Critical Review of Advances and Numerical Modeling in Absorbers and Desorbers of Absorption Chillers: CFD Applications, Constraints, and Future Prospects
Abstract
:1. Introduction
2. State-of-the-Art Literature Survey
3. Absorber and Desorber Technologies: CFD-Based Studies
3.1. Absorber and Desorber Technologies
3.1.1. Falling Film
3.1.2. Bubble
3.1.3. Membrane
3.2. General Discussion on the Different Sorption Exchanger Technologies
4. Artificial Intelligence Techniques for CFD Analysis in Absorption Refrigeration Systems
5. Final Critical Considerations for the Application of CFD Modeling to Absorbers and Desorbers
6. Conclusions and Recommendations
6.1. Conclusions
- It was found that the CFD techniques are essential for advancing the understanding of sorption processes, enabling detailed analysis of flow phenomena and the impact of operating parameters;
- AI integration—in particular, machine learning models—has shown potential for optimizing CFD simulations, reducing computational costs, and providing new insights into system behavior;
- Most studies have adopted the VOF method; however, when considering turbulence, the RNG κ-ε method is the most commonly used;
- The H2O-LiBr working fluid is the most extensively studied fluid for CFD-based studies on sorption exchangers for absorption refrigeration systems;
- The primary focus is optimizing absorption and desorption processes by enhancing exchangers and exploring new geometric configurations to improve the absorption or desorption flow of the binary fluid. Additionally, most research is aimed at understanding and enhancing the hydrodynamics of flows in heat and mass exchangers;
- Owing to its ease of implementation regarding flow characteristics, ANSYS FLUENT is widely used to simulate both the absorption and desorption processes, including those involving falling films, membranes, and bubbles. Furthermore, some researchers are developing proprietary codes to study the simultaneous transfer of heat and mass.
6.2. Recommendations
- ✓
- There is a significant need for the computational study of new technologies such as adiabatic absorbers and desorbers;
- ✓
- More CFD studies must be conducted with desorbers to explore and optimize the performance of these components. CFD modeling can help better understand the thermal phenomena and mass transfer occurring in the desorber, allowing for optimization of its performance and minimizing issues such as crystallization;
- ✓
- The role of new fluids in increasing absorption/desorption capacity is still an ongoing area of research, necessitating further studies in this field;
- ✓
- Potential research could be conducted to compare the behavior of absorption and desorption processes within heat exchangers by applying different multiphase and turbulence models. The goal would be to evaluate the models available in various software tools, identify any differences, and determine which model best represents real-world conditions;
- ✓
- The application of AI techniques, such as ANNs and machine learning algorithms, needs to be further explored, and also, the adaptation of CFD models for large-scale systems and the optimization of the results for industrial applications requires further investigation;
- ✓
- Advances have been evident in studies on the absorption process in absorbers and generators. However, gaps still need to be filled, such as models where thermophysical properties are varied, as well as a dynamic interface and more effective desorbent technology.
Author Contributions
Acknowledgments
Conflicts of Interest
References
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DOCUMENT TYPE | QUERY 1 | QUERY 2 | QUERY 3 |
---|---|---|---|
Article | 509 | 26 | 12 |
Conference paper | 100 | 3 | 0 |
Review | 18 | 2 | 0 |
Conference Review | 13 | 3 | 1 |
Book Chapter | 7 | 0 | 0 |
Total | 647 | 34 | 13 |
Software | Advantages | Disadvantages |
---|---|---|
ANSYS FLUENT [35] | High precision and robustness Intuitive interface Extensive technical support Student version (limited) | High license fee Significant computing resources required Steep learning curve |
ANSYS CFX [36] | High license fee Limited compared to ANSYS FLUENT for certain types of flows Significant computing resources required | |
COMSOL Multiphysics [37] | Easy integration with other physics (Multiphysics) Intuitive graphic interface Good documentation and technical support Student version (limited) | High license fee Requires powerful hardware for complex simulations Less specialized in pure CFD |
Open Source (general) [38] | Usually free or at a low cost Open source allowing for user customization User community support Simulations are typically configured using text files, which allows for easy linking of the simulation configuration to third-party applications (e.g., for optimization tools) | Unintuitive graphical interfaces Advanced programming knowledge may be required The associated licenses may have detailed and complex requirements and restrictions Less formal technical support Some advanced features found in commercial software may be missing |
Fluid | ANSYS FLUENT/CFX | COMSOL Multiphysics | OpenFOAM |
---|---|---|---|
H2O-LiBr | H2O properties included in its library [40]. The properties of H2O-LiBr must be defined by the user (typically through UDFs or manually entered data) [44]. | H2O properties included in its library [45]. The properties of H2O-LiBr must be defined by the user [46]. | H2O properties included in its library (initial configuration may be necessary) [47]. The properties of H2O-LiBr must be defined by the user [47]. |
NH3-H2O | NH3 properties included in its library (it may be necessary to set up UDFs for specific properties) [11,48]. The properties of binary mixtures must be defined by the user (typically through UDFs or manually entered data) [44]. | NH3 properties must be defined by the user [45]. The properties of binary mixture must be defined by the user [46]. | NH3 properties included in its library (an initial configuration may be required) [47]. The properties of binary mixture must be defined by the user [47]. |
NH3-LiNO3 |
Ref. | Exchanger Technology | Operating Mode | Working Fluid | Objective |
---|---|---|---|---|
[50] | Falling film | Absorber | H2O-LiBr | Capture the key parameters’ impact on the film’s flow. |
[52] | Simulate the distribution of wave speed and energy in the process of falling liquid film. | |||
[54] | Examine the absorption characteristics of the fluid from a fully coupled ALE-IT algorithm. | |||
[55] | H2O-(LiBr+nanoparticles) | Analyze the effect of adding copper oxide nanoparticles on the absorption performance of the falling film. | ||
[53] | Absorber/Desorber | H2O-LiBr | Analyze the influence of liquid charge and concentration on the hydrodynamics of the solution film. | |
[43] | NH3-H2O | Analyze how the existence of a porous substrate in the flow field affects the mass and momentum transfer performances. | ||
[48] | Bubbles | Absorber | NH3-LiNO3 | Analyze and validate a double vertical absorber. |
[60] | Analyze the performance considering global heat transfer parameters. | |||
[11] | NH3-H2O | Predict the hydrodynamic behavior of flat plate absorbers. | ||
[46] | H2O-LiBr | Study the absorption process under vacuum conditions. | ||
[58] | Desorber | H2O-LiBr | Investigate the effect of using fins and grooves in copper tubes on the boiling heat transfer rate, comparing it with smooth tubes. | |
[59] | Evaluate the spacing of the baffles inside the heat exchanger for the optimization of an exchanger. | |||
[63] | Membrane | Absorber | H2O-LiBr | Analyze the effects of membrane parameters on the absorption process. |
[40] | Discuss the influence of design variables on the absorption process. | |||
[41] | Investigate improvement strategies to reduce the pressure drop of the solution side and improve the absorption characteristics of the equipment. | |||
[42] | Absorber/Desorber | H2O-LiBr, H2O-LiBr/LiNO3/LiI/LiCl, H2O-[EMIM][OAc] and H2O-LiCl | Optimize absorbers and desorbers considering different design parameters. | |
[64] | Desorber | H2O-LiBr | Study an air gap membrane desorber. |
Ref. | Software | Properties | Basic Settings | Transport Phenomenon Models | Significant Findings | |
---|---|---|---|---|---|---|
Multi-Phase Models | Models and Complementary Equations | |||||
[48] | ANSYS FLUENT | Constant properties (database + external ref.) | 3D, transient state | VOF model; mixture model; Eulerian model | Viscous models: laminar, k-epsilon, k-omega | The VOF + realizable κ-epsilon model was the most appropriate. The model identified temperature profiles on the solution side of the absorber; these gradients were not identified in experimental studies or one-dimensional simulations. |
[50] | 2D/3D, steady state, laminar flow | VOF; continuous surface force method (CSF) | Species Transportation Model | The 2D model effectively tracked the impact of the various flow aspects on the heat and mass transfer processes. The computational cost and solution time of the 2D model are worth its use. | ||
[53] | 2D, transient state, laminar flow | VOF; continuous surface force method (CSF) | No information on the energy equation; Adiabatic condition (no heat flow) | Heat transfer performance is better at lower concentrations due to lower film thickness, more recirculation, higher velocity, and lower thermal resistance. | ||
[60] | 3D, transient state | VOF and mixture | Realizable κ-epsilon viscous models | The VOF model has a good performance in low-density mesh elements. The mixture model has better performance in smaller numbers of elements and smaller volumes. The absorbed mass flow and the heat transfer coefficient on the solution side are the most sensitive variables for CFD absorber performance. | ||
[59] | Constant properties (external ref.) | 3D, laminar flow | Not informed | Calculation of the global heat transfer coefficient using the Kern method | Reducing the spacing of the baffles significantly increased the heat transfer coefficient in the wall, with a 48% increase when reducing the spacing from 137 mm to 101 mm. There was also an increase in velocity and a drop in static pressure. | |
[58] | 2D, transient state | Two-phase Eulerian–Eulerian | RPI boiling model; extended RNG κ-ε turbulence model; energy equation is only determined for the liquid phase; the vapor phase is assumed to be at the saturation temperature | The use of finned tubes increases the boiling heat transfer coefficient, enhances the wettability of the solution, and increases the nucleation sites for bubbles, which leads to faster and more efficient boiling. | ||
[43] | No information on fluid properties | 2D, pseudo-steady state | Hybrid model (VOF and Euler–Euler) | Sherwood correlations for gas absorption and desorption; transport of concentrated species; no information on the energy equation | When the liquid film flows over a porous substrate, a greater thickness of the liquid film leads to poorer mass transfer performance. A non-linear and complex relationship exists between the mass transfer rate of the liquid phase and the flow rate of the liquid, which is also affected by the properties of the porous medium. | |
[63] | 2D, steady state, laminar flow | Single-phase simplified model approach with mass and heat sources | Transport of species | The porosity of the membrane had the greatest impact on the absorption rate, with a 32% increase in the absorption rate when increasing the porosity from 0.6 to 0.8. The introduction of inclined grooves significantly improved heat and mass transfer performance. Grid and inclined groove structures presented the best overall performance among the different groove geometries. | ||
[40] | 3D, steady state, laminar flow | Not informed | Species transport model with mass source terms | The average absorption rate increases with the inlet velocity of the solution, an ideal velocity of 0.004 m·s−1. As the thickness of the solution channel decreases, there is a decrease in the absorption rate and an increase in the pressure drop. A channel thickness of 0.5 mm is recommended for a balance between pump load and absorber performance. The addition of baffles increases the average absorption rate by around 20% and the volumetric cooling capacity by up to 3.3 times compared to conventional falling film absorbers. | ||
[41] | 3D, steady state, laminar flow | The author considered a single-stage model | Knudsen number to evaluate water vapor transport; transport of concentrated species | The width of the solution channel has a negligible impact on heat and mass transfer but causes a 16.6% increase in pressure drop when reduced from 1.8 mm to 1.0 mm. Among the groove structures analyzed, the circular groove was the most efficient, reducing the solution pressure drop by 13.17% and improving the absorption rate by 0.57%. The circular groove structure proved to be more effective than thinner channels, improving the absorption rate with a slightly lower pressure drop, evidencing that groove structures are promising for optimizing the hydraulic and absorption performance of microchannel membrane-based absorbers. | ||
[42] | 2D, steady state, laminar flow | Not specified | Species transport model with source terms; diffusion model; transport of concentrated species | Microchannels of 0.5 mm height performed better in absorbers and desorbers. The H2O-[EMIM][OAc] solution proved to be the most efficient in terms of absorption, while H2O-LiCl was the best for desorption. The optimum solution inlet velocity was 0.027 m·s−1. Different microchannel structures resulted in significant increases in absorption rates but also disadvantages in terms of pressure drop. | ||
[64] | Properties (no information on whether the properties are constant or variable): database + external ref. | 3D, steady state | Not specified | Realizable k-epsilon; Poiseuille flow; Knudsen diffusion Stefan diffusion model; porous media model; chemical species transport model | There is a temperature difference between the volume and the membrane interface of up to 288.15 K. Stagnant areas in the solution channel caused velocity differences of up to 5 orders of magnitude compared to the midpoint in the solution channel. There was a concentration difference of up to 1.35% between the interface and the middle of the membrane. Desorption rate can be improved with geometric modifications to the membrane desorption device. | |
[11] | ANSYS CFX | CFX library properties | 2D, steady state | Heterogeneous model; homogeneous model | - | Increases of 10% and 20% in the refrigerant vapor result in an increase of 0.93% and 1.7% of ammonia in the solution at the absorber outlet, respectively. Increases of 10% and 20% in the absorbent solution flow result in a 1% and 2% reduction in the mass fractions of ammonia in the absorbent solution. |
[55] | COMSOL Multiphysics | External references | 2D, steady state, laminar flow, constant liquid film | Two-phase flow | Transport of concentrated species | Reducing the temperature of the inlet solution and increasing its concentration improves the mass transfer process. The mass transfer coefficient reaches a maximum near the inlet and gradually decreases downstream. The addition of copper oxide nanoparticles significantly increases the mass transfer flow. The effect of the nanoparticles is more pronounced under conditions of high temperature and low solution concentration at the inlet. |
[46] | Variable property function of the solution temperature and concentration | 2D, laminar flow | Two-phase flow; phase field; | - | The diameter of the orifice and the speed of the bubble result in significant improvements in the transfer coefficients while increasing the concentration of the solution reduces them. The heat and mass transfer coefficients increase with increasing orifice diameter and bubble velocity but decrease with increasing LiBr solution concentration. | |
[52] | Not informed | No information on the properties | 2D, laminar flow followed by wave flow | LBM for multiphase flow | Periodic and random perturbation methods (to simulate fluctuations at the interface of falling films) | The wavy flow has an apparent increase in heat and mass transfer. When the falling film tube reaches a certain length, the absorption capacity starts decreasing. |
[54] | Constant properties (external ref.) | 2D, transient state, laminar flow | Simulating two-phase flow with a mobile interface using an ALE-IT algorithm | Transport of concentrated species | Unstable interfacial waves significantly enhance heat and mass transfer in the absorption process. Increasing the difference between the temperature of the inlet solution and the liquid sidewall resulted in higher interfacial heat and mass flow rates, both in stable and unstable flows. Varying the frequency of the inlet velocity oscillation affected the formation and dissipation of interfacial waves, directly impacting heat and mass transfer. |
Challenges | Proposed Solution | Justification | Ref. |
---|---|---|---|
Complexity of physical models | Steady State | Simplifies analysis by ignoring time variations. | [11,40,41,42,52,55,63,64] |
Boundary conditions | Facilitates the problem definition and solution. | [11,55,58,63] | |
Laminar flow | Facilitates mathematical modeling and reduces computing time. | [40,41,42,46,50,52,53,54,55,63,68] | |
Stationary and non-slip walls | Reduces the need for detailed resolution near walls. | [40,48,63] | |
Accurate representation of fluid properties | Constant fluid properties | Simplifies the energy and momentum equations. | [50,53,58,59,60] |
Use of User-Defined Functions (UDFs) for property updates during simulations | Allows for dynamic updates of fluid properties, improving simulation accuracy. | [40,42] | |
Incorporation of property libraries from experimental data or open-source databases | Enhances reliability by using validated data. | [11,46] | |
The vapor–liquid interface is at equilibrium | Assumes that the thermodynamic properties of both phases at the interface can be determined directly from the phase equilibrium conditions, making it easier to simulate and analyze the system’s behavior. | [46,50,54,55] | |
Incompressible fluid | Reduces the complexity of the mass conservation equation. | [46,50,64] | |
Computational limitations | Use of symmetry | Reduces the computational domain and computing time. | [46,50,53] |
Simplified mesh | Reduction in grid size or optimization of grid distribution in critical regions. | [40,50,53,55,64] | |
Simplified geometry | Simplifies meshing and reduces computing time. | [11,46,48,50,53,55,58,59,60,68] |
AUTHORS | OBJECTIVE |
---|---|
Panahizadeh et al. [25] | Optimize the best predictive model for the behavior of an absorption cooling system in a refinery, focusing on the COP and cooling capacity. This was achieved by applying three machine learning methods: Artificial Neural Networks (ANNs), support vector machines (SVM), and genetic programming. |
Alcântara et al. [71] | Propose a methodological strategy to determine the transient behavior of a single-effect H2O-LiBr absorption chiller, utilizing machine learning techniques such as linear regression (LR), decision trees (DT), random forests (RF), and ANNs. |
Al-Rbaihat et al. [72] | Employ a support vector machine regression method combined with particle swarm optimization to identify the optimal operational parameters of an NH3-H2O absorption chiller. |
May Tzuc et al. [27] | Train an ANN to correlate the thermal properties of the solution and the absorption flow with easily measurable parameters, including concentrations, mass flow rates, pressures of saturated and diluted solutions, ammonia vapor flow and temperature, ambient temperature, and solution temperature. |
Ashouri et al. [73] | Develop a multi-label machine learning model for membrane-based absorbers used in sorption heat exchangers, integrating the accuracy of numerical models with the efficiency of analytical models. |
Zhai et al. [74] | Utilize AI to develop more accurate models for heat and mass transfer, as well as pressure drop in the solution for microchannel membrane-based desorbers and absorbers in absorption refrigeration systems. |
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Alcântara, S.C.S.; da Costa, J.Â.P.; Ochoa, A.A.V.; Leite, G.d.N.P.; Lima, Á.A.S.; Silva, H.C.N.; Michima, P.S.A.; da Silveira, I.C.; de Araújo Caldas, A.M.; Altamirano, A. Critical Review of Advances and Numerical Modeling in Absorbers and Desorbers of Absorption Chillers: CFD Applications, Constraints, and Future Prospects. Energies 2025, 18, 314. https://doi.org/10.3390/en18020314
Alcântara SCS, da Costa JÂP, Ochoa AAV, Leite GdNP, Lima ÁAS, Silva HCN, Michima PSA, da Silveira IC, de Araújo Caldas AM, Altamirano A. Critical Review of Advances and Numerical Modeling in Absorbers and Desorbers of Absorption Chillers: CFD Applications, Constraints, and Future Prospects. Energies. 2025; 18(2):314. https://doi.org/10.3390/en18020314
Chicago/Turabian StyleAlcântara, Suellen Cristina Sousa, José Ângelo Peixoto da Costa, Alvaro Antonio Villa Ochoa, Gustavo de Novaes Pires Leite, Álvaro Augusto Soares Lima, Héber Claudius Nunes Silva, Paula Suemy Arruda Michima, Igor Cavalcanti da Silveira, Allysson Macário de Araújo Caldas, and Amín Altamirano. 2025. "Critical Review of Advances and Numerical Modeling in Absorbers and Desorbers of Absorption Chillers: CFD Applications, Constraints, and Future Prospects" Energies 18, no. 2: 314. https://doi.org/10.3390/en18020314
APA StyleAlcântara, S. C. S., da Costa, J. Â. P., Ochoa, A. A. V., Leite, G. d. N. P., Lima, Á. A. S., Silva, H. C. N., Michima, P. S. A., da Silveira, I. C., de Araújo Caldas, A. M., & Altamirano, A. (2025). Critical Review of Advances and Numerical Modeling in Absorbers and Desorbers of Absorption Chillers: CFD Applications, Constraints, and Future Prospects. Energies, 18(2), 314. https://doi.org/10.3390/en18020314