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               620                                                                                  Polymer Processing


               molecules there is some evidence that the following rela-  where R is the gas law constant, T 0  is the reference tem-
               tions hold:                                       perature, and  E  is the flow activation energy. Typical
                                                                 values of  E /R  for low-density polyethylene (LDPE),
                                                 ¯ 13.0
                          ¯ 6.8
                    η 0  ∝  M  (M > M c )    1,0  ∝  M  .  (23)
                           w                      w              high-density  polyethylene  (HDPE),  and  polypropylene
                                                                                                           3
                                                                                3
                                                                                            3
               In addition to the dependence of the magnitude of η 0  and  (PP) are 4.5 × 10 K, 2.83 × 10 K, and 5.14 × 10 K,
                 1,0  on  M w , the onset of shear-thinning behavior is af-  respectively. The flow curves shown in Fig. 4 for LDPE
               fected by M. As M increases, the onset of shear thinning  measured at various temperatures have the same shape.
               moves to lower shear rates. An increase in the breadth of  Because  of  this  they  can  be  reduced  to  a  single  mas-
               the molar mass distribution will also cause shear thinning  ter curve plotting the viscosity in reduced form (i.e., η r
               to occur at lower shear rates.                    versus  ˙γ r ) where  ˙γ r  = a T  ˙γ  and η r  = η/a T  and where a T
                 The melt flow index (MI) is commonly used in the poly-  is called the shift factor and is basically η 0 (T )/η 0 (T 0 ).
               olefin industry to distinguish between polymers of differ-  This shifting of viscosity to a master curve is reflective
               ent molar mass. A schematic of an MI device is shown in  of the principle of time–temperature superposition. This
               Fig. 13. A known weight is applied to a plunger, which  principle is based on the concept that at elevated temper-
               pushes polymer melt through a capillary of specified di-  atures the relaxation processes associated with changes
               mensions  (American  Society  for  Testing  of  Materials,  in  chain  conformation  are  much  faster  and  hence  the
               ASTM, specifications). The mass of polymer leaving the  molecule  can  respond  to  higher  deformation  rates.  At
               capillary over a 10-min period is collected and weighed.  low  temperatures  the  relaxation  processes  are  retarded
               Hence, 1.0 MI polymer means that 1 g of polymer was col-  and the molecule can respond to only low deformation
               lected in 10 min. The higher the MI, the lower the molar  rates.
               mass.
                                                                 III.  THERMAL PHYSICAL PROPERTIES
               G.  Effect of Temperature
                                                                 The thermal material properties that are pertinent to the
               The viscosity of homogeneous polymer melts is known to
                                                                 processing  of  polymers  are  the  density  ρ,  the  constant
               depend on temperature in a well-defined manner given by
               the following expression:                         pressure  heat  capacity  C p , (note:  when  ρ  is  constant
                                                                 C p  ≈ C v , the constant volume heat capacity), and the ther-

                                       E   1    1                mal conductivity k. Representative thermal properties for
                       η(T ) = η(T 0 ) exp   −      ,    (24)
                                       R   T    T 0              an amorphous polymer, in this case polycarbonate, are
                                                                 shown in Fig. 14 as a function of temperature. Here it
                                                                 is observed that all the quantities except C p  change con-
                                                                                                           ◦
                                                                 tinuously with increasing temperature. At about 153 C, a
                                                                 discontinuity in C p  is associated with the glass transition























               FIGURE  13  Melt  flow  index  device.  [From  Baird,  D.  G.,  and  FIGURE 14  Thermal physical properties of an amorphous poly-
               Collias, D. I. (1998). “Polymer Processing: Principles and Design,”  mer, polycarbonate. [From Baird, D. G., and Collias, D. I. (1998).
               Wiley, New York.]                                 “Polymer Processing: Principles and Design,” Wiley, New York.]
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