Abstract
The general three-dimensional hydrodynamic model SYSTEM 3 should be applicable to flow problems in which density variations and turbulence are important features. The mathematical modelling of such flows requires the solution of partial differential equations of the advective-diffusive type. It is foreseen that the direct flow modelling will require the solution of the transport equation for salinity, temperature, turbulent kinetic energy and dissipation of turbulent kinetic energy. This report describes the development of a numerical mentod for the solution of the advective-diffusive type of partial differential equation with appropriate initial and boundary conditions. The practical implementation of the method will be in form of a Fortran module which will be linked with the hydrodynamical model, to be run in conjunction or separately. (AB).
Citation Formats
Justesen, P, and Vested, H J.
System 3. A three dimensional hydrodynamical model. Vol. 3B. Finite difference scheme and solution algorithm. Advection - dispersion model.
Denmark: N. p.,
1989.
Web.
Justesen, P, & Vested, H J.
System 3. A three dimensional hydrodynamical model. Vol. 3B. Finite difference scheme and solution algorithm. Advection - dispersion model.
Denmark.
Justesen, P, and Vested, H J.
1989.
"System 3. A three dimensional hydrodynamical model. Vol. 3B. Finite difference scheme and solution algorithm. Advection - dispersion model."
Denmark.
@misc{etde_10144757,
title = {System 3. A three dimensional hydrodynamical model. Vol. 3B. Finite difference scheme and solution algorithm. Advection - dispersion model}
author = {Justesen, P, and Vested, H J}
abstractNote = {The general three-dimensional hydrodynamic model SYSTEM 3 should be applicable to flow problems in which density variations and turbulence are important features. The mathematical modelling of such flows requires the solution of partial differential equations of the advective-diffusive type. It is foreseen that the direct flow modelling will require the solution of the transport equation for salinity, temperature, turbulent kinetic energy and dissipation of turbulent kinetic energy. This report describes the development of a numerical mentod for the solution of the advective-diffusive type of partial differential equation with appropriate initial and boundary conditions. The practical implementation of the method will be in form of a Fortran module which will be linked with the hydrodynamical model, to be run in conjunction or separately. (AB).}
place = {Denmark}
year = {1989}
month = {Feb}
}
title = {System 3. A three dimensional hydrodynamical model. Vol. 3B. Finite difference scheme and solution algorithm. Advection - dispersion model}
author = {Justesen, P, and Vested, H J}
abstractNote = {The general three-dimensional hydrodynamic model SYSTEM 3 should be applicable to flow problems in which density variations and turbulence are important features. The mathematical modelling of such flows requires the solution of partial differential equations of the advective-diffusive type. It is foreseen that the direct flow modelling will require the solution of the transport equation for salinity, temperature, turbulent kinetic energy and dissipation of turbulent kinetic energy. This report describes the development of a numerical mentod for the solution of the advective-diffusive type of partial differential equation with appropriate initial and boundary conditions. The practical implementation of the method will be in form of a Fortran module which will be linked with the hydrodynamical model, to be run in conjunction or separately. (AB).}
place = {Denmark}
year = {1989}
month = {Feb}
}