| Symbol | Units | Description |
|---|---|---|
| K | temperature | |
| m | depth | |
| W/(m |
liquid-phase (molten-layer) thermal conductivity | |
| kg/m3 | liquid-phase density | |
| kg/mol | monomer molecular weight | |
| kg/mol | polymer molecular weight | |
| s-1 | intrinsic pre-exponential factor for |
|
| J/mol | intrinsic activation energy of beta scission | |
| correction factor to the pre-exponential factor | ||
| J/kg | heat of decomposition reaction | |
| J/kg | latent heat of polymer fusion | |
| J/(mol |
universal gas constant | |
| K | temperature at liquid-gas interface | |
| K | polymer melting point (temperature at solid-liquid interface) | |
| J/(s |
heat flux at liquid-gas interface | |
| m/s | regression rate of the molten polymer surface |
- Uniform in
$y$ ,$z$ directions. 1D steady state treatment. - Decomposition occurs in liquid phase only.
- Regression is due to beta-scission to release monomer.
- Radical initiation reaction is neglected.
- Constant
$k$ , MW,$\rho$ ,$\gamma$ .
An analytical steady-state model for calculating polymer surface regression rate at a given heat flux or surface temperature.
- Regression rate for given heat flux:
- Regression rate for given surface temperature:
where
- Decomposition product: formaldehyde (CH2O)
-
$k$ = 0.14 W/m$\cdot$ K 1 -
$\rho$ = 1.2 g/cm3 2 -
${\rm MW}_0$ = 30 g/mol -
${\rm MW}$ = 1$\times 10^5$ g/mol 3 -
$A_\beta$ = 1.8$\times 10^{13}$ s-1 4 -
$E_a$ = 30 kcal/mol 5 -
$\Delta_rH$ = 56 kJ/mol 6 -
$\Delta h_{\rm LH}$ = 150 J/g 7 -
$T_{\rm melt}$ = 438 K 89 -
$\gamma$ = 1 -
$R_u$ = 8.314 J/mol$\cdot$ K
Input: Liquid-gas interface temperature
|
|
|
|---|---|
| 800 | 5.34 |
| 700 | 1.22 |
| 600 | 1.75 |
Input: Liquid-gas interface heat flux
|
|
|
|---|---|
| 3 |
4.13 |
| 2 |
8.26 |
| 1 |
1.24 |
In "mechanism" folder: 13 species, 47 reactions. FFCM-2 10 formaldehyde sub-model.
- *.inp, *.dat: Chemkin format files
- *.cti, *.yaml: Cantera format files
Wendi Dong, Nikolaos Kateris, Nicholas J. Montes, Amitesh S. Jayaraman, Hai Wang
Mechanical Engineering Department, Stanford University, Stanford, California 94305, United States
Footnotes
-
S. Luftl, P. Visakh, S. Chandran, Polyoxymethylene handbook: structure, properties, applications and their nanocomposites, John Wiley & Sons, 2014. ↩
-
H. W. Starkweather Jr., G. A. Jones, P. Zoller, The pressure-volume-temperature relationship and the heat of fusion of polyoxymethylene, Journal of Polymer Science Part B: Polymer Physics 26 (2) (1988) 257–266. ↩
-
Estimated, ranging from 1x104 to 2x105 g/mol. ↩
-
L.-S. Tran, J. Pieper, H.-H. Carstensen, H. Zhao, I. Graf, Y. Ju, F. Qi, K. Kohse-Hoinghaus, Experimental and kinetic modeling study of diethylether flames, Proceedings of the Combustion Institute 36 (1) (2017) 1165–1173. ↩
-
G. Berkowicz, T. M. Majka, W. ̇Zukowski, The pyrolysis and combustion of polyoxymethylene in a fluidised bed with the possibility of incorporating CO2, Energy Conversion and Management 214 (2020) 112888. ↩
-
Group additivity calculation using NIST data. ↩
-
D. Czarnecka-Komorowska, T. Sterzynski, Effect of polyhedral oligomeric silsesquioxane on the melting, structure, and mechanical behavior of polyoxymethylene, Polymers 10 (2) (2018) 203. ↩
-
DURACON® POM report. https://www.polyplastics.com/en/support/mold/duracon/pom04c.html#:~:text=The%20melting%20point%20of%20DURACON,cylinder%20temperature%20(front%20section). ↩
-
K. Pielichowska, The influence of molecular weight on the properties of polyacetal/hydroxyapatite nanocomposites. Part 1. Microstructural analysis and phase transition studies, Journal of Polymer Research 19 (2) (2012) 9775. ↩
-
Y. Zhang, W. Dong, L. Vandewalle, R. Xu, G.P. Smith and H. Wang, Foundational Fuel Chemistry Model Version 2.0 (FFCM-2), https://web.stanford.edu/group/haiwanglab/FFCM2, 2023. ↩
