
(+)
++
+29
–31
Kevlar981,Tw
aron,
fi/hd
180–200
65–80/after
16weeks
(+)
++
+29
–31
KevlarHp
fi180–200
65–80/after
16weeks
(+)
++
+29
–31
Poly(ethylene
terephthalate)
(PET)
Dacron,Diolen,
st120–150
60–80/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–22
Fortrel,Grilene,
ap120–150
60–80/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–22
Terylene,S
erene,
fi120–150
60–80/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–22
Trevira,...
hd150–160
60–80/5–15
(+)
+90
–100/90
–100
90–100/90
–100
20–22
Poly(butylene
terephtalate)(PBT)
Trewira810,...813
st/fi
120
Poly(1,4-dim
ethylene
cyclohexaneterephthalate)
(PDCT)[59]
Kodel
st≈
200
+70
–80
HCl
50–70
Na 2
CO
3solutio
n
Polyarylate
Vectran,E
konol[60]
fi180–260
+/96
-36
Poly(ether
etherketone)
(PEEK)
Zyex
fi200–250
-99/23-74
selective
/95
30–35
Polyim
ide(PI)
P84
st/fi
260
80
(+)
36–38
Novolak
Kynol,P
hilene,
Novoloid
st200
+-
30–39
Fibers, 1. Survey 33Ta
ble9.
(Contin
ued)
Fibername/polymer
Trade
names
Fibertype
aHeat(air)
Light/weather
bBiologicalinfl
uencec
Chemicalsc
Fire
upto
t, C
Residual
Micro-
Insects
Residualtenacity,%
limiting
tenacity,%
organism
sAfter
1000
hat20
C/10hat100
Coxygen
[57],[58],
diluteacid
dilutealkali
index
[75],[76]
(LOI),%
Poly(amideim
ide)
(PAI)
Kermel
st250
-+
(+)
31–32
Poly(ether
imide)
(PEI)
st/fi
160–170
+95
–100/
85–100/
33Po
lyurethane
elastomers
(spandex)
Dorlastan,L
ycra,...
fi120
0/0
++
selective;polyether
moreresistantthan
polyester
Polym
erizatefib
ers
Polyethylene
(HD)-PE
Hiralon,V
egon,,...
fi70
–90
+−
(+)
++
(HM
–HD–PE
:Mr
>10
6)
Spectra1000
hd80
–90
+−
(+)
++
Polypropylene(PP)
Herculon,
Meraklon,...
st/fi
≈120
0/0
−(+)
++
19–20
Polyacrylonitrile
(PAN)
e.g.,D
ralonT
fi/st
140
60–80/50–60
(+)
+90
–100/80
–100
90–100/60
–100
18–20
Copolym
erizates
with
PAN
≥85
%Dolan,D
ralon,
Euroacril,
Leacril,...
st/fi
140
60–80/50–60
(+)
+90
–100/80
–100
90–100/60
–100
18–20
Modacrylics(50–84
%PA
N)
Kanekalon,S
EF,...
st120
lower
than
PAN
++
++
25–30
Poly(vinyl
chloride)
atactic
Clevyl,Rhovyl,...
st/fi
<65
60–90/
++
++
37–46
syndiotactic[61]
st+
++
+37
–46
Poly(vinyl
alcohol)(PVA)
Kuralon,M
ewlon,
st140(w
ater
vapor:
120)
betterthan
nylon
20
Solvron,Vilo
n,...
fi140(w
ater
vapor:
120)
+/(+)
(+)
(+)
betterthan
nylon
+20
(HM:M
r>
106)
hd140(w
ater
vapor:
120)
betterthan
nylon
+20
Poly(tetraflu
oroethylene)
(PTFE
)Gore-TexFibers,...
st/fi
180
++
++
40
Poly(phenylene
sulfide)
(PPS
)Procon,R
yton,...
st/fi
190–200
-+
++/100
+/100
34–35
Melam
ineresinfib
erBasofi
lst
200–220
0≈
70/
30
ast=staplefib
er,fi
=filam
ent,hd
=highly
draw
n,an
=annealed
ap=antip
illing;
bno
UVstabilizersadded,one-year
exposure
inFlorida;
c+resistant,(+)moderatelyresistant,
−notresistant.
34 Fibers, 1. Survey
Table 10. Dyeing behavior of fibers
Fiber name/polymer Trade name Dyes
Natural fibersCotton substantiveWool anionicSilk anionic, cationic, substantive, reactive, vatRegenerate celluloseViscose rayon Evlan, Fibro,... substantiveCuprammonium rayon Asahi Bemberg,... substantiveCellulose acetate Arnel, Celco, Dicel, substantive, disperseCellulose triacetate Estron, Silene, Tricel,... substantive, disperseNMMO fiber Lyocell, Tencel,... substantive, reactivePolycondensate fibersNylon 6 Perlon, Capron, Grilon,... anionic, metal-complex disperseNylon 66 Nylon, Antron, Ultron,... anionic, metal-complex, dispersePoly(m-phenyleneisophtalamide) (aramid) Nomex cationic plus carrier, high-temperature
conditionsPoly(ethylene therephthalate) Dacron, Diolen,... disperse plus carrier, high-temperature
conditionsPoly(1,4–dimethylenecyclohexane) Kodel disperse plus carrier, high-temperature
conditionsPoly(butylene terephthalate) Trevira 810,..813 disperseNovolak Kynol,... dispersePoly(ether imide) dispersePolyurethane elastomers Dorlastan, Lycra anionicPolymerizate fibersPolypropylene Herculon, Meraklon,... dispersePolyacrylonitrile Dralon, Dolan,... cationic, disperseModacrylics Kanekalon, SEF,... cationic, dispersePoly(vinyl chloride) Clevyl, Rhovyl,... dispersePoly(phenylene sulfide) Procon, Ryton disperse
Figure 8. Specific tenacity (σ/) and modulus (E/) of high-performance fibers (= density)
Fibers, 1. Survey 35
Figure 9. Highest temperatures for fiber application without significant loss in tenacity
Values for fiber elongation, fiber shrinkage,and relative properties such as wet tenacity, looptenacity and other parameters are expressed aspercent. If properties such as fiber resistance tolight, weather, chemicals, or organisms cannotbe expressed numerically, they are characterizedin a simplified qualitative manner in Table 9. Inindividual cases, the respective conditions andthe type of attack (e.g., by certain kinds of pests[57], [58]) are such that widely differing resultscan be expected.
Some promising fibers that are still being de-veloped have also been included, in particular,high-performance fibers made from highmolec-ular mass poly(vinyl alcohol), the thermoresis-tant PEEK, PAI, PI (see Fig. 9, and the polyary-late “ Ekonol,” an example of a thermotropicpolymer [59]. Among the inorganic fibers, apartfrom carbon and glass, the properties of siliconcarbide, and ceramic fibers have been included.Figure 8 shows the ranges ofYoung’smoduli andtenacities of presently known high-performancefibers usedmainly for reinforcing organic resins.
Although fibers are highly anisotropic com-pared with other materials and therefore espe-cially strong in the axial direction their Young’smodulus is always inferior to the theoretical
(crystal) modulus. The ratio of fiber to crys-tal modulus attains about 0.1 for textile com-modity fibers, 0.3 for high-performance fibers(e.g., from HM-HDPE), especially those withextended chain structure, and as high as 0.8 forthe LC polymer Kevlar 149 with unfolded, ori-ented PPTA molecules. The deficit of the fibermodulus is a consequence of incompletely un-coiled and disentangled macromolecules in as-spun and drawn fibers. Themechanical responseof fibers is controlled by the fraction of taut tiemolecules connecting neighboring crystallites.This fraction can be estimated from measure-ments of the elastic modulus by using a simplerheological model or other methods to be about0.05 – 0.1 for drawn fibers [83].
Compressibility and lateral compliance in-creasewith increasingfiber anisotropy (ondraw-ing) and this is undesirable for reinforcing fibers(e.g., Kevlar or carbon fibers) in composites. Insome cases thermal aftertreatment of such high-performance fibers allows a compromise to befound between the desired compressibility andlower tenacity (see also compressive strength offibers in Table 4).
The applicability of industrial fibers at highertemperatures (see Tables 6 and 7) is of current
36 Fibers, 1. Survey
interest. Figure 9 reviews the thermal long-termstability in air.
This compilation of important data is by nomeans complete. For further information, see→Fibers, 4. Synthetic Organic and →Fibers,5. Synthetic Inorganic.
9. References
General References1. H. Batzer (ed.): Polymere Werkstoffe, Thieme
Verlag, Stuttgart 1986.2. R. Bauer, H. J. Koslowski:
Chemiefaser-Lexikon, 10th ed. DeutscherFachverlag, Frankfurt 1993.
3. J. Brandrup, (ed.): Polymer Handbook , 2nded., Interscience, New York 1976.
4. R.M. Brown, (ed.): Cellulose and OtherNatural Polymer Systems, Plenum Publishing,New York 1982.
5. M. E. Carter: Essential Fiber Chemistry,Dekker, New York 1971.
6. J. G. Cook: Handbook of Textile Fibres,Merrow, Watford 1968.
7. H. Driesch: Welche Chemiefaser ist das,Franckh, Stuttgart 1962.
8. A.A Dembeck: Guidebook to Man-madeTextile Fibres and Textured Yarns of the World,3rd ed. The United Piece Dyed Works, NewYork 1969.
9. H. Doehner (ed.):Wollkunde, Parey, Berlin1964.
10. H. F. Mark (ed.): Encyclopedia of PolymerScience and Technology, “Plastics, resins,rubbers, fibres,” Wiley-Interscience, New York1967.
11. B. Falkai (ed.): Synthesefasern, VerlagChemie, Weinheim 1981.
12. F. Fourne (ed.): “Herstellung undVerarbeitung,” Synthetische Fasern,Wissenschaftl. Verlags GmbH, Stuttgart 1964.
13. B. C. Gaswami, J. G. Martindale, F. L.Scardino: Textile Yarns, Wiley-Interscience,New York 1977.
14. M. Grayson (ed.): Encyclopedia of Textiles,Fibers, and Nonwoven Fabrics,Wiley-Interscience, New York 1984.
15. F. Happey: Applied Fibre Science, AcademicPress, London 1979.
16. H.W. Haudek, E. Viti: Textilfasern, Bondi,Wien 1980.
17. High polymers, a Series of Monographs on theChemistry, Physics and Technology of High
Polymeric Substances, Interscience, NewYork.
18. Internat. Baumwoll-Inst. (ed.): Handbuch derBaumwollstoffe, Frankfurt 1983.
19. H. Klare: Geschichte derChemiefaserforschung, Akademie Verlag,Berlin 1985.
20. P.-A. Koch, (ed.): Großes Textil-Lexikon,Deutsche Verlagsanstalt, Stuttgart 1966.
21. H.A. Krassig, J. Lenz, H. F. Mark: FiberTechnology, Dekker, New York 1984.
22. R. Vieweg, G.W. Becker (ed.):Kunststoff-Handbuch, Hanser Verlag,Munchen 1965.
23. P. Lennox-Kerr: The World Fibres Book, TheTextile Trade Press, Mancheser, 1972.
24. M. Lewin, S. B. Sello (ed.): Handbook of FiberScience and Technology, Dekker, New York1983.
25. W. Loy: Chemiefaserstoffe, Schiele undSchon, Berlin 1978.
26. J. A. Maclaren, B. Milligan:Wool Science,Science Press, Marrickville 1981.
27. H. F. Mark (ed.):Man-made Fibers, Scienceand Technology, Interscience, New York 1968.
28. R. Meredith: Elastomeric Fibres, Merrow,Watford 1971.
29. B. E. Messerli (ed.): Seide,Textilwerkstattverlag Hannover, 1986.
30. L. Miles: Cotton, Wayland, Have 1980.31. R. Moncrieff:Man-made-Fibres, 4th ed.,
Heywood, London 1966.32. J. S. Robinson (ed.): Fiber-forming Polymers,
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34. J. S. Robinson (ed.):Manufactue of Yarns andFabrics from Synthetic Fibers, Noyes DataCorp., Park Ridge 1980.
35. W. J. Roff: Fibres, Films, Plastics andRubbers, Butterworths, London 1971.
36. Z. A. Rogovin: Chemiefasern, Thieme Verlag,Stuttgart 1982.
37. H. E. Schiecke: Wolle als textiler Rohstoff,Schiele und Schon, Berlin 1979.
38. K.A. Schmidt: Technologie textilerGlasfasern, Zechner, Speyer 1964.
39. Textil-Fakten: Markt- und Strukturdaten derTextil- und Bekleidungswirtschaft, DeutscherFachverlag, Frankfurt 1983.
40. Textile Faserstoffe, Fachbuchverlag, Leipzig1967.
41. C. A. Tisdell: Economics of Fibre Markets,Univ. New Castle, New Castle, Austr. 1977.
Fibers, 1. Survey 37
42. E. Wagner: Die textilen Rohstoffe, 6th ed.,Spohr, Wuppertal 1981.
43. A. Ziabicki: Fundamentals of Fibre Formation,Wiley Interscience, New York 1976.
44. A. Ziabicki: High Speed Fibre Spinning,Wiley Interscience, New York 1985.
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53. P.-A. Koch: Faserstoff-Tabellen,Konradin-Verlag Kohlhammer GmbH,Stuttgart 1968, 1977, 1979.
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