May 13, 2010
Raíces de ecuaciones
May 6, 2010
En español:
http://www.acatlan.unam.mx/acatlecas/mn/MN_02.htm#Método_de_Bairstow

In Inglish:
http://translate.google.com.co/translate?js=y&prev=_t&hl=es&ie=UTF-8&layout=1&eotf=1&u=http%3A%2F%2Fwww.acatlan.unam.mx%2Facatlecas%2Fmn%2FMN_02.htm&sl=es&tl=en
May 5, 2010
A Numerical Simulation is a recreation math of a natural process. Using numerical simulations we study physical processes in engineering, economic and even biological. The field of numerical simulations is therefore a large interdisciplinary field of research. Some scientific problems are studied primarily by using numerical simulations as the problems of chaos , fractality or complexity and in general all fields of nature governed by systems of nonlinear equations or not easily reproducible in the laboratory.
The use of numerical simulations to study a problem usually requires a careful study of numerical methods and algorithms to use and key processes to be included in the simulation.
A numerical simulation differs from a mathematical model that the former is a representation in every moment of the simulation process while the model is a mathematical abstraction of the fundamental equations necessary to study this phenomenon. Normally the use of a numerical simulation to study a given problem requires careful planning to use the mathematical model and algorithms necessary to solve this model.

Simulation of flow fields.
Models Black Oil (Black Oil): The petroleum engineering simulators are used to relate the data flow observed in the field with reservoir properties such as permeability, porosity, and saturation pressure distribution. Intuitively one might think to describe the reservoir properties in the scale of the pores. However, traditional approaches homogenized porary scale heterogeneities to macroscopic descriptions such as the Law of Darcy.

The general equation of conservation of mass:

Provides that any local change in the mass flow is due to a local source or a temporary change in density or porosity. The source q is the local production of a well, which would be zero for a location without producing wells.

Darcy's Law expresses the flow of fluids in terms of pressure and gravity:

Where k is the permeability. The second term on the right incorporates the gravitational effects, where g is gravitational acceleration.

Darcy's law is valid only for low flow rates, where turbulence and inertia are negligible. Darcy's law generalizes the multi-phase flow, oil, water, gas in porous media:


KRL Where is the relative permeability of each phase. The relative permeability is a function of saturation. 1979 Aziz discusses several empirical expressions for this dependence. The combination of Darcy's law with the equation of conservation of mass flow equations generates:

The equations related differences in pressure gradients (left side) to temporary changes in the saturation of pores. These equations are supplemented by three additional limitations:


The first equation states that the rock is saturated with three fluids. The two equations below relate capillary pressure and saturation and are usually empirical (Aziz and Settari (1979).

Bj parameters values of parameters related to surface conditions (indicated by the S) and reservoir conditions (indicated by the index R). The parameters are defined as relations of volumes:

And the constants are based on PVT (Pressure-Volume-Temperature) for thermodynamic equilibrium. The first equation deviates from the other two counts because the volume of dissolved gas VDG. Bj The volume ratio allows us to relate the density at reservoir conditions with the density at surface conditions:

The mass transfer between oil and gas phase is defined as:
Rs = [VDG / Vo] S.

Bj relations and mass transfer Rs, depends on the pressure multistage pj j = o, w, g. Although the compressibility of water is small, the ratio Bw = f (pw) can be approximated by the following equation:


Similar expressions for Bo, Bg, Rs, and nj are empirical and discussed by Aziz and Settari (1979).

The coefficients in equation (4) express transimisibilidades and are defined as:

The Oil and gas viscosity depends strongly on the pressure and temperature. The dependence of the pressure again is empirical and developed by Aziz and Settari (1979). The temperature dependence of viscosity is especially important in processes such as heat recovery steam injection. In general, dependence on the temperature approaches very well through the following equation:

Where no and T0 are reference points c is a constant fluid specific.

Finally, the porosity is often dependent on pressure:

where cR is the total compressibility of the rock.

Equations:

Tied in situ volumes of the equation q (1) qa production volumes as they appear on the wellhead standard surface conditions.

Comments from wells. In a field experiment, petroleum engineers control the pressure in the well. Well tests are performed by changing the pressure in the well and watching the reaction of the pressure in the reservoir (and their respective effect on the pressure well controlled). These experiments attempt to estimate the local reservoir transmissibility but has to account for the "skin effect": changes in the rock surrounding the well. Additionally, petroleum engineers record production volumes in the wells. Production volumes in the wells depend on the reservoir pressure p and pressure downhole well PWF:

Where q is the volumetric production rate per unit time at the surface (not the reservoir pressure), B is the formation volume factor, C represents the capacity of the well for storage of fluid, n is the normal diameter Well, S the surface of the well diameter.

Where d is transmissibility. Each grid point represents a homogenous cell in the basement.

The following figure shows snapshots of a reservoir transmissibility constant pressure and variable sources. The pressure pulses fade in time as you would expect from a solution of parabolic differential equation.


Fig 1. Snapshots of a flow simulator for a medium of transmission and sources of constant pressure points randomly. The panel shows the pressure field as time increases from left to right and from top to bottom. A source generates the momentum fades over time.

References:
- Landa, JL, 1997, Reservoir parameter estimation constrained to pressure transients, performance history, and saturation in distributed data: Petroleum Engineering Department Stanford
- Aziz, K., and Settari, A., 1979, Petroleum reservoir simulation: Applied Science Publishers.
- Raghavan, R., 1993, Well test analysis: Prentice Hall.
- Wave propagation in an hydrocarbon reservoir exploitation During: In a preliminary, Integrated study. Stanford Exploration Project 03/09/1999

About Me

My Photo
Eliana Gomez
Bucarmanga, Santander, Colombia
View my complete profile

Followers

DIMENSIONAL SIMULATOR

DIMENSIONAL SIMULATOR