Page 68 - Handbook of Properties of Textile and Technical Fibres
P. 68

Testing and characterization of fibers                              49

           with U 1 the transverse displacement (mm), F the applied load normalized by the
                                 1
           compressed length (N mm ), and R the fiber radius (mm).

           2.4.3  Four-point bending technique to determine compressive
                  properties

           A four-point bending beam method has been used to determine the compressive prop-
           erties of several different types of fiber. Raman spectroscopy has been used to follow
           the molecular deformation of aramid, carbon, and alumina-zirconia fibers (Young
           et al., 1996). Certain Raman bands have been found to be sensitive to the applied stress
           and shift to lower frequencies under tension and to higher frequencies on compression
           (Andrews et al., 1996; Vlattas and Galiotis, 1994). This behavior reflects the deforma-
           tion of the polymer backbones or other atomic bonds in response to the applied stress.
           It is necessary to know the Raman band shift as a function of stress of the fiber so that a
           stressestrain curve can be determined (Colomban, 2002). The fiber to be studied is
           placed on the surface of a rectangular polymethyl methacrylate (PMMA) beam and
           covered with a solution of PMMA/chloroform to seal it into the surface. The beam
           is loaded in four-point bending, and the strain gauges measure the strain of the concave
           surface. As described previously in Section 2.3.4, the shift in frequency of the Raman
           peak then gives a direct measurement of the strain of the fiber at the molecular level.


           2.4.4  Elastica loop test
           The loop test was originally described for obtaining the tensile properties of fibers
           (Sinclair, 1950; Jones and Johnson, 1971). However, in this type of test, most organic
           fibers will yield in compression by developing shear bands known as kink bands. The
           fiber is twisted into a loop and the size of the loop reduced until the first kink band is
           observed at the bottom of the loop where the radius of curvature is smallest. Fig. 2.19
           shows the experimental arrangement as described by Fidan et al. (1993). The test is
           usually conducted under a microscope with the fiber specimen positioned in an oil
           film, to aid observation, between two glass slides or in an SEM. When the first kink
           band is observed the loop size is recorded and the radius of curvature measured or
           calculated so as to obtain the critical compressive strain ε cr , which is given by:

                                                                          (2.19)
               ε cr ¼ d=2R m
                                             y


                                   MT                 MT
                        T                                        T
                    Y                          Rm        L

                                                                      x
           Figure 2.19 Elastica loop test. The fiber is twisted into a loop that is reduced in diameter until
           the plastic deformation or failure occurs.
   63   64   65   66   67   68   69   70   71   72   73