Abstract
Polymer dissolution is an important phenomenon in polymer science and engineering that has found applications in areas like microlithography, controlled drug delivery, and plastics recycling. This review focuses on the modeling efforts to understand the physics of the dissolution mechanism of glassy polymers. A brief review of the experimentally observed dissolution behavior is presented, thus motivating the modeling of the mechanism of dissolution. The main modeling contributions have been classified into four broad approaches — phenomenological models and Fickian equations, external mass transfer-control based models, stress relaxation models, and anomalous transport models and scaling law-based approaches. Another approach discussed is the appropriate accommodation of molecular theories in a continuum framework. The underlying principles and the important features of each approach are discussed in depth. Details of the important models and their corresponding predictions are provided. Experimental results seem to be qualitatively consistent with the present picture.
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Abbreviations
- A:
-
Constant of Eq. (71) dependent on polymer molecular weight, solvent viscosity and temperature
- a:
-
Primitive path step length
- ad :
-
Exponent in the free volume diffusivity model, Eq. (69)
- B:
-
Constant of Eq. (77) dependent on polymer molecular weight, solvent viscosity and temperature
- b:
-
Bond length
- bi :
-
Body force of component i
- c:
-
Polymer mass concentration
- D:
-
Macroscopic diffusion coefficient
- Dcoop :
-
Cooperative diffusion coefficient
- Dp :
-
Stokes-Einstein diffusion coefficient
- DR :
-
Rouse diffusion coefficient
- Dself :
-
Self diffusion coefficient
- D0 :
-
Preexponential factor in free volume diffusivity model, Eq. (69)
- D1 :
-
Free volume diffusion coefficient
- D12 :
-
Mutual diffusion coefficient
- D2 :
-
Reptation diffusion coefficient
- E:
-
Modulus in Maxwell element
- F:
-
Deformation gradient tensor
- F(t):
-
Fraction of polymer present in original tube
- fg :
-
Free volume fraction of polymer
- f1 :
-
Numerical factor for the diffusion coefficient of solvent in polymer, Eq. (1)
- f2 :
-
Numerical factor for diffusion coefficient of dissolved polymer in liquid solution, Eq. (2)
- ΔG:
-
Total change in Gibbs free energy
- ΔGE :
-
Change in Gibbs free energy due to elastic expansion
- ΔGM :
-
Change in Gibbs free energy due to mixing
- ΔG ORseg :
-
Orientational contribution to the Gibbs free energy of a segment
- g:
-
Volume fraction of polymer in an entanglement subunit
- ΔH:
-
Enthalpy change during elastic expansion
- ji :
-
Diffusional flux of component i
- K:
-
Parameter of kinetic model for glass transition, Eq. (21)
- k:
-
Boltzmann constant
- kd :
-
Disentanglement rate
- k1 :
-
Mass transfer coefficient
- L:
-
Parameter of Eq. (32) dependent on c (or π)
- L(t):
-
Average primitive path length
- l:
-
Half thickness of thin polymer slab
- Mc :
-
Critical molecular weight of polymer
- Me :
-
Molecular weight between entanglements
- \(\bar M\) n :
-
Number averaged molecular weight of the polymer
- mp :
-
Mobility of disengaging polymer chain
- Mp,∞ :
-
Maximum mobility of disengaging polymer chain
- N:
-
Number of repeating units
- Ne :
-
Number of moles of entanglements
- n:
-
Parameter of kinetic model for glass transition, Eq. (21)
- ni :
-
Number of moles of component i
- Pe:
-
Peclet number
- p +i :
-
Exchange of linear momentum between components
- R:
-
Position of glassy-rubbery interface
- Rd :
-
Dissolution rate
- Reff :
-
Effective disengagement rate
- R0 :
-
Radius of the polymer particle
- r:
-
Radial position
- rg :
-
Radius of gyration
- S:
-
Position of rubbery-solvent interface
- ΔS:
-
Entropy change
- Sh:
-
Sherwood number
- T:
-
Temperature
- Tg :
-
Glass transition temperature
- t:
-
Time
- td :
-
Disentanglement time
- trep :
-
Reptation time
- UR :
-
Reference velocity scale, Eq. (16)
- U∞ :
-
Velocity of solvent stream
- Vm :
-
Monomer volume
- V1 :
-
Average volume of solvent molecule
- \(\bar V\) :
-
Molar volume of the solvent
- V2 :
-
Average volume of a polymer chain
- \(\bar V\) 2 :
-
Molar volume of the polymer
- v:
-
Local swelling rate of the polymer
- v1 :
-
Convective velocity of the solvent in the x-direction
- x:
-
Position
- \(\bar x\) n :
-
Ratio of polymer molar volume to solvent molar volume
- Z:
-
Number of segments in the primitive path
- α:
-
Isotropic expansion factor
- β:
-
Scaling factor in expression for disentanglement time, Eq. (59)
- γ:
-
Constant for critical stress level, Eq. (48)
- δ:
-
Thickness of diffusion boundary layer
- ε:
-
One-dimensional deformation
- η:
-
Viscosity
- ϑ:
-
Overall dissolution time
- κ:
-
Constant appearing in Eq. (24)
- μi :
-
Chemical potential of component i
- μ 0i :
-
Chemical potential of pure component i
- μ OP1 :
-
Chemical potential of solvent due to osmotic pressure
- μ OR1 :
-
Chemical potential of solvent due to orientational contribution
- νeff :
-
Number of entanglements per polymer chain
- ξ:
-
Distance between entanglements
- π:
-
Osmotic pressure
- ρi :
-
Density of component i
- σ:
-
Stress in the rubbery polymer
- σc :
-
Critical stress for crazing
- σxx :
-
Normal stress component of the stress tensor
- τdif :
-
Characteristic diffusion time
- υd :
-
Equilibrium solubility of polymer in solvent
- υi :
-
Volume fraction of component i
- υ *1 :
-
Critical solvent volume fraction, at which mode of mobility changes
- υ1,eq :
-
Equilibrium solvent volume fraction
- υ1,t :
-
Threshold solvent volume fraction for swelling
- υ2,b :
-
Polymer volume fraction in the bulk liquid
- Φ:
-
Factor that determines the extent of local swelling, Eq. (37)
- χ:
-
Polymer-solvent interaction parameter
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Narasimhan, B., Peppas, N.A. (1997). The physics of polymer dissolution: Modeling approaches and experimental behavior. In: Polymer Analysis Polymer Physics. Advances in Polymer Science, vol 128. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-61218-1_8
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DOI: https://doi.org/10.1007/3-540-61218-1_8
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