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合成繊維?再生繊維集合体の圧縮クリープ特性

机译:合成纤维/再生纤维集合体的压缩蠕变特性

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In this study, compressive creep behaviors of staple fiber assemblies made of polyester fibers with heteromorphic section, round section and hollow section, PTT fibers and regenerated fibers such as cupra and lyocell fibers are investigated under two different stress conditions, and results are obtained as follows. (1) Creep deformation ratio of regenerated fiber assembly is larger than that of synthetic fiber assembly for each stress condition within the range of samples used here. (2) Creep deformation ratio of fiber assemblies that have same fineness and same fiber length is compared. For polyester fibers with heteromorphic and round sections, and cupra fiber, the order of magnitude is as follows; (cupra) > (round) > (heteromorphic). For polyester fibers with round and hollow sections, the order is (round) > (hollow). (3) Creep deformation ratio at high stress condition is twice as large as that of low stress condition for fine polyester fiber with hetermorphic section and thick polyester fiber with round and hollow sections. In contrast, creep deformation ratio at high stress is smaller than that of low stress condition for cupra and lyocell fibers with large length. (4) Compressive creep phenomena of staple fiber assembly is expressed by the creep equation derived from non-linear three element model as follows, εt =Y0 ln(vt+1) where, Y0 and v are constants determined by material properties, measurement condition and compressive stress. Y0 value has good correlation with apparent Young′s modulus, number of crimp and crimp ratio, and v value has good correlation with bending rigidity of fiber.
机译:在这项研究中,研究了在两种不同的应力条件下,由具有异形截面,圆形截面和中空截面的聚酯纤维,PTT纤维以及诸如cupra和lyocell纤维的再生纤维制成的短纤维组件的压缩蠕变行为,得出以下结果。 (1)在此处使用的样品范围内,每种应力条件下再生纤维组件的蠕变变形率均大于合成纤维组件的蠕变变形率。 (2)比较具有相同细度和相同纤维长度的纤维组件的蠕变变形率。对于具有异形和圆形截面的聚酯纤维以及铜氨纤维,量级如下: (cupra)>(round)>(heteromorphic)。对于具有圆形和中空截面的聚酯纤维,顺序为(圆形)>(空心)。 (3)对于具有异形截面的细聚酯纤维和具有圆形和空心截面的粗聚酯纤维,高应力条件下的蠕变变形率是低应力条件下的蠕变变形率的两倍。相反,对于长长度的铜氨和莱赛尔纤维,高应力下的蠕变变形率小于低应力条件下的蠕变变形率。 (4)短纤维组件的压缩蠕变现象由非线性三元模型的蠕变方程表示,如下:ε t = Y 0 ln(vt + 1)其中,Y 0 和v是由材料特性,测量条件和压应力确定的常数。 Y 0 值与表观杨氏模量,卷曲数和卷曲比具有良好的相关性,而v值与纤维的抗弯刚度具有良好的相关性。

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