Nonideal Reactor Design using POLYMATH - POLYMATH Software
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Nonideal Reactor Design using POLYMATH - POLYMATH Software
Nonideal Reactor Design using POLYMATH by Michael B. Cutlip, University of
Connecticut and. Mordechai Shacham, Ben-Gurion University of the Negev.
Nonideal Reactor Design using POLYMATH by Michael B. Cutlip, University of Connecticut and Mordechai Shacham, Ben-Gurion University of the Negev The latest version of POLYMATH is now available from the CACHE office. An order form is attached to this article. All users who have a continuing site license should have received this latest version. Please contact the CACHE office if you have not. There is also a special offer of a POLYMATH trial period for four months for an academic department before a site license needs to be purchased. Details are also at the end of this article. A number of improved and enhanced feature are now provided. Polymath programs now include capabilities for 1. Simultaneous Ordinary Differential Equations 2. Simultaneous Nonlinear Equations 3. Simultaneous Linear Equations 4. Polynomial, Linear and Nonlinear Regressions with the separate Linear Equation Solver being a new program. Number of Equations/Lines per Equation Most experience users will appreciate that the number of equations has been increase to 31 and up to three lines per equation are now allowed in the first three of the POLYMATH programs. These capabilities will allow much more complicated problems to be solved. Logical Variables An important new capability is the unlimited use of logical variables in the differential and nonlinear equations programs. This allows an IF, THEN, ELSE logic to specify changes in any of the program variables. A variety of operators can be used including >, =, = tau/2.) then (tau^2/(2.*t^3) else (0.0) Let us consider a second order, irreversible, liquid phase reaction occurring within the laminar flow reactor using the RTD function. This can easily be handled in
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POLYMATH by numerically solving the differential equation for the batch reactor given by dC A = − kC A 2 I. C. CA = 1.0 at t = 0 (3) dt during the during the simultaneous integration of the RTD differential equation (2) for C A . The initial condition (I. C.) on CA is considered to be 1.0 The POLYMATH equations for the case where k = 0.2 and tau=5.0 are shown below in Figure 1 as they appear on the screen prior to solution.
Figure 1 - Polymath Code for Laminar Flow Reactor The scaled and titled POLYMATH plot for the laminar flow reactor is shown in Figure 2. Note that the calculated concentration is approaching a constant value at t = 30.
Figure 2 - Graphical Output of the Conversion for Laminar Flow Reactor The RTD curve for the laminar flow reactor can also be plotted after the numerical solution has been obtained. This is shown in Figure 3 which nicely shows the breakthrough of the RTD curve at one half of the mean residence time where tau = 2.5.
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Figure 3 - RTD for Laminar Flow Reactor This simple example shows the usefulness of the logical variable capability with POLYMATH. This problem involving segregated flow modeling can easily be expanded to include the RTD functions for various ideal reactors and experimental RTD’s for real reactors as polynomial expressions. This is treated in the next section of this article. How to Compare Simulations Easily within POLYMATH The previous example can be extended to other reactors when the RTD functions are known or can be measured. Some of the commonly used ideal reactor RTD for the plug flow, CSTR and series of N CSTR’s are given below: EoftPLUG=if((t)=.99*tau)&(t