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- 2010 Annual Meeting
- Computing and Systems Technology Division
- Poster Session Area 10B Systems and Control
- (369c) Modeling of Tubular High-Pressure Polyethylene Reactors
As heat transfer processes are mainly governed by average reaction condition it is sufficient to compute the temperature and pressure profiles using moments kinetics. This ensures a fast convergence of iterative procedures needed to account for counter cooling. Complex cooling scenarios and multiple injections can be described. Special attention is dedicated to the transfer of kinetic data from independent laboratory experiments. By comparing model results with industrial data for different LDPE grades the model also serves as a test whether rate constants obtained on laboratory scale reactors can be directly transferred to large scale industrial plants. To compare computed distribution data directly with those from standard SEC and light scattering measurements, the results are modified to account for experimental band broadening effects assuming randomly distributed branches.
Having computed the temperature and pressure profiles using moment kinetics chain-length differentiated degrees of branching can be calculated using the concept of boundary density functions[2] in combination with the h-p Galerkin method implemented in PREDICI. For statistical processes this approach allows to reduce the two-dimensional problem (chain length and number of branches) to two one-dimensional subproblems: the rigorous computation of the molecular weight distribution and the evaluation of the leading moments of the branching density distribution. Assuming a binomial or Wesslau[3] distribution for the branching density bivariate chain-length/degree of branching distributions, which play a crucial role for structure-property relationships, can be obtained in a reasonable timeframe.
[1] M. Wulkow, Macromol. React. Eng. 2008, 2, 461 ? 494. [2] P. D. Iedema, M. Wulkow, H. C. J. Hoefsloot, Macromolecules 2000, 33, 7173 ? 7184. [3] M. Busch, Chem. Ing. Tech. 2004, 76, 780 ? 787.