Partial Differential Equation (PDE) modelling of a one-dimensional tubular heater for liquid fluids

Antonio Sala, UPV

Difficulty: **** ,       Relevance: PIC,      Duration: 16:16

*Enlace a Spanish version

Materials:    [ HeatExchModelEDPEnglish.pdf]

Summary:

This video pursues modelling a tubular heat exchanger with at heating resistor alongside it, as a connection of multiple (infinitely many of them) elements where each of the elements is a mini-heating-tank modelled as a first-order dynamical systems; modelling is briefly outlined in the first two minutes of this video, detailed explanations appear at video [term1eEN].

Once the inputs and outputs of each element are suitably named, the separation between elements will be set to “dx”. Conceptually, if one element’s temperature is T(x), that of the next element will be T(x + dx). As we are analysing the time evolution of temperature, we actually pursue findin the equations governing the evolution of T(x,t) at different positions and time instants.

Taking limits when dx 0, the following PDE (partial differential equation) is obtained:

T t = 1 SF T x κ¯ SρcT + Q¯ Sρc

The final part of the video discusses two frequent particular cases, well studied:

The first one is transport delay (no heating, perfect insulation), i.e., the transport PDE: T t = vT x being v = FS the linear speed of the fluid.

The second particular case is the steady-state heat exchanger (enforcing equilibrium condition T t = 0), considered for simplicity under no heating, i.e., Q¯ = 0. In that case, we obtain an ordinary differential equation (ODE) in the longitudinal position variable Teq x = κ¯ FρCe Teq which obviously has an exponential solution which is widely used and explained in depth in heat-exchanger textbooks.

Numerical simulation of PDE requires, in a general nonlinear case, the approximation (discretization) to a finite number of non-infinitesimal elements, as considered in the starting phases of the modelling procedure in this material. Nevertheless, in this particular case, for constant flow, there is a Laplace-transform solution (with delay) that can be simulated with the control system toolbox in Matlab; details on how to solve the PDE are in video [termedpsolEN], the step response of such solution is detailed in video [termedpstepEN].

*Link to my [ whole collection] of videos in English. Link to larger [ Colección completa] in Spanish.

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