Poly(lactic acid). Группа авторов
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Название: Poly(lactic acid)

Автор: Группа авторов

Издательство: John Wiley & Sons Limited

Жанр: Химия

Серия:

isbn: 9781119767466

isbn:

СКАЧАТЬ model from the α (α) form to the β form. The set of arrays A, B and A slip along the 110 planes.

      Source: Modified from the reference [20]. Reproduced from Wang et al., Macromolecules 2017, 44, 3285–3300.

      (c) The change of the X‐ray coherent domain size in the transition process from the α to δ to β forms.

      PLLA α form

      Elastic constants matrix,

c left-parenthesis upper G upper P a right-parenthesis equals Start 6 By 6 Matrix 1st Row 1st Column 2.50 2nd Column 6.48 3rd Column 7.15 4th Column 0.00 5th Column negative 1.45 6th Column 0.00 2nd Row 1st Column 6.48 2nd Column 12.38 3rd Column 9.07 4th Column 0.00 5th Column 2.28 6th Column 0.00 3rd Row 1st Column 7.15 2nd Column 9.07 3rd Column 17.87 4th Column 0.00 5th Column 3.98 6th Column 0.00 4th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 15.03 5th Column 0.00 6th Column 3.18 5th Row 1st Column negative 1.45 2nd Column 2.28 3rd Column 3.98 4th Column 0.00 5th Column 0.21 6th Column 0.00 6th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 3.18 5th Column 0.00 6th Column 3.90 EndMatrix s left-parenthesis upper G upper P a Superscript negative 1 Baseline right-parenthesis equals Start 6 By 6 Matrix 1st Row 1st Column 0.08 2nd Column negative 0.02 3rd Column 0.06 4th Column 0.00 5th Column negative 0.35 6th Column 0.00 2nd Row 1st Column negative 0.02 2nd Column 0.13 3rd Column negative 0.09 4th Column 0.00 5th Column 0.12 6th Column 0.00 3rd Row 1st Column 0.06 2nd Column negative 0.09 3rd Column 0.07 4th Column 0.00 5th Column 0.04 6th Column 0.00 4th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 0.08 5th Column 0.00 6th Column negative 0.07 5th Row 1st Column negative 0.35 2nd Column 0.12 3rd Column 0.04 4th Column 0.00 5th Column 0.16 6th Column 0.00 6th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column negative 0.07 5th Column 0.00 6th Column 0.31 EndMatrix

      PLLA δ form

c left-parenthesis upper G upper P a right-parenthesis equals Start 6 By 6 Matrix 1st Row 1st Column 3.52 2nd Column 3.26 3rd Column 6.49 4th Column 0.02 5th Column negative 0.88 6th Column negative 0.18 2nd Row 1st Column 3.26 2nd Column 10.53 3rd Column 9.21 4th Column negative 0.35 5th Column negative 2.05 6th Column 2.81 3rd Row 1st Column 6.49 2nd Column 9.21 3rd Column 24.72 4th Column 2.64 5th Column 0.53 6th Column negative 13.16 4th Row 1st Column 0.02 2nd Column negative 0.35 3rd Column 1.04 4th Column negative 0.61 5th Column 0.15 6th Column 1.89 5th Row 1st Column negative 0.88 2nd Column negative 2.05 3rd Column 0.53 4th Column 0.15 5th Column 2.78 6th Column negative 1.17 6th Row 1st Column negative 0.18 2nd Column 2.81 3rd Column negative 13.16 4th Column 4.89 5th Column negative 1.17 6th Column 1.25 EndMatrix s left-parenthesis upper G upper P a Superscript negative 1 Baseline right-parenthesis equals Start 6 By 6 Matrix 1st Row 1st Column 0.63 2nd Column negative 0.05 3rd Column negative 0.13 4th Column negative 0.26 5th Column 0.20 6th Column 0.00 2nd Row 1st Column negative 0.05 2nd Column 0.16 3rd Column negative 0.04 4th Column negative 0.17 5th Column 0.12 6th Column 0.00 3rd Row 1st Column negative 0.13 2nd Column negative 0.04 3rd Column 0.08 4th Column 0.21 5th Column negative 0.10 6th Column 0.00 4th Row 1st Column negative 0.26 2nd Column negative 0.17 3rd Column 0.21 4th Column 0.55 5th Column negative 0.19 6th Column 0.20 5th Row 1st Column 0.20 2nd Column 0.12 3rd Column negative 0.10 4th Column negative 0.19 5th Column 0.54 6th Column 0.00 6th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 0.20 5th Column 0.00 6th Column 0.02 EndMatrix

      PLLA β form

c left-parenthesis upper G upper P a right-parenthesis equals Start 6 By 6 Matrix 1st Row 1st Column 7.63 2nd Column 5.06 3rd Column 5.38 4th Column 0.34 5th Column 0.14 6th Column negative 0.95 2nd Row 1st Column 0.00 2nd Column 6.09 3rd Column 2.71 4th Column 0.46 5th Column negative 1.08 6th Column 1.59 3rd Row 1st Column 0.00 2nd Column 0.00 3rd Column 18.37 4th Column 0.87 5th Column negative 2.42 6th Column 0.66 4th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 1.21 5th Column negative 0.77 6th Column 0.45 5th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 0.00 5th Column 1.28 6th Column 0.32 6th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 0.00 5th Column 0.00 6th Column 1.25 EndMatrix s left-parenthesis upper G upper P a Superscript minus negative 1 Baseline right-parenthesis equals Start 6 By 6 Matrix 1st Row 1st Column 0.081 2nd Column 0.015 3rd Column negative 0.004 4th Column 0.175 5th Column 0.167 6th Column negative 0.249 2nd Row 1st Column 0.00 2nd Column 0.089 3rd Column negative 0.043 4th Column negative 0.231 5th Column negative 0.208 6th Column 0.24 3rd Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.065 4th Column negative 0.045 5th Column 0.034 6th Column 0.100 4th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 0.919 5th Column 0.188 6th Column 0.578 5th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 0.00 5th Column 0.621 6th Column 0.578 6th Row 1st Column 0.00 2nd Column 0.00 3rd Column 0.00 4th Column 0.20 5th Column 0.00 6th Column 0.019 EndMatrix

      The calculated Young’s moduli along the c‐axis (E c = 1/s 33) are compared among the α, δ, and β forms, as shown below:

       α form: E c = 14.7 GPa [66] (X‐ray observed 13.76 GPa [66, 73])

       δ form: E c = 12.5 GPa [66] (X‐ray observed 12.58 GPa [66])

       β form: E c = 15.4 GPa [20]

      The experimental evaluation of the Young’s modulus of the crystal lattice along the chain axis, which is often called the crystallite modulus, was performed using the X‐ray diffraction method [67], where the crystalline strain along the chain axis was measured under constant tensile stresses by assuming the stress working on the crystalline region was equal to the stress of the bulk sample (the assumption of homogeneous stress distribution) [67, 72]. The agreement between the observed and calculated values is relatively good. The crystallite modulus changes depending on the conformational regularity of the PLLA chain: the mesophase (6.7 GPa) < the δ form (12.9 GPa) < the α form (14.7 GPa) < the β form (15.4 GPa). For reference, the X‐ray‐measured crystallite modulus of PLLA/PDLA stereocomplex is 20 GPa, in which the PLLA or PDLA chain takes a 3/1 helical conformation similar to that of the β form [73].

      The crystallite modulus changes depending on the mechanical deformation mechanism of the molecular chain, i.e., the degree of change in the internal coordinates (bond lengths, bond angles, and torsional angles) induced by the external force [67–71]. For example, a planar‐zigzag polyethylene chain is deformed by the stretching of C─C bonds and the deformation of C─C─C bond angles, resulting in a Young’s modulus of 300 GPa [67, 69]. The deformation of a helical chain is induced mainly by the change of the torsional angles, giving 1–2 order lower modulus. The deformation of PLLA helical chains also occurs through the torsional angles around the skeletal C─C and C─O bonds. The disordered chain is more easily deformed due to the easier torsional angle changes. In addition, the methyl groups jutting from the main chain significantly increase the effective cross‐sectional area of the chain. The synergetic effect of these two factors results in the above‐mentioned order of the modulus among the meso, δ, α, and β forms. The crystallite modulus of PLLA chain (in the order of 15 GPa) is lower than those of isotactic polypropylene (34 GPa) and polyoxymethylene (70 GPa) [66, 70], which can be understood from the difference of the chain conformation; the latter two polymers have a tighter and more rigid helical conformation than the PLA chain.

      The anisotropic mechanical property is also important. The Young’s modulus in the plane perpendicular to the chain axis is governed mainly by the H…H interatomic interactions СКАЧАТЬ