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Optimal temperature profiles for tubular reactors implemented through a flow reversal strategy

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In this article, the authors propose an approach to implement the optimal temperature profiles in a jacketed tubular this article by using a trapezoidal shape along the reactor, where a first part the temperature is raised, then a constant temperature interval follows, and (possibly) a temperature is lowered towards the outlet.
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This article is published in Chemical Engineering Science.The article was published on 2007-09-01 and is currently open access. It has received 10 citations till now. The article focuses on the topics: Chemical reactor.

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Simulation of (bio)chemical processes with distributed parameters using Matlab

TL;DR: This paper compares different solution methods in a comprehensible way in order to provide practical guidelines for practitioners to rapidly evaluate different methods when setting-up their own process simulation code.
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Adaptive neuro-fuzzy inference system (ANFIS) – based model predictive control (MPC) for carbon dioxide reforming of methane (CDRM) in a plug flow tubular reactor for hydrogen production

TL;DR: In this article, an ANFIS approach was used to model the process and an MPC strategy was formulated for the process based on the model, and the generalized bell-shape membership functions were used and optimized based on empirical training data.
Journal ArticleDOI

Nested multigrid methods for time-periodic, parabolic optimal control problems

TL;DR: A nested multigrid method to optimize time-periodic, parabolic, partial differential equations (PDE), and considers a quadratic tracking objective with a linear parabolic PDE constraint.
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Enhanced model predictive control of a catalytic flow reversal reactor

TL;DR: In this paper, the combustion of lean methane air mixtures in a catalytic flow reversal reactor (CFRR) is studied using a two dimensional heterogeneous continuum model, based on mole and energy balance equations for the solid (the inert and catalytic sections of the reactor) and the fluid phases.
Journal ArticleDOI

Multi-objective dynamic optimisation of cyclic chemical reactors with distributed parameters

TL;DR: In this paper, a deterministic approach that integrates accurate scalarisation methods for multi-objective optimisation as Normal Boundary Intersection (NBI) and (Enhanced) Normalised Normal Constraint (E)NNC, with a fast direct multiple shooting approach for optimal control is presented.
References
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Journal ArticleDOI

Autothermal fixed-bed reactor concepts

TL;DR: In this paper, the principles, properties and applications of autothermal fixed-bed reactor concepts are presented and a simplified model is developed from which basic features of an optimal design can be deduced.
Journal ArticleDOI

Equivalence of one- and two-phase models for heat transfer processes in packed beds: one dimensional theory

TL;DR: In this article, the axial effective thermal conductivity in the one-phase model and the heat transfer coefficient in the twophase model were derived without assuming that the solid and gas temperatures are equal.
Journal ArticleDOI

Catalytic combustion with periodic flow reversal

TL;DR: In this paper, the influence of the operating parameters upon the shape of the temperature profiles in the stationary state als as well as the stability of the ignited state are studied by model calculations.
Journal ArticleDOI

Design of novel monolith catalyst supports for gas/solid reactions with heat exchange

TL;DR: In this paper, the potential of novel structured metallic catalysts for highly exothermic gas/solid reactions is parametrically investigated by means of a pseudo-continuous, heterogeneous 2D monolith reactor model.
Book

Catalytic Processes Under Unsteady-State Conditions

TL;DR: In this article, a non-stable state method for Sulphur dioxide Oxidation in SulphURic acid production is described. But this method is not suitable for the non-Steady-state regime.
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Q1. What are the contributions in "Optimal temperature profiles for tubular reactors implemented through a flow reversal strategy" ?

Optimal steady-state reactor temperature profiles in classic jacketed tubular reactors often exhibit a ( nearly ) trapezoidal shape along the reactor, i. e., in a first part the temperature is raised, then a constant temperature interval follows, and ( possibly ) the temperature is lowered towards the outlet. This article conceptually proves the feasibility of this concept and provides an optimisation procedure for its design and operation. 

Future work may evolve in several directions. 05. 027 sented proof of feasibility, both the classic jacketed tubular and the jacketed RFR configuration can be compared quantitatively for the case studied by Smets et al. ( 2002 ) and Logist et al. ( 2006 ). Second, a further validation can be performed through the use of more rigourous and complex models ( e. g., 2D and/or heterogeneous ) and/or through an experimental set-up. 

For all ignited operation regimes, the conversion cost J ′1 increases with increasing switching times due to lower averaged temperatures, the energy cost J ′2 exhibits a minimum, whereas a monotonous increase is observed for the energy cost J ′3. 

The value of this heat transfer coefficient is constant and positive in the jacketed zone, i.e., [L/2−Lj/2, L/2+Lj/2] with Lj [m] the jacket length, and zero in the insulated zones. 

Once the minimal length has been exceeded (i.e., Lj ≥ 0.4 m), symmetric profiles are obtained and the maximum temperature is hardly affected by the jacket length. 

As the jacket fluid temperature has the largest influence on the maximum reactor temperature, bounds on the jacket fluid temperature can be selected depending on the constant temperature level envisioned. 

The most important variables which influence this maximum temperature value are the heat transfer coefficient and the jacket fluid temperature. 

The decrease in energy cost J ′3 is easily explained by the fact that the extended high temperature plateau induces less deviations from the desired reference temperature Tref,2, whereas the decrease in energy cost J ′2 is related to the sharper gradients at the outlet causing the optimal switching time to shift towards lower values, i.e., closer to the here used fixed value of 100 s. 

From a cost point of view, the most important parameters to be determined in practice are the jacket temperature (i.e., to minimise mainly the conversion cost J ′1 and the energy cost J ′3) and the switching time and jacket length (i.e., to minimise mainly the energy cost J ′2). 

After 1500 s, during which the gas enters at high temperature (873 K), the feed temperature is decreased to 293 K and periodic flow reversals every 100 s are started. 

The corresponding optimal values for the jacket fluid temperature T ∗w and the switching time τ∗ are 846.9 K and 169.1 s, respectively. 

These criteria both consist of a trade-off between a conversion and an energy cost part, reflecting the current trend in process industry towards process integration and intensification, which relates to enhancing the over all plant performance by (i) optimising the performance of existing reactors or by (ii) adopting novel reactor types, which combine several unit operations into one, and by (iii) interconnecting material and energy streams plantwide. 

For classic jacketed tubular reactors where an exothermic first-order reaction takes place, optimal steady-state temperature profiles have∗ 

For a grid of jacket lengths, i.e., from 0.4 to 1 m in steps of 0.1 m, continuous optimisations are performed with the jacket fluid temperature and the switching time as decision variables. 

the following optimisation strategy is proposed, which combines discrete grid search and continuous optimisation procedures.