Search results

Filters

  • Journals
  • Authors
  • Keywords
  • Date
  • Type

Search results

Number of results: 28
items per page: 25 50 75
Sort by:
Download PDF Download RIS Download Bibtex

Abstract

One of the mathematical tools to measure the generation rate of new patterns along a sequence of symbols is the Lempel-Ziv complexity (LZ). Under additional assumptions, LZ is an estimator of entropy in the Shannon sense. Since entropy is considered as a measure of randomness, this means that LZ can be treated also as a randomness indicator. In this paper, we used LZ concept to the analysis of different flow regimes in cold flow combustor models. Experimental data for two combustor’s configurations motivated by efficient mixing need were considered. Extensive computer analysis was applied to develop a complexity approach to the analysis of velocity fluctuations recorded with hot-wire anemometry and PIV technique. A natural encoding method to address these velocity fluctuations was proposed. It turned out, that with this encoding the complexity values of the sequences are well correlated with the values obtained by means of RMS method (larger/smaller complexity larger/smaller RMS). However, our calculations pointed out the interesting result that most complex, this means most random, behavior does not overlap with the “most turbulent” point determined by the RMS method, but it is located in the point with maximal average velocity. It seems that complexity method can be particularly useful to analyze turbulent and unsteady flow regimes. Moreover, the complexity can also be used to establish other flow characteristics like its ergodicity or mixing.

Go to article

Authors and Affiliations

S. Blonski
A. Pregowska
T. Michalek
J. Szczepanski
Download PDF Download RIS Download Bibtex

Abstract

Results of a research study into the velocity field in combustion chamber of internal combustion engine are presented in the paper. Measurements of fresh charge flow velocity in the cylinder axis and near the cylinder squeezing surface were performed. The hot-wire anemometer was used. The measurement results were used for analysis of turbulence field in the examined combustion chamber. It turned out that in the axis of cylinder the maximum of velocity occurs 30 deg before TDC and achieves 6 m/s. In the studied combustion chamber, the maximum value of turbulence intensity was close to 0.2 and it was achieved 35 deg BTDC. Additionally, the maximal velocity dispersion in the following cycles of the researched engine was at the level of 2 m/s, which is 35% of the maximum value of flow velocity. At a point located near the squeezing surface of the piston, a similar level of turbulence, but a the smaller value of the average velocity was achieved. The turbulence field turned out to be inhomogeneous in the combustion chamber.

Go to article

Authors and Affiliations

Wojciech Tutak
Arkadiusz Jamrozik
Download PDF Download RIS Download Bibtex

Abstract

Aspiration dust probes of some isokinctic samplers have such a construction that enables them to measure the gas velocity at the point they arc placed in a duct, the measurement being required for maintaining isokinctic conditions and in determining the dust mass flow rate in the duct. The gas velocity is correlated with a probe specific pressure difference, a quantity measured directly when the train is in operation. This relationship is a mclrological characteristic of a given probe, being established in a calibration procedure. Two types of the above-mentioned probes, namely a pressure balance-type and an in-stack filtration probes (in two versions) combined with a type S velocity sensor, have been tested. The behaviour of the characteristics of the probes was studied in the flows of different turbulence at a laboratory stand. The achieved results, presented in the paper, show that the turbulence state of gas flow is the factor that shapes the mctrological characteristics. Facing the fact that the turbulence of gas flow in industrial installations is not identified during the dust concentration gravimetric measurements, this parameter constitutes a source of uncertainty of the gas velocity measurement. For the probes under test, the values of this uncertainty, varying with the gas velocity, were determined. The test and calculation procedures were described.
Go to article

Authors and Affiliations

Przemysław Kateusz
Zbigniew Popiołek
Jerzy Szulikowski
Download PDF Download RIS Download Bibtex

Abstract

This paper presents the results of experimental testing of parameters of the flow of an agitated liquid in a stirred tank with an eccentrically positioned shaft and with a Rushton turbine. The investigations were focused on the impact of the stirrer shaft shift in relation to the stirred tank vertical axis on the agitated liquid mean velocities and the liquid turbulent velocity fluctuations, as well as on the turbulence intensity in the tank. All the experiments were carried out in a stirred tank with the inner diameter of 286 mm and a flat bottom. The adopted values of the shaft eccentricity were zero (central position) and half the tank radius. The liquid flow instantaneous velocities were measured using laser Doppler anemometry.

Go to article

Authors and Affiliations

Jan Talaga
Piotr Duda
Download PDF Download RIS Download Bibtex

Abstract

This study aims to design a novel air cleaning facility which conforms to the current situation in China, and moreover can satisfy our demand on air purification under the condition of poor air quality, as well as discuss the development means of a prototype product. Air conditions in the operating room of a hospital were measured as the research subject of this study. First, a suitable turbulence model and boundary conditions were selected and computational fluid dynamics (CFD) software was used to simulate indoor air distribution. The analysis and comparison of the simulation results suggested that increasing the area of air supply outlets and the number of return air inlets would not only increase the area of unidirectional flow region in main flow region, but also avoid an indoor vortex and turbulivity of the operating area. Based on the summary of heat and humidity management methods, the system operation mode and relevant parameter technologies as well as the characteristics of the thermal-humidity load of the operating room were analyzed and compiled. According to the load value and parameters of indoor design obtained after our calculations, the airflow distribution of purifying the air-conditioning system in a clean operating room was designed and checked. The research results suggested that the application of a secondary return air system in the summer could reduce energy consumption and be consistent with the concept of primary humidity control. This study analyzed the feasibility and energy conservation properties of cleaning air-conditioning technology in operating rooms, proposed some solutions to the problem, and performed a feasible simulation, which provides a reference for practical engineering.

Go to article

Authors and Affiliations

X.R. Ding
Y.Y. Cino
Y.Y. Chen
Download PDF Download RIS Download Bibtex

Abstract

In the paper, the authors discuss the construction of a model of an exemplary urban layout. Numerical simulation has been performed by means of a commercial software Fluent using two different turbulence models: the popular k-ε realizable one, and the Reynolds Stress Model (RSM), which is still being developed. The former is a 2-equations model, while the latter – is a RSM model – that consists of 7 equations. The studies have shown that, in this specific case, a more complex model of turbulence is not necessary. The results obtained with this model are not more accurate than the ones obtained using the RKE model. The model, scale 1:400, was tested in a wind tunnel. The pressure measurement near buildings, oil visualization and scour technique were undertaken and described accordingly. Measurements gave the quantitative and qualitative information describing the nature of the flow. Finally, the data were compared with the results of the experiments performed. The pressure coefficients resulting from the experiment were compared with the coefficients obtained from the numerical simulation. At the same time velocity maps and streamlines obtained from the calculations were combined with the results of the oil visualisation and scour technique.

Go to article

Bibliography

[1] R. Yoshie, A. Mochida, Y. Tominaga, H. Kataoka, K. Harimoto, T. Nozu, and T. Shirasawa. Cooperative project for CFD prediction of pedestrian wind environment in the Architectural Institute of Japan. Journal of Wind Engineering and Industrial Aerodynamics, 95(9):1551–1578, 2007. doi: 10.1016/j.jweia.2007.02.023.
[2] A. Mochida and I.Y.F. Lun. Prediction of wind environment and thermal comfort at pedestrian level in urban area. Journal of Wind Engineering and Industrial Aerodynamics, 96(10):1498–1527, 2008. doi: 10.1016/j.jweia.2008.02.033.
[3] B. Blocken, T. Stathopoulos, J. Carmeliet, and J.L.M. Hensen. Application of computational fluid dynamics in building performance simulation for the outdoor environment: an overview. Journal of Building Performance Simulation, 4(2):157–184, 2011. doi: 10.1080/19401493.2010.513740.
[4] S.E. Kim and F. Boysan. Application of CFD to environmental flows. Journal of Wind Engineering and Industrial Aerodynamics, 81(1):145–158, 1999. doi: 10.1016/S0167-6105(99)00013-6.
[5] J. Franke, A. Hellsten, K.H. Schlunzen, and B. Carissimo. Best Practice Guideline for CFD Simulation of Flows in the Urban Environment: A Summary. University of Hamburg, Hamburg, 2007.
[6] J. Franke, A. Hellsten, K.H. Schlunzen, and B. Carissimo. The COST 732 best practice guideline for CFD simulation of flows in the urban environment: a summary. International Journal of Environment and Pollution, 44(1-4):419–427, 2011. doi: 10.1504/IJEP.2011.038443.
[7] S. Murakami, A. Mochida, and Y. Hayashi. Examining the k-ω model by means of a wind tunnel test and large-eddy simulation of the turbulence structure around a cube. Journal of Wind Engineering and Industrial Aerodynamics, 35:87–100, 1990. doi: 10.1016/0167-6105(90)90211-T.
[8] D.A. Köse and E. Dick. Prediction of the pressure distribution on a cubical building with implicit LES. Journal of Wind Engineering and Industrial Aerodynamics, 98(10):628–649, 2010. doi: 10.1016/j.jweia.2010.06.004.
[9] P.J. Richards and S.E. Norris. Appropriate boundary conditions for computational wind engineering models revisited. Journal of Wind Engineering and Industrial Aerodynamics, 99(4):257–266, 2011. doi: 10.1016/j.jweia.2010.12.008.
[10] D.A. Köse, D. Fauconnier, and E. Dick. ILES of flowover low-rise buildings: Influence of inflow conditions on the quality of the mean pressure distribution prediction. Journal of Wind Engineering and Industrial Aerodynamics, 99(10):1056–1068, 2011. doi: 10.1016/j.jweia.2011.07.008.
[11] S. Reiter. Validation process for CFD simulations of wind around buildings. In Proceedings of the European Built Environment CAE Conference, pages 1–18, London, June 2008.
[12] A. Kovar-Panskus, P. Louka, J.F. Sini, E. Savory, M. Czech, A. Abdelqari, P.G. Mestayer, and N. Toy. Influence of geometry on the mean flow within urban street canyons – a comparison of wind tunnel experiments and numerical simulations. Water, Air, and Soil Pollution: Focus, 2(5):365–380, 2002. doi: 10.1023/A:1021308022939.
[13] B. Blocken and J. Persoon. Pedestrian wind comfort around a large football stadium in an urban environment: CFD simulation, validation and application of the new Dutch wind nuisance standard. Journal of Wind Engineering and Industrial Aerodynamics, 97(5):255–270, 2009. doi: 10.1016/j.jweia.2009.06.007.
[14] M. Sakr Fadl and J. Karadelis. CFD simulations for wind comfort and safety in urban area: A case study of Coventry University central campus. International Journal of Architecture, Engineering and Construction, 2(2):131–143, 2013. doi: 10.7492/IJAEC.2013.013.
[15] B. Blocken, T. Stathopoulos, and J. Carmeliet. CFD simulation of the atmospheric boundary layer: wall function problems. Atmospheric Environment, 41(2):238–252, 2007. doi: 10.1016/j.atmosenv.2006.08.019.
[16] B. Blocken. 50 years of Computational Wind Engineering: past, present and future. Journal of Wind Engineering and Industrial Aerodynamics, 129:69–102, 2014. doi: 10.1016/j.jweia.2014.03.008.
[17] A. Flaga. Wind Engineering. Arkady, Warsaw, Poland, 2008. (in Polish).
[18] K. Klemm. A complex assessment of microclimate conditions found in widely spaced and dense urban structures. KILiW, Polish Academy of Sciences, 2011. (in Polish).
[19] K. Daniels. The Technology of Ecological Building. Birkhäuser, Basel-Boston-Berlin, 1997.
[20] R. Józwiak et al. An analysis of a potential influence on airing and wind conditions of the area surrounding an urban layout planned to be built at a lot situated in Warsaw, Powązkowska street 23/1. Warsaw University of Technology, 2013. internal, not published materials of Institute of Aeronautics and Applied Mechanics, (in Polish).
[21] B. Blocken and J. Carmeliet. Pedestrian wind environment around buildings: Literature review and practical examples. Journal of Thermal Envelope and Building Science, 28(2):107–159, 2004. doi: 10.1177/1097196304044396.
[22] E. Błazik-Borowa. Difficulties arising from the use of k-ω turbulence model for the purpose of determining the airflow around buildings.Lublin University of Technology Publisher, 2008. (in Polish).
[23] S. Murakami. Overview of turbulence models applied in CWE–1997. Journal of Wind Engineering and Industrial Aerodynamics, 74:1–24, 1998. doi: 10.1016/S0167-6105(98)00004-X.
[24] K. Hanjalic and B.E. Launder. A Reynolds stress model of turbulence and its application to thin shear flows. J. Fluid Mech, 52(4):609–638, 1972. doi: 10.1017/S002211207200268X.
[25] K. Gumowski, O. Olszewski, M. Pocwierz, and K. Zielonko-Jung. Comparative analysis of numerical and experimental studies of the airflow around the sample of urban development. Bulletin of the Polish Academy of Sciences Technical Sciences, 63(3):729–737, 2015. doi: 10.1515/bpasts-2015-0084.
[26] J.R. Taylor. Introduction to Error Analysis. University Science Books, 2nd edition, 1996.
[27] Y. Tominaga, A. Mochida, R.Yoshie, H. Kataoka, T.Nozu, M.Yoshikawa, and T. Shirasawa. AIJ guidelines for practical applications of CFD to pedestrian wind environment around buildings. Journal of Wind Engineering and Industrial Aerodynamics, 96(10):1749–1761, 2008. doi: 10.1016/j.jweia.2008.02.058.
[28] Ansys Fluent Theory Guide, version 14.0. Canonsburg, 2011.
[29] Ansys Fluent User’s Guide, version 14.0. Canonsburg, 2011.
[30] H. Montazeri and B. Blocken. CFD simulation of wind-induced pressure coefficients on buildings with and without balconies: validation and sensitivity analysis. Building and Environment, 60:137–149, 2013. doi: 10.1016/j.buildenv.2012.11.012.
Go to article

Authors and Affiliations

Mateusz Jędrzejewski
1
Marta Poćwierz
1
Katarzyna Zielonko-Jung
2

  1. Warsaw University of Technology, Institute of Aeronautics and Applied Mechanics, Warsaw, Poland
  2. Warsaw University of Technology, Faculty of Architecture, Warsaw, Poland
Download PDF Download RIS Download Bibtex

Abstract

The relevance of this study is explained by the growing interest in increasing heat transfer by the development of high-performance thermal systems. Increasing the thermal characteristics of heat-exchanger systems is necessary for the efficient use of an energy source. The purpose of this study is to review the existing methods of heat-transfer intensification and examine the mathematical model of such an increase in efficiency when using petal turbulators. This study is based on a high-quality, reliable combination of proven theoretical methods (analysis, synthesis, concretization, generalization, modelling), and empirical methods. It is the introduction of turbulators into the flow channel that is one of the best methods of increasing passive heat exchange through such advantages as ease of manufacture and operation in combination with low operating and production costs. This study contains both passive and active methods of heat-exchange intensification that have been extensively investigated over the past decade. For this purpose, the newest studies of mainly authors from other countries were used, their detailed analysis was conducted and the results were summed up. In addition, a mathematical model of increasing the thermal efficiency of convective heating surfaces in a bundle of smooth pipes using petal turbulators was investigated, the results of which were tested on an experimental installation. The paper may interest a circle of readers interested in the problem of improving the thermal characteristics of heat exchangers, including researchers, teachers and students of higher educational institutions in the field of heat-power engineering.
Go to article

Authors and Affiliations

Jiyenbeck Sugirov
1
Bibigul Atshybayeva
2
Marzhan Suimenova
1
Kulanda Shaikhiyeva
1
Gulbanu Yesbolay
1

  1. Department of Construction Engineering, Caspian University of Technology and Engineering named after Sh. Yessenov, Republic of Kazakhstan
  2. Department of Energy and Transport, Caspian University of Technology and Engineering named after Sh. Yessenov, Republic of Kazakhstan
Download PDF Download RIS Download Bibtex

Abstract

The article presents the possibility of using the Cobb-Douglas production function for planning in a turbulent environment. A case study was carried out – the Cobb-Douglas function was used to examine the condition of the Polish hard coal mining industry and the progress which has been made after undertaking certain activities aimed at increasing the competitiveness of coal companies over recent years. Only the correct and confirmed identification of the causes of irregularities in the production process can allow for the introduction of effective remedies. The effectiveness of the solutions proposed by the author has been confirmed thanks to the simulation during which the impact of the proposed production strategy on the parameters of the CD function was examined. Three variants of production functions models were created and production productivity rates and marginal substitution rates were determined. The results enabled the verification of the progress of restructuring as well as identification of the origin of the observed problems and comparison of the current state with the results of analyses carried out in previous years. Scenarios of possible trend developments for the factors introduced into the function model in order to present remedial measures that could improve the process of hard coal extraction were created. The scenarios were created using the ARIMA class models. Which scenario is the most favourable was determined. A computer program, created by the author, for optimising the level and use of labor resources at the level of the entire coal company has been presented.

Go to article

Authors and Affiliations

Aurelia Rybak
ORCID: ORCID
Download PDF Download RIS Download Bibtex

Abstract

Most of the formulations regarding the characteristics of a shell and tube heat exchanger have a common assumption; namely that the baffle plates are equidistant. This assumption fails to cater the real world scenario for defective baffles as the alteration in a shell and tube heat exchanger invalidates the equidistant baffle spacing of the plates. In this regard, a small six baffles heat exchanger was modeled in the computational fluid dynamics software package and studied by removing each baffle plate one at a time. Effect of removing each baffle plate on the temperature, pressure, heat transfer coefficient, and total heat transfer rate was recorded. It was observed that variation in the pressure drop for the same number of baffle plates varies along the axial order of the plates. The change in pressure drop due to the removal of the baffle plate near the inlet and the outlet was lowest and reaches a maximum in the axial center. It was also found that the plates below the radial center contribute higher towards the overall heat transfer as compared to those above.

Go to article

Authors and Affiliations

Abdullah Aziz
Shafique Rehman
Download PDF Download RIS Download Bibtex

Abstract

This paper presents new results for the dynamic behaviour of fluid around a rotating turbulator in a channel. The turbulator has a propeller form which is placed inside a flat channel. The research was carried out using 3D numerical simulation. The rationale of the experiment was as follows: we put a propeller-turbulator inside a flat channel, and then we insert a water flow inside the channel. The turbulator rotates at a constant and uniform speed. The main points studied here are the effect of the presence of turbulator and its rotational direction on the flow behaviour behind the turbulator. The results showed that the behaviour of flow behind the turbulator is mainly related to the direction of turbulator rotating. Also, the studied parameters affect coefficients of drag force and power number. For example, when the turbulator rotates in the positive direction, the drag coefficient decreases in terms of rotational speed of the turbulator, while the drag coefficient increases in terms of rotational speed when the turbulator rotates in the negative direction.
Go to article

Authors and Affiliations

Elhadi Zoubai
1
Houssem Laidoudi
1
Ismail Tlanbout
1
Oluwole Daniel Makinde
2

  1. University of Science and Technology of Oran Mohamed-Boudiaf, Faculty of Mechanical Engineering, Laboratory of Sciences and Marine Engineering, BP 1505, El-Menaouer, Oran, 31000, Algeria
  2. Stellenbosch University, Faculty of Military Science, Private Bag X2, Saldanha 7395, South Africa
Download PDF Download RIS Download Bibtex

Abstract

The airflow through a two-dimensional horizontal rectangular cross-section channel in the presence of two baffles has been numerically examined and analyzed in the steady turbulent regime. The baffles were of the zig-zag type or plane one. The calculations are based on the finite volume approach and the average Navier–Stokes equations along with the energy equation, have been solved using the SIMPLE algorithm. The nonuniform structured quadrilateral-type element mesh is used in this study. The fluid flow patterns represented for Reynolds numbers based on the hydraulic diameter of the channel ranging from 5000 to 20 000. Effects of various Reynolds number values on flow fields, dimensionless axial velocity profiles, as well as local and average friction coefficients in the test channel is presented. The obtained results show that the flow structure is characterized by strong deformations and large recirculation regions. In general, the fluid velocity and skin friction loss rise with the increase in the flow rate and hence the Reynolds number.

Go to article

Authors and Affiliations

Chafika Zidani
Boumédiènne Benyoucef
Faouzi Didi
Nabila Guendouz
Download PDF Download RIS Download Bibtex

Abstract

The problem of reducing noise in transportation is an important research field to prevent accidents and to provide a civilised environment for people. A material that has recently attracted attention in research to reduce noise is acoustic metamaterial, and most of the research projects so far have been limited to the case of static media without flow. We have studied the sound transmission properties of the acoustic metamaterials with turbulent flow to develop the acoustic metamaterials that are used in transportation. In this paper, the effects of geometrical structure, convection, and eddy on sound propagation in the acoustic metamaterials with turbulent flow are investigated, and the relationships between them are analysed. The effects of convection and eddy reduce the resonant strength of the sound transmission loss resulting from the unique geometry of the acoustic metamaterials, but move the resonant frequencies to opposite directions. In addition, when the convective effect and the eddy effect of the airflow, as well as the intrinsic interaction effect generated from the unique geometrical structure of the acoustic metamaterials cannot be ignored, they exhibit competition phenomena with each other, resulting in a widening of the resonance peak. As a result, these three effects cause the shift of the resonance frequency of the sound transmission loss and the widening of the resonance peak. The results of this study show that even in the case of turbulent flow, the metamaterials can be used for transportation by properly controlling its geometric size and shape.
Go to article

Bibliography

1. Ananthan V., Bernicke P., Akkermans R., Hu T., Liu P. (2020), Effect of porous material on trailing edge sound sources of a lifting airfoil by zonal oversetles, Journal of Sound and Vibration, 480: 115386, doi: 10.1016/j.jsv.2020.115386.
2. Bok E., Park J.J., Choi H., Han C.K., Wright O.B., Lee S.H. (2018), Metasurface for water-to-air sound transmission, Physical Review Letters, 120(4): 044302, doi: 10.1103/PhysRevLett.120.044302.
3. Brookea D.C., Umnova O., Leclaire P., Dupont T. (2020), Acoustic metamaterial for low frequency sound absorption in linear and nonlinear regimes, Journal of Sound and Vibration, 485: 115585, doi: 10.1016/j.jsv.2020.115585.
4. Carpio A.R., Avallone F., Ragni D., Snellen M., van der Zwaag S. (2019), Mechanisms of broadband noise generation on metal foam edges, Physics of Fluids, 31(10): 105110, doi: 10.1063/1.5121248.
5. Chaitanya P., Joseph P., Ayton L.J. (2020), Leading edge profiles for the reduction of airfoil interaction noise, AIAA Journal, 58(3): 1118–1129, doi: 10.2514/1.J058456.
6. Deuse M., Sandberg R.D. (2020), Different noise generation mechanisms of a controlled diffusion aerofoil and their dependence on Mach number, Journal of Sound and Vibration, 476: 115317, doi: 10.1016/j.jsv.2020.115317.
7. Du L., Holmberg A., Karlsson M., Åbom M. (2016), Sound amplification at a rectangular t-junction with merging mean flows, Journal of Sound and Vibration, 367: 69–83, doi: 10.1016/j.jsv.2015.12.042.
8. Fan L., Chen Z., Zhang S., Ding J., Li X., Zhang H. (2015), An acoustic metamaterial composed of multi-layer membrane-coated perforated plates for low-frequency sound insulation, Applied Physics Letters, 106(15): 151908, doi: 10.1063/1.4918374.
9. Gikadi J., Föller S., Sattelmayer T. (2014), Impact of turbulence on the prediction of linear aeroacoustic interactions: Acoustic response of a turbulent shear layer, Journal of Sound and Vibration, 333(24): 6548–6559, doi: 10.1016/j.jsv.2014.06.033.
10. Gu Z., Gao H., Liu T., Li Y., Zhu J. (2020), Dopant-modulated sound transmission with zero index acoustic metamaterials, The Journal of the Acoustical Society of America, 148(3): 1636–1641, doi: 10.1121/10.0001962.
11. Jiang X., Li Y., Zhang L.K. (2017), Thermoviscous effects on sound transmission through a metasurface of hybrid resonances, The Journal of the Acoustical Society of America, 141(4): EL363–EL368, doi: 10.1121/1.4979682.
12. Jung J.W., Kim J.E., Lee J.W. (2018), Acoustic metamaterial panel for both uid passage and broadband soundproofing in the audible frequency range, Applied Physics Letters, 112(4): 041903, doi: 10.1063/1.5004605.
13. Kundu P.K., Cohen I.M., Dowling D. (2012), Fluid mechanics, 5th ed., pp. 564–571, Elsevier, doi: 10.1016/C2009-0-63410-3.
14. Kusano K., Yamada K., Furukawa M. (2020), Aeroacoustic simulation of broadband sound generated from low-Mach-number flows using a lattice Boltzmann method, Journal of Sound and Vibration, 467: 115044, doi: 10.1016/j.jsv.2019.115044.
15. Li Y., Assouar B.M. (2016), Acoustic metasurfacebased perfect absorber with deep subwavelength thickness, Applied Physics Letters, 108(6): 063502, doi: 10.1063/1.4941338.
16. Lu K., Wu J., Guan D., Gao N., Jing L. (2016), A lightweight low-frequency sound insulation membrane- type acoustic metamaterial, AIP Advances, 6(2): 025116, doi: 10.1063/1.4942513.
17. Menter F. (1994), Two-equation eddy-viscosity turbulence models for engineering applications, AIAA Journal, 32(8): 1598–1605, doi: 10.2514/3.12149.
18. Nardini M., Sandberg R.D., Schlanderer S.C. (2020), Computational study of the effect of structural compliance on the noise radiated from an elastic trailing-edge, Journal of Sound and Vibration, 485: 115533, doi: 10.1016/j.jsv.2020.115533.
19. Ostashev V.E., Wilson D.K. (2016), Acoustics in Moving Inhomogeneous Media, 2ed., pp. 27–62, Taylor and Francis, doi: 10.1201/b18922.
20. Park J.J., Park C.M., Lee K.J., Lee S.H. (2015), Acoustic superlens using membrane-based metamaterials, Applied Physics Letters, 106(5): 051901, doi: 10.1063/1.4907634.
21. Pierce A.D. (2019), Acoustics: An Introduction to Its Physical Principles and Applications, 3rd ed., pp. 68– 70, Springer, doi: 10.1007/978-3-030-11214-1.
22. Qu S., Sheng P. (2020), Minimizing indoor sound energy with tunable metamaterial surfaces, Physical Review Applied, 14(3): 034060, doi: 10.1103/PhysRevApplied.14.034060.
23. Romani G., Ye Q.Q., Avallone F., Ragni D., Casalino D. (2020), Numerical analysis of fan noise for the NOVA boundary-layer ingestion configuration, Aerospace Science and Technology, 96: 105532, doi: 10.1016/j.ast.2019.105532.
24. Su H., Zhou X., Xu X., Hu G. (2014), Experimental study on acoustic subwavelength imaging of holeystructured metamaterials by resonant tunnelling, The Journal of the Acoustical Society of America, 135(4): 1686–1691, doi: 10.1121/1.4868395.
25. Sui N., Yan X., Huang T.Y., Xu J., Yuan F.G., Jing Y. (2015), A lightweight yet sound-proof honeycomb acoustic metamaterial, Applied Physics Letters, 106(17): 171905, doi: 10.1063/1.4919235.
26. Szoke M., Fiscaletti D., Azarpeyvand M. (2018), Effect of inclined transverse jets on trailing-edge noise generation, Physics of Fluids, 30(8): 085110, doi: 10.1063/1.5044380.
27. Szoke M., Fiscaletti D., Azarpeyvand M. (2020), Uniform flow injection into a turbulent boundary layer for trailing edge noise reduction, Physics of Fluids, 32(8): 085104, doi: 10.1063/5.0013461.
28. Tang H., Lei Y.L., Li X.Z. (2019), An acoustic source model for applications in low Mach number turbulent flows, such as a large-scale wind turbine blade, Energies, 12(23): 4596, doi: 10.3390/en12234596.
29. Wang X., Zhao H., Luo X., Huang Z. (2016), Membrane-constrained acoustic metamaterials for low frequency sound insulation, Applied Physics Letters, 108(4): 041905, doi: 10.1063/1.4940717.
30. Wang Y., Thompson D., Hu Z. (2019), Effect of wall proximity on the flow over a cube and the implications for the noise emitted, Physics of Fluids, 31(7): 077101, doi: 10.1063/1.5096072.
31. Yang Z.J. et al. (2015), Topological acoustics, Physical Review Letters, 114(11): 114301, doi: 10.1103/Phys RevLett.114.114301.
32. Yao H., Davidson L. (2019), Vibro-acoustics response of a simplified glass window excited by the turbulent wake of a quarter-spherocylinder body, The Journal of the Acoustical Society of America, 145(5): 3163–3176, doi: 10.1121/1.5109548.
33. Zheng M.Y., Park C., Liu X.N., Zhu R., Hu G.K., Kim Y.Y. (2020), Non-resonant metasurface for broadband elastic wave mode splitting, Applied Physics Letters, 116(17): 171903, doi: 10.1063/5.0005408.
Go to article

Authors and Affiliations

Myong Chol Pak
1
Kwang-Il Kim
1
Hak Chol Pak
1
Kwon Ryong Hong
2

  1. Department of Physics, Kim Il Sung University, Taesong District, Pyongyang, Democratic People’s Republic of Korea
  2. Institute of Natural Sciences, Kim Il Sung University, Taesong District, Pyongyang, Democratic People’s Republic of Korea
Download PDF Download RIS Download Bibtex

Abstract

CFD modelling of momentum and heat transfer using the Large Eddy Simulation (LES) approach has been presented for a Kenics static mixer. The simulations were performed with the commercial code ANSYS Fluent 15 for turbulent flow of three values of Reynolds number, Re = 5 000, 10 000 and 18 000. The numerical modelling began in the RANS model, where standard k−ε turbulence model and wall functions were used. Then the LES iterations started from the initial velocity and temperature fields obtained in RANS. In LES, the Smagorinsky–Lilly model was used for the sub-grid scale fluctuations along with wall functions for prediction of flow and heat transfer in the near-wall region. The performed numerical study in a Kenics static mixer resulted in highly fluctuating fields of both velocity and temperature. Simulation results were presented and analysed in the form of velocity and temperature contours. In addition, the surface-averaged heat transfer coefficient values for the whole insert length were computed and compared with the literature experimental data. Good compliance of the LES simulation results with the experimental correlation was obtained.

Go to article

Authors and Affiliations

Halina Murasiewicz
Barbara Zakrzewska
Download PDF Download RIS Download Bibtex

Abstract

On the basis of mathematical modeling of fluid flow in vortex devices verification of use of detached-eddy simulation method in the swirling flows in vortex chamber superchargers is made. Research of a flow with use of different turbulence models was made for vortex chamber supercharger in two working points of the characteristic: with the open exit channel and closed. Verification has been spent on integrated parameters, and also on kinematic, by comparison of static pressure value of on the top end cover of the device. It is received that the hybrid turbulence model DES does not allow, as well as model SST precisely to predict value of vacuum on an axis of the vortex chamber. The error makes an order of 20 %. However, DES predicts almost correct, on 20 % big, than model SST, values of vacuum on an axis in a throat axial diffuser on an input in the vortex chamber. Besides, by means of DES it is possible to describe more adequately unsteady structures near to an axis of the vortex chamber, and also vortex core precession that does not allow to make SST turbulence model. By optimization of vortex devices, and vortex chamber superchargers in particular, simulation time essentially is better to use SST turbulence model with rotation-curvature correction.
Go to article

Authors and Affiliations

A. Rogovyi
Download PDF Download RIS Download Bibtex

Abstract

An important phenomenon of delta wing is the mechanism of vortex core, which indicates the increase in lifting force until the occurrence of the vortex breakdown. The computational fluid dynamics (CFD) is very helpful in visualizing and providing analysis of the detailed data. The use of turbulent models will affect the quality of results in obtaining the vortex breakdown phenomenon. This study used several models of turbulence to capture the occurrence of vortex breakdown and compare it with experiments using water tunnel test facility. The results show that all turbulence models give good results at a low angle of attack (AoA), but at a high AoA the DES model gives the results closest to experimental ones with Cl error value of about 1 %. Taking into account the time required and the acceptable level of accuracy, the use of SST and k-ω models is an alternative option for use in the detection of vortex breakdown.
Go to article

Authors and Affiliations

Setyawan Bekti Wibowo
Sutrisno Sutrisno
Tri Agung Rohmat
Download PDF Download RIS Download Bibtex

Abstract

This paper presents a numerical analysis on turbulent flow and forced-convection characteristics of rectangular solar air heater tube fitted with staggered, transverse, V-shape, modern obstacles on the heated walls. Air, whose Prandtl number is 0.71, is the working fluid used, and the Reynolds number considered equal to 6×103. The governing flow equations are solved using a finite volume approach and the semi-implicit pressure linked equation (SIMPLE) algorithm. With regard to the flow characteristics, the quadratic upstream interpolation for convective kinetics differencing scheme (QUICK) was applied, and a second-order upwind scheme (SOU) was used for the pressure terms. The dynamic thermo-energy behavior of the V-shaped baffles with various flow attack angles, i.e., 50°, 60°, 70°, and 80° are simulated, analyzed, and compared with those of the conventional flat rectangular baffles with attack value of 90°. In all situations, the thermal transfer rate was found to be much larger than unity; its maximum value was around 3.143 for the flow attack angle of 90° and y = H/2.

Go to article

Authors and Affiliations

Younes Menni
Ali J. Chamkha
Chafika Zidani
Boumédiène Benyoucef
Download PDF Download RIS Download Bibtex

Abstract

As the cost of fuel rises, designing efficient solar air heaters (SAH) becomes increasingly important. By artificially roughening the absorber plate, solar air heaters’ performance can be augmented. Turbulators in different forms like ribs, delta winglets, vortex generators, etc. have been introduced to create local wall turbulence or for vortex generation. In the present work, a numerical investigation on a solar air heater has been conducted to examine the effect of three distinct turbulators (namely D-shaped, reverse D- and U-shaped) on the SAH thermo-hydraulic performance. The simulation has been carried out using the computational fluid dynamics, an advanced and modern simulation technique for Reynolds numbers ranging from 4000 to 18000 (turbulent airflow). For the purpose of comparison, constant ratios of turbulator height/hydraulic diameter and pitch/turbulator height, of 0.021 and 14.28, respectively, were adopted for all SAH configurations. Furthermore, the fluid flow has also been analyzed using turbulence kinetic energy and velocity contours. It was observed that the U-shaped turbulator has the highest value of Nusselt number followed by D-shaped and reverse D-shaped turbulators. However, in terms of friction factor, the D-shaped configuration has the highest value followed by reverse D-shaped and U-shaped geometries. It can be concluded that among all SAH configurations considered, the U-shaped has outperformed in terms of thermohydraulic performance factor.
Go to article

Authors and Affiliations

Abhishek Ghildyal
1
Vijay Singh Bisht
1
Prabhakar Bhandari
2
Kamal Singh Rawat
3

  1. Veer Madho Singh Bhandari Uttarakhand Technical University, Faculty of Technology, Dehradun 248007, India
  2. K.R. Mangalam University, School of Engineering and Technology, Department of Mechanical Engineering, Gurugram, Haryana 122103, India
  3. Meerut Institute of Engineering and Technology, Mechanical Engineering Department, Meerut 250005, India
Download PDF Download RIS Download Bibtex

Abstract

Local weather conditions have an impact on the availability of free-space optical (FSO) communication. The variation in meteorological parameters, such as temperature, humidity, and wind speed, leads to variations of the refractive index along the transmission path. These refractive index inhomogeneities produced by atmospheric turbulence induce optical turbulence which is responsible for random fluctuations in the intensity of the laser beam that carries the signal (irradiance) called scintillations that can significantly degrade the performance of FSO systems. This paper aims to investigate the feasibility of deploying FSO communication technology under scintillation effects in any urban region and atmospheric environment. To achieve that, firstly by utilizing the Hufnagel-Vally day with the Sadot and Kopeika models together, the scintillation strength for a specified region, Sulaimani City in north-eastern Iraq as an example, has been estimated through the calculation of the refractive index structure parameter (Cn2) over a period of 10 years and it was found to be at the strong turbulence level. Secondly, from the same estimated parameter, the scintillation attenuation of the signal carrying the laser beam intensity can be calculated to investigate the feasibility of FSO communication using Optysistem-7 software. The optimal link distance for north-eastern Iraq (Sulaimani City) has been found to be within the limit of about 5.5 km. Analysing the max. Q-factor, bit-error rate and signal to noise ratio for an average of 120 months between 2013–2022 assessed the best and worst seasons for FSO.
Go to article

Authors and Affiliations

Aras S. Mahmood
1

  1. Physics Department, College of Education, University of Sulaimani, Sulaimani, Kurdistan Region / Iraq
Download PDF Download RIS Download Bibtex

Abstract

In the presented work, the numerical simulations results of the liquid steel flow in the one strand tundish were shown. Influence of the modification and immersion depth in the liquid steel of the ladle shroud and subflux turbulence controller on hydrodynamic structure of the liquid steel movement in the working space of tundish were examined. The ladle shroud shape modification consisted on the decompression and compression of the main supplying stream of the tundish. The mathematical model used in the numerical simulations through physical modeling and industrial trials were validated. The numerical simulation results (using four variants of the modified ladle shroud immersion depth in the liquid steel) in the isothermal conditions using laboratory experiments on the water model were verified. Whereas, the numerical simulation results (using one of the tundish research variant) for non-isothermal were compared with the results from the industrial measurements. Three turbulence models: Realizable k-ε, RNG k-ε and SST k-ω were used in the computer calculations (performed via the Ansys-Fluent computer program). In order to obtain the actual view of the liquid steel flow hydrodynamic structure in the examined tundish for the two mathematical models using different turbulence models, which were most similar to the laboratory experiments and industrial measurements, the numerical simulations were performed in the non-isothermal conditions. The application in the computer calculations of the SST k-ω turbulence model caused the smallest differences between the numerical simulations, laboratory experiments and industrial measurements. Performed tests showed that ladle shroud can be used as a flow control device and the modified ladle shroud immersion at a depth of 0.1 m in the liquid steel caused the shortest range of the transition zone among the tested cases.

Go to article

Authors and Affiliations

M. Bartosiewicz
A. Cwudziński
ORCID: ORCID
Download PDF Download RIS Download Bibtex

Abstract

The homogeneity of an immiscible liquid–liquid system was investigated in a baffled vessel agitated by a Rushton turbine. The dispersion homogeneity was analyzed by comparing Sauter mean diameters and drop size distribution (DSD) determined in different measured regions for various impeller speeds. The sizes of droplets were obtained by the in-situ measurement technique and by the Image Analysis (IA) method. Dispersion kinetics was successfully fitted with Hong and Lee (1983) model. The effect of intermittency turbulence on drop size reported by Bałdyga and Podgórska (1998) was analyzed and the multifractal exponent ������ was evaluated.
Go to article

Bibliography

Bałdyga J., Bourne J.R., 1993. Drop breakup and intermittent turbulence. J. Chem. Eng. Japan, 26, 738–741. DOI: 10.1252/jcej.26.738.

Bałdyga J., Bourne J.R., 1995. Interpretation of turbulent mixing using fractals and multifractals. Chem. Eng. Sci., 50, 381–400. DOI: 10.1016/0009-2509(94)00217-F.

Bałdyga J., PodgórskaW., 1998. Drop break-up in intermittent turbulence. Maximum stable drop size and transient sizes of drops. Can. J. Chem. Eng., 76, 456–470. DOI: 10.1002/cjce.5450760316.

Bucciarelli E., Formánek R., Kysela B., Fort I., Šulc R., 2019. Dispersion kinetics in mechanically agitated vessel. EPJ Web Conf., 213, 02008. DOI: 10.1051/epjconf/201921302008.

Chen H.T., Middleman S., 1967. Drop size distribution in agitated liquid–liquid systems. AIChE J., 13, 989–995. DOI: 10.1002/aic.690130529.

Formánek R., Kysela B., Šulc R., 2019a. Drop size evolution kinetics in a liquid–liquid dispersions system in a vessel agitated by a Rushton turbine. Chem. Eng. Trans., 74, 1039–1044. DOI: 10.3303/CET1974174.

Formánek R., Kysela B., Šulc R., 2019b. Image analysis of particle size: effect of light source type. EPJ Web Conf., 213, 02021. DOI: 10.1051/epjconf/201921302021.

Formánek R., Šulc R., 2019c. Dispersion of immiscible liquid–liquid system in a vessel agitated by a Sawtooth impeller: Drop size time evolution. Proceedings of the International Conference Experimental Fluid Mechanics 2019. Franzensbad, Czech Republic, 19–22 November 2019, 136–139.

Formánek R., Šulc R., 2020. The liquid–liquid dispersion homogeneity in a vessel agitated by a high-shear sawtooth impeller. Processes, 8, 1012. DOI: 10.3390/pr8091012.

Hinze J.O., 1955. Fundamentals of the hydrodynamic mechanism of splitting in dispersion processes. AIChE J., 1, 289–295. DOI: 10.1002/aic.690010303.

Hong P.O., Lee J.M., 1983. Unsteady-state liquid–liquid dispersions in agitated vessels. Ind. Eng. Chem. Process Des. Dev., 22, 130–135. DOI: 10.1021/i200020a021.

Jasikova D., Kotek M., Kysela B., Sulc R., Kopecky V., 2018. Compiled visualization with IPI method for analysing of liquid–liquid mixing process. EPJ Web Conf., 180, 02039. DOI: 10.1051/epjconf/201818002039.

Khalil A., Puel F., Chevalier Y., Galvan J.-M., Rivoire A., Klein J.-P., 2010. Study of droplet size distribution during an emulsification process using in situ video probe coupled with an automatic image analysis. Chem. Eng. J., 165, 946–957. DOI: 10.1016/j.cej.2010.10.031.

Kolmogorov A.N., 1949. On the breakage of drops in a turbulent flow. Dokl. Akad. Nauk SSSR, 66, 825–828. Kraume M., Gäbler A., Schulze K., 2004. Influence of physical properties on drop size distribution of stirred liquid–liquid dispersions. Chem. Eng. Technol., 27, 330–334. DOI: 10.1002/ceat.200402006.

Maaß S., Kraume M., 2012. Determination of breakage rates using single drop experiments. Chem. Eng. Sci., 70, 146–164. DOI: 10.1016/j.ces.2011.08.027.

Malík M., Primas J., Kotek M., Jašíková D., Kopecký V., 2019. Mixing of two immiscible phases measured by industrial electrical impedance tomography system. Mech. Ind., 20, 707. DOI: 10.1051/meca/2019081.

Maluta F., Montante G., Paglianti A., 2020. Analysis of immiscible liquid–liquid mixing in stirred tanks by Electrical Resistance Tomography. Chem. Eng. Sci., 227, 115898. DOI: 10.1016/j.ces.2020.115898.

Pacek A.W., Chamsart S, Nienow A.W., Bakker A., 1999. The influence of impeller type on mean drop size and drop size distribution in an agitated vessel. Chem. Eng. Sci., 54, 4211–4222. DOI: 10.1016/S0009-2509(99)00156-6.

Rodgers T.L., Cooke M., 2012. Correlation of drop size with sheat tip speed. 14��ℎ European Conference on Mixing. Warszawa, Poland, 10–13 September 2012, 407–412.

Šulc R., Ditl P., Fort I., Jašíkova D., Kotek M., Kopecký V., Kysela B., 2017. Local velocity scaling in T400 vessel agitated by Rushton turbine in a fully turbulent region. EPJ Web Conf., 143, 02120. DOI: 10.1051/epjconf/201714302120.

Šulc R., Pešava V., Ditl P., 2015. Local turbulent energy dissipation rate in a vessel agitated by a Rushton turbine. Chem. Process Eng., 36, 135–149. DOI: 10.1515/cpe-2015-0011.

Zhou G, Kresta S.M., 1998. Evolution of drop size distribution in liquid–liquid dispersions for various impellers. Chem. Eng. Sci., 53, 2099–2113. DOI: 10.1016/S0009-2509(97)00437-5.
Go to article

Authors and Affiliations

Roman Formánek
1
Radek Šulc
1

  1. Czech Technical University in Prague, Faculty of Mechanical Engineering, Department of Process Engineering, Technická 4, 160 00 Prague, Czech Republic
Download PDF Download RIS Download Bibtex

Abstract

Underwater Wireless Optical Communication (UWOC) offers significant research prospective with major challenges in the design and implementation. UWOC is capable of providing high rate of data transmission across large distances. This paper attempts to focus on the intricacies of practical implementations and open research issues of UWOC systems. Critical advances and progresses made in the field, modelling techniques and link design challenges are summarised. The purpose of this review is to give suggestions towards feasible and reliable UWOC design with improved performance. Finally the major points are summarized so that it will assist the future research in UWOC.
Go to article

Authors and Affiliations

Lenin Joseph
1
Sangeetha Anandan
1

  1. VIT University, Vellore, India
Download PDF Download RIS Download Bibtex

Abstract

Underwater wireless optical communication is the best alternative for many applications especially for high bandwidth data communication between underwater objects and vehicles. The implementation of coding scheme along with advanced modulation technique and equalisation methods is identified as a key research scope for enhancing the performance of the system. In this paper, the coded generalised frequency division multiplexing (GFDM) technology is employed to provide high-data rates and less out-of-band emission. The Bose-Chaudhuri-Hocquenghem (BCH) and Reed-Solomon (RS) coding schemes along with equalisation techniques namely normalised least mean square (NLMS)-based decision feedback equalisers (DFE), minimum mean square error (MMSE) and zero forcing (ZF) are utilized to reduce inter symbol interference (ISI). The bit error rate (BER) performance is evaluated in the presence of pointing error (PE) and turbulence using Monte Carlo channel modelling simulations. The results showed that RS coding with NLMS-DFE outperforms other techniques and achieves a BER of roughly 10−5 with a signal-to-noise ratio levels below 20 dB. The simulation results demonstrate that RS code with 15 total symbols per code word and 3 data symbols, i.e., RS (15, 3) and BCH code with 31 total symbols in a code word and 6 data symbols, i.e., BCH (31, 6) provided the best error performance among other coding schemes employed. It is inferred that RS (15, 3) coded 2 × 2 multiple input multiple output systems with NLMS-DFE achieved a BER value of 1.1925 ×  10−5 at 11 dB which is 16 dB less than uncoded system. Thus, the coded GFDM improves overall BER performance and has the potential to provide higher reliability for internet of underwater things (IoUT) applications.
Go to article

Authors and Affiliations

R. Hema
1
Ananthi A.
Diana D. C.
1

  1. Department of Electronics and Communication Engineering, Easwari Engineering College, 162 Bharathi Salai, Ramapuram, Chennai, Tamil Nadu 600089, India

This page uses 'cookies'. Learn more