Page 55 - Handbook of Properties of Textile and Technical Fibres
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36                              Handbook of Properties of Textile and Technical Fibres


         (a)                      (b)
                                      100
                                                          955  1130
                                                                         1635
                                                           1048  1235  1445
            Intensity               Intensity   515 595           1300
                                                            1060
                                                           1048
                                                        900         1390
                                           335                     1340  1545
                                               465  705  795
                                                  640
            –400 –200  0  200 400    0  200  400  600  800 1000 1200 1400 1600
                Wavenumber/cm –1                   Wavenumber/cm –1
         Figure 2.9 Polarized Raman spectra of PA66 parallel and perpendicular to the fiber axis from
         Marcellan et al. (2004). (a) Low wave number range (collective or squeletal motions). (b)
         Stokes Raman scattering in the 100e1800 cm  1  range.

            A comparison of Raman scattering obtained from fibers drawn to different extents
         shows clearly the rise of peaks at certain frequencies which can therefore be associated
         with crystalline or amorphous regions and in some cases, such as PET, the transforma-
         tion of gauche to transmolecular conformations, aiding crystallinity (Colomban et al.,
         2006).
            As illustrated in Fig. 2.10, by coupling a tensile testing device, Raman spectroscopy
         can be used in-situ to examine changes in the molecular morphology of fibers during
         mechanical loading and in this way can act as a strain measurement device at the
         molecular level. A shift in a peak can be interpreted as showing a varying stress state
         in the fiber. As the various molecular entities react very much like mechanical resona-
         tors, an applied tensile stress will stretch the bond and result in a shift toward lower


          (a)                          (b)
                                                  100.8
             0.8                                  100.4
           Wavenumber shift / cm –1  –0.4         Wavenumber / cm –1  100.0
             0.4
             0.0
            –0.8
                                                   99.6
            –1.2
            –1.6
                    σ
                              –1
                           –3
            –2.0    S  = –2.46 10  cm /MPa         99.2
            –2.4                                   98.8
               0    200  400  600  800               0.0  0.2  0.4  0.6  0.8  1.0
                           /MPa
                      Stress t0                             Relative position
         Figure 2.10 Micro-Raman extensometry applied to polyamide 66 (PA66) fiber from Marcellan
         et al. (2004). (a) Wave number shift plotted as a function of increasing applied stress, showing
         the onset of main crystalline and oriented amorphous chain deformation at an applied stress of
         around 350 MPa. The single fiber was held in a tensile device. (b) Line-scan across a fiber
         diameter of 24 mm for a free-standing PA66 fiber and corresponding micrograph. Raman
         spectra were collected through an optical confocal microscope. Variation of wave number
         reveals that the surface is in compression compared to the core.
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