FRACTURABLE FIBER CROSS SECTIONS

Abstract: Fracturable continuous filaments. The filaments can be used to produce continuous filament yarns which have a spun like character. The filaments of the invention have a cross section comprising a body section (34) and one or more wing members (32) joined to the body section, the one or more wing members varying up to twice their minimum thickness along their width and characterized in that at the junction of the body section and the one or more wing members the respective faired surfaces thereof define a radius of concave curvature (RC) on one side of the cross section and a generally convex curve located on the other side of the cross section generally opposite the radius of concave curvature (RC), the body section comprising 25 to 95 % of the total mass of the filament and the wing members comprising 5 to 75 %, the filament being further characterized by a wing-body interaction (WBI) defined by <IMAGE> where the ratio of the width of the filament cross section to the wing member thickness (LT/Dminis <=30).

Description: FRACTURABLE FIBER CROSS SECTIONS This invention relates to novel synthetic filaments, which may be used as textile filaments. The filaments have a special geometry, which if subjected to preselected processing conditions, will give controlled fracturability so as to produce free protruding ends. Historically, fibers used by man to manufac¬ ture textiles, with the exception of silk, were of short length. Vegetable fibers such as cotton, animal fibers such as wool, and bast fibers such as flax all had to be spun into yarns to be of value in producing fabrics. However, the very property of short staple length of these fibers requiring that the yarns made therefrom be spun yarns also resulted in bulky yarns having very good covering power, good insulating properties and a good, pleasing hand. The operations involved in spinning yarns from staple fibers are rather extensive and thus are quite costly. For example, the fibers must be carded and formed into slivers, then drawn to reduce the diameter, and finally spun into yarn. Yarns made from continuous filaments having cross sections described in U.S. Patent 4,245,001, have a spun yarn character. The filaments described in this patent are continuous filaments which are fracturable. That is, when these filaments are subjected to certain conditions, portions of the filaments break away ..from the main bulk of the filament thereby providing the spun character to the yarns made from the filament even though the filament is continuous. More particularly, the yarn comprises a bundle of continuous fractured filaments, the filaments having a continuous body section with at least one wing member extending from and along the body section, the wing member being intermittently separated from the body section. A fraction of the OMPI • separated wing members are broken to provide free protruding ends extending from the body section to provide the spun yarn character. The yarn is further characterized in that portions of the wing member are separated from the body section to form bridge loops, the wing member portion of the bridge loop being attached at each end thereof to the body section, the wing member portion of the bridge loop being shorter in length than the corresponding body section por- tion. In order to be "fracturable", the body portion and the wing portion of the filament cross section have a particular relationship referred to as wing- body interaction or WBI. WBI will be more fully discussed below. The yarns made from the filaments described in U.S. Patent 4,245,001 are a major improvement over previous attempts at continuous filament yarns having a spun-like character. However, there has been a continuing need for alternate filament cross sections which provide this desirable property. The present invention provides such a fracturable filament. According to the invention there is provided a filament having a cross section comprising a body section and one or more wing members joined to the body section, the one or more wing members varying up to twice their minimum thickness along their width and characterized in that at the junction of the body section and the one or more wing members the respec¬ tive faired surfaces thereof define a radius of concave curvature (R c ) on one side of the cross section and a generally convex curve located on the other side of the cross section generally oposite the radius of concave curvature (R r ) , the body section comprising 25 to 95% of the total mass of the filament and the wing members comprising 5 to 75%, the filament being further characterized by a wing-body interaction (WBI) defined by where the ratio of the width of the filament cross section to the wing member thickness (L-/D . is <30. Yarns made from the filaments of the present invention are fracturable. Further, the filaments are fracturable over a somewhat wider range of WBI than are the specific filaments of U.S. Patent 4,245,001. For the type of cross section of the present invention, it is sufficient for the WBI to be greater than or equal to 1 to be fracturable rather than <L0 as in U.S. Patent 4,245,001. Brief Description of Drawings The details of the invention will be des- cribed in connection with the accompanying drawings in which Figures 1A and IB are drawings of represen¬ tative spinineret orifices showing the nature and location of typical measurements to be made; Figure 2 is a drawing of a representative filament cross section having a body section and two wing members and showing where the overall length of a wing member cross section (Iv,) and the overall or total length of a filament cross section (L τ ) are measured, where on the wing member the thickness (Dmm. ) of the win σ member is measured, where on the body section the filament body J diameter (Dmax)' is measured and the location of the radius of curvature Figure 3 is a photomicrograph of one embodi¬ ment of a spinneret orifice in a spinneret; Figure 4 is a photomicrograph of a filament cross section of a filament spun from the spinneret orifice shown in Figure 3; Figure 5 is a photomicrograph of a second embodiment of a spinneret orifice in a spinneret; Figure 6 is a photomicrograph of a filament cross section of a filament spun from the spinneret orifice shown in Figure 5; Figure 7 is a photomicrograph of a third embodiment of a spinneret orifice in a spinneret; Figure 8 is a photomicrograph of a filament cross section of a filament cross section spun from the spinneret orifice shown in Figure 7; Figure 9 is a drawing of a spinneret orifice having a single-segment body section and a single- segment wing member having an angle therebetween of 90°; Figure 10 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 9; Figure 11 is a drawing of a spinneret orifice having a single-segment body section and a two-segment wing member; Figure 12 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 11; Figure 13 is a drawing of a spinneret orifice having a single-segment body section and a one-segment wing member intersecting at 105° at one end of the body section and another one-segment wing member intersecting at 90° with the other end of the body section, and with the lengths of the wing members differing from each other; Figure 14 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 13; OMPI Figure 15 is a drawing of a spinneret orifice having a single-segment body section and a one-segment wing member intersecting at 120 at one end of the body section, with each wing member being of the same length as the other; Figure 16 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 15; Figure 17 is a drawing of a spinneret orifice having a single-segment body section and a single-segment wing member intersecting at one end of the single-segment body section at an angle of 60° and a four-segment wing member intersecting at the other end of the single-segment body section at an angle of 60°; Figure 1 ' 8 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 17; Figure 19 is a drawing of a spinneret orifice having a dual-segment body section having an angle therebetween of 60° and having a single-segment wing member intersecting at each end of the dual-seg¬ ment body section at an angle of 60°; Figure 20 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 19; Figure 21 is a drawing of a spinneret orifice having a dual-segment body section having an angle therebetween of 90° and having a three-segment wing member intersecting with each other and at each end of the dual-segment body section at an angle of 90°; Figure 22 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 21; Figure 23 is a drawing of a spinneret orifice having a dual-segment body section having an OMPI WIPO angle therebetween of 50° and having a three-segment wing member intersecting with each other and at each end of the dual-segment body section at an angle of 50°; Figure 24 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 23; Figure 25 is a drawing of a spinneret orifice having a dual-segment body section having an angle therebetween of 60° and having a three-segment wing member, as viewed to the left of the body section, intersecting and at one end of the body section at an angle of 60°, and having a four-segment wing member, as viewed to the right of the body section, intersecting and at the other end of the body section at an angle of 60°, with the lengths of the segments in one wing member differing from those in the other wing member; Figure 26 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 25; Figure 27 is a drawing of a spinneret orifice having a tapering dual-segment body section having an angle therebetween of 90° and having a tapering two-segment wing member intersecting with each other at an angle of 90° and with the body section at an angle of 75°; Figure 28 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 27; Figure 29 is a drawing of a spinneret orifice having a three-segment body section intersecting with each other at an angle of 60° and having a single-segment wing member intersecting at one end of the body section at an angle of 60°; Figure 30 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 29; Figure 31 is a drawing of a spinneret orifice having a four-segment body section intersect¬ ing with each other at an angle of 30° and having two five-segment wing members each intersecting at an end of the body section at an angle of 40°, and the five segments of each wing member intersecting with each other from the outer end toward the body section, respectively, at angles of 60°, 60°, 50° and 45°; Figure 32 illustrates the approximate configuration a filament cross section will have when spun from the spinneret orifice shown in Figure 31; Figure 33 is a drawing of a spinneret orifice having an enlarged two-segment body section intersecting with each other at an angle of 90° and having two four-segment wing members each intersect¬ ing at each end of the body section at an angle of 90°, and each wing member segment intersecting with an adjacent wing member segment at an angle of 90°; Figure 34 illustrates the approximate cross section a filament cross section will have when spun from the spinneret orifice shown in Figure 33; Figure 35 is a drawing of a spinneret orifice having a three-segment body section inter¬ secting with each other at an angle of 60° and four wing members, each being in four segments and the segments intersecting with each other at an angle of 60° with two diagonally opposite wing members inter¬ secting the body section at an angle of 120° and the other diagonally opposite two wing members inter- secting the body section at an angle of 60°; Figure 36 illustrates the approximate cross section a filament cross section will have when spun from the spinneret orifice shown in Figure 35; Figure 37 is a photomicrograph of fractured and non-fractured filament cross sections; Figure 38 shows tracings of fibers from a yarn to illustrate bridge loops and free protruding ends; and OMPI Figure 39 illustrates six classifications of observed events occurring when yarn is fractured. The present invention relates to filaments having a cross section which has a body section and one or more wing members joined to the body section. The wing members vary up to twice their minimum thickness along their width. At the junction of the body section and the one or more wing members the respective faired surfaces thereof define a radius of concave curvature ( -r) o n o ne side of the cross section and a generally convex curve located on the other side of the cross section generally opposite the radius of curvature (R c ) , that is, a V-shape is formed. The body section constitutes 25 to 95% of the total mass of the filament and the wing member or wing members constitute 5 to 75% of the total mass of the filament, with the filament being further charac¬ terized by a wing-body interaction (WBI) defined by WBI - >1 where the ratio of the width of the filament cross section to the wing member thickness ( -/D . ) is 30. It is critical to this invention that the cross section of the filaments be such that the filaments are fracturable. To be fracturable, the WBI, as defined above, should be equal to or greater than 1 and the ratio of the width of the filament cross section to the wing member thickness (L-,/- D in^ " s 4^* Referr ing in particular to the photomicrograph in Figure 4, for instance, there is illustrated how the fiber cross-sectional shape characterization and thus WBI calculation is accom¬ plished. OMPI 1. Make a negative of a filament cross section at 500X magnification from the undrawn or partially oriented feeder yarns by embedding yarn filaments in wax, slicing the wax into thin sections with a microtome and mounting them on glass slides. Then make a photoenlarge ent from the negative that will be eight times larger than the original negative. It is important to note that drafting of undrawn or partially oriented filaments does not change the shape of the filaments. Thus, except for the inher¬ ent difficulties in preserving accurate representa¬ tions of the fiber cross section at 500X or greater and in cutting fully oriented and heatset fibers, the geometrical characterization can be accomplished using measurements made from the photoenlargements of fully oriented and heatset filaments. 2. Measure Dmm.„,' D„ma α x'. L τ W τ and L τ T using ° any convenient scale. These parameters are shown in the Figures, for instance, and are defined as follows: a. Dmm.„ is the thickness of the wing ° member for essentially uniform wing members and the minimum thickness close to the body section when the thickness of the wing member is variable. b. Dma„x is the maximum thickness of the body section. c. L ™ is the overall length of the filament cross section. d. L- j is the overall length of an individual wing member. in all cases the above dimensions are measured from the outside of the "black" to the inside of the "white" in the photomicrograph. It was found more reproducible measurements can be obtained using this procedure. The "black" border is caused primarily by the nonperfect cutting of the sections, the nonper¬ fect alignment of the section perpendicular to the viewing direction, and by interference bands at the s. wi p o edge of the filaments. Thus it is important in producing these photographs to be as careful and especially consistent in the photography and measur¬ ing of the cross sections as is practically pos- sible. Average values are obtained on a minimum of 10 filaments. 3. Measure the radius of curvature (R ) of the intersection of the wing member and body section as shown for example in the Figures. Use the same ι o length units which were used to measure D , D min» etc - One convenient way is to use a circle template and match the curvature of the intersection to a particular circle curvature. c is measured at all possible locations per filament cross section -JC and the sum total of the R c 's is averaged to get a representative - ' . For example, in Figure 20 each filament cross section has 2 Rς's which are averaged to give the final R Q . The averaged Rς* s for individual filaments are then averaged to get an 2 Q c which is indicative of the filaments in a complete yarn strand. R^. values are usually determined on a minimum of 20 filaments from at least two different cross section photographs. 4. To determine the percent total mass of the 25 body section and of the wing member(s) , a photocopy of the cross section is made on paper with a uniform weight per unit area. The cross section is cut from the paper using scissors or a razor blade and then the wings are cut from the body along the dotted 30 lines as shown in Figure 4. A minimum of 20 indi¬ vidually similar cross sections from at least two different cross sections are photographed and cut with the total number of body sections being weighed collectively and the total number of wing members 5 being weighed collectively to the nearest 0.1 g. The percent areas in the wing member and body section are defined as % Cross-sectional Area in Wing Members * Collective weight of wing member(s) (gms.) Collective weight o£ wing member(s) and body section (gms.) % Cross-sectional Area in Body Section ■ Collective weight of body section (gms.) Collective weight o£ wing member(s)i and body section (gms.) The cross section of the filament may have a single wing member, or two or more wing members. The filament cross section may also have one or more wing members that are curved, or the wing member(s) may be angular. The filament cross section may also have two wing members and one of the wing members may be nonidentical to the other wing member. The thickness of the wing member(s) may vary up to twice the minimum thickness and the greater thipkness may be along the free edge of the wing member(s). Stated in another manner, a portion of each wing member may be of a greater thickness than the remainder of the wing member. The periphery of the body section may define one central convex curve on the one side of the cross section and one central concave curve located on the other side of the cross section generally opposite the aforementioned one central convex curve. The periphery of the body section may also define on the one side of the filament cross section at least one central convex curve and at least one central concave curve connected together, and on the other side of the cross section at least one central concave curve and at least one central convex curve connected together. The periphery of the body section may further define on the one side of the filament cross section two central convex curves and a central concave curve connected therebetween and on the other side of the cross section two central concave curves and a central convex curve connected therebetween. Each of the one or more wing members may have along the periphery of its cross section on the one side of the filament cross section a convex curve joined to the aforementioned radius of concave curvature (R c ) and on the other side of the cross section a concave curve joined to the first-mentioned convex curve that is generally opposite the radius of concave curvature (R.-,) . Each of the one or more wing members may also have along the periphery of the filament cross section on the one side thereof two or more curves alternating in order of convex to concave with the latter mentioned convex curve being joined to the aforementioned radius of concave curvature (R c ) and on the other side of the cross section two or more curves alternating in order of concave to convex with the latter mentioned concave curve being joined to the first mentioned convex curve that is generally opposite the radius of concave curvature (R c ) • The filament cross section may have four wing members and a portion of the periphery of the body section defines on one side thereof at least one central concave curve and on the opposite side thereof at least one central concave curve, each central concave curve being located generally offset from the other. The body section of each filament remains continuous throughout the yarn when the yarn is fractured and thus provides load-bearing capacity, whereas the one or more wing members are broken intermittently along the length of the filament and provide free protruding ends. The filaments may be provided with luster- modifying means which may be finely dispersed titani- um dioxide (TiO- ^ ) or finely dispersed kaolin clay. The filaments of this invention are prefer¬ ably made from polyester or copolyester polymer. Polymers that are particularly useful are polyethyl¬ ene terephthalate) and ρoly(l,4-cyclohexylenedi- methylene terephthalate) . These polymers may be modified so as to be basic dyeable, light dyeable, or deep dyeable as is known in the art. These polymers m y be produced as disclosed in U.S. Patents 3,962,189 and 2,901,466, and by conventional pro¬ cedures well known in the art of producing fiber- forming polyesters. Also the filaments can be made from polymers such as poly(butylene terephthalate) , a polyolefin such as polypropylene, or a polyamide, for example, nylon such as nylon 6 and 66. The filament may be oriented such that its elongation to break is less than 50% and has been heat stabilized to a boiling water shrinkage of <15%., and thereby rendered fracturable. The filaments are preferably formed into a yarn characterized by a denier of 15 or more, a tenacity of 1.1 grams per denier or more, an elonga¬ tion of 8 percent or more, a modulus of 25 grams per denier or more, a specific volume in cubic centi¬ meters per gram at one tenth gram per denier tension of 1.3 to 3.0, and with a boiling water shrinkage of <L5%. The yarn of fractured filaments may have a laser characterization where the absolute b value is at least 0.25, the absolute value of a/b is at least 100 and the L+7 value ranges up to 75. The absolute b value- may also be 0.6 to 0.9, the absolute a/b value may be 500 to 1000; and the L+7 value may be 0 to 10. The absolute b value may still also be 1.3 to 1.7; the absolute a/b value may be 700 to 1500; and the L+7 value may be 0 to 5. Further, the absolute b value may be 0.3 to 0.6; the absolute a/b value may be 1500 to 3000; and the L+7 value may be 25 to 75. The yarn disclosed herein may still further be characterized by a normal mode Uster evenness of 6% or less. Details regarding the measurement of various yarn parameters such as, for example, laser char¬ acterization values, specific volume and the like are known in the art and are found for example in U.S. Patent 4,245,001. The filaments after spinning are drawn, heatset, and subjected to an air jet to fracture the wing member or wing members to provide a yarn having spunlike characteristics. The process for producing the filaments of the present invention involves (a) melt spinning a filament-forming polymeric material through a spin¬ neret orifice the planar cross section of which defines intersecting quadrilaterals in connected series with the L/W (length to width ratio) of each quadrilateral varying from 2 to 10 and with one or more of the defined quadrilaterals being greater in width than the width of the remaining quadrilaterals, with the wider quadrilaterals defining body sections and with the remaining quadrilaterials defining wing members; (b) quenching the filament at a rate suffi¬ cient to maintain at least a wing-body interaction (WBI) of the spun filament of greater athan or equal to 1 where the ratio of the width of the filament to the width of the wing σ member (L_i/Dmm. ) is —<30; and (c) taking up the filament under tension. The fracturing apparatus may comprise a fluid fracturing jet operating at a brittleness parameter (Bp*) of 0.03-0.8 for the yarn being fractured. A suitable fracturing jet that may be used is the one disclosed in U.S. Patent 4,095,319 and also in Figure 20 of the aforementioned U.S. Patent 4,245,001. The fluid fracturing jet may be operated at a brittleness parameter (Bp*) of 0.03-0.6, and preferably at a brittleness parameter of 0.03 to 0.4. Brittleness parameter is a term known in the art and is described for example in U.S. Patent 4,245,001. The specific volume of the fractured yarn may be made to vary along the yarn strand by varying the fracturing jet air pressure. Yarns made from the filaments of the present invention retain the versatility described of the yarns in U.S. Patent 4,245,001. By fracturable yarn is meant a yarn which at a preselected input temperature, generally room temperature, and when properly processed with respect to frequency and intensity of the energy input will exhibit brittle behavior in some part of the fiber cross section (wing members in particular) such that a preselected level of free protruding broken sec- tions (wing members) can be realized. It is within the framework o'f this general definition that the specific cross section requirements for providing yarns possessing textile utility is defined. In the spinneretts for the filaments of the invention, the tips or extreme ends of the connected series of intersecting quadrilaterals which make up the shape of the orafice are preferably rounded or are in the form of circular bores having a greater diameter than the width of the quadrilateral with which it intersects. The purpose of these circular bores is to promote a greater flow of polymer through the thinner end portions of the spinneret orifices so that the cross sections of the spinneret orifice will be filled out with polymer during spinning. More specifically, and with reference to Figure 1A in the drawings, the planar cross section of each spinneret orifice defines intersecting quadrilaterals in connected series with the length- to-width ratio (L/W) of each quadrilateral varying from 2 to 10. At least one of the intersecting quadrilaterals being characterized by having a width greater than the width of the remaining quadri- lateral(s), with the wider quadrilateral(s) defining body sections and with the remaining quadrilateral(s) defining wing member(s) . The intersecting quadi- laterals form a V shape or a series of interconnected V shapes. The number of intersecting quadrilaterals may vary from 5 to 14 and preferably 8; the number of body section quadrilaterals may vary from 1 to 4 and preferably 2; and the number of wing member quadri- laterals for each wing member may vary from 1 to 5 and preferably 3. The angle between adjacent body section quadrilaterals may vary from 30° to 90° and preferably from 45° to 90°, and the angle fci y between adjacent wing member quadrilaterals may vary from 45° to 150° and prefer-ably from 45° to 90°. It has been found that if the angle is less than 120°, the resulting filament will produce a fiber having reduced glitter. Glitter refers to the reflection of specular light from the yarn or from fabrics made from the yarn giving the material a shinny appearance which Is undesirable for certain applications. Reference is made to U.S. Patent 3,846,969 (Reissue 29,363) for a description of glitter. The length-to-width (L β /W B ) of the body section quadrilaterals is preferably in proportional relationship from 1.5 to 10 and still more preferably from 2 to 5.5, the length-to-width (L„/W„) of the wing member quadrilaterals is preferably from 3 to 10 and more preferably from 4 to 6, and the maximum width of the body section quadrilateral, W *, to the minimum width of the body section quadrilateral, W- g , is preferably from 1 to 3. The diameter (D) of the circular base at the extremities of the spinneret orifice cross section divided by the width of the wing member (W.,) is preferably in proportional relationship from 1.5 to 2.5 and preferably 2. In reference to Figure IB, 10 illustrates a characteristic form that a spinneret orifice cross section made by an electric erosion process may have to spin the filament cross section of this inven¬ tion. The designated dimensions of the circular bores 58 and the intersecting quadrilaterals 14, 16, 18, 20, 22, 24, 26 and 28 are all normalized to wing member quadrilateral dimension W such that W is always 1. The intersections of the quadrilaterals are represented by dotted lines. Dimension W should be as small as practical consistent with good spin¬ ning practice. For instance, W may be 84 microns. An intersecting quadrilateral for a body section is preferably 1.4 W, as may be observed from Figure IB, and the circular bore at the extremities of the spinneret orifice cross section may preferably be 2W. The wider quadrilaterals 20, 22 form the body section and the remaining quadrilaterals form the wing members. The different widths illustrated are in proportional relationships to the width W, such as 5W, 6W, etc., as illustrated. Figure 4 shows a photomicrograph of a filament cross section 38 that is spun from the spinneret orifice cross section shown in Figure 3. In Figure 2, 30 illustrates a characteristic form that a filament cross section may have, showing the approximate locations of the minimum dimension (D . ) of the wing members 32; the maximum dimen¬ sion (D ) of the body section 34; the radius of curvature K„) in the area of which fracturing - TRΪ OMPI V^ IPO takes place, athereby separating the wing member from the body section; the wing member width (L^) ; and the width (L ™ ) of the filament cross section. In the filament cross section 38 shown in Figure 4, it will be observed that there are a number of concave and convex curves along the periphery of the cross section forming a series of connected V shapes. A rather central appearing convex curve 60 which is flanked on either side by a concave curva¬ ture 62 and is positioned generally opposite a central appearing concave curve 64, the latter in turn having adjacent on either side convex curves 66. These curves, and the others shown but not specifically designated, bear a one-for-one corres¬ pondence with the number of quadrilateral intersec¬ tions in the spinneret orifice cross section 36. The size of the curves is dependent upon whether they were spun from the body section or wing member quadrilaterals, the length and width of the quadri¬ laterals and the angles between adjacent intersecting quadrilaterals of the spinneret orifice cross sec¬ tion. The body section of the filament cross section essentially is outlined in part by the central appearing convex curve 60, the oppositely located concave curve 64 and its adjacent convex curves 66. The concave curves 62 form the radius of curvatures (R c ) which join the wing members to the body section. When polymer is spun from the spinneret orifice cross section 36 (Figure 3), for Instance, there is a greater mass of flow through the body section than the wing member portions so that the body section polymer is flowing faster than the wing member polymer. As the body section polymer and wing member polymer begin to equalize, the wing member polymer speeds up while the body section polymer slows down with the results that the body section -W-ΪE OMPI ^ WIPO ^NAT tends to expand while the wing members tend to contract. Hence, also, the angles in the filament cross section tend to open out slightly over the angles shown in the spinneret cross section orifice. For instance, the angle a, between intersecting quadrilaterals 42 and 44 is 45°; between 44 and 46 is 48°; between 46 and 48 is 45°; between 50 and 52 is 45°; between 52 and 54 is 47°; and between 54 and 56 is 45°. The angle θ_ between intersecting quadrilaterals 48 and 50 is 47°. The spinneret orifice cross section 68 in Figure 5 and the filament cross section 70 in Figure 6 more graphically illustrate the expansion of the resulting body section of the filament cross section and the contraction of the wing member portion of the filament cross section. Note the appearance of the length of the body section 72 in Figure 6 by compari¬ son to the length of expanse across the larger intersecting quadrilaterals 74 in Figure 5, whereas the longer appearing expanse of length across the wing member quadrilaterals 76, 78, 80 or 82, 84, 86 in Figure 5 result in shorter appearing wing members 88 or 90 in the filament cross section 70 shown in Figure 6. The width of each body section quadri- lateral 74 is 2W, as shown in Figure 5. The extremi¬ ties of the spinneret cross section are defined by circular bores 92. Table I below shows the shape factor para¬ meters, for instance, of the filament cross section 70, the measurements having been made in the manner as described for four filament cross sections of the type represented by filament cross section 70. TABLE I Example Example Example Example 1 2 3 4 69.0 D max mm 64.0 65.0 70.0 D min mm 24.0 24.0 26.0 24.0 R mm 17.5 18.0 16.0 19.0 Ly mm 35.0 41.0 36.0 40.0 Lrp mm 237.0 227.0 235.0 228.0 WBI 3.333 4.432 4.283 4.155 L T /D min 9.87 9.46 9.04 9.50 In reference to Table I, the mean and percent coefficient of variation of WBI for these four filaments representing the population of fila¬ ments in Figure 6 is 4.05 and 12.1%, respectively. The spinneret orifice cross section 94 in Figure 7 has intersecting quadrilaterals 96, 98, 100, 102, 104, 106, 108 and 110, with the wider intersect¬ ing quadrilaterals 102 and 104 designating the body section quadrilaterals while the others designated wing member intersecting quadrilaterals. The width of the body section quadrilaterals is 1.4W, as shown. The extremities of the spinneret orifice cross section are defined by bores 112, which have a diameter of 2W. It will be noted in Figure 7 that the width of the two body section intersecting quadrilaterals 102, 104 is somewhat irregular near their intersec¬ tion. This was due to a defect in the electric erosion process for this particular spinneret and would not be representative of a conventional operat¬ ing electric erosion process. Figure 8 shows the resulting filament cross section 114 from the spinneret orifice cross section of Figure 7. Note the clear definitions of the concave and convex curves, which is due in part to use of a preferred 1.4W body section quadrilateral (Figure 7) . Compare the filament cross section of OMPI Figure 8 with that of Figure 6, for instance, where the spinneret body section width is 2W. Figure 8 reflects more clearly the one-for-one correspondence of the quadrilateral intersections than the filament cross section of Figure 4. The spinneret orifice cross section 136 in Figure 9 has intersecting quadrilaterals 138, 140 with the single wider intersecting quadrilateral 138 also forming a single segment body section and the other single intersecting quadrilateral 140 also forming a single segment wing member. The two segments have an angle therebetween of 90°. The width of the body section quadrilateral is 1.4W while the width of the wing member quadrilateral is W. The extremities of the spinneret orifice cross section are defined by circular bores 142. Figure 10 shows the resulting filament cross section 144 as spun from the spinneret orifice of Figure 9. This filament cross section is in the shape of a single V and has a single wing member 146, which is connected to the body section 148, and a generally convex curve 150 located on the other side of the filament cross section generally opposite radius of curvature (R«) . The spinneret orifice cross section 152 in Figure 11 has intersecting quadrilaterals 154, 156 and 158 with the single wider intersecting quadri¬ lateral 158 forming a single segment body section and the other two intersecting quadrilaterals 154, 156 forming a two segment, single wing member. The angle between the body section and wing member Is 60°. The width of the body section quadrilateral is 1.4W while the width of the wing member quadrilaterals is W. The extremities of the spinneret orifice cross section are defined by circular bores 160°. Figure 12 shows the resulting filament cross section 162 as spun from the spinneret orifice cross section of Figure 11, with the filament cross section having a single wing member 164, which is connected to the body section 166, and a generally convex curve 168 located on the other side of the filament cross section generally opposite the illustrated radius of curvature (R ) . The single wing member 164 has along its periphery a convex curve 170 located generally opposite a concave curve 172. The spinneret orifice cross section 174 in Figure 13 has intersecting quadrilaterals 176, 178, 180 with the single wider intersecting quadrilateral 178 forming a single segment body section and the other single intersecting quadrilaterals 176 and 180 forming two single segment wing members. The angles between the body section and the wing members are, respectively, lOS^ and 90° as illustratred in Figure 13. The width of the body section quadrilateral is 1.4W while the width of the wing member quadri¬ laterals is W. The extremities of the spinneret orifice are defined by circular bores 182. Figure 14 shows the resulting filament cross section 184 as spun from the spinneret orifice cross section of Figure 13 with the filament cross section having two wing members 186, 188, which are con- nected, respectively, to an end of the body section 190, and two generally convex curves 192, 194 each located on the other side of the filament cross section generally opposite one of the ilustrated radius of curvatures (R c ) . Wing member 188 is longer than wing member 186. The spinneret orifice cross section 218 in Figure 15 has intersecting quadrilaterals 220, 222, 224 with the single wider intersecting quadrilateral 222 forming a single segment body section and the other single intersecting quadrilaterals 220 and 224 forming two single segment wing members. The angles between the body section and the wing members are each 120° as illustrated in Figure 15. The width of the body section is 1.4W while the width of the wing member quadrilaterals is W. The extremities of the spinneret orifice are defined by circular bores 226. Figure 16 shows the resulting filament cross section 228, with the filament cross section having two wing members 230, 232, which are connected, respectively, to an end of the body section 234, and two generally convex curves 236, 238, each located on the other side of the filament cross section gen¬ erally opposite one of the Ilustrated radius of curvatures (Rp) . The spinneret orifice cross section 308 in Figure 17 has intersecting quadrilaterals 310, 312, 314, 316, 318, 320, with the single wider intersect¬ ing quadrilateral 312 forming a single segment body section and the other intersecting quadrilaterals 310 and 314, 316, 318, 320 forming, respectively, a single segment wing member (310) and a four segment wing member (314, 316, 318, 320). The angles between the body section and the wing members are each 60°, as illustrated in Figure 17, and the angles between the segments of four segment wing member are each 60°, as also illustrated. The width of the body section is 1.4W while the width of the wing member quadrilaterals is W. The extremities of the spin¬ neret orifice are defined by circular bores 322. Figure 18 shows the resulting filament cross section 324, as spun from the spinneret orifice cross section of Figure 18, with the filament cross section having two wing members 326, 328, which are con¬ nected, respectively, to an end of the body section 330, and two generally convex curves 332, 334, each located on the other side of the filament cross section generally opposite one of the ilustrated radius of curvatures (R c ) • The quadri-segmentation of the wing member 328 results in the formation of additional convex curves, each of which is located on the other side of the filament cross section generally opposite, respectively, of concave curves 342, 344, 346. The convex and concave curves mentioned alternate also around the periphery of the filament cross section forming a series of connected V shapes. The spinneret orifice cross section 370 in Figure 19 has intersecting quadrilaterals 372, 374, 376, 378, with the two wider intersecting quadri¬ laterals 374, 376 forming a dual segment body section and the other intersecting quadrilaterals 372 and 378 forming, respectively, two single segment wing members. The angle between the body section and each wing member is 60°, as illustrated in Figure 19, and the angle between the two segments of the body section is 60°, as also illustrated. The width of the body section is 1.4W while the width of the wing member quadrilaterals is W. The extremities of the spinneret orifice are defined by circular bores 380. Figure 20 shows the resulting filament cross section 382, as spun from the spinneret orifice cross section shown in Figure 19, with the filament cross section having two single segment wing members 384, 386, which are connected, respectively, to an end of the body section 388, and two generally convex curves 390, 392, each located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R c ) . The dual segmentation of the body section 388 also results in the formation of an additional convex curve or central convex curve 394 located on the other side of the filament cross section general- ly opposite central concave curve 396. The convex and concave curves mentioned alternate around the periphery of the filament cross section. OMPI The spinneret orifice cross section 490 in Figure 21 has intersecting quadrilaterals 492, 494, 496, 498, 500, 502, 504,.506, with the two wider intersecting quadrilaterals 498, 500 forming a dual segment body section and the other intersecting quadrilaterals 492, 494, 496 and 502, 504, 506 forming, respectively, two tri-segment wing members. The angle between the body section and each wing member is 90°, as illustrated in Figure 21, the angle between the dual segment body section is 90°; and the angle between the each of the wing member quadri¬ laterals is 90°. The width of the body section is 1.4W while the width of the wing member quadri¬ laterals is W. The extremities of the spinneret orifice are defined by circular bores 508. Figure 2 ' 2 shows the resulting filament cross section 510, as spun from the spinneret orifice cross section shown in Figure 21, with the filament cross section having two tri-segment wing members 512, 514, which are connected, respectively, to an end of the body section 516, and two generally convex curves 518, 520, each located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R c ) . The dual segmentation of the body section results in the formation of an additional convex curve or central convex curve 522 located on the other side of the filament cross section generally opposite central concave curve 524; the tri-segmenta- tion of wing members results in the formation of additional convex curves 526, 528, 530, 532 located on the other side of the filament cross section generally opposite, respectively, concave curves 534, 536, 538, 540. The convex and concave curves mentioned alternate around the periphery of the filament cross section. The spinneret orifice cross section 542 in Figure 23 has intersecting quadrilaterals 544, 546, 548, 550, 552, 554, 556, 558, with the two wider intersecting quadrilaterals 550, 552 forming a dual segment body section and the other intersecting quadrilaterals 544, 546, 548 and 554, 556, 558 forming, respectively, two tri-segment wing members. The angle between the body section and each wing member is 50°; and the angle between the each of the wing member quadrilaterals is 50°. The width of the body section Is 2W while the width of the wing member quadrilaterals is W. The extremities of the spin¬ neret orifice are defined by circular bores 560. Figure 24 shows the resulting filament cross section 562, as spun from the spinneret orifice cross section shown in Figure 23, with the filament cross section having two tri-segment wing members 564, 566, which are connected, respectively, to an end of the body section 568, and two generally convex curves 570, 572, each located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R ) . The spinneret orifice cross section 594 in Figure 25 has intersecting quadrilaterals 596, 598, 600, 602, 604, 606, 608, 610, 612, with the two wider intersecting quadrilaterals 602, 604 forming a dual segment body section; intersecting quadrilaterals 596, 598, 600 forming a tri-segment wing member; and intersecting quadrilaterals 606, 608, 610, 612 forming a quadri-segment wing member. The angle between the body section and each wing member is 60°, as illustrated in Figure 25; and the angle between each of the segments of the wing members is also 60°. The width of the body section Is 1.4W while the width of the wing member quadrilaterals is W. The extremities of the spinneret orifice are defined by circular bores 614. Figure 26 shows the resulting filament cross section 616, as spun from the spinneret orifice cross section shown in Figure 25, with the filament cross section having a tri-segment wing member 618 and a quadri-segment wing member 620, which are connected, respectively, to an end of the body section 622, and two generally convex curves 624, 626, each located on the other side of the filament cross section general¬ ly opposite one of the illustrated radius of curva- tures ( c ) . The dual segmentation of the body section results in the formation of an additional convex curve or central convex curve 628 located on the other side of the filament cross section generally opposite central concave curve 630; the tri-segmenta- tion of wing member 618 results in the formation of additional convex curves 632, 634 located on the other side of the filament cross section generally opposite, respectively, concave curves 636, 638; and the quadrisegmentation of wing member 620 results in the formation of additional convex curves 640, 642, 644 located on the other side of the filament cross section generally opposite, respectively, concave curves 646, 648, 650. The convex and concave curves mentioned alternate around the periphery of the filament cross section. The spinneret orifice cross section 710 in Figure 27 has tapered intersecting quadrilaterals 712, 714, 716, 718, 720, 722, with the two wider tapered intersecting quadrilaterals 716, 718 forming a dual segment body section; and tapered intersecting quadrilaterals 712, 714 and 720, 722 forming, respec¬ tively, two dual segment wing members. The angle between the body section and each wing member is 75°, and the angle between wing member segments is 90°, as illustrated in Figure 27. The width of the body section at its widest point is 1.4W while the width of the wing member quadrilaterals at their corres¬ ponding widest point is W. The extremities of the spinneret orifice cross section are defined by circular bores 724. Figure 28 shows the resulting filament cross section 726, as spun fron the spinneret orifice cross section shown in Figure 27, with the filament cross section having, respectively, dual segment wing members 728, 730, which are each connected to an end of the body section 732, and two generally convex curves 734, 736, each located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R ) . The dual segmentation of the body section results in the formation of an additional convex curve or central convex curve 738 located on the other side of the filament cross section generally opposite central concave curve 740; and the dual segmentation of the wing members 728, 730 results in the formation of additional convex curves 742, 744 located on the other side of the filament cross section generally opposite, respectively, concave curves 746, 748. The convex and concave curves mentioned alternate around the periphery of the filament cross section. The spinneret orifice cross section 750 in Figure 29 has intersecting quadrilaterals 752, 754, 756, 758, with the three wider intersecting quadri¬ laterals 754, 756, 758 forming a tri-segment body section; and intersecting quadrilaterial 754 forming a single segment wing member. The angle between the body section and the wing member is 60°; the angle between each segment of the body section is 60°, as illustrated in Figure 29. The width of the body section is 1.4W while the width of the wing members is W. The extremities of the spinneret orifice are defined by circular bores 760. OMPI > Figure 30 shows the resulting filament cross section 762, as spun from the spinneret orifice cross section shown in Figure 29, with the filament cross section having a single-segment wing member 764 connected to an end of the tri-segment body section 766, and a single generally convex curve 768 located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R ) . The tri-segmentation of the body section results in the formation of additional convex curves or central convex curves 770, 772 located on the other side of the filament cross section generally opposite, respectively, central concave curves 774, 776. The convex and concave curves mentioned alter¬ nate around the periphery of the filament cross section. The spinneret orifice cross section 918 in Figure 31 has intersecting quadrilaterals 920, 922, 924, 926, 928, 930, 932, 934, 936, 938, 940, 942, 944, 946 with the four wider intersecting quadri¬ laterals 920, 922, 924, 926, 928 and 938, 940, 942, 944, 946 forming respectively, two quinti-segment wing members. The angle between the body section and each wing member is 40°; the angles between the wing member segments (starting to the left of Figure 19) for each wing member are, respectively, 60°, 60°, 50°, 45° and 45°, 50°, 60°, 60°; and the angles between the body section segments are 30°, as illus- trated in Figure 31. The width of the body section is 1.4W while the width of the wing members is W. The extremities of the spinneret orifice are defined by circular bores 948. Figure 32 shows the resulting filament cross section 950, as spun from the spinneret orifice cross section shown in Figure 31, with the filament cross section having quinti-segment wing members 952, 954, each connected to an end of the quadri-segment body section 956, and two generally convex curves 958, 960 located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R . The quadri-segmentation of the body section results in the formation of additional convex curves or central convex curves 962, 964, 966 located on the other side of the filament cross section generally opposite, respectively, central concave curves 968, 970, 972; and the quinti-segmentation of each of the wing members results in the formation of additional convex curves 974, 976, 978, 980, 982, 984, 986, 988 located on the other side of the filament cross section generally opposite, respectively, concave curves 990, 992, 994, 996, 998, 1000, 1002, 1004. The convex and concave curves mentioned alternate around the periphery of the filament cross section. The spinneret orifice cross section 1006 in Figure 33 has intersecting quadrilaterals 1008, 1010, 1012, 1014, 1016, 1018, 1020, 1022, 1024, 1026, with the wider intersecting quadrilaterals 1016, 1018 forming a dual segment body section, and intersecting quadrilaterals 1008, 1010, 1012, 1014 and 1020, 1022, 1024, 1026 forming, respectively, two quadri-segment wing members. The angle between the body section and each wing member is 90°; and the angles between the segments of the wing members are each 90°, as illus¬ trated in Figure 33. The width of the body section is 1.4W while the width of the wing members is W. The extremities of the spinneret orifice are defined by circular bores 1028. Figure 34 shows the resulting filament cross section 1030, as spun from the spinneret orifice cross section shown in Figure 34, with the filament cross section having quadri-segment wing members 1032, 1034, each connected to an end of the dual segment body section 1036, and two generally convex curves 1038, 1040 located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R c ) . The dual segmentation of the body section results in the formation of an additional convex curve or central convex curve 1042 located on the other side of the filament cross section generally opposite concave curve 1044, and the shouldered formation of the body section adjacent the connection of each wing member results in the formation of further additional convex curves 1046, 1048 and 1050, 1052, as illustrated in Figure 22. As further illustrated, the quadri-segmentation of the wing members results in the formation of additional convex curves 1054, 1056, 1058, 1060 located on the other side of the filament cross section generally opposite, respectively, concave curves 1062, 1064, 1066, 1068. The convex and concave curves mentioned alternate around the periphery of the filament cross section. The spinneret orifice cross section 1070 in Figure 35 has intersecting quadrilaterals 1072, 1074, 1076, 1078, 1080, 1082, 1084, 1086, 1088, 1090, 1092, 1094, 1096, 1098, 1100, 1102, 1104, 1106, 1108. The three wider intersecting quadrilaterals 1080, 1082, 1100 form a tri-segment body section. Intersecting quadrilaterals 1071, 1073, 1076, 1078; 1084, 1086, 1088, 1090; 1092, 1094, 1096, 1098; and 1102, 1104, 1106, 1108 form, respectively, first, second, third, fourth or four quadri-segment wing members. The angle between the body section and each of the first and third wing members is 120°, and the angle between the body section and each of the second and fourth wing members is 60°, as illustrated in Figure 35. The angle between each of the body section segments is 60°; and the angles between the segments of each OMPI wing member are from the body section toward the outer extremity, respectively, 120°, 60°, and 60°. The width of the body section is 1.4W while the width of the wing members is W. The extremities of the spinneret orifice are defined by circular bores 1110. Figure 36 shows the resulting filament cross section 1112, as spun from the spinneret orifice cross section shown in Figure 35, with the filament cross section having quadri-segment wing members 1114, 1116, 1118, 1120, each connected to an end of the trisegment body section 1122, and four generally convex curves 1124, 1126, 1128, 1130 located on the other side of the filament cross section generally opposite one of the illustrated radius of curvatures (R c ) • The tri-segmentation of the body section results in the formation of an additional convex curve or central convex curve 1132 located on the other side of the filament cross section generally opposite central concave curve 1134. There is at least one other concave or central concave curve 1136 which is offset from the other central concave curve, but the convex curve opposite it blends into and with the previously identified convex curve 1130 so that it becomes a matter of choice whether to separately identify it or the convex portion and the latter has already been identified as convex curve 1130 which is located generally opposite one of the radius of curvatures ( c ) . The quadri-segmentation of each of the wing members results in the formation of additonal convex curves 1138, 1140, 1142, 1144, 1146, 1148, 1150 located on the other side of the filament cross section generally opposite, respectively, concave curves 1152, 1154 [which blends into and with the adjacent radius of curvature (R c )], 1156, 1158, 1160, 1162, 1164. The convex and concave curves mentioned alternate around the periphery of the filament cross section. It has been noted from an inspection of yarns comprising filament cross sections of the present invention and of those comprising filament cross sections disclosed in the aforementioned U.S. Patent 4,245,001, that a typical yarn will have many free protruding ends distributed along the surface and throughout the yarn bundle. As mentioned in U.S. Patent 4,245,001, the yarn is coherent due to the entangling and intermingling of neighboring fibers. These free protruding ends are formed as the feed yarn is fed through a fracturing jet as is shown in Figure 20 of the patent. Figure 38 herein shows tracings of a 22.5X enlargement of fibers from one such typical yarn. These single fibers were separated from yarn samples, mounted on transparent sheets for projection, and the projected shadow photographed at 22.5C using a microfilm reader-printer. The filaments 1178 in Figure 38 were traced because the resulting negative photos were not clear enough to be reproduced herein. What- appears to be "hairs" are not broken filaments but rather they represent small segments of fiber wings which have been torn away from the fiber body. The cross sectional shape of the fibers is a necessary condition for the formation of these free protruding ends 1180. In the turbulent violence of the air-jet fracturing process, there are very high stresses concentrated at the intersection of the wing member- body section. These stresses will sometimes cause a wing member to break away from the body section. If such a fracture or crack extends for some length along the fiber and the wing member is ruptured at some point, a free protruding end will result. Figure 39 shows what has been observed to be six classes of fibrils or free protruding ends. In Class A and D the wing member and body section remain intact but have separated from one another along their length. These classes are shown in Figure 38. As disclosed in U.S. Patent 4,245,001, these are known as "bridge loops". These bridge loops 1182 (Figure 39) are visible loops, some of which break to provide the aforementioned free protruding ends 1180 and those that do not break always have the unusual feature that the separated wing member is essentially straight, as shown at 1184, and the body section from which it is separated is curved, as shown at 1186. The separated wing member 1184 is unexpectedly shorter than the body section 1186 from which it is separated. Class D (Figure 39) is distinguished from Class A by the presence of very fine microfibrils 1188.within the loop, some of which may bridge the g a P« The appearance of Class D suggests that the bridge loops begin as microcracks which propagate along the filament. Class D occurs when the Initia¬ tion points are closely spaced, Class A occurs when the initiation points are widely spaced. When the fibers are held under tension, it becomes obvious that there is a significant differ¬ ence in the lengths of the separated wing members and of the body section of the fiber. I have no explana¬ tion for this phenomenon. Rupture of the loaded wing members is distributed randomly over their lengths, giving rise to Classes C and C f . The probability of simple tensile fracture occurring exactly at the end of the loop, as in B and B', is zero. Interestingly, the fibrils of Class B and B 1 seem always to be anchored at the upstream end, as will be noted by the direc¬ tion of the arrows 1190 or rather this appears to be the preferred direction for most of such filament s observed . In summary, therefore, Class A shows a bridge loop 1182 where the loop is intact and there are no microfibril connectors. Class D shows a bridge loop 1182 where the loop is intact and there are microfibril connectors 1188. Class C shows a broken loop having no microfibril connectors. Class C' shows a broken loop having microfibril connectors 1188. Class B shows a simple free protruding and having no microfibril connectors. Class B' shows a simple free protruding end having microfibril con¬ nectors 1188. Examples 1-3 The filaments shown in Figures 4, 6 and 8 were made using the spinning apparatus described in Example 1 of U.S. Patent 4,245,001. The preferred fracturing jet design is a jet using high pressure gaseous fluid to fracture the wings from the filament body and to entangle the filaments making up the yarn bundle as well as distributing uniformly the protruding ends formed by the fracturing operation throughout the yarn bundle and along the surface of the yarn bundle. The yarn is usually overfed slightly through the jet from 0.05% to 5% with 0.5% being especially desirable. A particularly useful fracturing jet (herein called the Nelson jet) is that disclosed in U.S. Patent 4,095,319. In using the jet it is adjusted to give a blowback of 13.79 kpa as determined by the following procedure. A constant 137.9 kpa air source is attached to the air inlet of the jet by a rubber hose. The yarn inlet of the jet is pressed and sealed against a pressure gauge. The threaded member 56 is adjusted until 13.79 kpa is obtained on the pressure gauge. This jet is said to be adjusted to a blowback of 13.79 kpa. The following examples concern the filament cross sections disclosed, respectively, in Figures 4, 6 and 8. Example 1 1. Spinneret has 25 holes each having a spinneret orifice cross section as illustrated in Figure 1. W = 84 microns 2. Extrusion Conditions Polymer: poly(ethylene terephthalate) 0 I.V.: 0.62, 0.3% Ti0 2 Melt temperature: 285°C. As-spun denier: 260 Take-up speed: 3014 meters/minute 170 denier/25 filaments 5 3. Drafting and Fracturing Conditions Draw Ratio: 1.55X Feed roll temperature: 90°C. Slit heaters (2): 240°C. Speed: 600 meters/minute (1% overfeed) o Fracture jets (2): pressure: 3447.5 kpa (0.184 scmm/jet) 4. Fractured Yarn Properties Tenacity: 2.6 grams/denier Elongation: 22% 5 Modulus: 61 grams/denier Boiling water shrinkage: 6.3% Sp. vol. § 0.1 G/D tension: 2.00 cc./gm. Laser |b| : 0.57 Laser j /b1 : 578 0 Laser L+7: 9 The fractured yarn showed no glitter when inspected under specular illumination. Example 2 1. Spinneret has 30 holes, each having a spinneret 5 orifice cross section as illustrated in Figure 3. W •» 84 microns 2. Extrusion Conditions Same as Example 1 except 170 denier/30 filaments. * Drafting and Fracturing Conditions Draw ratio: 1.50X Feed roll temperature: 95°C. Slit heaters (2): 240°C. Speed: 800 meters/minute (1% overfeed) Fracture jets (2): pressure: 3447.5 kpa (0.184 scmm/jet) 4. Fractured Yarn Properties Tenacity: 2.1 grams/denier Elongation: 18% Modulus: 40 grams/denier Boiling water shrinkage: 10% Sp. vol. @ 0.1 G/D tension: 1.85 cc./gm. Laser |b| : 0.65 Laser fa/ | : 425 Laser L+7: 9 % Wing member(s): 23 % Body sections: 77 The fractured yarn showed no glitter when inspected under specular illumination. Example 3 1. Spinneret has 30 holes, each having a spinneret orifice cross section as illustrated in Figure 5. W = 84 microns. 2. Extrusion Conditions Same as Example 1 except 170 denier/30 filaments. 3. Drafting and Fracturing Conditions Draw ratio: 1.48X Feed roll temperature: 85°C. Slit heaters (2): 240°C. Speed: 800 meters/minute (3% overfeed) Fracture jets (2): pressure: 3447.5 kpa (0.184 scmm/jet) 4. Fractured Yarn Properties Tenacity: 1.7 grams/denier Elongation: 14% Modulus: 39 grams/denier Boiling water shrinkage: 8% Sp. vol. @ 0.1 G/D tension: 2.22 cc./gm. Laser |b| : 0.62 Laser |a/b[ : 833 Laser L+7: 4 % Wing member(s): 44 % Body section: 56 The fractured yarn showed no glitter when inspected under specular illumination. In reference to Figure 37, the photomicro¬ graph shows fractured and non-fractured filament cross sections to give a better idea of the locations where fractures occur. Fractures generally occur at the radius of curvature (R c ) where the wing members intersect with the body section. Filament cross section 1166 is an example of one such fractured filament cross section showing one of the wing members 1168 having been fractured o.r separated from the body section 1170. Because of the undulatory type surface of the wing members, fracturing may occur at locations away from the intersections of the body section and wing members, as shown by filament cross section 1172 where a portion of one wing member has been fractured and is shown as missing at 1174. This secondary fracturing, however, usually is a small percentage of the total amount of fracturing observed. Filament cross section 1176 in Figure 37 is an example of a filament cross section where both wing members have fractured from the body section.

Claims: Claims: 1. A filament having a cross section comprising a body section and one or more wing members joined to said body section, said one or more wing members varying up to twice their minimum • thickness along their width and characterized in that at the junction of the body section and said one or more wing members the respective faired surfaces thereof define a radius of concave curvature (R c ) on one side of said cross section and a generally convex curve located on the other side of said cross section generally oposite said radius of concave curvature (R c ) > said body section comprising 25 to 95% of the total mass of the filament and said wing members comprising 5 to 75%, said filament being further characterized by a wing-body interaction (WBI) defined by WBI = (Dmax-Dmm. ) y mm 2 V 3 min where the ratio of the width of said filament cross section to the wing member thickness ( -/D is 1<-30. 2. A filament as defined in claim 1 wherein said filament cross section has two wing members. 3. A filament as defined in claim 1 wherein said filament cross section has two wing members and one of said wing members is nonidentical to the other wing member. 4. A filament as defined in claim 1 wherein the periphery of said body section defines one central convex curve on said one side of the cross section and one central concave curve located on said other side of the cross section generally opposite said at least one central convex curve. 5. A filament as defined in claim 1 wherein the periphery of said body section defines on one side at least one central convex curve and at least one central concave curve connected together, and on the other side at least one central concave curve and at least one central convex curve connected together. 6. A filament as defined in claim 1 wherein said periphery of said body section defines on one side two central convex curves and a central concave curve connected therebetween and on the other side two central concave curves and a central convex curve connected therebetween. 7. A filament as defined in claim 1 wherein said one or more wing members each has along the periphery of its cross section on one side a convex curve joined to a radius of concave curvature and on said other side a concave curve joined to the first-mentioned convex curve opposite said radius of concave curvature. 8. A filament as defined in claim 1 wherein said one or more wing members each has along the periphery of the cross section on one side two or more curves alternating in order of convex to concave with the latter-mentioned convex curve being joined to a radius of concave curvature and on said other side two or more curves alternating in order of concave to convex with the latter-mentioned concave curve being joined to the first-mentioned convex curve opposite said radius of concave curvature. 9. A filament as defined in claim 1 wherein said filament cross section has four wing members and wherein a portion of the periphery of said body section defines on one side thereof at least one central concave curve and on the opposite side thereof at least one central concave curve, each central concave curve being located generally offset from the other. 10. A filament as defined in any preceding claim wherein the portion of each of said wing members at the free edge thereof is of a greater thickness than is the remainder of each of said wing members. 11. A filament as defined in any preceding claim wherein said filament is provided with luster- modifying means. 12. A filament as defined in claim 11 wherein said luster-modifying means is finely dis¬ persed titanium dioxide. 13. A filament as defined in claim 11 wherein said luster-modifying means is finely dis¬ persed kaolin clay. 14. A filament as defined in any preceding claim wherein said filament is comprised of a fiber- forming polyester. 15. A filament as defined in claim 14 wherein said polyester is poly(ethylene terephthal- ate). .16. A filament as defined in claim 14 wherein said polyester is ρoly(l,4-cyclohexylenedi- methylene terephthalate) . 17. A filament as defined in any preceding claim wherein said filament has been oriented such that its elongation to break is less than 50%, and has been heat stabilized to a boiling water shrinkage of <15%. 18. Yarn comprising fractured filaments of claim 1 wherein said yarn is characterized by a denier of 15 or more, a tenacity of 1.1 grams per denier or more, an elongation of 8 percent or more, a modulus of 25 grams per denier or more, a specific volume in cubic centimeters per gram at one tenth gram per denier tension of 1.3 to 3.0, and with a boiling water shrinkage of <15%. gtJRE j OMPI ^ 19. Yarn of claim 18 wherein said yarn has a laser characterization where the absolute b value is at least 0.25, the absolute value of a/b is at least 100 and the L+7 value ranges up to 75. 20. Yarn of claim 19 wherein the absolute b value is 0.6 to 0.9, the absolute a/b value is 500 to 1000; and the L+7 value is 0 to 10. 21. Yarn of claim 18 wherein the absolute b value is 1.3 to 1.7; the absolute a/b value is 700 to 1500; and the L+7 value is 0 to 5. 22. Yarn of claim 18 wherein the absolute b value is 0.3 to 0.6; the absolute a/b value is 1500 to 3000; and the L+7 value is 25 to 75. 23. Yarn of claim 19 wherein the yarn is characterized by a Uster evenness of 6% or less. 24. Yarn comprising fractured filaments of claim 1 and characterized by the yarn being partially oriented. 25. Textile fabric comprising fractured filaments of claim 1.

Inventors: PHILLIPS BOBBY MAL, PHILLIPS, BOBBY, MAL
Applicants: EASTMAN KODAK CO, EASTMAN KODAK COMPANY
Application year: 1983
Main classification: D02G3
IPC codes: D01D5, D01F6, D02G3, D02J3, D03D15, D04B1