Search results

Filters

  • Journals
  • Authors
  • Keywords
  • Date
  • Type

Search results

Number of results: 39
items per page: 25 50 75
Sort by:
Download PDF Download RIS Download Bibtex

Abstract

The article presents methodology for testing the electric strength of vacuum chambers designed for modern medium voltage switchgear developed by the authors, using two innovative test stands designed and constructed by the research team above. Verification of the correctness of operation of the test stands, as well as the validity of the developed methodology was carried out by performing a series of tests. It was determined that below certain pressure values in the tested chamber (from about 5.0×10 0 Pa for station 1 and for about 4.0×10 -1 Pa for station 2), the electric strength maintains a constant value, which guarantees stable operation of the vacuum chamber. The values of the total measurement uncertainty for the electric strength tests were also estimated.

Go to article

Authors and Affiliations

Paweł Węgierek
ORCID: ORCID
Michał Lech
ORCID: ORCID
Czesław Kozak
Justyna Pastuszak
Download PDF Download RIS Download Bibtex

Abstract

The Centro de Desarrollo Tecnológico del Gas developed a static expansion system to enable the calibration of medium and high vacuum pressure gauges in Colombia. The system can generate pressures between 0.1 Pa and 100 kPa. The characterization tests included the evaluation of pressure stability and desorption rate, a trueness test, and the analysis of the uncertainty budget of the calibration result. The pressure stability test was successfully completed and showed the positive effect of baking on the final pressure in the system. The trueness test allowed concluding that the calibration results with the system are comparable with those obtained with a reference meter traceable to a national metrology institute. The uncertainty budget analysis indicated the dominance of the pressure of the unit under calibration and of the initial pressure in the small tank in different pressure ranges on the uncertainty of the result. A comparison with a Monte Carlo simulation led to the conclusion that in this situation, the GUM (Guide to the Expression of Uncertainty in Measurement) method is not ideal for estimating the uncertainty of the results.
Go to article

Bibliography

[1] Khan,W., Hong, H. H., Satar, T., Ahmed, M., Khan, Z. A.,& Khan, M. Z. (2016). The KRISS primary vacuum gauge calibration standards:Areview. Journal of the Vacuum Society of Japan, 59(8), 222–235.
[2] Astrua, M., Mari, D., & Pasqualin, S. (2019). Improvement of INRiM static expansion system as vacuum primary standard between 10(-4) Pa and 1000 Pa. 19th International Congress of Metrology, 27007. https://doi.org/10.1051/metrology/201927007
[3] Semwal, P., Khan, Z., Dhanani, K. R., Pathan, F. S., George, S., Raval, D. C., Thankey, P. L., Paravastu, Y., & Himabindu, M. (2012). Spinning rotor gauge based vacuum gauge calibration system at the Institute for Plasma Research. Journal of Physics: Conference Series, 390, 012027. https://doi.org/10.1088/1742-6596/390/1/012027
[4] Bergoglio, M., & Calcatelli, A. (2004). Uncertainty evaluation of the IMGC-CNR static expansion system. Metrologia, 41, 278–284. https://doi.org/10.1088/0026-1394/41/4/009
[5] Greenwood, J. C. (2006). Simulation of the operation and characteristics of static expansion pressure standards. Vacuum, 80, 548–553. https://doi.org/10.1016/j.vacuum.2005.09.003
[6] Soriano Cardona, B., Torres Guzmán, J., & Santander Romero, L. (2001). Sistema de referencia nacional para la medición de vacío. Simposio de Metrología CENAM 2001, México.
[7] Bergoglio, M., Calcatelli, A., Marzola, L., & Rumiano, G. (1988). Primary pressure measurements down to 10(-6) Pa. Vacuum, 38(8–10), 887–891. https://doi.org/10.1016/0042-207X(88)90486-1
[8] Fedchak, J. A., Abbott, P. J., & Hendricks, J. H. (2018). Review Article: Recommended practice for calibrating vacuum gauges of the ionization type. Journal of Vacuum Science & Technology A, 36, 030802. https://doi.org/10.1116/1.5025060
[9] Torres Guzmán, J. C., Santander, L. A., & Jousten, K. (2005). Realization of the medium and high vacuum primary standard inCENAM,Mexico.Metrologia, 42(6), S157–S160. https://doi.org/10.1088/0026-1394/42/6/S01
[10] Jousten, K., Röhl, P., & Aranda Contreras, V. (1999). Volume ratio determination in static expansion systems by means of a spinning rotor gauge. Vacuum, 52(4), 491–499. https://doi.org/10.1016/S0042-207X(98)00337-6
[11] Herranz, D., Ruiz, S., & Medina, N. (2009). Volume ratio determination in static expansion systems by means of two pressure balances. XIX IMEKO World Congress, Fundamental and Applied Metrology, Portugal. https://www.imeko2009.it.pt/Papers/FP_280.pdf
[12] Phanakulwijit, S.,&Pitakarnnop, J. (2019). Establishment of Thailand’s national primary vacuum standard by a static expansion method. Journal of Physics: Conference Series, 1380, 012003. https://doi.org/10.1088/1742-6596/1380/1/012003
[13] Jitschin, W. (2002). High-accuracy calibration in the vacuum range 0.3 Pa to 4000 Pa using the primary standard of static gas expansion. Metrologia, 39(3), 249–261. https://doi.org/10.1088/0026-1394/39/3/2
[14] Kangi, R., Ongun, B., & Elkatmis, A. (2004). The new UME primary standard for pressure generation in the range from 9 × 10 -4 Pa to 103 Pa. Metrologia, 41(4), 251–256. https://doi.org/10.1088/ 0026-1394/41/4/005
[15] International Organization for Standardization. (2011). Vacuum gauges – Calibration by direct comparison with a reference gauge ISO Standard No. 3567:2011. https://www.iso.org/standard/59372.html
[16] Antsukova, A. I., Gorobei, V. N., Liubomirov, A. B., Pimenova, A. A.,&Chernyshenko, A. A. (2019). Calibration of measuring instruments of low absolute pressures. IOP Conference Series: Journal of Physics: Conference Series, 1313, 012002. https://doi.org/10.1088/1742-6596/1313/1/012002
[17] Ruiz González, S. (2011). Desarrollo de un nuevo patrón nacional de presión. Desde la columna de mercurio a patrones primarios de vacío [Doctoral dissertation, Universidad de Valladolid]. UVaDOC Repositorio Documental de la Universidad de Valladolid. https://doi.org/10.35376/10324/830
[18] Joint Committee for Guides in Metrology. (2008). Evaluation of measurement data – Guide to the expression of uncertainty in measurement (JCGM 100:2008). http://www.bipm.org/utils/common/ documents/jcgm/JCGM_100_2008_E.pdf
[19] Joint Committee for Guides in Metrology. (2008). Evaluation of measurement data – Supplement 1 to the “Guide to the expression of uncertainty in measurement” – Propagation of distributions using a Monte Carlo method (JCGM 101:2008). https://www.bipm.org/documents/20126/2071204/ JCGM_101_2008_E.pdf

Go to article

Authors and Affiliations

Jonathan Javier Duarte Franco
1
Carlos Mauricio Villamizar Mora
2
Carlos Eduardo García Sánchez
1

  1. Corporación Centro de Desarrollo Tecnológico del Gas, Grupo de Investigación en Fluidos y Energía, Carrera 23# 106-08, ZIP 680004, Bucaramanga, Colombia
  2. Universidad Industrial de Santander, Escuela de Ingeniería Mecánica, Grupo de Investigación en Energía y MedioAmbiente, Carrera 27 calle 9, ZIP 680002, Bucaramanga, Colombia
Download PDF Download RIS Download Bibtex

Abstract

This paper presents the recent advances in pervaporative reduction of sulfur content in gasoline. Methods of preliminary selection of membrane active layer material are presented. Interactions between gasoline components (typical hydrocarbon and sulfur species) and membranes are showed. Influence of pervaporation process parameters i.e. feed temperature, downstream pressure and feed flow rate on the separation efficiency is discussed. Investigations of the influence of sulfur concentration in fluid catalytic cracking (FCC) gasoline on membrane performance have been conducted. A series of PV tests was carried out to investigate the separation properties of the commercial composite membrane with an active layer made of poly(dimethylsiloxane) and to determine the efficiency of organic sulphur compound (thiophene) removal from model thiophene/n-heptane mixture depending on its concentration.

Go to article

Authors and Affiliations

Katarzyna Rychlewska
Michał Bodzek
Krystyna Konieczny
Download PDF Download RIS Download Bibtex

Abstract

This study manufactured a SiC coating layer using the vacuum kinetic spray process and investigated its microstructure and wear properties. SiC powder feedstock with a angular shape and average particle size of 37.4 μm was used to manufacture an SiC coating layer at room temperature in two different process conditions (with different degrees of vacuum). The thickness of the manufactured coating layers were approximately 82.4 μm and 129.4 μm, forming a very thick coating layers. The SiC coating layers consisted of α-SiC and β-SiC phases, which are identical to the feedstock. Cross-sectional observation confirmed that the SiC coating layer formed a dense structure. In order to investigate the wear properties, ball crater tests were performed. The wear test results confirmed that the SiC coating layer with the best wear resistance achieved approximately 4.16 times greater wear resistance compared to the Zr alloy. This study observed the wear surface of the vacuum kinetic sprayed SiC coating layer and identified its wear mechanism. In addition, the potential applications of the SiC coating layer manufactured using the new process were also discussed.

Go to article

Authors and Affiliations

Gi-Su Ham
Kyu-Sik Kim
Kee-Ahn Lee
Download PDF Download RIS Download Bibtex

Abstract

The carbothermic reduction of calcined magnesite in vacuum was studied. By thermodynamic analysis, the starting temperature of reduction reaction dropped from 2173K to 1523K when system pressure dropped from 1 atmosphere to 100 Pa. The experiments were carried out at different conditions under 10~100 Pa and the experimental results shown that the reduction extent of MgO improved by increasing the reaction temperature and time, the pellet forming pressure as well as adding fluoride as catalyst. The rate-determining step of carbothermic reduction process was gas diffusion with the apparent activation energy of 241.19~278.56 kJ/mol.
Go to article

Authors and Affiliations

Qifeng Tang
1
ORCID: ORCID
Jinqing Ao
1
ORCID: ORCID
Biyou Peng
1
ORCID: ORCID
Biao Guo
1
ORCID: ORCID
Tao Yang
1
ORCID: ORCID

  1. Xihua University, College of Materials Science and Engineering, Chengdu 610039, PR China
Download PDF Download RIS Download Bibtex

Abstract

This paper discusses issues related to optimising the technological parameters of the process of brazing gold in a vacuum

furnace. An investigation of the brazing process was carried out for materials used in constructing components for aircraft engine

fuel systems. The vacuum brazed material was AMS 5510 stainless steel (in the form of plates and pipes). AMS 4787 (BAu-4) was

used as the brazing filler. In particular, the influence of the method of preparing the surface on solder spreading and the thickness

of the diffusion zone were analysed. The best spreading of solder was obtained for nickel plated surfaces. When the sample surface

was more rough or scratched, the effect of the spreading of solder was limited and the diffusion process of the solder into the base

material became dominant. Moreover, the influence of the brazing temperature on microstructure changes and on interdiffusion

of the AMS 5510 stainless steel/BAu-4 solder system was determined. It was observed that an increase in the brazing temperature

modifies the morphology of the formed joint by forming a massive and rounded phase. Furthermore, an increase in the brazing

temperature enhances the exchange of components.

Go to article

Authors and Affiliations

M. Hebda
P. Kaczor
K. Miernik
Download PDF Download RIS Download Bibtex

Abstract

Brazing of two dissimilar structural materials; Zircaloy-4 and SS-316L was performed at 900oC under high vacuum conditions. The metallic glass ribbons (Zr55Cu30Al10Ni2Fe3-at. %) of 30 µm thickness, were used as an interlayer. The bonded region was characterized by scanning electron microscope (SEM), energy dispersive spectroscope (EDS) and microhardness testing. The metallurgical bond formation was due to compositional changes in the molten interlayer and later on its subsequent solidification. Assessment of the bonded zone (BZ) revealed three distinct regions (Region-I, Region-II and Region-III). Diffusion transformation was observed in Region-I and Region-III which were interface with base alloys SS-316L and Zircaloy-4 respectively. However, Region-II at the middle of the BZ was composed of isothermally and athermally solidified portions. The highest values of Microhardness were observed in Region-III which was due to the presence of hard phases. Moreover, a crack parallel to BZ was observed in Region-III and was attributed to differential contraction of base alloys during cooling. Maximum shear stress acting on the BZ was calculated and correlated to the brittle phase cracking.

Go to article

Authors and Affiliations

A. Munis
Maosheng Zheng
J.I. Akhter
M. Ahmad
Download PDF Download RIS Download Bibtex

Abstract

The article presents the results of laboratory measurements of Ud breakdown voltages in a high-voltage vacuum insulating system for different pressures, contact gaps, type of electrode contacts and type of residual gas inside the discharge chamber. First of all, the electrical strength of the discharge chamber with a contact system terminated with contact pads made of W 70Cu 30 and Cu 75Cr 25 material was compared for selected values of contact gaps. It was found that below a pressure of p = 3.0 x 10 -1 Pa the electrical strength reaches an approximately constant value for each of the set contact gaps d. Analytical relationships were determined to calculate this value for each of the contact pads used. Above a pressure of p = 3.0 x 10 -1 Pa, the measured values of Ud breakdown voltages decrease sharply. The values of breakdown voltages in the discharge chamber with residual gases in the form of air, argon, neon and helium were also determined for selected values of contact gaps d. Depending on the residual gases used, significant differences were noted in the values of pressure p at which the loss of insulating properties in the discharge chamber occurred. These values were 3.3 x 10 -1 Pa for argon, 4.1 x 10 -1 Pa for air, 6.4 x 10 -1 Pa for neon, and 2.55 x 10 0 Pa for helium, respectively.
Go to article

Authors and Affiliations

Michał Lech
1
ORCID: ORCID
Paweł Węgierek
1
ORCID: ORCID

  1. Faculty of Electrical Engineering and Computer Science, Lublin University of Technology, Nadbystrzycka 38A str., 20-618 Lublin, Poland
Download PDF Download RIS Download Bibtex

Abstract

Liquid Metal Extraction process using molten Mg was carried out to obtain Nd-Mg alloys from Nd based permanent magnets at 900oC for 24 h. with a magnet to magnesium mass ratio of 1:10. Nd was successfully extracted from magnet into Mg resulting in ~4 wt.% Nd-Mg alloy. Nd was recovered from the obtained Nd-Mg alloys based on the difference in their vapor pressures using vacuum distillation. Vacuum distillation experiments were carried out at 800oC under vacuum of 2.67 Pa at various times for the recovery of high purity Nd. Nd having a purity of more than 99% was recovered at distillation time of 120 min and above. The phase transformations of the Nd-Mg alloy during the process, from Mg12Nd to α-Nd, were confirmed as per the phase diagram at different distillation times. Pure Nd was recovered as a result of two step recycling process; Liquid Metal Extraction followed by Vacuum Distillation.
Go to article

Bibliography

[1] J.D. Widmer, R. Martin, M. Kimiabeigi, SM&T. 3, 7-13 (2015).
[2] S . Kruse, K. Raulf, T. Pretz, B. Friedrich, J. Sustain. Metall. 3, 168-178 (2017).
[3] N. Haque, A. Hughes, S. Lim, C. Vernon, Resources. 3 (4), 614- 635 (2014).
[4] D . Schüler, M. Buchert, R. Liu, S. Dittrich, C. Merz, Study on Rare Earths and Their Recycling Final Report for the Greens/European Free Alliance Group in the European Parliament, Germany 2011.
[5] Saleem H. Ali, Resources 3, 123-134 (2014).
[6] T.H. Okabe, Trans. Inst. Min. Metall. 126 (1-2), 22-32 (2016).
[7] K . Halada, J. Mater. Cycles Waste Manag. 20 (2), 49-58 (2009).
[8] T.H. Okabe, O. Takeda, K. Fukuda, Y. Umetsu, Mater. Trans. 44 (4), 798-801 (2003).
[9] Y. Xu, L.S. Chumbley, F.C. Laabs, J. Mater. Res. 15 (11), 2296- 2304 (2000).
[10] H .J. Chae, Y.D. Kim, B.S. Kim, J.G. Kim, T.S. Kim, J. Alloys Compd. 586 (s1), 143-149 (2014).
[11] T. Akahori, Y. Miyamoto, T. Saeki, M. Okamoto, T.H. Okabe, J. Alloys Compd. 703, 337-343 (2017).
[12] S . Delfino, A. Saccone, R. Ferro, Metall. Trans. A. 21A, 2109-2114 (1990).
[13] A.A. Nayeb-Hashemi, J.B. Clark, Phase Diagrams of Binary Manganese Alloys, ASM International, Ohio (1988).
[14] [H. Okamoto, J. Phase Equilib. 12, 249 (1991).
[15] S . Gorssea, C.R. Hutchinsonb, B. Chevaliera, J.F. Nieb, J. Alloys Compd. 392, 253-262 (2005).
[16] I . Barin, Thermochemical Data of Pure Substances, Germany (1989).
Go to article

Authors and Affiliations

Mohammad Zarar Rasheed
1 2
ORCID: ORCID
Sun-Woo Nam
2
ORCID: ORCID
Sang-Hoon Lee
2
ORCID: ORCID
Sang-Min Park
2
ORCID: ORCID
Ju-Young Cho
2
ORCID: ORCID
Taek-Soo Kim
1 2
ORCID: ORCID

  1. University of Science and Technology, Industrial Technology, Daejeon, Republic of Korea
  2. Korea Institute for Rare Metals, Korea Institute of Industrial Technology, Incheon, Republic of Korea
Download PDF Download RIS Download Bibtex

Abstract

Refractories are the basic material for the construction of the lining of a melting furnace used, among other things, in the foundry industry. The article describes a comparative study of the influence of the type of moulding on the quality of the finished refractory product. A method for making products from refractory materials was proposed and a test methodology was developed. The results, based on a classic study of the quality of these materials, confirm a strong influence on the quality of the materials obtained in terms of reduced porosity and homogeneity of pore size.
Go to article

Authors and Affiliations

Alicja Trela
1
ORCID: ORCID
Alena Pribulová
2
ORCID: ORCID
Peter Futas
2
ORCID: ORCID

  1. AGH University of Krakow, Faculty of Foundry Engineering, Al. Mickiewicza 30, 30-059 Kraków, Poland
  2. Technical University Kosice, Department of Metallurgy, Slovakia
Download PDF Download RIS Download Bibtex

Abstract

The formation process of one of the most common casting defects, a shrinkage depression concerned to shrinkage cavity, was studied. The methodology, device and the experimental set up were developed to study the shrinkage cavity growth. The kinetics of vacuum formation in the cavity of the spherical casting of Al-Si-Mg alloy at its solidification in the sand-and-clay form was investigated. The data were analysed taking in mind the temperature variation in the centre of crystallizing casting. The causes of the shrinkage depression in castings were clarified. It was determined that atmospheric pressure leads to the retraction and curvature of metal layer on the surface of the casting with lower strength below which the shrinkage cavity is formed. To avoid such defects it was recommended to use the external or internal chills, feeders and other known technological methods. Deep shrinkage cavities inside the castings could be removed with an air flow through a thin tubular needle of austenitic steels for medical injections.
Go to article

Bibliography

[1] DSTU 9051:2020. Castings of cast iron and steel. Defects. Terms and definitions. Since 01.04.2021. Pg. 15. (in Ukrainian) http://ptima.kiev.ua/images/stories/Standart/IRONSTEEL/dstu19200-80.pdf
[2] Rowley, M.T. (2007). International Atlas of Casting Defects. American Foundry Society. ISBN: 978-0874330533.
[3] GOST 19200-80. Castings of cast iron and steel. Terms and definitions of defects. (1980). (in Russian).
[4] Atlas of foundry defects. (2004). 136 Summit avenue. Montvale, NJ 07645-1720. Institute of Foundry Casting. Technopark. Pg. 23.
[5] Reisa, A., Xub, Z., Tolb, R.V. & Netoc, R. (2012). Modelling feeding flow related shrinkage defects in aluminum castings. Journal of Manufacturing Processes. 14(1), 1-7. DOI: 10.1016/j.jmapro.2011.05.003
[6] Voronin, Y.F., Kamaev V.A. (2005). Atlas of foundry defects. Moscow: Mechanical Engineering. Pg. 327. (in Russian). https://www.twirpx.com/file/914318/
[7] Chokkalingam, B. & Mohamed Nazirudeen, S.S. (2009). Analysis of casting defect through defect diagnostic study approach. Journal of Engineering Annals of the Faculty of Engineering Hunedoara. 2, 209-212. ISSN 1584-2665
[8] Beeley, P. (2001). Foundry Technology. 719. Oxford: Butterworth Heinemann. ISBN 0750645679. https://www.academia.edu/4161769/foundry_technology_by_peter_beeley/
[9] Khrychikov, V.E., Semenov, O.D., Menyaylo, O.V., Shalevskaya, I.A., & Myanovskaya, Ya.V. (2021). Elimination of weights in artistic castings with different wall thickness (Removal of shrinkage depression in art castings with different wall thickness). Casting processes (Затвердіння сплавів). 4(146). 14-21. (in Ukrainian). https://plit-periodical.com.ua/en/arhiv/removal-shrinkage-depression-art-castings-different-wall-thickness
[10] GOST R ISO 9626-2020. (2021). Stainless steel needle pipes for the manufacture of medical devices. Requirements and test methods. Pg. 28. (in Russian).
[11] Dunphy, R.P., Akerlind, C.G. & Pellini, W.S. (1954). Solidification, feed characteristics of gray cast irons and nodular cast irons. Foundry. 82(6), 106-121.
[12] Rogelberg I.L, Beilin V.M. (1983). Alloys for thermocouples (handbook). Moscow: Metallurgy. 76-77. (in Russian) https://knizhen-pazar.net/products/books/597200-splav-dlya-termopar
[13] Leibenzon, V.O., Pilyushenko, V.L., Kondratenko, V.M., Khrychikov, V.E., Nedopyokin, F.V., Bilousov, V.V. Dmitriev, Yu.V. (2009). Hardening of metals and metal compositions. Kyiv: Scientific thought. 447. (in Ukrainian. https://nmetau.edu.ua/file/tverdinnya_metaliv_i_metalevih_kompozitsiy._pidruchnik.pdf
[14] Khrychikov, V.E., Semenov, O.D., Menyaylo, O.V. (2021). Application for the patent № a202101129. Ukraine. IPC (2021.01) B22D 27/13 (2006.01), B22D 25/00. Method of removing weights in castings with thickened parts of wall. (in Ukrainian). https://base.uipv.org/searchInvStat/showclaimdetails.php?IdClaim=336807&resId=1

Go to article

Authors and Affiliations

V. Khrychikov
1
ORCID: ORCID
O. Semenov
1
ORCID: ORCID
H. Meniailo
1
ORCID: ORCID
Y. Aftandiliants
2
ORCID: ORCID
S. Gnyloskurenko
2 3
ORCID: ORCID

  1. Ukrainian State University of Science and Technologies, Ukraine
  2. National University of Life and Environmental Sciences of Ukraine, Ukraine
  3. Physical and Technological Institute of Metals and Alloys, National Academy of Sciences of Ukraine, Ukraine
Download PDF Download RIS Download Bibtex

Abstract

Blast mitigation continues to be a popular field of research when military vehicles are concerned. The main problem is coping with the vehicle global motion consequences following an explosion. The paper presents a potential application of the linear vacuum packed particle (VPP) damper as a supplementation for a viscous shock absorber in a traditional blast mitigation seat design. The paper also presents field test results for the underbelly blast explosion, comparing them to the laboratory tests carried out on the impact bench. To collect accelerations, the anthropomorphic test device, i.e. the Hybrid III dummy, was used. A set of numerical simulations of the modified blast mitigation seat with the additional VPP linear damper were revealed. The VPP damper was modeled according to the Johnson–Cook model of viscoplasticity. The Hertzian contact theory was adopted to model the contact between the vehicle and the ground. The reduction of the dynamic response index (DRI) in the case of the VPP damper application was also proved.
Go to article

Bibliography

  1.  F. Melanie and P.V.S. Lee, Military Injury Biomechanics The Cause and Prevention of Impact Injuries. CRC Press, 2017.
  2.  H. Kamel, O. Harraz, M. Yacoub, and A. Ali, “Developing a custom Anthropomorphic Test Device for measuring blast effects on occupants inside armored vehicles”, J. Eng. Sci. Mil. Technol., vol. 3, no. 2, pp. 70–76, 2019, doi: 10.21608/ejmtc.2019.15041.1127.
  3.  I. Overton, “A decade of global IED harm reviewed |AOAV”, Action on Armed Violence, 2020. [Online]. Available: https:// aoav.org.uk/2020/a- decade-of-global-ied-harm-reviewed/ (accessed Feb. 05, 2021).
  4.  M. Müller, U. Dierkes, and J. Hampel, “Blast protection in military land vehicle programmes: Approach, methodology and testing”, WIT Trans. Built Environ., vol. 87, pp. 247–257, Jun. 2006, doi: 10.2495/SU060251.
  5.  A. Iluk, “Estimation of spine injury risk as a function of bulletproof vest mass in case of Under Body Blast load”, 2014 IRCOBI Conf. Proc. – Int. Res. Counc. Biomech. Inj., 2014, pp. 809–820.
  6.  Research and Technology Organisation North Atlantic Treaty Organisation, Protection level of armoured vehicles volume 2, AEP-55, vol. 2, no. AUGUST. Allied Engineering Publication, 2011.
  7.  Research and Technology Organisation North Atlantic Treaty Organisation, “Test Methodology for Protection of Vehicle Occupants against Anti-Vehicular Landmine Effects,” 2007.
  8.  M. Cheng, D. Bueley, J.P. Dionne, and A. Makris, “Survivability evaluation of blast mitigation seats for armored vehicles”, 26th Int. Symp. Ballist., 2011.
  9.  P. Baranowski and J. Malachowski, “Numerical study of selected military vehicle chassis subjected to blast loading in terms of tire strength improving”, Bull. Polish Acad. Sci. Tech. Sci., vol. 63, no. 4, pp. 867–878, 2015, doi: 10.1515/bpasts-2015-0099.
  10.  V. Denefeld, N. Heider, A. Holzwarth, A. Sättler, and M. Salk, “Reduction of global effects on vehicles after IED detonations”, Def. Technol., vol. 10, no. 2, pp. 219–225, 2014, doi: 10.1016/j.dt.2014.05.005.
  11.  M. Żurawski and R. Zalewski, “Damping of Beam Vibrations Using Tuned Particles Impact Damper”, Appl. Sci., vol. 10, p. 6334, 2020, doi: 10.3390/app10186334.
  12.  J. Ramalingam and R. Thyagarajan, “Analysis of Design Range for a Stroking Seat on a Stroking Floor to Mitigate Blast Loading Effects”, NATO Sci. Technol. Organ. Publ., 2017.
  13.  G. Hiemenz, M. Murugan, W. Hu, N. Wereley, and J.H. Yoo, “Adaptive Seat Energy Absorbers for Enhanced Crash Safety: Technology Demonstration,” 2016.
  14.  S.A. Venkatesh Babu, R. Thyagarajan, “Retractor-Based Stroking Seat System and Energy-Absorbing Floor to Mitigate High Shock and Vertical Acceleration”, NATO/STO AVT-221 Spec. Meet. “Design Prot. Technol. L. Amphib. NATO Veh.”, 2014.
  15.  S.P. Desjardins, “The evolution of energy absorption systems for crashworthy helicopter seats”, J. Am. Helicopter Soc., vol. 51, no. 2, pp. 150–163, 2006, doi: 10.4050/JAHS.51.150.
  16.  M. Żurawski, B. Chiliński, and R. Zalewski, “A Novel Method for Changing the Dynamics of Slender Elements Using Sponge Particles Structures”, Materials (Basel)., vol. 13, no. 21, p. 4874, 2020, doi: 10.3390/ma13214874.
  17.  P. Bartkowski and R. Zalewski, “A concept of smart multiaxial impact damper made of vacuum packed particles”, MATEC Web Conf., vol. 157, p. 05001, 2018.
  18.  G. Bienioszek and S. Kciuk, “Determination of Boundary Conditions for the Optimization Process of Blast Mitigation”, in 23rd International Conference Engineering Mechanics 2017, 2017.
  19.  R. Zalewski, P. Chodkiewicz, and M. Shillor, “Vibrations of a mass-spring system using a granular-material damper”, Appl. Math. Model., vol. 40, no. 17–18, pp. 8033–8047, 2016, doi: 10.1016/j.apm.2016.03.053.
  20.  R. Zalewski and T. Szmidt, “Application of Special Granular Structures for semi-active damping of lateral beam vibrations”, Eng. Struct., vol. 65, pp. 13–20, 2014, doi: 10.1016/j.engstruct.2014.01.035.
  21.  R. Zalewski and M. Pyrz, “Mechanics of Materials Experimental study and modeling of polymer granular structures submitted to internal underpressure”, Int. J. Mech. Mater., vol. 57, pp. 75–85, 2013, doi: 10.1016/j.mechmat.2012.11.002.
  22.  E. Brown et al., “Universal robotic gripper based on the jamming of granular material”, Proc. National Academy of Sciences, vol. 107, no. 44 pp. 18809–18814, 2010, doi: 10.1073/pnas.1003250107.
  23.  M.D. Luscombe and J.L. Williams, “Comparison of a long spinal board and vacuum mattress for spinal immobilisation”, Emerg. Med. J., vol. 20, pp. 476–478, 2003.
  24.  P. Bartkowski, R. Zalewski, and P. Chodkiewicz, “Parameter identification of Bouc-Wen model for vacuum packed particles based on genetic algorithm”, Arch. Civ. Mech. Eng., vol. 19, pp. 322–333, 2019, doi: 10.1016/j.acme.2018.11.002.
  25.  D. Rodak and R. Zalewski, “Innovative Controllable Torsional Damper Based on Vacuum Packed Particles”, Materials (Basel)., vol. 13, p. 4356, 2020.
  26.  Y. Tsuji, T. Tanaka, and T. Ishida, “Lagrangian numerical simulation of plug flow of cohesionless particles in a horizontal pipe”, Powder Technol., vol. 71, pp. 239–250, 1992.
  27.  R. Chakrabarty and J. Song, “A modified Johnson–Cook material model with strain gradient plasticity consideration for numerical simulation of cold spray process”, Surf. Coat. Technol., vol. 397, p. 125981, 2020, doi: 10.1016/j.surfcoat.2020.125981.
  28.  I.P. Herman, Biological and Medical Physics, Biomedical Engineering. Springer, 2008. p.16–17.
Go to article

Authors and Affiliations

Dominik Rodak
1
ORCID: ORCID
Mateusz Żurawski
1
ORCID: ORCID
Michał Gmitrzuk
2
ORCID: ORCID
Lech Starczewski
2

  1. Faculty of Automotive and Construction Machinery Engineering, Warsaw University of Technology, Poland
  2. Military Institute of Armoured and Automotive Technology, Poland
Download PDF Download RIS Download Bibtex

Abstract

Refractories are the basic material for the construction of the lining of a melting furnace used, among other things, in the foundry industry. The article describes a comparative study of the influence of the type of moulding on the quality of the finished refractory product. A method for making products from refractory materials was proposed and a test methodology was developed. The results, based on a classic study of the quality of these materials, confirm a strong influence on the quality of the materials obtained in terms of reduced porosity and homogeneity of pore size.
Go to article

Authors and Affiliations

Alicja Trela
ORCID: ORCID
M. Brzeziński
1
ORCID: ORCID
A. Pribulova
2
ORCID: ORCID
Peter Futas
ORCID: ORCID

  1. AGH University of Krakow, Faculty of Foundry Engineering, Al. Mickiewicza 30, 30-059 Krakow, Poland
  2. Technical University, Department of Metallurgy, Kosice, Slovakia
Download PDF Download RIS Download Bibtex

Abstract

Electromagnetic processing of molten copper is provided in a special kind of electrical furnace called an induction furnace with a cold crucible (IFCC), making it possible to successfully remove impurities from the workpiece. In order to analyze the process in a sufficient way not only electromagnetic, thermal and flow but also metallurgical and mass transfer phenomena in the coupled formulation should be taken into consideration. The paper points to an analysis of the kinetic process of lead evaporation from molten copper. It was shown that mass transport in the gas phase determines the rate of the analyzed evaporation process. The possibility of removal of lead from molten copper is analyzed and described.
Go to article

Authors and Affiliations

Albert Smalcerz
1
ORCID: ORCID
Leszek Blacha
1
ORCID: ORCID
Jerzy Barglik
1
ORCID: ORCID
Ivo Dolezel
2
ORCID: ORCID
Tadeusz Wieczorek
1
ORCID: ORCID

  1. Silesian University of Technology Krasinskiego 8, 40-019 Katowice, Poland
  2. Faculty of Electrical Engineering, University of West Bohemia Univerzitní 26, 301 00 Pilsen, Czech Republic
Download PDF Download RIS Download Bibtex

Abstract

Accurate temperature prediction is vital for the canned permanent magnet synchronous motor (CPMSM) used in the vacuum pump, as it experiences severe heating. In this paper, a novel motor temperature calculation method is proposed, which takes into account the temperature impact on the heat transfer capacity. In contrast to existing electromagnetic-thermal coupled calculation methods, which solely address the temperature effect on the motor electromagnetic field, the proposed method comprehensively considers its impact on motor losses, permanent magnet magnetic properties, thermal conductivity, and heat dissipation ability of motor components, resulting in a motor temperature simulation that closely resembles the actual physical process. To verify the reliability of the proposed temperature calculation method, a 1.5 kW CPMSM was chosen as the research subject. The method was used to analyze the temperature distribution characteristics of the motor and assess the impact of ambient temperature on motor temperature rise. Furthermore, a prototype was fabricated, and an experimental platform was established to test the motor temperature. The results demonstrate good agreement between the calculated results obtained using the proposed method and the experimental data. This research not only provides a theoretical foundation for optimizing the design of the CPMSM but also provides valuable insights into its operational safety and reliability.
Go to article

Authors and Affiliations

Ming Li
1
ORCID: ORCID
Shuxian Lun
1
Haiqi Mu
1
Wei Wang
1
ORCID: ORCID

  1. School of Control Science and Engineering, Bohai University No.19, Keji Road, Jinzhou, People’s Republic of China
Download PDF Download RIS Download Bibtex

Abstract

Titanium alloys belonging to the group of modern metallic materials used in many industries, including the aerospace industries. Induction crucible vacuum furnaces and induction furnaces with cold crucible are most commonly used for their smelting. When operating these devices, one can deal with an adverse phenomenon of decrease in the content of alloy elements that are characterized by higher equilibrium vapour pressure than the matrix metal or titanium, in the metal bath. In the paper, results of the study on aluminium evaporation from the Ti-Al-Nb, Ti-Al-V and Ti-Al alloys (max 6.2 % wt.) during smelting in a vacuum induction melting (VIM) furnace are presented. The experiments were performed at 10 to 1000 Pa for 1973 K and 2023 K. A significant degree of aluminium loss has been demonstrated during the analysed process. The values of relative aluminium loss for all the alloys ranged from 4 % to 25 %. Lowering the pressure in the melting system from 1000 Pa to 10 Pa resulted in increased values of aluminium evaporation flux from 4.82⋅10-5 to 0.000327 g⋅cm-2⋅s-1 for 1973 K and from 9.28⋅10-5 to 0.000344 g⋅cm-2⋅s-1 for 2023 K. The analysis of the results obtained took into account the value of the actual surface of the liquid metal. In the case of melting metals in an induction furnace, this surface depends on the value of power emitted in the charge. At greater power, we observe a significant increase in the bath surface due to the formation of a meniscus.
Go to article

Bibliography

[1] Kostov, A. & Friedrich, B. (2005). Selection of crucible oxides in molten titanium and titanium aluminium alloys by thermo-chemistry calculation. Journal of Mining and Metallurgy. 41B, 113-125. DOI: 10.2298/JMMB0501113K.
[2] Kuang, J.P., Harding, R.A. & Campbell, J. (2000). Investigation into refractories as crucible and mould materials for melting and casting gamma-TiAl alloys. Materials Science and Technology. 16, 1007-1016. DOI: 10.1179/026708300101508964.
[3] Tetsui, T., Kobayashi, T., Mori, T., Kishimoto, T. & Harada, H. (2010). Evaluation of yttrium applicability as a crucible for induction melting of TiAl alloy. Materials Transactions. 51, 1656-1662. DOI: 10.2320/matertrans.MAW20100.
[4] Myszka, D., Karwiński, A., Leśniewski, W. & Wieliczko, P. (2007). Influence of the type of ceramic moulding materials on the top layer of titanium precision castings. Archives of Foundry Engineering. 7(1), 153-156. DOI: 10.7356/ iod.2015.24.
[5] Szkliniarz, A. & Szkliniarz, W. (2011). Assessment quality of Ti alloys melted in induction furnace with ceramic crucible. Solid State Phenomena. 176, 139-148. DOI: 10.4028/www.scientific.net/SSP.176.139.
[6] Jinjie, G., Jun, J., Yuan, S.L., Guizhong, L., Yanqing, S. & Hongsheng, D. (2000). Evaporation behavior of aluminum during the cold crucible induction skull melting of titanium aluminum alloys. Metallurgical and Materials Transactions B. 31B, 837-844. DOI: 10.1007/s11663-000-0120-1.
[7] Isawa, T., Nakamura, H. & Murakami, K. (1992). Aluminum evaporation from titanium alloys in EB hearth melting. ISIJ International. 32, 607-615.
[8] Ivanchenko, V., Ivasishin, G. & Semiatin, S. (2003). Evaluation of evaporation losses during electron-beam melting of Ti-Al-V alloys. Metallurgical and Materials Transactions B. 34B, 911-915. DOI: 10.1007/s11663-003-0097-7.
[9] Su, Y., Guo, J., Jia, J., Liu, G. & Liu, Y. (2002). Composition control of a TiAl melt during the induction skull melting (ISM) process. Journal of Alloys and Compounds. 334, 261-266. DOI: 10.1016/S0925-8388(01)01766-2.
[10] Guo, J., Liu, G., Su, Y., Ding, H., Jia, J. & Fu, H. (2002). The critical pressure and impeding pressure of Al evaporation during induction skull melting processing of TiAl. Metallurgical and Materials Transactions A. 31A, 3249-3253. DOI: 10.1007/s11661-002-0311-2.
[11] Gou, J., Liu, Y., Su, Y., Ding, H., Liu, G. & Jia, J. (2000). Evaporation behaviour of aluminum during the cold crucible induction skull melting of titanium aluminum alloys. Metallurgical and Materials Transactions B. 31B, 837-844. DOI: 10.1007/s11663-000-0120-1.
[12] HSC Chemistry ver. 6.1. Outocumpu Research Oy, Pori.
[13] Semiatin, S., Ivanchenko, V., Akhonin, S.O. & Ivasishin, O.M. (2004). Diffusion models for evaporation losses during electron-beam melting of alpha/beta-titanium alloys. Metallurgical and Materials Transactions B. 35B, 235-245. DOI: 10.1007/s11663-004-0025-5.
[14] Song, J.H., Min, B.T., Kim, J. H., Kim, H.W., Hong, S.W. & Chung, S.H. (2005). An electromagnetic and thermal analysis of a cold crucible melting. International Communications in Heat and Mass Transfer. 32, 1325-1336. DOI: 10.1016/j.icheatmasstransfer.2005.07.015.
[15] Zhu, Y., Yang, Y.Q. & Sun, J. (2004). Calculation of activity coefficients for components in ternary Ti alloys and intermetallics as matrix of composites. Transactions of Nonferrous Metals Society of China. 14, 875-879.
[16] Belyanchikov, L.N. (2010). Thermodynamics of Titanium-Based Melts: I. Thermodynamics of the Dissolution of Elements in Liquid Titanium. Russian Metallurgy. 6, 565-567. DOI: 10.1134/S0036029510060194.
[17] Blacha, L. & Labaj, J. (2012). Factors determining the rate of the process of metal bath components. Metalurgija. 51, 529-533.
[18] Ward, R.G. (1963). Evaporative losses during vacuum induction melting of steel. Journal of the Iron and Steel Institute. 1, 11-15.
[19] Labaj, J. (2010). Copper evaporation kinetics from liquid iron. Wydawnictwo Oldprint. (in Polish).
[20] Ozberk, E. & Guthrie, R. (1985). Evaluation of vacuum induction melting for copper refining. Transactions of the Institution of Mining and Metallurgy, Section C: Mineral Processing and Extractive Metallurgy. 94, 146-157.
[21] Ozberk, E. & Guthrie, R. (1986). A kinetic model for the vacuum refining of inductively stirred copper melts. Metallurgical Transactions B. 17, 87-103.
[22] Przyłucki, R., Golak, S., Oleksiak, B. & Blacha, L. (2012). Influence of an induction furnace's electric parameters on mass transfer velocity In the liquid phase. Metalurgija. 1, 67-70.
[23] Blacha, L., Przylucki, R., Golak, S. & Oleksiak, B. (2011). Influence of the geometry of the arrangement inductor - crucible to the velocity of the transport of mass in the liquid metallic phase mixed inductive. Archives of Civil and Mechanical Engineering. 11, 171-179. DOI: 10.1016/S1644-9665(12)60181-2.
[24] Blacha, L., Golak, S., Jakovics, S. & Tucs, A. (2014). Kinetic analysis of aluminum evaporation from Ti-6Al-7Nb. Archives of Metallurgy and Materials. 59, 275-279. DOI: 10.2478/amm-2014-0045
[25] Spitans, S., Jakovics, A., Baake, E. & Nacke, B. (2010). Numerical modelling of free surface dynamics of conductive melt in the induction crucible furnace. Magnetohydrodynamics. 46, 425-436
[26] Spitans, S., Jakovics, A., Baake, E. & Nacke, B. (2011). Numerical modelling of free surface dynamics of melt in an alternate electromagnetic field. Magnetohydrodynamics. 47, 385-397.
[27] Golak, S. & Przylucki, R. (2008). The optimization of an inductorposition for minimization of a liquid metal free surface, Przegląd Elektrotechniczny. 84, 163-164.
[28] Golak, S. & Przyłucki R. (2009). A simulation of the coupled problem of magnetohydrodynamics and a free surface for liquid metals. WIT Transactions of Engineering Science. 48, 67-76. DOI: 10.2495/MPF090061.
Go to article

Authors and Affiliations

Albert Smalcerz
ORCID: ORCID
Leszek Blacha
ORCID: ORCID
J. Łabaj
1
ORCID: ORCID

  1. Silesian University of Technology, Faculty of Materials Engineering and Metallurgy, ul. Krasińskiego 8, 40-019 Katowice, Poland
Download PDF Download RIS Download Bibtex

Abstract

In this paper, the results of the study on aluminium evaporation from the Al-Zn alloys (4.2% weight) during remelting in a vacuum induction furnace (VIM) are presented. The evaporation of components of liquid metal alloys is complex due to its heterogeneous nature. Apart from chemical affinity, its speed is determined by the phenomena of mass transport, both in the liquid and gas phase. The experiments were performed at 10-1000 Pa for 953 K - 1103 K. A significant degree of zinc loss has been demonstrated during the analysed process. The relative values of zinc loss ranged from 4 to 92%. Lowering the pressure in the melting system from 1000 Pa to 10 Pa caused an increase in the value of density of the zinc evaporating stream from 3.82⋅10-5 to 0.000564 g⋅cm-2⋅s-1 at 953 K and 3.32⋅10-5 to 0.000421 g⋅cm-2⋅s-1 for 1103 K. Based on the results of the conducted experiments. it was found that evaporation of zinc was largely controlled by mass transfer in the gas phase and only for pressure 10 Pa this process was controlled by combination of both liquid and gas phase mass transfer.
Go to article

Bibliography

[1] Guo, J., Liu, Y. & Su, Y. (2002). Evaporation of multi-components in Ti-25Al-25Nb melt during induction skull melting process. Transaction of Nonferrous Metals Society of China. 12(4), 587-591.
[2] Blacha, L., Mizera, J. & Folega, P. (2013). The effects of mass transfer in the liquid phase on the rate of aluminium evaporation from the Ti-6Al-7Nb alloy. Metalurgija, 53(1), 51-54.
[3] HSC Chemistry ver. 6.1. Outocumpu Research Oy. Pori.
[4] Plewa, J. (1987). Examples of calculations from the theory of metallurgical processes. Gliwice: Wydawnictwo Politechniki Śląskiej. (in Polish).
[5] Ozberk, E. & Guthrie, R. (1986). A kinetic model for the vacuum refining of inductively stirred copper melts. Metallurgical Transactions B. 17, 87-103.
[6] Nash, P.M. & Steinemann, S.G. (2006). Density and thermal expansion of molten manganese. Iron. Nickel. Copper. Aluminium and Tin by Means of the Gamma-Ray Attenuation Technique. Physics and Chemistry of Liquids, An International Journal. 29(1), 43-58.
[7] Assael, M., Kakosimos, K. & Banish, R. (2006). Reference data for the density and viscosity of liquid aluminum and liquid iron. Journal of Physical and Chemical Reference Data. 35(1), 285-301.
[8] Smalcerz, A., Węcki B. & Blacha L. (2021) Influence of the power of various types of induction furnaces on the shape of the metal bath surface. Advances in Science and Technology Research Journal. 15(3), 34-42. DOI: 10.12913/22998624/138245
[9] Homma, M., Ohno, R., & Ishida, T. (1996). Evaporation of manganese. copper. and tin from molten iron under, vacuum. Science Reports of the Research Institutes, Tohuku University. Series A – Physics. chemistry and metallurgy. 18, 356-365.
[10] Ohno, R. & Ishida, T. (1967). Solution rate of solid iron in liquid copper, ISIJ International. 31(10), 1164-1169.
[11] Chen, X. & Ito, N. (1995). Evaporation rate of copper in high carbon iron melt under reduced pressure. Tetsu-to-Hagane. 81(10), 959-964.
[12] Savov, L. & Janke, D. (2000). Evaporation of cu and sn from induction-stirred iron-based melts treated at reduced pressure. ISIJ International. 40(2), 95-104.
[13] Łabaj, J. (2012). Kinetics of cooper evaporation from the Fe-Cu Alloys under Reduced Pressure. Archives of Metallurgy and Materials. 57(1), 165-172.
[14] Maruyama, T., Katayama, H., Momono, T., Tayu, Y, & Takenouchi, T. (1998). Evaporation rate of copper from molten iron by urea spraying under reduced pressure. Tetsu-to-Hagane. 84(4), 243-248.
[15] Ono-Nakazato, H. & Taguchi, K. (2003). Effect of silicon and carbon on the evaporation rate of copper in molten iron. ISIJ International. 43(11), 1691-169.
[16] Bellot, J.P., Duval, H., Ritchie, M., Mitchell, A. & Ablitzer, D. (2001). Evaporation of Fe and Cr from induction-stirred austenitic stainless steel-influence of the inert gas pressure, ISIJ International. 41(7), 696-705.
[17] Siwiec, G. (2013). The kinetics of aluminium evaporation from the Ti-6Al-4V alloy. Archives of Metallurgy and Materials. 58(4), 1155-1160.
[18] Blacha, L. Golak, S. Jakovics, S. & Tucs A. (2014) Kinetic analysis of aluminum evaporation from Ti-6Al-7Nb. Archives of Metallurgy and Materials. 59, 275-279. DOI: 10.2478/amm-2014-0045.
[19] Blacha, L., Burdzik, R. Smalcerz, A. & Matuła, T. (2013). Effects of pressure on the kinetics of manganese evaporation from the OT4 alloy. Archives of Metallurgy and Materials. 58(1), 197-201.
[20] Harris, R. (1984). Vacuum refining copper melts to remove bismuth, arsenic and antimony. Metallurgical Transaction B. 15, 251-257.
[21] Harris, R., McClincy, R.J. & Riebling, E.F. (1987). Bismuth, arsenic and antimony removal from anode copper via vacuum distillation. Canadian Metallurgical Quarterly. 26(1), 1-4.
[22] Ozberk, B., Guthire, R.I.L. (1987). Vacuum melting of copper evaporation – evaporation of impurities. Proc. 6th Int. Vacuum Metallurgy Conf. American Vacuum Society. San Diego. 248-267.
[23] Machlin, E.S. (1961). Kinetics of vacuum induction refining – theory. the american institute of mining. Metallurgical. and Petroleum Engineers.
[24] Tarapore, E.D. & Evans, J. (1976). Fluid velocities in induction melting furnaces: Part I. Theory and laboratory experiments. Metallurgical Transaction B. 7, 343-351.
[25] Tarapore, E.D., Evans, J. & Langfeld, J. (1977). Fluid velocities in induction melting furnaces: Part II. large scale measurements and predictions. Metallurgical Transaction B. 8, 179-184.
[26] Szekely, J., Chang, W. & Johnson, W. (1977). Experimental measurement and prediction of melt surface velocities in a 30.000 lb inductively stirred melt. Metallurgical Transaction B. 8, 514-517.
[27] Przyłucki, R. Golak, S. Oleksiak, B. & Blacha L. (2012). Influence of an induction furnace's electric parameters on mass transfer velocity In the liquid phase. Metalurgija. 1, 67-70.
[28] Blacha, L. Przylucki, R. Golak, S. & Oleksiak B. (2011). Influence of the geometry of the arrangement inductor - crucible to the velocity of the transport of mass in the liquid metallic phase mixed inductive. Archives of Civil and Mechanical Engineering. 11, 171-179 DOI: 10.1016/S1644-9665(12)60181-2
[29] Du, Y., Chang, Y., Huang, B., Gong, W. & Jin, Z. (2003). Diffusion coefficients of some solutes in fcc and liquid Al: critical evaluation and correlation. Materials Science and Engineering: A. 363(1-2), 140-151.
[30] Harris, R. & Davenport, W.G. (1982). Vacuum distillation of liquid metals: Part I. Theory and experimental study. Metallurgical Transactions B. 13, 581-588.

Go to article

Authors and Affiliations

Albert Smalcerz
ORCID: ORCID
Leszek Blacha
ORCID: ORCID
B. Węcki
1
ORCID: ORCID
D.G. Desisa
2
ORCID: ORCID
J. Łabaj
3
ORCID: ORCID
M. Jodkowski
1
ORCID: ORCID

  1. Department of Testing and Certification "ZETOM", Poland
  2. Department of Industrial, Informatics Silesian University of Technology, Joint Doctorate School, Poland
  3. Faculty of Materials Engineering, Silesian University of Technology, Poland
Download PDF Download RIS Download Bibtex

Abstract

The work deals with the influence of change in the filling conditions of the ceramic moulds with plaster binder on the presence of gaseous

porosity and the microstructure of the achieved test castings with graded wall thickness. Castings made of EN AC-44000 alloy, produced

either by gravity casting, or by gravity casting with negative pressure generated around the mould (according to the Vacumetal

technology), or by counter-gravity casting were compared. The results of examinations concerning the density of the produced castings

indicate that no significant change in porosity was found. The increased size of silicon crystals was found for the increased wall

thicknesses due to the slower cooling and solidification of castings.

Go to article

Authors and Affiliations

M. Nadolski
Z. Konopka
M. Łągiewka
A. Zyska
Download PDF Download RIS Download Bibtex

Abstract

Deoxidation of steel with carbon under reduced pressure is often used for increasing the steel purity. Suitable units for this purpose in

foundries are vacuum induction furnaces. Possibilities of increasing the steel purity by deoxidation with carbon in the vacuum induction

furnace were studied for the steel for the petrochemistry of specific composition 25Cr/35Ni. The charge composed of the return material

only was melted in the air. During melting the charge oxidized and the oxidizing slag formed. Chemical composition of steel, morphology,

chemical composition of inclusions in the steel and chemical composition of slag after vacuuming were studied on the basis of samples

taken before and after vacuuming. Temperature and oxygen activity were measured before and after vacuuming. Globular inclusions with

dominant content of silicon and manganese were observed in steel before and after vacuuming. Contents of total oxygen in steel didn’t

change significantly during vacuuming. On the basis of composition of inclusions and measured oxygen activity the activity of Cr2O3

in

inclusions was calculated. A slag sample was taken after vacuuming and equilibrium oxygen activity in steel with regard to the Cr2O3

content in the slag was estimated from the slag composition. Equilibrium oxygen activity in relation to the Cr2O3 content in the slag was

higher than equilibrium activity measured in the steel. For this reason it is not possible, under the studied conditions, to decrease oxygen

content in steel during vacuuming.

Go to article

Authors and Affiliations

J. Šenberger
V. Pernica
Download PDF Download RIS Download Bibtex

Abstract

The paper presents the results of investigations concerning the influence of negative (relative) pressure in the die cavity of high pressure

die casting machine on the porosity of castings made of AlSi9Cu3 alloy. Examinations were carried out for the VertaCast cold chamber

vertical pressure die casting machine equipped with a vacuum system. Experiments were performed for three values of the applied gauge

pressure: -0.3 bar, -0.5 bar, and -0.7 bar, at constant values of other technological parameters, selected during the formerly carried initial

experiments. Porosity of castings was assessed on the basis of microstructure observation and the density measurements performed by the

method of hydrostatic weighing. The performed investigation allowed to find out that – for the examined pressure range – the porosity of

castings decreases linearly with an increase in the absolute value of negative pressure applied to the die cavity. The negative pressure value

of -0.7 bar allows to produce castings exhibiting porosity value less than 1%. Large blowholes arisen probably by occlusion of gaseous

phase during the injection of metal into the die cavity, were found in castings produced at the negative pressure value of -0.3 bar. These

blowholes are placed mostly in regions of local thermal centres and often accompanied by the discontinuities in the form of interdendritic

shrinkage micro-porosity. It was concluded that the high quality AlSi9Cu3 alloy castings able to work in elevated temperatures can be

achieved for the absolute value of the negative pressure applied to the die cavity greater than 0.5 bar at the applied set of other parameters

of pressure die casting machine work.

Go to article

Authors and Affiliations

Z. Konopka
M. Łągiewka
A. Zyska
M. Nadolski
Download PDF Download RIS Download Bibtex

Abstract

The performed examinations concerning the process of filling the plaster ceramic moulds with aluminium alloys allowed to assess the

influence of various methods of introducing the metal into the mould cavity on the macro- and microstructure of the obtained experimental

castings. The comparison was performed for castings with graded wall thickness made either of EN AC-44000 alloy or of EN AC-46000

alloy, produced either by gravity casting, or by gravity casting with negative pressure generated around the mould (according to the

Vacumetal technology), or by counter-gravity casting. It was found that the silicon crystals grow in size with an increase in wall thickness

due to the slower cooling and solidification of castings.

Go to article

Authors and Affiliations

M. Nadolski
Z. Konopka
M. Łągiewka
A. Zyska
Download PDF Download RIS Download Bibtex

Abstract

Vacuum conditions in foundry installations are generated using electric-driven vacuum pumps. The purpose of the experiment is to evaluate the performance of a vacuum-assisted system for compaction of moulding sand basing on registered plots of selected electric power parameters of the power-supplying system of the pumps. Model testing done on an experimental vacuum system installation, power-supplied from a system incorporating the recorders of instantaneous current and voltage values. Following the numerical procedure, the experimental data are analysed to yield mathematical relationships between the variations of the generated vacuum pressure levels and variations of selected electric power parameters. Registered and computed values of selected parameters: instantaneous and RMS voltage and current values, active, reactive and apparent power levels and power coefficient allow for diagnosing the adequacy and reliability of the system operation. According to the authors, the applied monitoring of the power parameters of a vacuum-assisted installation may become an effective and easy practical method of evaluating the performance of such installations, used also in foundry plants.

Go to article

Authors and Affiliations

M. Brzeziński
E. Ziółkowski
R. Wrona
K. Smyksy
P. Zyzak
Download PDF Download RIS Download Bibtex

Abstract

In this article the main problems related with the proper choice of the design and operation parameters of vacuum installation in vacuum moulding system have been discussed. In such system a vacuum are generated using electric-driven vacuum pumps. The aim of the experiment is to evaluate the performance of a vacuum system basing on registered plots of selected electric power parameters of the power-supplying system of the pumps with parallel measurements instantaneous values of pressure in selected points of model stand. The measurements system for power-supply unit has incorporated the recorders of instantaneous current and voltage values. Following the suitable numerical procedure, the experimental data are analysed to yield mathematical relationships between the variations of the generated vacuum pressure levels and variations of selected electric power parameters. According to the authors, the applied measurements system of the parameters of a vacuum-assisted installation may become an effective and easy practical method of evaluating the performance of such installations, used also in industry.

Go to article

Authors and Affiliations

K. Smyksy
E. Ziółkowski
M. Brzeziński
R. Wrona
Download PDF Download RIS Download Bibtex

Abstract

The paper presents the use of rapid prototyping technology of three dimensional printing (3DP) to make a prototype shell casting mold. In

the first step, for identification purposes, a mold was prepared to enable different alloys to be cast. All molds being cast were designed in a

universal CAD environment and printed with the zp151 composite material (Calcium sulfate hemihydrate) with a zb63 binder (2-

pyrrolidone). It is designated to be used to prepare colourful models presenting prototypes or casting models and molds. The usefulness of

3DP technology for use with copper alloys, aluminum and zinc was analyzed. The strength of the mold during casting was assumed as a

characteristic comparative feature in the material resistance to high temperature, the quality of the resulting casting and its surface

roughness. Casting tests were carried out in vacuum – pressure casting. The casting programs applied, significantly increased the quality of

castings and enabled precise mold submergence. Significant improvement was noted in the quality compared to the same castings obtained

by gravity casting.

Go to article

Authors and Affiliations

G. Skorulski

This page uses 'cookies'. Learn more