enthalpy formulation
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2019 ◽  
Vol 4 (1) ◽  
pp. 43
Author(s):  
Dede Tarwidi

Stefan problem is a problem involving phase transition from solid to liquid or vice versa where boundary between solid and liquid regions moves as function of time. This paper presents numerical solution of one-dimensional two-phase Stefan problem by using finite element method. The governing equations involved in Stefan problem consist of heat conduction equation for solid and liquid regions, and also transition equation in interface position (moving boundary). The equations are difficult to solve by ordinary numerical method because of the presence of moving boundary. As consequence, the equations is reformulated into the form of internal energy (enthalpy). By the enthalpy formulation, solution of the heat conduction equations is no longer concerning the phase state of material. The advantage of the enthalpy formulation is that, finite element method can be easily implemented to solve Stefan problem. Numerical simulation of interface position, temperature profile, and temperature history has good agreement with the exact solution. The approximation of interface position using finite element method was found that it is more accurate than the approximation by using Godunov method. The simulation results also reveal that the finite element method for solving Stefan problem have smaller mean absolute error than the Godunov method.


2018 ◽  
Author(s):  
Agah D. Garnadi

In this paper we describe an implementation of approximate solution to the enthalpy formulation of the Stefan problem. We allow the thermal properties to have a space and temperature dependence. The algorithm is not explicit in the timevariable and hence the stability condition on the time steps is not too severe.The main aim of this note is program documentation of solving non-linear heat equation implementedin ALBERT(A) an adaptive finite element method package.


Energy ◽  
2014 ◽  
Vol 66 ◽  
pp. 919-926 ◽  
Author(s):  
T. Kousksou ◽  
M. Alaphilippe ◽  
A. Jamil ◽  
T. El Rhafiki ◽  
M. Mouqalid ◽  
...  

2014 ◽  
Vol 378 (4) ◽  
pp. 374-381 ◽  
Author(s):  
Johann Miranda Fuentes ◽  
Frédéric Kuznik ◽  
Kévyn Johannes ◽  
Joseph Virgone

2012 ◽  
Vol 58 (209) ◽  
pp. 441-457 ◽  
Author(s):  
Andy Aschwanden ◽  
Ed Bueler ◽  
Constantine Khroulev ◽  
Heinz Blatter

AbstractPolythermal conditions are ubiquitous among glaciers, from small valley glaciers to ice sheets. Conventional temperature-based ‘cold-ice’ models of such ice masses cannot account for that portion of the internal energy which is latent heat of liquid water within temperate ice, so such schemes are not energy-conserving when temperate ice is present. Temperature and liquid water fraction are, however, functions of a single enthalpy variable: a small enthalpy change in cold ice is a change in temperature, while a small enthalpy change in temperate ice is a change in liquid water fraction. The unified enthalpy formulation described here models the mass and energy balance for the threedimensional ice fluid, for the surface runoff layer and for the subglacial hydrology layer, together in a single energy-conserving theoretical framework. It is implemented in the Parallel Ice Sheet Model. Results for the Greenland ice sheet are compared with those from a cold-ice scheme. This paper is intended to be an accessible foundation for enthalpy formulations in glaciology.


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