*Enlace a Spanish version
Materials: [ HeatExchModelEDPEnglish.pdf]
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 [
Once the inputs and outputs of each element are suitably named, the separation between elements will be set to “”. Conceptually, if one element’s temperature is , that of the next element will be . As we are analysing the time evolution of temperature, we actually pursue findin the equations governing the evolution of at different positions and time instants.
Taking limits when , the following PDE (partial differential equation) is obtained:
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: being the linear speed of the fluid.
The second particular case is the steady-state heat exchanger (enforcing equilibrium condition ), considered for simplicity under no heating, i.e., . In that case, we obtain an ordinary differential equation (ODE) in the longitudinal position variable 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 [
*Link to my [ whole collection] of videos in English. Link to larger [ Colección completa] in Spanish.