Abel Bustos’s research while affiliated with Pontificia Universidad Javeriana - Cali and other places

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Publications (5)


Fig. 1 Oil permeability depends not only on the fluid saturation but also on the hysteresis parameter and on the saturation tendency (imbibition and drainage processes)
Table 3 L n q -errors related to numerical approximations reported in Fig. 6
Fig. 5 In the left frame, the exact Riemann solution is formed by shock, connecting the state (S L o = 1 − S R w = 0.7; π L = 0.8) (and S R w = 0.3) to an intermediate state (S 1 o = 0.8762; π 1 = 0.1968) (and S R w = 0.1238) (numerical (S 1 o = 0.8741; π 1 = 0.1987)) on the scanning curve. The analytical (resp. numeric) shock speed is −1.624 (resp. −1.622). The scanning shock is obtained from the water fractional flow function (left frame). On the right frame (oil saturation S o ) we see that the wave pattern is then formed by a "shock" followed by a rarefaction, from the previous intermediate state (S 1 w ; π 1 ) to right (equilibrium) state (S R o = 1 − S R w = 1.0; π R = 0.0). The two-phase water-oil numerical results in one space dimension are in very good agreement with analytical results obtained from our Riemann problem analysis. Here we use σ g = 1.8 (P c = 8.36266 × 10 3 ) and −u < 0. This is an example of the second case of Sect. 3.1.7
Fig. 6 The pair (S w , u f w + σ g G) is on the left frame. On the right frame, we show the hysteresis wave propagating in both left and right directions (numerical solution for saturations are not shown in figures). For a fixed time, the exact Riemann solution is formed by a shock connecting the left Riemann initial data (S L w = 0.7; π L = 0.8) to an intermediate state (S 1 w = 0.464; π 1 = 0.6292) (numerical (S 1 w = 0.4637; π 1 = 0.6371)) on the scanning curve. From the trailing edge of state (S 1 w ; π 1 ), we have a rarefaction wave to (S 2 w = 0.385; π 2 = 0.5419) (numerical (S 2 w = 0.3853; π 2 = 0.5326)) and then, a stationary shock wave from (S 2 w ; π 2 ) to (S 3 w = 0.31; π 3 = 0.3095) (numerical (S 3 g = 0.3121; π 3 = 0.3139)). Now, from the trailing edge of state (S 3 w ; π 3 ), we have a small rarefaction wave to (S 4 w = 0.303; π 4 = 0.3095) (numerical (S 4 w = 0.303; π 4 = 0.3139)) and then a shock to the "right Riemann data" (S R w = 0.2; π R = 0.3075), that is the projection of right date (0.2, 0.4) into the equilibrium region. We use σ g = 1.1 (P c = 2.93028 × 10 4 ) and u = 0. We notice that the exact (resp. numerical) negative water shock RH speed is −0.914 (−0.915), the zero (resp. 0.047) stationary shock and the gas shock RH speed is 1.798 (resp. 1.797). It is an example of the third case described in Sect. 3.1.7
Fig. 7 (Left frame): Imbibition, drainage and fractional flows for the first regime. The arrow indicates the direction that λ s is an increasing function. I s is the inflection of family s. (Right frame): For a fixed left state L, figure shows all 7 right regions, R 1 to R 7 , for which the Riemann sequence is the same in each region. The solid curve represents rarefaction (R s ) and dashed curves represent shocks (S c or S s ). States P 1 , P 2 and line S L are explained along of the text 123

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A Relaxation Projection Analytical–Numerical Approach in Hysteretic Two-Phase Flows in Porous Media
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  • Full-text available

June 2019

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268 Reads

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19 Citations

Journal of Scientific Computing

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Abel Bustos

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Hysteresis phenomenon plays an important role in fluid flow through porous media and exhibits convoluted behavior that are often poorly understood and that is lacking of rigorous mathematical analysis. We propose a twofold approach, by analysis and computing to deal with hysteretic, two-phase flows in porous media. First, we introduce a new analytical projection method for construction of the wave sequence in the Riemann problem for the system of equations for a prototype two-phase flow model via relaxation. Second, a new computational method is formally developed to corroborate our analysis along with a representative set of numerical experiments to improve the understanding of the fundamental relaxation modeling of hysteresis for two-phase flows. Using the projection method we show the existence by analytical construction of the solution. The proposed computational method is based on combining locally conservative hybrid finite element method and finite volume discretizations within an operator splitting formulation to address effectively the stiff relaxation hysteretic system modeling fundamental two-phase flows in porous media.

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Asymptotic Behavior of a Solution of Relaxation System for Flow in Porous Media

June 2018

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52 Reads

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3 Citations

We introduce a novel modeling of phase transitions in thermal flow in porous media by using hyperbolic system of balance laws, instead of system of conservation laws. We are interested in two different behaviors of the balance system: the long time behavior, in which we study the solution with fixed relaxation term and very large time; and the behavior of the solution when the relaxation term is taken to zero and the time is fixed. We also are interested in solving the question: “Does this balance system tend to the conservation system under equilibrium hypothesis?”. To answer this question, we introduce a projection technique for the wave groups appearing in the system of equations and we study the behavior of each group. For a particular Riemann datum, using the projection method, we show the existence of a decaying traveling profile supported by source terms and we analyze the behavior of this solution. We corroborate our analysis with numerical experiments.


A unsplitting finite volume method for models with stiff relaxation source terms

March 2016

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24 Reads

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2 Citations

Boletim da Sociedade Brasileira de Matemática

We developed an unsplitting finite volume scheme to account the delicate nonlinear balance between numerical approximations of the hyperbolic flux function and the source linked to balance laws. The method is Riemann-solver-free and no upwinding technique is used. By means of this new approach, we conducted an analysis for two new models of balance laws linked to compositional and thermal flow in porous media problems, under and without a thermodynamic equilibrium hypothesis. For concreteness, we adopt the nitrogen and steam injection models in a porous media. To this model we found an interesting behavior linked to the relaxation term, which is the existence of a non-monotonic traveling wave. We applied this numerical technique to others well-known differential models with relaxation terms available in the literature. Qualitatively we were able to reproduce the expected results.


Non-monotonic traveling wave and computational solutions for gas dynamics Euler equations with stiff relaxation source terms

September 2015

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24 Reads

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5 Citations

Computers & Mathematics with Applications

We study the existence of non-monotone traveling wave solutions and its properties for an isothermal Euler system with relaxation describing the perfect gas flow. In order to confront our results, we first apply a mollification approach as an effective regularization method for solving an ill-posed problem for an associated reduced system for the Euler model under consideration, which in turn is solved by using the method of characteristics. Next, we developed a cheap unsplitting finite volume scheme that reproduces the same traveling wave asymptotic structure as that of the Euler solutions of the continuous system at the discrete level. The method is conservative by construction and relatively easy to understand and implement. Although we do not have a mathematical proof that our designed scheme enjoys the asymptotic preserving and well-balanced properties, we were able to reproduce consistent solutions for the more general Euler equations with gravity and friction recently published in the specialized literature, which in turn are procedures based on a Godunov-type scheme and based on an asymptotic preserving scheme, yielding good verification and performance to our method.


Citations (4)


... The retention curve consists of two main branches: the wetting and draining branches. Various approaches have been proposed to model the hysteresis, including those by Mualem (1976), Lenhard and Parker (1987), Parker and Lenhard (1987), Beliaev andHassanizadeh (2001), McNamara (2014), Schweizer (2017), and Abreu et al. (2019). ...

Reference:

Modeling 2D gravity-driven flow in unsaturated porous media for different infiltration rates
A Relaxation Projection Analytical–Numerical Approach in Hysteretic Two-Phase Flows in Porous Media

Journal of Scientific Computing

... However, a lack of rigorous mathematical analysis in hysteresis modeling is very limited and in particular when involving systems of equations as discussed in this work. In [104] the authors introduced a hysteresis modeling for a scalar two-phase flow in porous media via relaxation and in [3] a formalism to deal with relaxation system for flow in porous media was introduced and the analysis includes the latter equations. ...

Asymptotic Behavior of a Solution of Relaxation System for Flow in Porous Media

... Moreover, one can use any numerical method for the resulting system of equations with variables (s w , y). To implement this procedure, Godunov (see [31]), Nessyahu-Tadmor extension (see [32]), or any higher order methods together with splitting are useful. Here, we consider the upwind method adequate (see [26,33]). ...

A unsplitting finite volume method for models with stiff relaxation source terms
  • Citing Article
  • March 2016

Boletim da Sociedade Brasileira de Matemática

... For problems in multiphase flow, in [3], we introduce a novel modeling of phase transitions in thermal flow in porous media by using hyperbolic system of balance laws, instead of a system of conservation laws. Roughly speaking, relaxation encompass entropy conditions in a natural and general form for scalar and systems (see [3,4,80,98,104] and references therein). It is worth mentioning that our relaxation interpretation of entropy conditions discussed in this paper (see [3]) agree with a previous work of Natalini and Tesei [102], which was proposed by Barenblatt [26] to describe non-equilibrium two phase fluid flow in permeable porous media; see also [14,81]. ...

Non-monotonic traveling wave and computational solutions for gas dynamics Euler equations with stiff relaxation source terms
  • Citing Article
  • September 2015

Computers & Mathematics with Applications