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Engineering properties of spider silk                             203

           Techniques for the computation of the relaxation spectra from experimental data were
           suggested by Hopkins (Hopkins and Hamming, 1957; Hopkins, 1961, 1963) and
           Meluch (1974). Tobolsky (1960) used relaxation spectra to relate relaxation and
           dynamic response of textile fibers.
              The criteria used in this study for selection of a spectrum is that they will make G(t)
           and J(t) compatible with experimental observations. In particular, the spectrum of
           relaxation times should reflect the frequency insensitivity in the dynamic response,
           that is to say, S(s) should be nearly constant over a wide range of frequency.
              For this study, a spectrum first introduced by Becker (1925) is used:

                     c
               SðsÞ¼    for s 1 < s < s 2                                 (6.16)
                     s
           where C is a constant and (s) is the relaxation time in the interval [s 1 , s 2 ].



           6.3.3.4  Computation methods

           By substitution of Eq. (6.16), Eqs. (6.13)e(6.15) can be reduced to the following
           computational forms:


                              t        t
                     1 þ E 1       E 1
                              s 2      s 1
               GðtÞ¼                                                      (6.17)
                                   s 1
                         1 þ C ln
                                   s 2
                                  t            t

                     1   C E 1           E 2
                               C þ s 2      C þ s 1
                JðtÞ¼                                                     (6.18)
                                     C þ s 2
                              1   Cln
                                     C þ s 1
                             
     2 2     
    2 2  	      1           1
                     1 þ :5C  1 þ u s 2    ln 1 þ u s 1  þ i tan  ðus 2 Þ  tan  ðus 1 Þ
              MðuÞ¼
                                                    s 2
                                             1 þ ln
                                                    s 1
                                                                          (6.19)

           where E l (z) is the exponential integral
                       Z  N  t
                           e
               E 1 ðZÞ¼       dt                                          (6.20)
                        Z   t
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