Page 366 - Biosystems Engineering
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Food Package Engineering      343

                                    2
               where  J = flux, mol/cm s
                     D = diffusion coefficient, cm /s
                                             2
                     c = concentration of water vapor or gas, mol/cm 3
                     x = film thickness, cm
               It is convenient to measure vapor pressure (p) than measure the actual
               concentration of gas or vapor. Under steady-state conditions, Eq. (11.1)
               can be integrated across the total thickness of the polymer film and
               vapor pressure across the film [Eq. (11.2)]:
                                             Δ
                                      Q   PA p
                                        =                            (11.2)
                                       t    x
               where Q = amount of gas or water vapor, cm 3
                      t = time, s
                                              2
                                       3
                      P = permeability cm  cm/cm  s atm
               Over 30 different units for P are reported in the literature. Some of
                                                          2
               the common units of permeability are cm  cm/cm  s Pa, mL mm/m 2
                                                  3
               day kPa, and mL cm/m  day atm. Equation (11.2) assumes (1)
                                      2
               steady-state diffusion, (2) a linear concentration gradient across the
               film, (3) unidirectional diffusion, and (4) permeability independent
               of concentration.
                   Unsteady-state transport of water vapor or gas through poly-
               meric film is described using Fick’s second law [Eq. (11.3)]:
                                        ∂ 2 c  dc
                                      D    =                         (11.3)
                                        dx 2  dt
               where t is time (s).
                   The permeability of a polymer is affected by the nature of the
               polymer, the nature of the gas or water vapor, and ambient condi-
               tions. The barrier properties of a polymer’s gas and vapor is increased
               with the increasing polarity of certain types of polymer, regularity of
               molecular structure, and close chain-to-chain packing in the polymer
               matrix. Crystalline polymers have lower gas permeability than amor-
               phous polymers.  Permeability (diffusivity × solubility) also depends
                             8
               on the molecular size of the gas and its chemical affinity to the poly-
               mer. Larger gas molecules generally have lower diffusivity and higher
               solubility compared to smaller molecules. Temperature and relative
               humidity also affect a gas’s permeability.
                   Many methods are used for measurement of water vapor and gas
               permeability of polymer-based packaging.  One method is based on
                                                   1,2
               the permeation rate equation [see Eq. (11.2)]. Quantity of water vapor
               (Q) transferred through a film is measured using a precision balance,
               whereas a sensitive detector is used in a permeation cell to quantify
               the amount of gas transfer. The exposed surface area (A) of the poly-
               mer film is accurately defined by the opening in the permeation
               cell. The pressure difference (Δp) across the film is controlled by the
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