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Title: Advanced Topics in Heat, Momentum and Mass Transfer


1
Advanced Topics in Heat, Momentum and Mass
Transfer
  • Lecturer
  • Payman Jalali, Docent
  • Faculty of Technology
  • Dept. Energy Environmental Technology
  • Lappeenranta University of Technology

2
  • What are the approaches for an engineer or
    scientist making a research or solving a problem?
  • Approach Method of solution, method of
    scientific working.
  • There are 3 major approaches for any scientific
    or technological problem, as follows
  • Experimental approach The problem under
    consideration is totally analyzed in experimental
    facilities of the laboratory.
  • Analytical approach The problem is modeled
    theoretically (formulated mathematically) and
    solved with a number of simplifications.
  • Computational approach The problem is modeled
    theoretically but it is solved with no (or
    little) simplifications.
  • Computational approach solves the governing
    equations of physical phenomena accurately using
    computers. If the computational approach is used
    in fluid dynamics problems, it is called
    computational fluid dynamics (CFD).
  • The next slide simply draws the differences
    between the three approaches!

3
Problem Fluid flow and drag around a cylinder
4
  • What are advanced topics in heat, momentum and
    mass transfer?
  • They are topics related to some important
    phenomena such as diffusion, convection,
    radiation and advanced computational methods to
    deal with these phenomena in fluid mechanics and
    heat transfer.
  • The following tasks will be fulfilled in this
    course
  • Review governing equations for the transport of
    mass, momentum and energy in fluids.
  • Numerical study of diffusion problems using CFD.
  • Investigate how convection will change the domain
    created by diffusion.
  • How can we transfer partial differential
    equations (PDE) into algebraic equations needed
    in CFD?
  • Developing codes in MATLAB to solve diffusion
    problems.
  • Using commercial software (FLUENT) to solve
    complex problems in fluid and heat flows.

5
  • What is transport phenomenon?
  • Transport phenomena are dealing with all physical
    processes which cause the movement or
    transportation of mass, momentum and thermal
    energy (heat).
  • Transport properties of substances are different
    and they are characterized by the coefficient of
    viscosity (for momentum), conductivity (for
    thermal energy), and diffusivity (for mass
    concentration).

6
  • What is diffusion and how related to transport
    phenomena?
  • Diffusion is the natural propagation mechanism
    of some physical quantities such as mass, thermal
    energy and momentum through a medium of certain
    state.
  • Diffusion of mass is driven due to concentration
    gradient ? mixing of different species, or if
    there is 1 component it is called self-diffusion.
  • Diffusion of thermal energy (heat) is driven by
    temperature gradient ? heat conduction.
  • Diffusion of momentum is caused by velocity
    gradient ? shearing fluids.
  • The physics of diffusion can be associated with
    either random molecular motions or combined
    effects (such as molecular motion and turbulence
    etc.). Mathematically, the diffusion phenomenon
    is expressed as following

If we are talking about thermal energy (Fouriers
law) Heat flux (q) Thermal
conductivity(k)x temperature gradient (dT/dx) In
case of mass diffusion (Ficks law) Heat flux
(m) Thermal conductivity(D)x temperature
gradient (dC/dx)
7
  • What is the mathematical equation for diffusion?
  • Consider that a species (for example O2 in air)
    with concentration C is distributed along x axis
    at time t. Writing the mass balance equation for
    this species gives

species
(I)
(II)
This is diffusion equation when the diffusivity
is taken a constant. Its extension to 3D will be
as follows
8
  • Examples of diffusion problems
  • a) Transient diffusion of a dye in a medium.

The growth of the width of the dye is a
diffusion-type process, which can be formulated
as
Here, C is the concentration of the dye, Dr is
the radial diffusivity and r is radial position.
For large enough values of R we can assume the
following boundary conditions and initial
conditions
The initial condition C0 is the initial
concentration at the origin x0. Boundary
condition 1 Symmetry boundary condition at the
origin. Boundary condition 2 Zero concentration
at infinity.
9
The solution of diffusion equation under
mentioned initial and boundary conditions is
found as
10
b) Transient diffusion from a source to
semi-infinite medium.
We can solve diffusion equation analytically with
the given boundary conditions as follows
11
Error function
The mass flux can be found by the Ficks law
12
Graphical plots of the above-mentioned solution
is shown below
Concentration distribution in time
Flux distribution in time
13
  • Why do we need computational fluid dynamics
    (CFD)?
  • The two examples given above showed that exact
    mathematical (analytical) solutions to governing
    equations of fluid mechanics may be too
    difficult. Therefore, computational approach can
    be the practical method to solve equations in
    fluid mechanics such as the diffusion equation in
    complex geometries under various boundary
    conditions.
  • Major steps in any CFD calculations
  • a) Domain discretization Create nodes and
    elements (small control volumes) in the domain of
    solution. It is also called mesh generation which
    sometimes obeys complicated mathematical
    processes and calculations.
  • b) Equations discretizations The governing
    equations of fluid dynamics are algebraically
    discretized. It means that the governing
    equations which are partial differential
    equations (PDE) are written for the meshes
    (elements) produced from step a. Then we get a
    system of algebraic equations whose unknowns
    correspond to the nodes (elements).
  • c) Solution Discretized algebraic equations are
    solved with considerations of initial and
    boundary conditions.
  • d) Postprocessing The solution must be
    processed, visualized and interpreted.

14
  • How can we use CFD in practice?
  • a) Developing own codes A CFD work can be done
    independently by performing all the
    above-mentioned steps in a series of codes
    developed by a group of researchers. Depending on
    the level of complexity of the problem, the
    software for programming and postprocesses can
    vary. In rather simple problems, MATLAB is an
    appropriate tool for solving and postprocessing
    in a CFD problem. For more complex and large
    systems, one must develop the codes in one of the
    languages such as FORTRAN and C.
  • b) Commercial software Various computer
    packages are developed for handling professional
    problems in CFD. For instance, FLUENT, FIDAP,
    CFX, Finflo are some examples of such CFD
    software packages. The package for mesh
    generation is usually given separately, for
    example, GAMBIT is one of the packages used for
    creating the geometry and discretizing it into
    various types of elements appropriate for the
    methods employed by the CFD packages.

15
  • REFERENCES
  • - J.D. Anderson, Computational Fluid Dynamics,
    McGraw-Hill, Inc. 1995.
  • - D.A. Anderson, J.C. Tannehill, R.H. Pletcher,
    Computational Fluid Mechanics and Heat Transfer,
    McGraw-Hill, Inc. 1984.
  • - J.H. Ferziger, M. Peric, Computational Methods
    for Fluid Dynamics, Springer-Verlag 1996.
  • - C. Hirsch, Numerical Computation of Internal
    and External Flows, Volume 1 Fundamentals of
    Numerical Discretization, John Wiley Sons, 1988
  • - J.M. Haile, Molecular Dynamics Simulation
    Elementary Methods, John Wiley Sons, Inc.,
    1992.
  • - R.B. Bird, W.E. Stewart, E.N. Lightfoot,
    Transport Phenomena, John Wiley Sons,
    Inc.,1960.
  • - J. Crank, The Mathematics of Diffusion, Oxford
    University Press. 1975.
  • - MATLAB user manual.
  • - FLUENT user manual.
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