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Abstract

Detailed studies have suggested that the critical heat flux in the form of dryout in minichannels occurs when the combined effects of entrainment, deposition, and evaporation of the film make the film flow rate go gradually and smoothly to zero. Most approaches so far used the mass balance equation for the liquid film with appropriate formulations for the rate of deposition and entrainment respectively. It must be acknowledged that any discrepancy in determination of deposition and entrainment rates, together with cross-correlations between them, leads to the loss of accuracy of model predictions. Conservation equations relating the primary parameters are established for the liquid film and vapor core. The model consists of three mass balance equations, for liquid in the film as well as two-phase core and the gas phase itself. These equations are supplemented by the corresponding momentum equations for liquid in the film and the two-phase core. Applicability of the model has been tested on some experimental data.

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Authors and Affiliations

Dariusz Mikielewicz
Jan Wajs
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Abstract

The paper presents experimental studies on boiling heat transfer in rectangular minichannels. The investigations focus on the transition from single phase forced convection to nucleate boiling, i.e., in the zone of boiling incipience. The experiment has been carried out with FC-72, R-123 and R-11 at the Reynolds number below 4700, corresponding to mass flow rate range 95-710 kg/(m s). The main part of the test section is a minichannel of pre-set depth from 0.7 to 2 mm and width (20, 40 and 60 mm), with different spatial orientations from vertical to horizontal and 30% inclination angle adjustment. The objective of the paper includes the impact of selected parameters (liquid flow velocity, pressure and inlet liquid subcooling, channel dimensions and spatial orientation) on the boiling incipience in minichannels. The investigations are intended to develop a correlation for the calculations of the Nusselt number under the conditions of boiling incipience in the minichannel as a function of changeable parameters.
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Authors and Affiliations

Magdalena Piasecka
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Abstract

In the paper presented is the analysis of the results of calculations using a model to predict flow boiling of refrigerants such as R134a, R600a and R290. The latter two fluids were not used in the development of the model semiempirical correction. For that reason the model was verified with present experimental data. The experimental research was conducted for a full range of quality variation and a relatively wide range of mass velocity. The aim of the present study was also to test the sensitivity of developed model to a selection of the model of two-phase flow multiplier and the nonadiabatic effects. For that purpose two models have been analysed namely the one due to Müller-Steinhagen and Heck, and Friedel. In addition, the work shows the importance of taking surface tension into account in the calculation of the flow structure.
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Authors and Affiliations

Dariusz Mikielewicz
Blanka Jakubowska
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Abstract

Experimental investigation of heat transfer during pool boiling of two nanofluids, i.e. water-Al2O3 and water-Cu has been carried out. Nanoparticles were tested at the concentration of 0.01%, 0.1%, and 1% by weight. The horizontal smooth stainless steel tubes having 10 mm OD and 0.6 mm wall thickness formed the test heater. The experiments have been performed to establish the influence of nanofluids concentration on heat transfer characteristics during boiling at different absolute operating pressure values, i.e. 200 kPa, ca. 100 kPa (atmospheric pressure) and 10 kPa. It was established that independent of nanoparticle materials (Al2O3 and Cu) and their concentration, an increase of operating pressure enhances heat transfer. Generally, independent of operating pressure, sub- and atmospheric pressure, and overpressure, an increase of nanoparticle concentration caused heat transfer augmentation.

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Authors and Affiliations

Janusz Cieśliński
Tomasz Kaczmarczyk
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Abstract

The heat transfer coefficient during the pool boiling on the outside of a horizontal tube can be predicted by correlations. Our choice was based on ten correlations known from the literature. The experimental data were recovered from the recent work, for different fluids used. An evaluation was made of agreement between each of the correlations and the experimental data. The results of the present study firstly showed a good reliability for the correlations of Labuntsov [10], Stephan and Abdeslam [11] with deviations of 20% and 27%, respectively. Also, the results revealed acceptable agreements for the correlations of Kruzhlin [6], Mc Nelly [7] and Touhami [15] with deviations of 26%, 29% and 29% respectively. The remaining correlations showed very high deviations from the experimental data. Finally, improvements have been made in the correlations of Shekriladze [12] and Mostinski [9], and a new correlation was proposed giving convincing results.
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Bibliography

[1] I.L. Pioro, W. Rohsenow, and S.S. Doerffer. Nucleate pool-boiling heat transfer. II: Assessment of prediction methods. International Journal of Heat and Mass Transfer, 47(23):5045–5057, 2004. doi: 10.1016/j.ijheatmasstransfer.2004.06.020.
[2] A. Sathyabhama and R.N. Hegde. Prediction of nucleate pool boiling heat transfer coefficient. Thermal Science, 14(2):353–364, 2010. doi: 10.2298/TSCI1002353S.
[3] T. Baki, A. Aris, and M. Tebbal. Investigations on pool boiling of refrigerant R141b outside a horizontal tube, Archive of Mechanical Engineering, 68(1):77–92, 2021. doi: 10.24425/ame.2021.137042.
[4] T. Baki. Survey on the nucleate pool boiling of hydrogen and its limits. Journal of Mechanical and Energy Engineering, 4(2):157–166, 2020. doi: 10.30464/jmee.2020.4.2.157.
[5] T. Baki. Pool boiling of ammonia, assessment of correlations. International Journal of Air-Conditioning and Refrigeration, 29(02):2150012, 2021. doi: 10.1142/S2010132521500127.
[6] G.N. Kruzhilin. Free-convection transfer of heat from a horizontal plate and boiling liquid. Doklady AN SSSR (Reports of the USSR Academy of Sciences), 58(8):1657–1660, 1947.
[7] M.J. Mc Nelly. A correlation of rates of heat transfer to nucleate boiling of liquids. Journal of Imperial College Chemical Engineering Socoiety, 7:187–34, 1953.
[8] H.K. Forster, and N. Zuber. Dynamics of vapor bubbles and boiling heat transfer. AIChE Journal, 1(4):531–535, 1955. doi: 10.1002/aic.690010425.
[9] I.L. Mostinski. Application of the rule of corresponding states for calculation of heat transfer and critical heat flux. Teploenergetika, 4(4):66–71, 1963.
[10] D.A. Labuntsov. Heat transfer problems with nucleate boiling of liquids. Thermal Engineering, 19(9):21–28, 1972.
[11] K. Stephan, and M. Abdelsalam. Heat-transfer correlations for natural convection boiling. International Journal of Heat and Mass Transfer, 23(1):73–87, 1980. doi: 10.1016/0017-9310(80)90140-4.
[12] I.G. Shekriladze. Boiling heat transfer: mechanisms, models, correlations and the lines of further research. The Open Mechanical Engineering Journal, 2:104–127, 2008. doi: 10.2174/1874155X00802010104.
[13] V.V. Yagov. Nucleate boiling heat transfer: Possibilities and limitations of theoretical analysis. Heat and Mass Transfer, 45(7):881–892, 2009. doi: 10.1007/s00231-007-0253-8.
[14] S. Fazel and S. Roumana. Pool boiling heat transfer to pure liquids. In WSEAS Conf, 2010.
[15] T. Baki, A. Aris, and M. Tebbal. Proposal for a correlation raising the impact of the external diameter of a horizontal tube during pool boiling. International Journal of Thermal Sciences, 84:293–299, 2014. doi: 10.1016/j.ijthermalsci.2014.05.023.
[16] M.G. Kang. Effect of surface roughness on pool boiling heat transfer. International Journal of Heat and Mass Transfer, 43(22):4073–4085, 2000. doi: 10.1016/S0017-9310(00)00043-0.
[17] M.G. Kang. Local pool boiling coefficients on a horizontal tubes. Journal of Mechanical Science and Technology, 19(3):860–869, 2005. doi: 10.1007/BF02916134.
[18] J.S. Mehta and S.G. Kandlikar. Pool boiling heat transfer enhancement over cylindrical tubes with water at atmospheric pressure, Part II: Experimental results and bubble dynamics for circumferential V-groove and axial rectangular open microchannels. International Journal of Heat and Mass Transfer, 64:1216–1225, 2013. doi: 10.1016/j.ijheatmasstransfer.2013.04.004.
[19] S.K. Das, N. Putra, and W. Roetzel. Pool boiling of nano-fluids on horizontal narrow tubes. International Journal of Multiphase Flow, 29(8):1237–1247, 2003. doi: 10.1016/S0301-9322 (03)00105-8.
[20] G. Prakash Narayan, K.B. Anoop, G. Sateesh, and S.K. Das. Effect of surface orientation on pool boiling heat transfer of nanoparticle suspensions. International Journal of Multiphase Flow, 34(2):145–160, 2008. doi: 10.1016/j.ijmultiphaseflow.2007.08.004.
[21] D. Gorenflo, F. Gremer, E. Danger, and A. Luke. Pool boiling heat transfer to binary mixtures with miscibility gap: Experimental results for a horizontal copper tube with 4.35~mm O.D. Experimetal Thermal Fluides Sciences, 25(5):243–254, 2001. doi: 10.1016/S0894-1777(01)00072-3.
[22] Z.H. Liu and Y.H. Qiu. Enhanced boiling heat transfer in restricted spaces of a compact tube bundle with enhanced tubes. Applied Thermal Engineering, 22(17):1931–1941, 2002. doi: 10.1016/S1359-4311(02)00111-4.
[23] Y.H. Qiu and Z.H. Liu. Boiling heat transfer of water on smooth tubes in a compact staggered tube bundle. Applied Thermal Engineering, 24(10):1431–1441, 2004. doi: 10.1016/j.applthermaleng.2003.11.021.
[24] K.G. Rajulu, R. Kumar, B. Mohanty, and H. K. Varma. Enhancement of nucleate pool boiling heat transfer coefficient by reentrant cavity surfaces. Heat and Mass Transfer, 41(2):127–132, 2004. doi: 10.1007/s00231-004-0526-4.
[25] A. Fazel, A. Safekordi, and M. Jamialahmadi. Pool boiling heat transfer in water/amines solutions. International Journal of Engineering, 21(2):113–130, 2008.
[26] S.M. Peyghambarzadeh, M. Jamialahmadi, S.A. Alavi Fazel, and S. Azizi. Experimental and theoretical study of pool boiling heat transfer to amine solutions. Brazilian Journal of Chemical Engineering, 26:26–33, 2009. doi: 10.1590/S0104-66322009000100004.
[27] S. Bhaumik, V.K. Agarwal, and S.C. Gupta. A generalized correlation of nucleate pool boiling of liquids. Indian Journal of Chemical Technology, 2004.
[28] W.C. Elrod, J.A. Clark, E.R. Lady, and H. Merte. Boiling heat transfer data at low heat flux. Journal of Heat Transfer, 87(C):235–243, 1967.
[29] Y. Chen, M. Groll, R. Mertz, and R. Kulenovic. Pool boiling heat transfer of propane, isobutane and their mixtures on enhanced tubes with reentrant channels. International Journal of Heat and Mass Transfer, 48(11):2310–2322, 2005. doi: 10.1016/j.ijheatmasstransfer.2004.10.037.
[30] D. Jung, H. Lee, D. Bae, and S. Oho. Nucleate boiling heat transfer coefficients of flammable refrigerants, International Journal of Refrigeration, 27(4):409–414, 2004. doi: 10.1016/j.ijrefrig.2003.11.007.
[31] J.X. Zheng, G.P. Jin, M.C. Chyu, and Z.H. Ayub. Boiling of ammonia/lubricant mixture on a horizontal tube in a flooded evaporator with inlet vapor quality. {\em Experimental Thermal Fluides Sciences, 30(3):223–231, 2006. doi: 10.1016/j.expthermflusci.2005.06.001.
[32] V. Trisaksri, and S. Wongwises. Nucleate pool boiling heat transfer of TiO2-R141b nanofluids. International Journal of Heat and Mass Transfer, 52(5-6):1582–1588, 2009. doi: 10.1016/j.ijheatmasstransfer.2008.07.041.
[33] J.M.S. Jabardo, G. Ribatski, and E. Stelute. Roughness and surface material effects on nucleate boiling heat transfer from cylindrical surfaces to refrigerants R-134a and R-123. Experimetal Thermal Fluides Sciences, 33(4):579–590, 2009. doi: 10.1016/j.expthermflusci.2008.12.004.
[34] D. Jung, K. An, and J. Park. Nucleate boiling heat transfer coefficients of HCFC22, HFC134a, HFC125 and HFC32 on various enhanced tubes. International Journal of Refrigeration, 27(2):202–206, 2004. doi: 10.1016/S0140-7007(03)00124-5.
[35] S.P. Rocha, O. Kannengieser, E.M. Cardoso, and J.C. Passos. Nucleate pool boiling of R-134a on plain and micro-finned tubes. International Journal of Refrigeration, 36(2):456–464, 2013. doi: 10.1016/j.ijrefrig.2012.11.031.
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Authors and Affiliations

Touhami Baki
1
ORCID: ORCID
Djamel Sahel
2
ORCID: ORCID

  1. Mechanical Faculty, Gaseous Fuels and Environment Laboratory, USTO-MB, El-M'Naouer, Oran, Algeria
  2. Department of Technical Sciences, Amar Telidji of Laghouat, Algeria
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Abstract

In the paper the experimental analysis of dryout in small diameter channels is presented. The investigations were carried out in vertical pipes of internal diameter equal to 1.15 mm and 2.3 mm. Low-boiling point fluids such as SES36 and R123 were examined. The modern experimental techniques were applied to record liquid film dryout on the wall, among the others the infrared camera. On the basis of experimental data an empirical correlation for predictions of critical heat flux was proposed. It shows a good agreement with experimental data within the error band of 30%. Additionally, a unique approach to liquid film dryout modeling in annular flow was presented. It led to the development of the three-equation model based on consideration of liquid mass balance in the film, a two-phase mixture in the core and gas. The results of experimental validation of the model exhibit improvement in comparison to other models from literature.

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Authors and Affiliations

Jan Wajs
Dariusz Mikielewicz
Michał Gliński
ORCID: ORCID
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Abstract

The paper deals with pool boiling of water-Al2O3and water-Cu nanofluids on rough and porous coated horizontal tubes. Commercially available stainless steel tubes having 10 mm outside diameter and 0.6 mm wall thickness were used to fabricate the test heater. The tube surface was roughed with emery paper 360 or polished with abrasive compound. Aluminium porous coatings of 0.15 mm thick with porosity of about 40% were produced by plasma spraying. The experiments were conducted under different absolute operating pressures, i.e., 200, 100, and 10 kPa. Nanoparticles were tested at the concentration of 0.01, 0.1, and 1% by weight. Ultrasonic vibration was used in order to stabilize the dispersion of the nanoparticles. It was observed that independent of operating pressure and roughness of the stainless steel tubes addition of even small amount of nanoparticles augments heat transfer in comparison to boiling of distilled water. Contrary to rough tubes boiling heat transfer coefficient of tested nanofluids on porous coated tubes was lower compared to that for distilled water while boiling on porous coated tubes. A correlation equation for prediction of the average heat transfer coefficient during boiling of nanofluids on smooth, rough and porous coated tubes is proposed. The correlation includes all tested variables in dimensionless form and is valid for low heat flux, i.e., below 100 kW/m2.

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Authors and Affiliations

Tomasz Z. Kaczmarczyk
Janusz T. Cieśliński
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Abstract

In the paper a method developed earlier by authors is applied to calculations of pressure drop and heat transfer coefficient for flow boiling and also flow condensation for some recent data collected from literature for such fluids as R404a, R600a, R290, R32,R134a, R1234yf and other. The modification of interface shear stresses between flow boiling and flow condensation in annular flow structure are considered through incorporation of the so called blowing parameter. The shear stress between vapor phase and liquid phase is generally a function of nonisothermal effects. The mechanism of modification of shear stresses at the vapor-liquid interface has been presented in detail. In case of annular flow it contributes to thickening and thinning of the liquid film, which corresponds to condensation and boiling respectively. There is also a different influence of heat flux on the modification of shear stress in the bubbly flow structure, where it affects bubble nucleation. In that case the effect of applied heat flux is considered. As a result a modified form of the two-phase flow multiplier is obtained, in which the nonadiabatic effect is clearly pronounced.

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Authors and Affiliations

Dariusz Mikielewicz
Jarosław Mikielewicz
Rafał Andrzejczyk
Blanka Jakubowska
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Abstract

Technology advancements entail a necessity to remove huge amounts of heat produced by today’s electronic devices based on highly integrated circuits, major generators of heat. Heat transfer to boiling liquid flowing through narrow minichannels is a modern solution to the problem of heat transfer enhancement. The study was conducted for FC-72 boiling in a rectangular, vertical and asymmetrically heated minichannel that had depths of 0.5-1.5 mm, a width of 20 mm and a length of 360 mm. The heat flux increased and decreased within the range of 58.3-132.0 kWm−2, the absolute pressure ranged from 0.116 to 0.184 MPa and the mass flux was 185-1139.2 kgm−2s−1. The boiling process took place on a flat vertical heating surface made of Haynes-230 0.1 mm thick acid-proof rolled plate with the surface roughness of 121 μm.

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Authors and Affiliations

Robert Kaniowski
Mieczysław Poniewski
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Abstract

In the paper presented are the results of calculations using authors own model to predict heat transfer coefficient during flow boiling of carbon dioxide. The experimental data from various researches were collected. Calculations were conducted for a full range of quality variation and a wide range of mass velocity. The aim of the study was to test the sensitivity of the in-house model. The results show the importance of taking into account the surface tension as the parameter exhibiting its importance in case of the flow in minichannels as well as the influence of reduced pressure. The calculations were accomplished to test the sensitivity of the heat transfer model with respect to selection of the appropriate two-phase flow multiplier, which is one of the elements of the heat transfer model. For that purpose correlations due to Müller-Steinhagen and Heck as well as the one due to Friedel were considered. Obtained results show a good consistency with experimental results, however the selection of two-phase flow multiplier does not significantly influence the consistency of calculations.

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Authors and Affiliations

Dariusz Mikielewicz
Blanka Jakubowska
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Abstract

Miniature heat exchangers are used to provide higher cooling capacity for new technologies. This means a reduction in their size and cost but the identical power. The paper presents the method for determination of boiling heat transfer coefficient for a rectangular minichannel of 0.1 mm depth, 40 mm width and 360 mm length with asymmetric heating. Experimental research has focused on the transition from single phase forced convection to nucleate boiling, i.e., the zone of boiling incipience. The ‘boiling front’ location has been determined from the temperature distribution of the heated wall obtained from liquid crystal thermography. The experiment has been carried out with R-123, mass flux 220 kg/(m2s), pressure at the channel inlet 340 kPa. Local values of heat transfer coefficient were calculated on the basis of empirical data from the experiment following the solution of the two-dimensional inverse heat transfer problem. This problem has been solved with the use of the finite element method in combination with Trefftz functions. Temperature approximates (linear combinations of Trefftz functions) strictly fulfill the governing equations. In presented method the inverse problem is solved in the same way as the direct problem. The results confirmed that considerable heat transfer enhancement takes place at boiling incipience in the minichannel flow boiling. Moreover, under subcooling boiling, local heat coefficients exhibit relatively low values.

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Authors and Affiliations

Magdalena Piasecka
Beata Maciejewska
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Abstract

In the present research, an experimental investigation was conducted to assess the heat transfer coefficient of aqueous citric acid mixtures. The experimental facility provides conditions to assess the influence of various operating conditions such as the heat flux (0–190 kW/m2), mass flux (353–1059 kg/m2s) and the concentration of citric acid in water (10%– 50% by volume) with a view to measure the subcooled flow boiling heat transfer coefficient of the mixture. The results showed that two main heat transfer mechanisms can be identified including the forced convective and nucleate boiling heat transfer. The onset point of nucleate boiling was also identified, which separates the forced convective heat transfer domain from the nucleate boiling region. The heat transfer coefficient was found to be higher in the nucleate boiling regime due to the presence of bubbles and their interaction. Also, the influence of heat flux on the heat transfer coefficient was more pronounced in the nucleate boiling heat transfer domain, which was also attributed to the increase in bubble size and rate of bubble formation. The obtained results were also compared with those theoretically obtained using the Chen type model and with some experimental data reported in the literature. Results were within a fair agreement of 22% against the Chen model and within 15% against the experimental data.

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Authors and Affiliations

Mohammad Amin Abdolhossein Zadeh
Shima Nakhjavani
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Abstract

Batch dark fermentation of wheat straw and boiled potato wastes at volatile suspended solids (VSS) 5 g VSS/L are examined and compared. Investigations on dark fermentation of potatowastes and wheat straw were carried out at different pH and OFR (oxygen flow rate) values and inoculum pretreatment. The obtained hydrogen yield from waste potato was 70 mL/g VSS, while for hydrolysed wheat straw it amounted to 80 mL/g VSS. The optimum conditions for potato dark fermentation are acidic pH 6.0 and OFR 1.0 mL/h, while for the wheat straw, optimal conditions are pH 6.4 and OFR 4.6 mL/h. The comparison revealed a significant difference in hydrogen production due to the type of substrate, inoculum stressing and DF conditions applied.
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Bibliography

Achinas S., Li Y., Achinas V., Euverink G.J.W., 2019. Biogas potential from the anaerobic digestion of potato peels: Process performance and kinetics evaluation. Energies, 12, 2311. DOI: 10.3390/en12122311.
Aly S.S., Imai T., Hassouna M.S., Kim Nguyen D.M., Higuchi T., Kanno A., Yamamoto K., Akada R., Sekine M., 2018. Identification of factors that accelerate hydrogen production by Clostridium butyricum RAK25832 using casamino acids as a nitrogen source. Int. J. Hydrogen Energy, 43, 5300–5313. DOI: 10.1016/j.ijhydene.2017.08.171.
Bartacek J., Zabranska J., Lens P.N.L., 2007. Developments and constraints in fermentative hydrogen production. Biofuels, Bioprod. Biorefin., 1, 201–214. DOI: 10.1002/bbb.17.
Bundhoo Z.M.A., 2019. Potential of bio-hydrogen production from dark fermentation of crop residues: A review. Int. J. Hydrogen Energy, 44, 17346–17362. DOI: 10.1016/j.ijhydene.2018.11.098.
Chaganti S.R., Kim D.H., Lalman J.A., 2012. Dark fermentative hydrogen production by mixed anaerobic cultures: Effect of inoculum treatment methods on hydrogen yield. Renewable Energy, 48, 117–121. DOI: 10.1016/j.renene.2012.04.015.
Chi C.H., Chen K.W., Huang J.J., Chuang Y.C., Wu M.H., 1995. Gas composition in Clostridium septicum gas gangrene. J. Formos. Med. Assoc., 94, 757–759.
De Cicco A., Jeanty J.-C., 2017. The EU potato sector – statistics on production, prices and trade – Statistics Explained. Statistic Explained. Available at: https://ec.europa.eu/eurostat/statistics-explained/index.php?title= The_EU_potato_sector_-_statistics_on_production,_prices_and_trade.
Dessě P., Lakaniemi A.M., Lens P.N.L., 2017. Biohydrogen production from xylose by fresh and digested activated sludge at 37, 55 and 70 °C. Water Res., 115, 120–129. DOI: 10.1016/j.watres.2017.02.063.
Gallipoli A., Braguglia C.M., Gianico A., Montecchio D., Pagliaccia P., 2020. Kitchen waste valorization through a mild-temperature pretreatment to enhance biogas production and fermentability: Kinetics study in mesophilic and thermophilic regimen. J. Environ. Sci., 89, 167–179. DOI: 10.1016/j.jes.2019.10.016.
Garcia-Bernet D., Steyer J.-P., Bernet N., 2017. Traitement anaérobie des effluents industriels liquides Traitement anaérobie des effluents industriels liquides. Techniques de l’Ingénieur, Réf : J3943 v2.
García Depraect O., Muńoz R., van Lier J.B., Rene E.R., Diaz-Cruces V.F., León Becerril E., 2020. Three-stage process for tequila vinasse valorization through sequential lactate, biohydrogen and methane production. Bioresour. Technol., 307, 123160. DOI: 10.1016/j.biortech.2020.123160.
Han W., Ye M., Zhu A.J., Zhao H.T., Li Y.F., 2015. Batch dark fermentation from enzymatic hydrolyzed food waste for hydrogen production. Bioresour. Technol., 191, 24–29. DOI: 10.1016/j.biortech.2015.04.120.
Hawkes F.R., Hussy I., Kyazze G., Dinsdale R., Hawkes D.L., 2007. Continuous dark fermentative hydrogen production by mesophilic microflora: Principles and progress. Int. J. Hydrogen Energy, 32, 172–184. DOI: 10.1016/j.ijhydene.2006.08.014.
Hernández C., Alamilla-Ortiz Z.L., Escalante A.E., Navarro-Díaz M., Carrillo-Reyes J., Moreno-Andrade I., Valdez- Vazquez I., 2019. Heat-shock treatment applied to inocula for H2 production decreases microbial diversities, interspecific interactions and performance using cellulose as substrate. Int. J. Hydrogen Energy, 44, 13126– 13134. DOI: 10.1016/j.ijhydene.2019.03.124.
Kumar G., Bakonyi P., Periyasamy S., Kim S.H., Nemestóthy N., Bélafi-Bakó K., 2015. Lignocellulose biohydrogen: Practical challenges and recent progress. Renewable Sustainable Energy Rev., 44, 728–737. DOI: 10.1016/j.rser. 2015.01.042.
Laurinavichene T.V., Belokopytov B.F., Laurinavichius K.S., Tekucheva D.N., Seibert M., Tsygankov A.A., 2010. Towards the integration of dark- and photo-fermentative waste treatment. 3. Potato as substrate for sequential dark fermentation and light-driven H2 production. Int. J. Hydrogen Energy, 35, 8536–8543. DOI: 10.1016/j.ijhydene.2010.02.063.
Leszczyński, W., 2000. Jakość ziemniaka konsumpcyjnego. Żywność, Nauka, Technologia, Jakość, Supl., 4(25), 5–27.
Li Y., Zhang Q., Deng L., Liu Z., Jiang H., Wang F., 2018. Biohydrogen production from fermentation of cotton stalk hydrolysate by Klebsiella sp. WL1316 newly isolated from wild carp (Cyprinus carpio L.) of the Tarim River basin. Appl. Microbiol. Biotechnol., 102, 4231–4242. DOI: 10.1007/s00253-018-8882-z.
Moriarty K., 2013. Feasibility study of anaerobic digestion of food waste in St. Bernard, Louisiana. A study prepared in partnership with the Environmental Protection Agency for the RE-Powering America’s Land Initiative: Siting renewable energy on potentially contaminated land and mine sites. National Renewable Energy Laboratory (NREL), Technical Report, NREL/TP-7A30-57082. DOI: 10.2172/1067946.
Nasirian N., Almassi M., Minaei S., Widmann R., 2011. Development of a method for biohydrogen production from wheat straw by dark fermentation. Int. J. Hydrogen Energy, 36, 411–420. DOI: 10.1016/j.ijhydene.2010.09.073.
Paillet F., Maron, A., Moscovi, R., Steyer J.P., Tapia-Venegas E., Bernet N., Trably E., 2019. Improvement of biohydrogen production from glycerol in micro-oxidative environment. Int. J. Hydrogen Energy, 44, 17802– 17812. DOI: 10.1016/j.ijhydene.2019.05.082.
Patel A.K., Debroy A., Sharma S., Saini R., Mathur A., Gupta R., Tuli D.K., 2015. Biohydrogen production from a novel alkalophilic isolate Clostridium sp. IODB-O3. Bioresour. Technol., 175, 291–297. DOI: 10.1016/j.biortech.2014.10.110.
Sekoai P.T., Ayeni A.O., Daramola M.O., 2019. Parametric optimization of biohydrogen production from potato waste and scale-up study using immobilized anaerobic mixed sludge. Waste Biomass Valorization, 10, 1177–1189. DOI: 10.1007/s12649-017-0136-2.
Si B.C., Li J.M., Zhu Z.B., Zhang Y.H., Lu J.W., Shen R.X., Zhang C., 2016. Continuous production of biohythane from hydrothermal liquefied cornstalk biomass via twostage highrate anaerobic reactors. Biotechnol. Biofuels, 9, 254. DOI: 10.1186/s13068-016-0666-z.
Słupek E., Kucharska K., Ge˛bicki J., 2019. Alternative methods for dark fermentation course analysis. SN Appl. Sci., 1, 469. DOI: 10.1007/s42452-019-0488-2.
Sołowski G., Konkol I., Cenian A., 2019a. Perspectives of hydrogen production from corn wastes in Poland by means of dark fermentation. Ecol. Chem. Eng. S, 26, 255–263. DOI: 10.1515/eces-2019-0031.
Sołowski G., Konkol, I., Hrycak B., Czylkowski D., 2019b. Hydrogen and methane production under conditions of anaerobic digestion of key-lime and cabbage wastes. Agritech, 39(3), 243–250. DOI: 10.22146/agritech.35848.
Sołowski G., Konkol I., Cenian A., 2020a. Production of hydrogen and methane from lignocellulose waste by fermentation. A review of chemical pretreatment for enhancing the efficiency of the digestion process. J. Cleaner Prod., 267, 121721. DOI: 10.1016/j.jclepro.2020.121721.
Sołowski G., Konkol I., Cenian A., 2020b. Methane and hydrogen production from cotton waste by dark fermentation under anaerobic and micro-aerobic conditions. Biomass Bioenergy, 138, 105576. DOI: 10.1016/j.biombioe.2020.105576.
Woodward J., Orr M., Cordray K., Greenbaum E., 2000. Enzymatic production of biohydrogen. Nature, 405, 1014–1015. DOI: 10.1038/35016633.
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Authors and Affiliations

Gaweł Sołowski
1
Izabela Konkol
1
Marwa Shalaby
2
Adam Cenian
1

  1. Institute of Fluid-Flow Machinery Polish Academy of Sciences, Physical Aspects of Ecoenergy Department, 14 Fiszera St., 80-231 Gdańsk, Poland
  2. National Research Center in Cairo, Department of Chemical Engineering and Pilot Plant, El Bijouth St., Dokki, Cairo, Egypt 12622
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Abstract

In this experimental investigation, the critical heat flux (CHF) of aqua-based multiwalled carbon nanotube (MWCNT) nanofluids at three different volumetric concentrations 0.2%, 0.6%, and 0.8% were prepared, and the test results were compared with deionized water. Different characterization techniques, including X-ray diffraction, scanning electron microscopy and Fourier transform infrared, were used to estimate the size, surface morphology, agglomeration size and chemical nature of MWCNT. The thermal conductivity and viscosity of the MWCNT at three different volumetric concentrations was measured at a different temperature, and results were compared with deionized water. Although, MWCNT-deionized water nanofluid showed superior performance in heat transfer coefficient as compared to the base fluid. However, the results proved that the critical heat flux is increased with an increase in concentrations of nanofluids.

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Authors and Affiliations

D. Vasudevan
D. Senthil Kumar
A. Murugesan
C. Vijayakumar
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Abstract

In this work we investigate the present capabilities of computational fluid dynamics for wall boiling. The computational model used combines the Euler/Euler two-phase flow description with heat flux partitioning. This kind of modeling was previously applied to boiling water under high pressure conditions relevant to nuclear power systems. Similar conditions in terms of the relevant non-dimensional numbers have been realized in the DEBORA tests using dichlorodifluoromethane (R12) as the working fluid. This facilitated measurements of radial profiles for gas volume fraction, gas velocity, bubble size and liquid temperature as well as axial profiles of wall temperature. After reviewing the theoretical and experimental basis of correlations used in the ANSYS CFX model used for the calculations, we give a careful assessment of the necessary recalibrations to describe the DEBORA tests. The basic CFX model is validated by a detailed comparison to the experimental data for two selected test cases. Simulations with a single set of calibrated parameters are found to give reasonable quantitative agreement with the data for several tests within a certain range of conditions and reproduce the observed tendencies correctly. Several model refinements are then presented each of which is designed to improve one of the remaining deviations between simulation and measurements. Specifically we consider a homogeneous MUSIG model for the bubble size, modified bubble forces, a wall function for turbulent boiling flow and a partial slip boundary condition for the liquid phase. Finally, needs for further model developments are identified and promising directions discussed.
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Authors and Affiliations

Roland Rzehak
Eckhard Krepper
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Abstract

The pool boiling characteristics of dilute dispersions of alumina, zirconia and silica nanoparticles in water were studied. These dispersions are known as nanofluids. Consistently with other nanofluid studies, it was found that a significant enhancement in Critical Heat Flux (CHF) can be achieved at modest nanoparticle concentrations (<0.1% by volume). Buildup of a porous layer of nanoparticles on the heater surface occurred during nucleate boiling. This layer significantly improves the surface wettability, as shown by a reduction of the static contact angle on the nanofluid-boiled surfaces compared with the pure-water-boiled surfaces. CHF theories support the nexus between CHF enhancement and surface wettability changes. This represents a first important step towards identification of a plausible mechanism for boiling CHF enhancement in nanofluids.

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Authors and Affiliations

S.J. Kim
I.C. Bang
J. Buongiorno
L.W. Hu

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