Search results

Filters

  • Journals
  • Authors
  • Keywords
  • Date
  • Type

Search results

Number of results: 24
items per page: 25 50 75
Sort by:
Download PDF Download RIS Download Bibtex

Abstract

RADAR plays a vital role in military applications since its origin in the 2nd world war. Recently it has been used in surface inception, health monitoring, infrastructure health monitoring, etc. In these applications, Ultra-wideband RADAR systems are more popular than traditional RADAR systems. Impulse RADAR is a special kind of ultra-wideband RADAR, which is mostly used for surface penetration, through-wall imaging, antimissile detection, anti-stealth technology, etc. because of its high resolution and low center frequency. Out of all these applications, impulse RADAR has been used intensively as a ground-penetrating RADAR for the detection of land mines, underlying pipelines, buried objects, etc. This report has attempted to provide the steps for designing the impulse ground penetrating RADAR (GPR) as well as provides the value of crucial parameters required in the design process of commercial GPR systems.
Go to article

Bibliography

[1] M.G.M. Hussain, “Ultra-wideband impulse RADAR-An overview of the principles,” IEEE Aerosp. Electron. Syst. Mag., vol. 13, no. 9, pp. 9 -14, 1998. DOI: https://doi.org/10.1109/62.715515.
[2] D. L. Black, “An overview of impulse RADAR phenomenon,” IEEE AES Systems Magazine, pp. 6-11, Dec. 292. DOI: https://doi.org/10.1109/NAECON.1992.220600.
[3] M. I. Skolnik, “An Introduction To Impulse RADAR”, 1990.
[4] D. Daniels, “Applications of impulse RADAR technology,” Proc. RADAR Systems (RADAR 97), pp. 667 -672. DOI: https://doi.org/10.1049/cp:19971759.
[5] M. Sato, “Principles of mine detection by ground-penetrating RADAR,”Anti-personnel Landmine Detection for Humanitarian Demining, Springer London, 2009. 19-26. DOI: https://doi.org/10.1007/978-1-84882-346-4_2.
[6] M. N. Cohen, “An overview of high range resolution radar techniques,” NTC ’91 - National Telesystems Conference Proceedings, Atlanta, GA, USA, 1991, pp. 107-115, DOI: https://doi.org/10.1109/NTC.1991.147997.
[7] J. S. Lee and C. Nguyen, “Novel low-cost ultra-wideband, ultra-short-pulse transmitter with MESFET impulse-shaping circuitry for reduced distortion and improved pulse repetition rate,” IEEE Microwave Wireless Compon. Lett. , vol.11, pp. 208 -210, 2001. DOI: https://doi.org/10.1109/7260.923030.
[8] J. S. Lee and C. Nguyen, “Uniplanar picosecond pulse generator using step-recovery diode,” Electron. Lett., vol. 37, pp. 504–506, 2001. DOI: https://doi.org/10.1049/el:20010350
[9] J. Han and C. Nguyen, “Ultra-wideband electronically tuneable pulse generators,” IEEE Microw. Wireless Compon. Lett., vol. 14, no. 3, pp. 112 -114, 2004. DOI: https://doi.org/10.1109/LMWC.2004.825184.
[10] J. Han and C. Nguyen, “A new ultra-wideband, ultra-short monocycle pulse generator with reduced ringing,” IEEE Microwave Wireless Compon. Lett., vol. 12, pp. 206 -208, 2002. DOI: https://doi.org/10.1109/LMWC.2002.1009996.
[11] Yan Xiao, Zhong-Yong Wang, Li, J., Zi-Lun Yuan , “Design of a Second-Derivative Gaussian pulse generator,” IEEE International Conference on Signal Processing, Communication and Computing (ICSPCC), pp. 1 – 4, 2013. DOI: https://doi.org/10.1109/ICSPCC.2013.6663994.
[12] M.S. Nikoo, S.M.A. Hashemi., “High-Power Nanosecond Pulse Generator With High-Voltage SRD and GDT Switch,” IEEE Trans. Plasma Sci. ,vol. 43, no. 9, pp. 3268-3276, Sept. 2015. DOI: https://doi.org/10.1109/TPS.2015.2411251.
[13] M. Cavallaro, E. Ragonese and G. Palmisano, “An ultra-wideband transmitter based on a new pulse generator,” Proc. IEEE Radio Freq. Integ. Circuits Symp, pp. 43-46, 2008. DOI: https://doi.org/10.1109/RFIC.2008.4561382.
[14] El-Gabaly, “Pulsed RF Circuits for Ultra Wideband Communications and RADAR Applications,” Ph.D dissertation, Dept. Elect. Comput. Eng., Queen’s University, Canada, Aug. 2011.
[15] S. Bourdel et. al., “A 9-Pj/Pulse 1.42-Vpp OOK CMOS UWB pulse generator for the 3.1-10.6-GHz FCC band,” IEEE Trans. Microw. Theory Tech., vol. 58, no. 1, pp. 65, 2010. DOI: https://doi.org/10.1109/TMTT.2009.2035959.
[16] Aitykul Omurzakov, Ahmet K. Keskin., “Avalanche Transistor Short Pulse Generator Trials for GPR,” 2016 8th International Conference on Ultra wideband and Ultra short Impulse Signals), Dec. 2016. DOI: https://doi.org/10.1109/UWBUSIS.2016.7724188.
[17] Ran Zhang, Lai-Liang Song., “Research on narrow pulse generation for ultra-wideband communication,” 2016 13th International Computer Conference on Wavelet Active Media Technology and Information Processing (ICCWAMTIP), Dec. 2016. DOI: https://doi.org/10.1109/ICCWAMTIP.2016.8079860.
[18] S. Sim, D. Kim and S. Hong, “A CMOS UWB Pulse Generator for 6–10 GHz Applications,” IEEE Microwave and Wireless Components Letters, vol. 19, no. 2, pp. 83-85, Feb. 2009, DOI: https://doi.org/10.1109/LMWC.2008.2011318.
[19] K. Zhou, C. L. Huang and M. Lu, “A nanosecond pulse generator based on avalanche transistor,” 2016 16th International Conference on Ground Penetrating Radar (GPR), Hong Kong, 2016, pp. 1-5, DOI: https://doi.org/10.1109/ICGPR.2016.7572649.
[20] P. Protiva, J. Mrkvica, and J. Macháč, “A compact step recovery diode subnanosecond pulse generator,” Microw. Opt. Technol. Lett., 52: 438-440. DOI: https://doi.org/10.1002/mop.24945 .
[21] T.P. Montoya, G.S. Smith, “A study of pulse radiation from several broad-band loaded monopoles,” IEEE Trans. Antennas Propag., vol. 44, no. 8, pp. 1172-1182, Aug 1996. DOI: https://doi.org/10.1109/8.511827.
[22] David J. Daniels, Ground Penetrating RADAR, 2nd Edition, IET, 2005. DOI: https://doi.org/10.1049/PBRA015E.
[23] S. Vitebskiy, L. Carin, M. A. Ressler and F. H. Le, “Ultra-wideband, short-pulse ground-penetrating radar: simulation and measurement,” IEEE Transactions on Geoscience and Remote Sensing, vol. 35, no. 3, pp. 762-772, May 1997, DOI: https://doi.org/10.1109/36.581999.
[24] M.A. Gonzalez-Huici, U. Uschkerat, V. Seidel, C. Pedlow, “A preliminary study of the radiation characteristic of an experimental GPR antenna for underground cavity detection,” IEEE International Conference on Microwaves, Communications, Antennas and Electronics Systems (COMCAS), 2011, pp. 1-5, 7-9 Nov 2011. DOI: https://doi.org/10.1109/COMCAS.2011.6105908.
[25] A .P.Annan, Ground Penetrating RADAR Principles, Procedures & Applications, 2003.
[26] Greg Barrie, “UWB Impulse RADAR Characterization and Processing Techniques,” Defence R&D Canada, Ottawa, Tech. Rep. TR 2004-251, Dec. 2004.
[27] Y.J. Park et al., “Development of a UWB GPR System for Detecting Small Objects Buried under Ground,” IEEE Conf. on ultra-wideband systems and Technologies, 2003, pp.384-388. DOI: https://doi.org/10.1109/UWBST.2003.1267869.
[28] M. Yan, M. Tian, L. Gan and X. Chen, “Impulse Ground Penetrating Radar Hardware System Design,” 2006 6th International Conference on ITS Telecommunications, Chengdu, 2006, pp. 1244-1247, DOI: https://doi.org/10.1109/ITST.2006.288852.
[29] A.P. Annan, L.T. Chua, “Ground penetrating RADAR performance predictions,” Ground penetrating RADAR, ed. J. Pilon; Geological Survey of Canada, Paper 90-4, pp. 5-13, 1992.
[30] Jeong Soo Lee, Cam Nguyen and T. Scullion, “A novel, compact, low-cost, impulse ground-penetrating radar for nondestructive evaluation of pavements,” IEEE Transactions on Instrumentation and Measurement, vol. 53, no. 6, pp. 1502-1509, Dec. 2004, DOI: https://doi.org/10.1109/TIM.2004.82730.
Go to article

Authors and Affiliations

Saket Kumar
1
Amit Kumar
2
Vikrant Singh
3
Abhishek Kumar Singh
4

  1. Department of Electronics and Communication Engineering, Muzaffarpur Institute of Technology, Muzaffarpur, Bihar, India
  2. Department of Electronics and Communication Engineering, Bharati Vidyapeeth (Deemed to be University) College of Engineering, Pune, India
  3. Department of Electrical and Electronics Engineering, IIT Guwahati, India
  4. School of Advanced Sciences, Department of Physics, Vellore Institute of Technology, Vellore, Tamil Naidu, India
Download PDF Download RIS Download Bibtex

Abstract

Activated tungsten inert gas (ATIG) welding has a good depth of penetration (DOP) as compared to the conventional tungsten inert gas (TIG) welding. This paper is mainly focused on ATIG characterization and mechanical behavior of aluminum alloy (AA) 6063-T6 using SiO2 flux. The characterization of the base material (BM), fusion zone (FZ), heat affected zone (HAZ) and, partially melted zone is carried out using the suitable characterization methods. The weld quality is characterized using ultrasonic-assisted non-destructive evaluation. A-scan result confirms that the ATIG welded samples have more DOP and less bead width as compared to conventional TIG. The recorded tensile strength of ATIG with SiO2 is better than the conventional TIG welding. The failure mode is ductile for ATIG welding with larger fracture edges and is brittle in the case of conventional TIG welding.

Go to article

Bibliography

  1.  S. Jannet, P.K. Mathews, and R. Raja, “Comparative investigation of friction stir welding and fusion welding of 6061T6 – 5083 O aluminum alloy based on mechanical properties and microstructure”, Bull. Pol. Ac.: Tech. 62(4), 791‒795 (2014), doi: 10.2478/bpasts-2014-0086.
  2.  S.T. Amancio-Filho, S. Sheikhi, J.F. dos Santos, and C. Bolfarini, “Preliminary study on the microstructure and mechanical properties of dissimilar friction stir welds in aircraft aluminium alloys 2024-T351 and 6056-T4”, J. Mater. Process. Technol. 206. 132–142 (2008), doi: 10.1016/j.jmatprotec.2007.12.008.
  3.  P. Mukhopadhyay, “Alloy Designation, Processing, and Use of AA6XXX Series Aluminium Alloys”, ISRN Metall. 2012, 165082 (2012), doi: 10.5402/2012/165082.
  4.  B. Choudhury and M. Chandrasekaran, “Investigation on welding characteristics of aerospace materials – A review”, Mater. Today Proc. 4, 7519–7526 (2017), doi: 10.1016/j.matpr.2017.07.083.
  5.  R.R. Ambriz and V. Mayagoitia, “Welding of Aluminum Alloys”, in Welding, Brazing and Soldering, pp. 722–739, ASM International, 2018. doi: 10.31399/asm.hb.v06.a0001436.
  6. [6]  P.J. Modenesi, “The chemistry of TIG weld bead formation”, Weld. Int. 29, 771–782 (2015), doi: 10.1080/09507116.2014.932990.
  7.  A.K. Singh, V. Dey, and R.N. Rai, “Techniques to improveweld penetration in TIG welding (A review)”, Mater. Today Proc. 4, 1252–1259 (2017), doi: 10.1016/j.matpr.2017.01.145.
  8.  R.S. Vidyarthy and D.K. Dwivedi, “Activating flux tungsten inert gas welding for enhanced weld penetration”, J. Manuf. Process. 22, 211–228 (2016), doi: 10.1016/j.jmapro.2016.03.012.
  9.  R.S. Vidyarthy and D.K. Dwivedi, “Microstructural and mechanical properties assessment of the P91 A-TIG weld joints”, J. Manuf. Process. 31, 523–535 (2018), doi: 10.1016/j.jmapro.2017.12.012.
  10.  K.D. Ramkumar, V. Varma, M. Prasad, N.D. Rajan, and N.S. Shanmugam, “Effect of activated flux on penetration depth, microstructure and mechanical properties of Ti-6Al-4V TIG welds”, J. Mater. Process. Technol. 261, 233–241 (2018), doi: 10.1016/j.jmatprotec.2018.06.024.
  11.  H. Kumar and N.K. Singh, “Performance of activated TIG welding in 304 austenitic stainless steel welds”, Mater. Today Proc. 4, 9914–9918 (2017), doi: 10.1016/j.matpr.2017.06.293.
  12.  R.S. Vidyarthy, A. Kulkarni, and D.K. Dwivedi, “Study of microstructure and mechanical property relationships of A-TIG welded P91–316L dissimilar steel joint”, Mater. Sci. Eng. A. 695, 249–257 (2017), doi: 10.1016/j.msea.2017.04.038.
  13.  E.R. Imam Fauzi, M.S. Che Jamil, Z. Samad, and P. Muangjunburee, “Microstructure analysis and mechanical characteristics of tungsten inert gas and metal inert gas welded AA6082-T6 tubular joint: A comparative study”, Trans. Nonferrous Met. Soc. China (English Ed.) 27, 17–24 (2017), doi: 10.1016/S1003-6326(17)60003-7.
  14.  R.S. Coelho, A. Kostka, J.F. dos Santos, and A. Kaysser-Pyzalla, “Friction-stir dissimilar welding of aluminium alloy to high strength steels: Mechanical properties and their relation to microstructure”, Mater. Sci. Eng. A. 556, 175–183 (2012), doi: 10.1016/j.msea.2012.06.076.
  15.  A.S. Zoeram, S.H.M. Anijdan, H.R. Jafarian, and T. Bhattacharjee, “Welding parameters analysis and microstructural evolution of dissimilar joints in Al/Bronze processed by friction stir welding and their effect on engineering tensile behavior”, Mater. Sci. Eng. A. 687, 288–297, (2017). doi: 10.1016/j.msea.2017.01.071.
  16.  K.H. Dhandha and V.J. Badheka, “Effect of activatingfluxes on weld bead morphology of P91 steelbead-on-platewelds by flux assisted tungsteninert gas welding process”, J. Manuf. Process. 17, 48–57 (2015), doi: 10.1016/j.jmapro.2014.10.004.
  17.  A. Krajewski, W. Włosiński, T. Chmielewski, and P. Kołodziejczak, “Ultrasonic-vibration assisted arc-welding of aluminum alloys”, Bull. Pol. Ac.: Tech. 60(4), 841‒852 (2012), doi: 10.2478/v10175-012-0098-2.
  18.  H.S. Patil and S.N. Soman, “Effect of tool geometry and welding speed on mechanical properties and microstructure of friction stir welded joints of aluminum alloys AA6082-T6”, Arch. Mech. Eng. 61, 455‒468 (2014), doi: 10.2478/meceng-2014-0026.
Go to article

Authors and Affiliations

Rajiv Kumar
1
S.C. Vettivel
2
Harmesh Kumar Kansal
1

  1. Department of Mechanical Engineering, UIET, Panjab University, Chandigarh, India
  2. Department of Mechanical Engineering, Chandigarh College of Engineering and Technology (Degree Wing), Chandigarh, India
Download PDF Download RIS Download Bibtex

Abstract

This paper presents a suggested approach for forensic investigation of bridge decks in which Ground penetrating radar (GPR) consisting of two antennas is used to assess the current conditions. The methodology was tested on a bridge deck in central Sicily. The acquired data were analyzed for identifying the asphalt overlay thickness, concrete cover depth and deck thickness and location of the rebar reinforcement. In the proposed approach for assessing bridge deck conditions the GPR survey was complemented with (i) a site investigation on layer thicknesses for calibration/verification purposes of the GPR response and (ii) a Terrestrial Laser Scanning system (TLS) to verify the bridge design slab curvature. The study shows that this methodology has significant merits on accurately assessing such bridge deck components when bridge design records are non-existing, and by using non-invasive methods such as laser scanning and GPR. The great advantage provided by the TLS technique is the possibility to obtain a 3D output model of the scanned element with the accuracy of the best topographic instruments in order to complement GPR data surveys for bridge inspection.

Go to article

Authors and Affiliations

S. Cafiso
A. Di Graziano
D. Goulias
M. Mangiameli
G. Mussumeci
Download PDF Download RIS Download Bibtex

Abstract

The ground-penetrating radar (GPR) method has been used for many years in archaeological research. However, this method is still not widely used in studies of past architecture. The biggest problem with the implementation of the GPR method at such sites is usually connected with extensive debris layers, plant cover and standing relics of walls and other features that restrict the available measurement area. Despite of these, properly performed GPR surveys, even on a small area, can yield significant information concerning underground architectural relicts. Moreover, the results of GPR profiling integrated with historical and archeological data allow for three-dimensional reconstruction of the examined architectural monuments and in the next step, they track architectural transformations. Relics of the Romanesque St. Peter monastery, located in the northern part of the Island of Rab, is a good example of the successful GPR survey. Results of the performed geophysical reconnaissance in conjunction with the query of archival materials made it possible to visualize a spatial (3D) appearance of three main phases of the site architectural development, despite a very limited area available for geophysical survey. According to the authors, such a comprehensive approach should be a standard in contemporary geophysical research focused on relics of the past architecture.
Go to article

Authors and Affiliations

Fabian Welc
1
Ana Konestra
2
ORCID: ORCID

  1. Cardinal Stefan Wyszyński University, Institute of Archaeology, Wóycickiego 1/3, bud. 23, 01-938 Warsaw, Poland
  2. Institute of Archaeology, Jurjevska ulica 15, 10000 Zagreb, Croatia
Download PDF Download RIS Download Bibtex

Abstract

This paper presents the impact of microwave penetration depth on the process of heating the moulding sand with sodium silicate. For each material it is affected by: the wavelength in vacuum and the real and imaginary components of the relative complex electrical permittivity εrfor a selected measurement frequency. Since the components are not constant values and they change depending on the electrical parameters of materials and the frequency of the electromagnetic wave, it is indispensable to carry out laboratory measurements to determine them. Moreover, the electrical parameters of materials are also affected by: temperature, packing degree, humidity and conductivity. The measurements of the dielectric properties of moulding sand with sodium silicate was carried out using the perturbation method on a stand of waveguide resonance cavity. The real and imaginary components of the relative complex electrical permittivity was determined for moulding sand at various contents of sodium silicate and at various packing degrees of the samples. On the basis of the results the microwave penetration depth of moulding sand with sodium silicate was established. Relative literature contains no such data that would be essential to predicting an effective process of microwave heating of moulding sand with sodium silicate. Both the packing degree and the amount of sodium silicate in moulding sand turned out to affect the penetration depth, which directly translates into microwave power density distribution in the process of microwave heating of moulding sand with sodium silicate.

Go to article

Authors and Affiliations

D. Nowak
Download PDF Download RIS Download Bibtex

Abstract

The main goal of the article is to identify artificially created defects like lack of fusion and incomplete penetration in butt weld joint using non-destructive volumetric methods. These defects are the most serious defects in welds of steel constructions from the safety point of view. For identification, an ultrasonic phased array technique and a conventional X-ray using digital imaging were used. The theoretical part of the article describes the current state of the given issue and provides basic theoretical knowledge about ultrasonic and X-ray welding tests. In the experimental part, the procedure and results of testing butt weld joint are described by both non-destructive methods. The butt weld joint was made from steel S420MC. Each indication obtained by the ultrasonic and x-ray technique is supplemented by the macrostructure of the weld taken from the indication position. The results of the experimental work mentioned in the article point to the possibility and reliability of the identification of melting defects by selected nondestructive methods in terms of their character and orientation.

Go to article

Authors and Affiliations

R. Koňár
M. Mičian
M. Boháčik
M. Gucwa
Download PDF Download RIS Download Bibtex

Abstract

The aim of the study is to identify the relevant aspects of numerical analysis of impact of projectiles with soft cores into a package composed of thin flexible plies located on the plastic backing. In order to illustrate the problem, normal impact of 7.62 mm TT projectile into an unclamped package comprising 36 plies of Dyneema SB71 supported on the plastic backing was selected. The problem was solved with the use of the finite element method (FEM) with the explicit integration scheme (central difference method) of motion equations in the matrix form. Based on the conducted numerical computations, it was revealed that obtaining the extreme deformations of a projectile soft core and the backing material in Lagrangian description requires employment of adaptive methods. The proposed R-adaptive method performs its role but must be used carefully due to the mass loss which may appear during calculations.

Go to article

Bibliography

[1] A. Valera-Medina, A. Giles, D. Pugh, S. Morris, M. Pohl, and A. Ortwein. Investigation of combustion of emulated biogas in a gas turbine test rig. Journal of Thermal Science, 27:331–340, 2018. doi: 10.1007/s11630-018-1024-1.
[2] K. Tanaka and I. Ushiyama. Thermodynamic performance analysis of gas turbine power plants with intercooler: 1st report, Theory of intercooling and performance of intercooling type gas turbine. Bulletin of JSME, 13(64):1210–1231, 1970. doi: 10.1299/jsme1958.13.1210.
[3] H.M. Kwon, T.S. Kim, J.L. Sohn, and D.W. Kang. Performance improvement of gas turbine combined cycle power plant by dual cooling of the inlet air and turbine coolant using an absorption chiller. Energy, 163:1050–1061, 2018. doi: 10.1016/j.energy.2018.08.191.
[4] A.T. Baheta and S.I.-U.-H. Gilani. The effect of ambient temperature on a gas turbine performance in part load operation. AIP Conference Proceedings, 1440:889–893, 2012. doi: 10.1063/1.4704300.
[5] F.R. Pance Arrieta and E.E. Silva Lora. Influence of ambient temperature on combined-cycle power-plant performance. Applied Energy, 80(3):261–272, 2005. doi: 10.1016/j.apenergy.2004.04.007.
[6] M. Ameri and P. Ahmadi. The study of ambient temperature effects on exergy losses of a heat recovery steam generator. In: Cen, K., Chi, Y., Wang, F. (eds) Challenges of Power Engineering and Environment. Springer, Berlin, Heidelberg, 2007. doi: 10.1007/978-3-540-76694-0_9.
[7] M.A.A. Alfellag: Parametric investigation of a modified gas turbine power plant. Thermal Science and Engineering Progress, 3:141–149, 2017. doi: 10.1016/j.tsep.2017.07.004.
[8] J.H. Horlock and W.A. Woods. Determination of the optimum performance of gas turbines. Proceedings of the Institution of Mechanical Engineers, Part C: Journal of Mechanical Engineering Science, 214:243–255, 2000. doi: 10.1243/0954406001522930.
[9] L. Battisti, R. Fedrizzi, and G. Cerri. Novel technology for gas turbine blade effusion cooling. In: Proceedings of the ASME Turbo Expo 2006: Power for Land, Sea, and Air. Volume 3: Heat Transfer, Parts A and B. pages 491–501. Barcelona, Spain. May 8–11, 2006. doi: 10.1115/GT2006-90516.
[10] F.J. Wang and J.S. Chiou. Integration of steam injection and inlet air cooling for a gas turbine generation system. Energy Conversion and Management, 45(1):15–26, 2004. doi: 10.1016/S0196-8904 (03)00125-0.
[11] Z. Wang. 1.23 Energy and air pollution. In I. Dincer (ed.): Comprehensive Energy Systems, pp. 909–949. Elsevier, 2018. doi: 10.1016/B978-0-12-809597-3.00127-9.
[12] Z. Khorshidi, N.H. Florin, M.T. Ho, and D.E. Wiley. Techno-economic evaluation of co-firing biomass gas with natural gas in existing NGCC plants with and without CO$_2$ capture. International Journal of Greenhouse Gas Control, 49:343–363, 2016. doi: 10.1016/j.ijggc.2016.03.007.
[13] K. Mohammadi, M. Saghafifar, and J.G. McGowan. Thermo-economic evaluation of modifications to a gas power plant with an air bottoming combined cycle. Energy Conversion and Management, 172:619–644, 2018. doi: 10.1016/j.enconman.2018.07.038.
[14] S. Mohtaram, J. Lin, W. Chen, and M.A. Nikbakht. Evaluating the effect of ammonia-water dilution pressure and its density on thermodynamic performance of combined cycles by the energy-exergy analysis approach. Mechanika, 23(2):18110, 2017. doi: 10.5755/j01.mech.23.2.18110.
[15] M. Maheshwari and O. Singh. Comparative evaluation of different combined cycle configurations having simple gas turbine, steam turbine and ammonia water turbine. Energy, 168:1217–1236, 2019. doi: 10.1016/j.energy.2018.12.008.
[16] A. Khaliq and S.C. Kaushik. Second-law based thermodynamic analysis of Brayton/Rankine combined power cycle with reheat. Applied Energy, 78(2):179–197, 2004. doi: 10.1016/j.apenergy.2003.08.002.
[17] M. Aliyu, A.B. AlQudaihi, S.A.M. Said, and M.A. Habib. Energy, exergy and parametric analysis of a combined cycle power plant. Thermal Science and Engineering Progress. 15:100450, 2020. doi: 10.1016/j.tsep.2019.100450.
[18] M.N. Khan, T.A. Alkanhal, J. Majdoubi, and I. Tlili. Performance enhancement of regenerative gas turbine: air bottoming combined cycle using bypass valve and heat exchanger—energy and exergy analysis. Journal of Thermal Analysis and Calorimetry. 144:821–834, 2021. doi: 10.1007/s10973-020-09550-w.
[19] F. Rueda Martínez, A. Rueda Martínez, A. Toleda Velazquez, P. Quinto Diez, G. Tolentino Eslava, and J. Abugaber Francis. Evaluation of the gas turbine inlet temperature with relation to the excess air. Energy and Power Engineering, 3(4):517–524, 2011. doi: 10.4236/epe.2011.34063.
[20] A.K. Mohapatra and R. Sanjay. Exergetic evaluation of gas-turbine based combined cycle system with vapor absorption inlet cooling. Applied Thermal Engineering, 136:431–443, 2018. doi: 10.1016/j.applthermaleng.2018.03.023.
[21] A.A. Alsairafi. Effects of ambient conditions on the thermodynamic performance of hybrid nuclear-combined cycle power plant. International Journal of Energy Research, 37(3):211–227, 2013. doi: 10.1002/er.1901.
[22] A.K. Tiwari, M.M. Hasan, and M. Islam. Effect of ambient temperature on the performance of a combined cycle power plant. Transactions of the Canadian Society for Mechanical Engineering, 37(4):1177–1188, 2013. doi: 10.1139/tcsme-2013-0099.
[23] T.K. Ibrahim, M.M. Rahman, and A.N. Abdalla. Gas turbine configuration for improving the performance of combined cycle power plant. Procedia Engineering, 15:4216–4223, 2011. doi: 10.1016/j.proeng.2011.08.791.
[24] M.N. Khan and I. Tlili. New advancement of high performance for a combined cycle power plant: Thermodynamic analysis. Case Studies in Thermal Engineering. 12:166–175, 2018. doi: 10.1016/j.csite.2018.04.001.
[25] S.Y. Ebaid and Q.Z. Al-hamdan. Thermodynamic analysis of different configurations of combined cycle power plants. Mechanical Engineering Research. 5(2):89–113, 2015. doi: 10.5539/mer.v5n2p89.
[26] R. Teflissi and A. Ataei. Effect of temperature and gas flow on the efficiency of an air bottoming cycle. Journal of Renewable and Sustainable Energy, 5(2):021409, 2013. doi: 10.1063/1.4798486.
[27] A.A. Bazmi, G. Zahedi, and H. Hashim. Design of decentralized biopower generation and distribution system for developing countries. Journal of Cleaner Production, 86:209–220, 2015. doi: 10.1016/j.jclepro.2014.08.084.
[28] A.I. Chatzimouratidis and P.A. Pilavachi. Decision support systems for power plants impact on the living standard. Energy Conversion and Management, 64:182–198, 2012. doi: 10.1016/j.enconman.2012.05.006.
[29] T.K. Ibrahim, F. Basrawi, O.I. Awad, A.N. Abdullah, G. Najafi, R. Mamat, and F.Y. Hagos. Thermal performance of gas turbine power plant based on exergy analysis. Applied Thermal Engineering, 115:977–985, 2017. doi: 10.1016/j.applthermaleng.2017.01.032.
[30] M. Ghazikhani, I. Khazaee, and E. Abdekhodaie. Exergy analysis of gas turbine with air bottoming cycle. Energy, 72:599–607, 2014. doi: 10.1016/j.energy.2014.05.085.
[31] M.N. Khan, I. Tlili, and W.A. Khan. thermodynamic optimization of new combined gas/steam power cycles with HRSG and heat exchanger. Arabian Journal for Science and Engineering, 42:4547–4558, 2017. doi: 10.1007/s13369-017-2549-4.
[32] N. Abdelhafidi, İ.H. Yılmaz, and N.E.I. Bachari. An innovative dynamic model for an integrated solar combined cycle power plant under off-design conditions. Energy Conversion and Management, 220:113066, 2020. doi: 10.1016/j.enconman.2020.113066.
[33] T.K. Ibrahim, M.K. Mohammed, O.I. Awad, M.M. Rahman, G. Najafi, F. Basrawi, A.N. Abd Alla, and R. Mamat. The optimum performance of the combined cycle power plant: A comprehensive review. Renewable and Sustainable Energy Reviews, 79:459–474, 2017. doi: 10.1016/j.rser.2017.05.060.
[34] M.N. Khan. Energy and exergy analyses of regenerative gas turbine air-bottoming combined cycle: optimum performance. Arabian Journal for Science and Engineering, 45:5895–5905, 2020. doi: 10.1007/s13369-020-04600-9.
[35] A.M. Alklaibi, M.N. Khan, and W.A. Khan. Thermodynamic analysis of gas turbine with air bottoming cycle. Energy, 107:603–611, 2016. doi: 10.1016/j.energy.2016.04.055.
[36] M. Ghazikhani, M. Passandideh-Fard, and M. Mousavi. Two new high-performance cycles for gas turbine with air bottoming. Energy, 36(1):294–304, 2011. doi: 10.1016/j.energy.2010.10.040.
[37] M.N. Khan and I. Tlili. Innovative thermodynamic parametric investigation of gas and steam bottoming cycles with heat exchanger and heat recovery steam generator: Energy and exergy analysis. Energy Reports, 4:497–506, 2018. doi: 10.1016/j.egyr.2018.07.007.
[38] M.N. Khan and I. Tlili. Performance enhancement of a combined cycle using heat exchanger bypass control: A thermodynamic investigation. Journal of Cleaner Production, 192:443–452, 2018. doi: 10.1016/j.jclepro.2018.04.272.
[39] M. Korobitsyn. Industrial applications of the air bottoming cycle. Energy Conversion and Management, 43(9-12):1311–1322, 2002. doi: 10.1016/S0196-8904(02)00017-1.
[40] T.K. Ibrahim and M.M. Rahman. optimum performance improvements of the combined cycle based on an intercooler–reheated gas turbine. Journal of Energy Resources Technology, 137(6):061601, 2015. doi: 10.1115/1.4030447.
Go to article

Authors and Affiliations

Andrzej Morka
Piotr Kędzierski
Roman Gieleta

Download PDF Download RIS Download Bibtex

Abstract

This study attempts to evaluate the field performance of various mining equipment used at the development galleries of coal mines. These are hand-held and jumbo rock drills, and a roadheader used in mechanical excavation. For this purpose, the penetration rates of rock drills were monitored and measured in the field. The physical, mechanical, and drillability properties were determined through the collected samples in order to understand the complex interactions between the rock and bit/pick. The abrasive mineral content was also analyzed with XRD analysis to examine the wear on the cutting/drilling tools. Besides, the specific energy of the equipment was calculated relying on the operational parameters. A comparison of the monthly advance and production rates of the drilling rigs and roadheader was made. The relations among operating power, specific energy, and design of buttons/picks were investigated. It has been found that the average advance and production rates of the mining equipment are consistent with the penetration rate. The results verified that the roadheader used in mechanical excavation and the jumbo drill used in drilling and blasting technique are the machines maximizing the advance and production rates.

Go to article

Authors and Affiliations

Okan Su
ORCID: ORCID
Download PDF Download RIS Download Bibtex

Abstract

In this paper, the macroscopic and microscopic deformation caused by sodium penetration in the carbon cathode has been studied during aluminum electrolysis. The distributions of sodium concentration in the carbon cathode has been measured by SEM-EDS. The microstructure change caused by the gradient of the sodium concentration in the carbon cathode has been studied using transmission electron microscopy (TEM). The results indicate that sodium penetration decreases with the increase of the penetration depth. The stresses caused by the gradient of the sodium concentration result in a remarkable change for the microstructure of the carbon cathode. The formation of dislocations resulting in dislocation arrays and the development of kink band networks bring about material damage growth and possibly subsequent weakening of the cathode. These results can provide useful information that is helpful in developing an improved comprehending of the microscopic deformation mechanism of the carbon cathode during aluminum electrolysis.
Go to article

Authors and Affiliations

Haitao Liu
1 2 3
ORCID: ORCID
Yunhong Huang
4
ORCID: ORCID
Wei Wang
1 2 3
ORCID: ORCID
Ziyang Zhang
1 2 3
ORCID: ORCID
Hengyao Dang
5
ORCID: ORCID

  1. Henan University of Science and Technology, College of Materials Science and Engineering, Luoyang 471023, China
  2. Collaborative Innovation Center of Nonferrous Metals Henan Province, Luoyang 471023, China
  3. Henan Key Laboratory of Non-ferrous Materials Science & Processing Technology, Luoyang 471023, China
  4. Henan University of Science and Technology, Engineering Training Center, Luoyang 471023, China
  5. Luoyang Ship Material Research Institute, Luoyang 471023, China
Download PDF Download RIS Download Bibtex

Abstract

Porous asphalt mixture (PA), known as open-graded surfaces over a stone bed underneath, allows water to go through. These factors can affect the porous asphalt mixture adhesive strength. The high amount of course aggregate promotes the structure of air voids have certain impacts on the acoustic properties of porous asphalt. The materials properties are consisting of both aggregate and bitumen tests. This study also details out the aggregates sieve analysis test to develop new aggregate gradation for PA. According to five ASEAN countries’ specifications, the sieve analysis test was done. The countries included are Malaysia, Vietnam, Thailand, Singapore, and Indonesia. The test for the binder includes the softening point, penetration, and ductility. This study also investigates the addition of kenaf fiber in the mixture as an additive. Mechanical performance test for PA using Marshall Stability test to identify the strength and the properties of the conventional PA with the addition of kenaf fiber compared to the new gradation of PA incorporating kenaf fiber. From the results, the addition of 0.3% kenaf modified PA improved the performance of PA in terms of Marshall Stability and volumetric properties.
Go to article

Authors and Affiliations

Nur Ezreen Jasni
1
ORCID: ORCID
Khairi Azman Masri
1
ORCID: ORCID
Ramadhansyah Putra Jaya
1
ORCID: ORCID
Mohd Mustafa Al Bakri Abdullah
2
ORCID: ORCID
Rafiza Abd Razak
3
ORCID: ORCID
Marcin Nabiałek
4
ORCID: ORCID
Katarzyna Błoch
4
ORCID: ORCID
Agata Śliwa
5
ORCID: ORCID

  1. Department of Civil Engineering, College of Engineering, Universiti Malaysia Pahang, 26300 Gambang, Kuantan, Pahang, Malaysia
  2. Faculty of Chemical Engineering Technology, Universiti Malaysia Perlis, 02600 Arau, Perlis, Malaysia
  3. Center of Excellence Geopolymer and Green Technology, Universiti Malaysia Perlis, 01000 Kangar, Perlis, Malaysia
  4. Department of Physics, Czestochowa University of Technology, 42-201 Czestochowa, Poland
  5. Division of Materials Processing Technology and Computer Techniques in Materials Science, Silesian21 University of Technology, Poland
Download PDF Download RIS Download Bibtex

Abstract

The article presents application of the new geophysical amplitude data comparison method (ADCM), resulting from integrated geophysical survey using ground-penetrating radar (GPR) and magnetometry. The ADCM was applied to recognize the horizontal and vertical stratigraphy of a Roman senatorial villa located in Santa Marina (western part of Croatian Istria). The measurements were carried out in 2017−2019 at this site, accompanied by a use of GPR and gradientometer. These two methods significantly differ from each other, but on the other hand, they are complementary to some extent. This is due to the fact that the methods register different types of underground materials. The GPR records electromagnetic waves reflected from real buried remains or boundaries between geological or archaeological layers that differ significantly in electrical properties. The magnetic method, in turn, records the anomalies of the magnetic field intensity resulting from the underground concentration of ferromagnetic minerals, hence it is ideal for searching structures filled with organic matter or burning material. However, a separate usage of these methods does not guarantee a full picture of archaeological structures that are preserved underground. Only the application of the ADCM allowed for a comparison of GPR and magnetic amplitude data reading, following which a spatial image (2D and 3D) of the preserved archaeological structures and the geological stratigraphy of the Santa Maria site were obtained.

Go to article

Authors and Affiliations

Fabian Welc
Corinne Rousse
Gaetano Bencic
Download PDF Download RIS Download Bibtex

Abstract

This study used ground penetrating radar soundings to examine a tongue-shaped rock glacier (64°04’S 58°25’W) on James Ross Island, Antarctic Peninsula, in January 2005. The rock glacier studied has multiple well-developed transverse ridges and approximately 800 m long from the talus of its head to its frontal slopes and is 300 m wide in the middle. The longitudinal ground penetrating radar profile identified debris bands which dip up-glacier, similar to the thrust structures in the compression zone of a valley glacier. Transverse ground penetrating radar profiles indicated a layered structure which is inclined towards the central part of the rock glacier and which resembles the transverse foliation of a valley glacier. Consequently, the internal structure of the rock glacier is revealed as being similar to the “nested spoons” common in the interior of valley glaciers. We concluded that this rock glacier has been created by the deformation of a glacier ice core and a thick and continuous debris mantle.

Go to article

Authors and Affiliations

Kotaro Fukui
Toshio Sone
Jorge A. Strelin
Cesar A. Torielli
Junko Mori
Download PDF Download RIS Download Bibtex

Abstract

The paper presents the results of a series of Cone Penetration Test CPTu performed near the city of Wroclaw (Poland). The tests were carried out in 13 testing points located in close distance to each other. To verify the results of the penetration tests, fine-grained soil samples from selected depths were taken for laboratory tests. The study focuses on the evaluation of soil type, unit weight, and undrained shear strength cu, and compression index Cc. The grain size distribution of the soil and its mechanical parameters on the basis of a uniaxial compression and an oedometer tests were estimated. A comparison of laboratory and CPTu for selected values is presented. Determination of soil type was carried out on the basis of ISBT and IC values and good agreement with the granulometric composition was found. For undrained shear strength, commonly used correlations based on Nk, Nkt and Nke were adopted. However, the values obtained from the CPT are significantly lower than the results from laboratory tests. Therefore, values of cone factors suitable for investigated soil type and reference test were proposed. In the case of the compression index, the coefficient values βc and αm obtained agreed with those available in the literature. The findings presented in the paper indicate that laboratory tests remain necessary to identify soil properties from CPTu. The presented results are also a contribution to the knowledge of local soil conditions in the Lower Silesia area (Poland).
Go to article

Bibliography

[1] F.H. Kulhawy, P.W. Mayne, Manual on estimating soil properties for foundation design (No. EPRI-EL-6800). Electric Power Research Inst., Palo Alto, CA (USA ); Cornell Univ., Ithaca, NY (USA ), Geotechnical Engineering Group (1990).
[2] T . Lunne, P.K. Robertson, J.J.M. Powell, Cone Penetration Testing in Geotechnical Practice. Blackie Academic/ Routledge Publishing, New York (1997).
[3] K . Karlsrud, T. Lunne, D.A. Kort, S. Strandvik, CPTU correlations for clays. In: Proceedings of the International Conference on Soil Mechanics and Geotechnical Engineering 16 (2), p. 693 (2005).
[4] P.K. Robertson, Interpretation of cone penetration tests — a unified approach. Can. Geoech. J. 46 (11), 1337-1355 (2009), DOI: https://doi.org/10.1139/T09-065
[5] P .K. Robertson, The James K. Mitchell Lecture: Interpretation of in-situ tests-some insights. In: Proc. 4th Int. Conf. on Geotechnical and Geophysical Site Characterization – ISC 4, 3-24 (2012).
[6] P .W. Mayne, Interpretation of geotechnical parameters from seismic piezocone tests. In: Proc. 3rd Intl. Symposium on Cone Penetration Testing, CPT’14, 47-73 (2014).
[7] A. Eslami, S. Moshfeghi, H. MolaAbasi, M.M. Eslami, Piezocone and Cone Penetration Test (CPTu and CPT) Applications in Foundation Engineering. Butterworth-Heinemann (2019).
[8] P.K. Robertson, Soil behaviour type from the CPT. In: Proc. 2nd Int. Symposium on Cone Penetration Testing, CPT’10 (2010).
[9] P.K. Robertson, Cone penetration test (CPT)-based soil behaviour type (SBT) classification system — an update. Can. Geotech. J. 53 (12), 1910-1927 (2016) DOI: https://doi.org/10.1139/cgj-2016-0044
[10] P.K. Robertson, K.L. Cabal, Estimating soil unit weight from CPT. In: Proc. 2nd Int. Symposium on Cone Penetration Testing, CPT’10 (2010).
[11] P.W. Mayne, J. Peuchen, D. Bouwmeester, Soil unit weight estimation from CPTs. In: Proc. 2nd Int. Symposium on Cone Penetration Testing, CPT’10, (2010).
[12] L .Y. Ju, C. Miao, Z.J. Cao, P. Hubbard, K. Soga, K., D.Q. Li, Geo-Congress 2020: Modeling. Geomaterials and Site Characterization, 558-568 (2020).
[13] K . Karlsrud, K. Brattlien, T. Lunne, Improved CPTU interpretations based on block samples. NGI (1997).
[14] H.E. Low, T. Lunne, K.H. Andersen, M.A. Sjursen, X. Li, M.F. Randolph, Estimation of intact and remoulded undrained shear strengths from penetration tests in soft clays. Géotechnique 60 (11), 843-859 (2010), DOI: https://doi.org/10.1680/geot.9.P.017
[15] Z . Rémai, Correlation of undrained shear strength and CPT resistance. Per. Pol. Civil Eng. 57 (1), 39-44 (2013), DOI: https://doi.org/10.3311/PPci.2140
[16] A .K.M. Zein, International Journal of Geo-Engineering 8 (1), (2017), DOI: https://doi.org/10.1186/s40703-017- 0046-y
[17] P.W. Mayne, J. Peuchen, Evaluation of CPTU Nkt cone factor for undrained strength of clays. In: Proc. 4th Intl. Symposium on Cone Penetration Testing (CPT’18), 423-429 (2018).
[18] A. Drevininkas, G. Creer, M. Nkemitag, Comparison of consolidation characteristics from CPTu, DMT and laboratory testing at Ashbridges Bay, Toronto, Ontario. in: Proceedings of the 64th Canadian Geotechnical Conference and 14th PanAmerican Conference on Soil Mechanics and Geotechnical Engineering, Toronto, Canada (2011).
[19] K . Koster, G. Erkens, C. Zwanenburg, A new soil mechanics approach to quantify and predict land subsidence by peat compression. Geophysical Research Letters 43, 10792-10799 (2016), DOI: https://doi.org/10.1002/2016GL 071116
[20] M. Mir, A. Bouafia, K. Rahmani, N. Aouali, Analysis of load-settlement behaviour of shallow foundations in saturated clays based on CPT and DPT tests. Geomech. Eng. 13 (1), 119-139 (2017), DOI: https://doi.org/10.12989/ gae.2017.13.1.119
[21] B. Di Buò, J. Selänpää, T. Lansivaara, M. D’Ignazio, Evaluation of existing CPTu-based correlations for the deformation properties of Finnish soft clays. In: Proc. 4th Int. Symposium on Cone Penetration Testing (CPT’18), 185-191 (2018).
[22] Z . Bednarczyk, R. Sandven, Comparison of CPTU and laboratory tests interpretation for Polish and Norwegian clays. In: International Site Characterization Conference, ISC-2. International Society of Rock Mechanics (ISRM), International Association Engineering Geology (IAEG), Geo-Institute of the American Society of Civil Engineers (ASCE), Portuguese Association of Engineers (OE) and British Council (BC). Porto, Portugal (2004).
[23] P . Zawrzykraj, P. Rydelek, A. Bąkowska, Geo-engineering properties of Eemian peats from Radzymin (central Poland) in the light of static cone penetration and dilatometer tests. Eng. Geol. 226, 290-300 (2017), DOI: https://doi.org/10.1016/j.enggeo.2017.07.001
[24] J. Konkol, K. Międlarz, L. Bałachowski, Geotechnical characterization of soft soil deposits in Northern Poland. Eng. Geol. 259, 105187 (2019), DOI: https://doi.org/10.1016/j.enggeo.2019.105187
[25] J. Nawrocki, A. Becker (red.), Atlas geologiczny Polski. Państ. Inst. Geol., Warszawa (2017).
[26] PN -EN ISO 17892, Geotechnical investigation and testing. Laboratory testing of soil.
[27] PN -EN ISO 14688, Geotechnical investigation and testing. Identification and classification of soil.
[28] S. Shimobe, G. Spagnoli, Relationships between undrained shear strength, liquidity index, and water content ratio of clays. Bull. Eng. Geol. Environ. 79, 4817-4828 (2020), DOI: https://doi.org/10.1007/s10064-020-01844-5
[29] P.K. Robertson, C.E. Wride, Evaluating cyclic liquefaction potential using the cone penetration test. Can. Geoecht. J. 35 (3), 442-459 (1998), DOI: https://doi.org/10.1139/t98-017
[30] I. Bagińska, Estimating and verifying soil unit weight determined on the basis of SCPTu tests. Ann. Warsaw Univ. Life Sci. – SGGW. Land Reclam. 48 (3), 233-242 (2016), DOI: https://doi.org/10.1515/sggw-2016-0018
[31] P.W. Mayne, Evaluating effective stress parameters and undrained shear strengths of soft-firm clays from CPT and DMT. Australian Geomechanics Journal 51 (4), 27-55 (2016).
[32] A. Cheshomi, Empirical relationships of CPTu results and undrained shear strength. J. GeoEng. 13 (2), 49-57 (2018), DOI: http://dx.doi.org/10.6310/jog.201806_13(2).1
[33] C.P. Wroth, The interpretation of in situ soil tests. Geotechnique 34 (4), 449-489 (1984), DOI: https://doi.org/10.1680/geot.1984.34.4.449
[34] R. Larsson, M. Mulabdic, Piezocone tests in clay. Swedish Geotechnical Institute, Linköping, Report 42, (1991).
[35] Y .J. Shin, D. Kim, Assessment of undrained shear strength based on Cone Penetration Test (CPT) for clayey soils. J. Civ. Eng. 15 (7), 1161-6 (2011), DOI: https://doi.org/10.1007/s12205-011-0808-6
[36] A .H. El-Bosraty, A.M. Ebid, A.L. Fayed, Estimation of the undrained shear strength of east Port-Said clay using the genetic programming. Ain Shams Engineering Journal 11 (4), 961-969 (2020), DOI: https://doi.org/10.1016/j.asej.2020.02.007
[37] L . Bałachowski, K. Międlarz, J. Konkol, Strength parameters of deltaic soils determined with CPTU, DMT and FVT. In: Proc. 4th Int. Symposium on Cone Penetration Testing (CPT’18), 117-121 (2018).
[38] S.J. Hong, M. Lee, J. Kim, W. Lee, Evaluation of undrained shear strength of Busan clay using CPT. In: Proc. 2nd Int. Symposium on Cone Penetration Testing, CPT’10 (2010).
[39] K . Koster, G. De Lange, R. Harting, E. de Heer, H. Middelkoop, Characterizing void ratio and compressibility of Holocene peat with CPT for assessing coastal–deltaic subsidence. Q. J. Eng. Geol. Hydrogeol. 51 (2), 210-218 (2018), DOI: https://doi.org/10.1144/qjegh2017-120
[40] G. Sanglerat, The Penetrometer and Soil Exploration. Dev. Geotech. Eng. (1972).
[41] P.W. Mayne, Cone penetration testing (Vol. 368). Transportation Research Board (2007).



Go to article

Authors and Affiliations

Matylda Tankiewicz
1
ORCID: ORCID
Irena Bagińska
2
ORCID: ORCID

  1. Wrocław University of Environmental and Life Sciences, 25 Norwida Str., 50-375 Wrocław, Poland
  2. Wroclaw University of Science and Technology, 27 Wybrzeże Wyspiańskiego st., 50-370 Wrocław, Poland
Download PDF Download RIS Download Bibtex

Abstract

In this paper, the authors analyse the propagation of surface Love waves in an elastic layered waveguide (elastic guiding layer deposited on an elastic substrate) covered on its surface with a Newtonian liquid layer of finite thickness. By solving the equations of motion in the constituent regions (elastic substrate, elastic surface layer and Newtonian liquid) and imposing the appropriate boundary conditions, the authors established an analytical form of the complex dispersion equation for Love surface waves. Further, decomposition of the complex dispersion equation into its real and imaginary part, enabled for evaluation of the phase velocity and attenuation dispersion curves of the Love wave. Subsequently, the influence of the finite thickness of a Newtonian liquid on the dispersion curves was evaluated. Theoretical (numerical) analysis shows that when the thickness of the Newtonian liquid layer exceeds approximately four penetration depths 4δ of the wave in a Newtonian liquid, then this Newtonian liquid layer can be regarded as a semi-infinite half-space. The results obtained in this paper can be important in the design and optimization of ultrasonic Love wave sensors such as: biosensors, chemosensors and viscosity sensors. Love wave viscosity sensors can be used to assess the viscosity of various liquids, e.g. liquid polymers.

Go to article

Authors and Affiliations

Piotr Kiełczyński
Marek Szalewski
Andrzej Balcerzak
Krzysztof Wieja
Download PDF Download RIS Download Bibtex

Abstract

In this work, a comparative study on the ballistic behaviour of friction stir processed AL6061 targets had been made. Base Metal AL6061 (BM) plates with 25 mm thickness were friction stir processed by adding Multi Walled Carbon Nano Tubes (MWCNT) and Graphene (G), producing AL6061-MWCNT and AL6061-G surface composites. Optical microscopy and microhardness test on BM, AL6061-MWCNT and AL6061-G samples were performed as per the standard procedure. It was noticed that uniform dispersion of ceramic particles and refined grains were obtained for the friction stir processed surface composites. From the microhardness test, it was perceived that friction stir processing had induced strengthening of surface composites, hence increasing the microhardness of AL6061-MWCNT and AL6061-G by ~60.3% and ~73.6% respectively. Also, ballistic experiments were conducted at 680±10 m/s by impacting Ø7.62×51 mm projectiles. AL6063 backing plates were placed to compare the ballistic behaviours AL6061-MWCNT and AL6061-G targets by depth of penetration. It was noted that the depth of penetration of AL6061-MWCNT and AL6061-G targets were 37.81% and 65.84% lesser than the BM target. Further, from the results of Post ballistic microscopy it was observed that the microstructure near and away from the penetration channel edge looks unchanged in BM target. However, the AL6061-MWCNT and AL6061-G targets showed considerable change in their morphology, by forming Adiabatic Shear Bands.
Go to article

Authors and Affiliations

U. Magarajan
1
ORCID: ORCID
S. Suresh Kumar
2
ORCID: ORCID

  1. Sri Venkateswara College of Engineering, Chennai, India
  2. Sri Sivasubramaniya Nadar College of Engineering, Chennai, India
Download PDF Download RIS Download Bibtex

Abstract

Due to the skin effect of eddy currents, the depth of cracks which can be detected by the traditional eddy current probe is very limited. In order to improve the ability of eddy current probes to inspect deep cracks in metal thick-walled structures, a new eddy current probe using an excitation system with phase shifted fields was proposed. Its feasibility for detecting deep cracks was verified by simulation and experiments. The results showed that the penetration depth of eddy currents in austenitic stainless steel is effectively enhanced by using the new probe.

Go to article

Authors and Affiliations

Meixian Wu
Dongli Zhang
Chuanglong Wang
Download PDF Download RIS Download Bibtex

Abstract

This paper discusses the use of mechanical cone penetration test CPTM for estimating the soil unit weight of selected organic soils in Rzeszow site, Poland. A search was made for direct relationships between the empirically determined the soil unit weight value and cone penetration test leading parameters (cone resistance qc, sleeve friction fs. The selected, existing models were also analysed in terms of suitability for estimating the soil unit weight and tests were performed to predict the value soil unit weight of local, different organic soils. Based on own the regression analysis, the relationships between empirically determined values of soil unit weight and leading parameters cone penetration test were determined. The results of research and analysis have shown that both existing models and new, determined regression analysis methods are poorly matched to the unit weight values determined in laboratory, the main reason may be the fact that organic soils are characterized by an extremely complicated, diverse and heterogeneous structure. This often results in a large divergence and lack of repeatability of results in a satisfactorily range. Therefore, in addition, to improve the predictive performances of the relationships, analysis using the artificial neural networks (ANN) was carried out.
Go to article

Bibliography


[1] EN 1997-1: 2008. Eurocode 7: Geotechnical Design – Part 1: General rules.
[2] EN 1997-2: 2009. Eurocode 7: Geotechnical Design – Part 2: Ground Investigation and Testing.
[3] P.K. Robertson, K.L. Cabal, “Guide to Cone Penetration Testing for Geotechnical Engineering”. Gregg Drilling & Testing, Inc, 5-th Edition, 2012.
[4] Y. Cal, “Soil classification by neural-network”, Adv. Eng. Softw. 22: pp. 95–97, 1995.
[5] A. Goh, “Empirical design in geotechnics using neural networks”, Geotechnique 45: pp. 709–714, 1995. https://doi.org/10.1680/geot.1995.45.4.709
[6] M. Shahin, M. Jaksa, H. Maier, “Artificial neural network applications in geotechnical engineering”, Aust. Geomech. 36: 49–62, 2001.
[7] N. Nawari, R, Liang, J. Nusairat, “Artificial intelligence techniques for the design and analysis of deep foundations”. Electron. J. Geotech. Eng. 4: pp 1–21, 1999. Available online: http://geotech.civeng.okstate.edu/ejge/ppr9909/index.html (accessed on).
[8] D. Penumadu, C. Jean-Lou, “Geomaterial modeling using artificial neural networks”, In Artificial Neural Networks for Civil Engineers: Fundamentals and Applications, ASCE: Reston, WV, USA, pp 160–184, 1997.
[9] C.H. Zhiming, M. Guotao, Z. Ye, Z. Yanjie, H. Hengyang, “The application of artificial neural network in geotechnical engineering”, In Proceedings of the 2018 International Conference on Civil and Hydraulic Engineering (IConCHE 2018), Qingdao, China, 23–25 November 2018; IOP Publishing: Bristol, UK, 2018; http://dx.doi.org/10.1088/1755-1315/189/2/022054
[10] Z. Wang, Y. Li, “Correction of soil parameters in calculation of embankment settlement using a BP network back-analysis model”, Eng. Geol. 91: pp. 168–177, 2007. https://doi.org/10.1016/j.enggeo.2007.01.007
[11] M.J. Sulewska, “Applying Artificial Neural Networks for analysis of geotechnical problems”, Comput. Assist. Methods Eng. Sci. 18: pp. 230–241, 2011.
[12] M.J. Sulewska, “Artificial Neural modeling of compaction characteristics of cohesionless soil”, Comput. Assist. Methods Eng. Sci. 17: pp. 27–40, 2010.
[13] M.J. Sulewska, “Artificial Neural Networks in the Evaluation of Non-Cohesive Soil Compaction Parameters”, Committee Civil Engineering of the Polish Academy of Sciences: Warsaw, Poland, 2009.
[14] M.J. Sulewska, “Prediction Models for Minimum and Maximum Dry Density of Non-Cohesive Soils”, Pol. J. Environ. Stud. 19: pp. 797–804, 2010.
[15] M. Ochmański, J. Bzówka, “Selected examples of the use of artificial neural networks in geotechnics”, Civ. Environ. Eng. 4: pp. 287–294, 2013.
[16] A. Borowiec, K. Wilk, “Prediction of consistency parameters of fen soils by neural networks”, Comput. Assist. Methods Eng. Sci.21: pp. 67–75, 2014.
[17] M. Kłos, M.J. Sulewska, Z. Waszczyszyn, “Neural identification of compaction characteristics for granular soils”, Comput. Assist. Methods Eng. Sci.18: pp. 265–273, 2011.
[18] G. Wrzesiński, M.J. Sulewska, Z. Lechowicz, “Evaluation of the Change in Undrained Shear Strength in Cohesive Soils due to Principal Stress Rotation Using an Artificial Neural Network”, Appl. Sci. 8: p. 781, 2018. https://doi.org/10.3390/app8050781
[19] Z. Lechowicz, M. Fukue, S. Rabarijoely, M.J. Sulewska, “Evaluation of the Undrained Shear Strength of Organic Soils from a Dilatometer Test Using Artificial Neural Networks”, Appl. Sci. 8: p. 1395, 2018. https://doi.org/10.3390/app8081395
[20] S. Rabarijoely, “A new Approach to the Determination of Mineral and Organic Soil Types Based on Dilatometer Tests (DMT)”, Appl. Sci.8 (11):, p. 2249, 2018. https://doi.org/10.3390/app8112249
[21] G. Straż, A. Borowiec, “Estimating the Unit Weight of Local Organic Soils from Laboratory Tests Using Artificial Neural Networks”, Appl. Sci. 10 (7): p. 2261, 2020. http://dx.doi.org/10.3390/app10072261
[22] Voivodship Inspectorate for Environmental Protection in Rzeszów, “Report on the state of the environment of the Podkarpackie Voivodeship in 2013–2015”, Environmental Monitoring Library, Rzeszow, 2016.
[23] Geotech, Ltd. Department of Geological Services Design and Construction and the Environment, “Geological and Engineering Geological Conditions for Recognition – Engineering for the Construction of Multi-Storey Building at UL; Witolda in Rzeszów”: Rzeszow, Poland, 2010.
[24] PN-EN ISO 17892-2:2014. Geotechnical Investigation and Testing – Laboratory Testing of Soil – Part 2: Determination of Bulk Density.
[25] PN-EN ISO 22476-12:2009. Geotechnical Investigation and Testing – Field Testing – Part 12: Mechanical Cone Penetration Test.
[26] L. Wysokiński, W. Kotlicki, T. Godlewski, “Geotechnical design according to Eurocode 7”, Guide. ITB, Warsaw, 2011.
[27] P.W. Mayne, G.J. Rix, “Correlations Between Shear Wave Velocity and Cone Tip Resistance in Clays”, Soils and Foundations 35 (2): pp. 107–110, 1995.
[28] P.W. Mayne, “The 2nd James K. Mitchell Lecture: Undisturbed Sand Strength from Seismic Cone Tests,” Geomechanics and Geoengineering Vol. 1, No. 4: pp. 239–247, 2006.
[29] P.W. Mayne, “Cone Penetration Testing”, “A Synthesis of Highway Practice”, NCHRP Synthesis 368; Transportation Research Board: Washington, DC, USA, 2007.
[30] P.W. Mayne, J. Peuchen, D. Bouwmeester, “Soil unit weight estimation from CPTs”, In Proceedings of the 2nd International Symposium on Cone Penetration Testing, Huntington Beach, CA, USA, 9–11 May, pp 169–176, 2010.
[31] P.W. Mayne, “Evaluating effective stress parameters and undrained shear strengths of soft-firm clays from CPTu and DMT”, Geotechnical and Geophysical Site Characterisation 5 – Lehane, Acosta-Martínez & Kelly (Eds) © Australian Geomechanics Society, Sydney, Australia, 2016.
[32] P. Robertson, K. Cabal, “Estimating soil unit weight from CPT”, In Proceedings of the 2nd International
[33] Symposium on Cone Penetration Testing, Huntington Beach, CA, USA, 9–11 May, 2010.
[34] A.T. Ozer, S.F. Bartlett, E.C. Lawton, “CPTU and DMT for estimating soil unit weight of Lake Bonneville Clay”, Geotechnical and Geophysical Site Characterization 4: pp. 291–296, 2012.
[35] R.K. Ghanekar, “Unit weight estimation from CPT for Indian offshore soft calcareous clay”, in: “CPTU and DMT in soft clays and organic soils” (eds. Z. Młynarek and J. Wierzbicki), Exlemplum Press, Poznań, Poland, pp. 31–44, 2014.
[36] M.S. Kovacevic, K.G. Gavin, C. Reale, L. Libric, “The use of neural networks to develop CPT correlations for soils in northern Croatia”, Cone Penetration Testing 2018 – Hicks, Pisano & Peuchen (eds), Delft University of Technology, June 2018, The Netherlands.
[37] G. Straż, “Estimating soil unit weight from CPT for selected organic soils”, in: “Selected technical, economic and ecological aspects of contemporary construction” (eds. K. Pujer), Exante, pp. 63–77, 2016.
[38] S.O. Haykin, “Neural Networks and Learning Machines”, 3rd ed.; Pearson Education: Upper Saddle River, NJ, USA, 798, 2009.
[39] M.T. Hagan, H.B. Demuth, M.H. Beale, “Neural Network Design”, PWS Publishing: Boston, MA, USA, 1996.
[40] D. Marquardt, “An Algorithm for Least-Squares Estimation of Nonlinear Parameters”, SIAM J. Appl. Math.3: 11, pp. 431–441, 1963.
[41] M.T. Hagan, M. Menhaj, “Training feed-forward networks with the Marquardt algorithm”. IEEE Trans. Neural Netw. 5: pp. 989–993, 1994.
[42] J.E. Dennis, R.B. Schnabel, “Numerical Methods for Unconstrained Optimization and Nonlinear Equations”, Prentice-Hall: Englewood Clis, NJ, USA, 1983.
[43] D.J.C. MacKay, “Bayesian interpolation”, Neural Comput.4: pp. 415–447, 1992.
[44] Beale, M.H.; Hagan, M.T.; Demuth, H.B.Neural Network ToolboxUser’s Guide; TheMathWorks: Natick, MA,USA, 2010.
[45] GEO5. Geotechnical software. Fine – Civil Engineering Softwere. https://www.finesoftware.pl/.
[46] Statistica 13.3. TIBCO Software Inc. https://www.statsoft.pl/Czytelnia .
Go to article

Authors and Affiliations

Grzegorz Straż
1
ORCID: ORCID
Artur Borowiec
1
ORCID: ORCID

  1. Rzeszow University of Technology, Faculty of Civil and Environmental Engineering and Architecture Civil Engineering, Powstańców Warszawy 12 Av., 35-959 Rzeszow, Poland
Download PDF Download RIS Download Bibtex

Abstract

This study investigates the effects of Nano SiO 2 (NS) and Silica fume (SF) on the mechanical properties and durability of Portland cement concrete. On specimens with varying NS and SF concentrations, compressive strength, flexural strength, abrasion resistance, elastic modulus, and chloride ion penetration were all tested. All specimens were subjected to the proposed method/technique cured at the ages of 3, 7, 28, and 60 days. NS particles were added to cement concrete at various replacements of 0, 0.5, 1.0, 1.5, and 2.0% by the mass of the binder. The water/binder ratio has remained at 0.37 for all mixes. Then, for cement-concrete were prepared 45 MPa (C45) with NS and SF. The specimens confirm the new method effectiveness evaluation were prepared under two different categories: (1) Portland cement replacement with NS of 0%, 0.5%, 1.0%, 1.5%, and 2.0%, by weight for adhesives; (2) Portland cement replacement with NS of 0.5%, 1.0% and each NS content in combination with SF of 5%, 10%, and 15%, respectively, by weight for adhesives. The results indicated that the abrasion resistance and Chloride ion penetration of concrete containing NS and SF are improved. Finally, an analytical model for forecasting the Elastic modulus, flexural strength, and compressive strength of cement concrete was established from obtained data.
Go to article

Authors and Affiliations

Huu-Bang Tran
1
Vu To-Anh Phan
2

  1. Faculty of Architecture, Thu Dau Mot University, Binh Duong Province, Vietnam
  2. Faculty of Civil Engineering, Ton Duc Thang University, Ho Chi Minh City, Vietnam
Download PDF Download RIS Download Bibtex

Abstract

From the construction made in the “white box” technology, first of all tightness is required - on the structural elements there should not be any cracks or scratches, through which water could penetrate, which in consequence may lead to deformation of structural elements and even loosing of their load-bearing capacity. Among the methods enabling the location of weakened places in watertight concrete, the ground penetrating radar (GPR) method is effective because the local occurrence of water in the structure evokes a clear and unambiguous anomaly on the radargram. In addition, the GPR method allows you to indicate places where water flows without the necessity of excluding the object from use and interference in the construction layers. The designation of such locations will make it possible to undertake technical activities that can facilitate the takeover of water and thus ensure the desired load-bearing capacity and usability of the object. Using the GPR method, you can also designate places that have already been deformed – discontinuities or breaking. The article presents a case study of investigations that determine the causes of leakage of tunnels made in the “white box” technology in: twice within the bottom slab of the tunnel (1 GHz air-coupled and 400 MHz ground-coupled antenna) and once in the case of tunnel walls (1.6 GHz ground-coupled antenna).

Go to article

Authors and Affiliations

Anna Lejzerowicz
ORCID: ORCID
Małgorzata Wutke
Download PDF Download RIS Download Bibtex

Abstract

GPR method is perfectly suited for recognizing of sedimentary facies diversity in shallowly occurring sediments if there is a contrast of electrical properties between and/or within each layer. The article deals with the issue of the correlation between GPR surveys results and sedimentological analyses. As a result of this correlation a conceptual model of depositional systems of studied areas was developed. Studies were performed in two areas located in central Poland, where glacial deposits formed in the Middle Polish (Saalian) Glaciation are present. The study was based on 49 sediment samples and 21 GPR profiles. Analyses of lithofacies as well as granulometric and mineralogical composition of deposits of collected samples were carried out, showing the diversity of glacial deposits in both study sites. During GPR measurements shielded antenna with a frequency of 500 MHz was used which allowed high-resolution mapping of the internal structure of deposits and to identify four characteristic radar facies. Correlation of GPR profiles with point, one-dimensional sedimentological studies allowed the unambiguous interpretation of the GPR image and draw conclusions about the formation environment of individual units. Geophysical and sedimentological data obtained during study provide a new and detailed insight into selected glacial deposits in central Poland.

Go to article

Authors and Affiliations

Anna Lejzerowicz
ORCID: ORCID
Anna Wysocka
Sebastian Kowalczyk
Download PDF Download RIS Download Bibtex

Abstract

The main scientific goal of this work is the presentation of the role of selected geophysical methods (Ground-Penetrating Radar GPR and Electrical Resistivity Tomography ERT) to identify water escape zones from retention reservoirs. The paper proposes a methodology of geophysical investigations for the identification of water escape zones from a retention fresh water lake (low mineralised water). The study was performed in a lake reservoir in Upper Silesia. Since a number of years the administrators of the lake have observed a decreasing water level, a phenomenon that is not related to the exploitation of the object. The analysed retention lake has a maximal depth between 6 and 10 m, depending on the season. It is located on Triassic carbonate rocks of the Muschelkalk facies. Geophysical surveys included measurements on the water surface using ground penetration radar (GPR) and electrical resistivity tomography (ERT) methods. The measurements were performed from watercrafts made of non-metal materials. The prospection reached a depth of about 1 to 5 m below the reservoir bottom. Due to large difficulties of conducting investigations in the lake, a fragment with an area of about 5,300 m 2, where service activities and sealing works were already commenced, was selected for the geophysical survey. The scope of this work was: (1) field geophysical research (Ground-Penetrating Radar GPR and Electrical Resistivity Tomography ERT with geodesic service), (2) processing of the obtained geophysical research results, (3) modelling of GPR and ERT anomalies on a fractured water reservoir bottom, and (4) interpretation of the obtained results based on the modelled geophysical anomalies. The geophysical surveys allowed for distinguishing a zone with anomalous physical parameters in the area of the analysed part of the retention lake. ERT surveys have shown that the water escape zone from the reservoir was characterised by significantly decreased electrical resistivities. Diffraction hyperboles and a zone of wave attenuation were observed on the GPR images in the lake bottom within the water escape zone indicating cracks in the bottom of the water reservoir. The proposed methodology of geophysical surveys seems effective in solving untypical issues such as measurements on the water surface.

Go to article

Authors and Affiliations

Radosław Mieszkowski
ORCID: ORCID
Emilia Wójcik
Mikołaj Kozłowski
Paweł Popielski
ORCID: ORCID
Download PDF Download RIS Download Bibtex

Abstract

Large-scale stone-banked lobes and terraces are distributed over an area of 1 km2 of gentle slope on Rink Plateau in the northern part of James Ross Island, Antarctic Peninsula region. Topographically, there are two main features: relatively high risers up to 5 m high and distinct frontal ridges. In order to understand the processes responsible for these lobes and terraces, the authors have monitored air and ground temperatures and movement of stones on the surface over the period 1995-2005. In February 2005, the subsurface structures were surveyed by ground penetrating radar and drilling. The ground penetrating radar profiles identified the bedrock surface. The surface morphology of the lobes corresponds closely with that of the bedrock. The relatively high risers of these lobes are presumed to be due to a cessation of frontal advance.

Go to article

Authors and Affiliations

Junko Mori
Kotaro Fukui
Toshio Sone
Jorge A. Strelin
Cesar A. Torielli
Download PDF Download RIS Download Bibtex

Abstract

Measurements were made of sediment characteristics, benthic microbial activity and optimum temperature for sulfate reduction at Signy Island, South Orkney Islands, Antarctica . There was little evidence to support any seasonal variation in oxygen penetration of surface sediments. Oxygen penetrated to only 1.5 to 3 mm throughout the year, despite bioturbation from a dense amphipod population. The distribution of acid volatile sulfides increased with depth below 1 cm and above this, surface sediments were lighter in colour and contained fewer sulfides. The rates of sulfate reduction increased during winter under sea-ice cover, and remained high after ice break up. Seasonal water temperature was relatively constant between –1.8 and 0.5°C. Optimum temperature for anaerobic sediment respiration was investigated using different substrates and was found to be in the range 17–27°C, suggesting that sulfate reducing bacteria are psychrotolerant as they were inhibited by low temperatures.

Go to article

Authors and Affiliations

Tony R. Walker

This page uses 'cookies'. Learn more