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Number of results: 7
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Abstract

A mixed pseudo-orthogonal frequency coding (Mixed-POFC) structure is proposed as a new spreadspectrum technique in this paper, which employs frequency and time diversity to enhance tag properties and balances the spectrum utilization and code diversity. The coding method of SAW RFID tags in this paper uses Mixed-POFC with multi-track chip arrangements. The cross-correlation and auto correlation of Mixed-POFC and POFC are calculated to demonstrate the reduced overlap between the adjacent center frequencies with the Mixed-POFC method. The center frequency of the IDT and Bragg reflectors is calculated by a coupling of modes (COM) module. The combination of the calculation results of the Bragg reflectors shows that compared with a 7-chip POFC, the coding number of a 7-chip Mixed-POFC is increased from 120 to 144 with the same fractional bandwidth of 12%. To demonstrate the validity of Mixed-POFC, finite element analysis (FEA) technology is used to analyze the frequency characteristics of Mixed-POFC chips. The maximum error between designed frequencies and simulation frequencies is only 1.7%, which verifies that the Mixed-POFC method is feasible.

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Authors and Affiliations

Mengru Xu
Xia Xiao
Qing Yuan
Yong Zong
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Abstract

Linear arrays of ultrasonic transducers are commonly used as ultrasonic probes in medical diagnostics for imaging the interior of a human body in vivo. The crosstalk phenomenon occurs during the operation of transducers in which electrical voltages and mechanical vibrations are transmitted to adjacent components. As a result of such additional excitation of the transducers in the array, the directivity characteristics of the aperture used changes, and consequently there is interference with properoperation of a given array and the emergence of distortions in the obtained ultra sound image that reduce its quality. This paper studies the manner of propagation of mechanical crosstalk in the designed model of a linear array of ultrasonic transducers on the basis of unwanted signals, which appeared on elementary piezo-electric transducers when power is supplied to the selected transducer in the array. The universal model of linear array of ultrasonic transducers, which has been developed, allowed the simulation of mechanical crosstalk, taking in to account the cross-coupling phenomenon in all of its structure with the use of finite elements method (FEM) implemented in COMSOL Multiphysics software. The analysis of crosstalk signals showed that they consist of aggregated pulses propagating with different speeds and frequencies. This signifies the formation of different vibration modes transmitted simultaneously via different paths. The paper is an original approach which enables to identify different vibration modes and estimate their participation in the crosstalk signal and their ways of propagation. Conclusions from the research allow predicting specific design changes which are significant due to the minimization of mechanical crosstalk in linear arrays of ultrasonic transducers.

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Authors and Affiliations

Mateusz Celmer
Krzysztof J. Opieliński
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Abstract

Solar cell performance decreases with increasing temperature, heat can reduce output efficiency by 10–25%. The operating temperature plays a key role in the photovoltaic conversion process. Increase in electrical efficiency depends on cooling techniques, in particular photovoltaic modules installed in the high temperature regions. A cooling process using a single nozzle of photovoltaic panel operating under different configurations was simulated. The simulation contains two parts: the first is a thermodynamic investigation of fluid impingement upon the sensor front face. The second is a performance comparison between two types of glass cover. The major result that emerges from this simulation is the effect of a single nozzle arrangement to enhance the cooling process, under a low cadence of impinging droplets in the range 0.1–1.7 m/s.
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Bibliography

[1] Chokmaviroj S., Wattanapong R., Suchart Y.: Performance of a 500 kWp grid connected photovoltaic system at Mae Hong Son province Thailand. Renew. Energ. 31(2006), 1, 19–28.
[2] Omubo-Pepple V.B., Israel-Cookey C., Alaminokuma G.I.: Effects of temperature, solar flux and relative humidity on the efficient conversion of solar energy to electricity. Eur. J. Sci. Res. 35(2009), 2, 173–180.
[3] Kawamura T., Harada K., Ishihara Y., Todaka T., Oshiro T., Nakamura H., Imataki M.: Analysis of MPPT characteristics in Photovoltaic power system. Sol. Energ. Mat. Sol. C. 47(1997), 1-4, 155–165.
[4] Skoplaki E., Palyvos J.A.: On the temperature dependence of photovoltaic module electrical performance: A review of efficiency/power correlations. Sol. Energy 83(2009), 5, 614–624.
[5] Smith M.K., Selbak H., Wamser C.C., Day N.U., Krieske M., Sailor D.J., Rosenstiel T.N.: Water cooling method to improve the performance of fieldmounted, insulated, and concentrating photovoltaic modules. J. Sol. Energ. Eng. 136(2014), 3, 034503.
[6] Tonui J.K., Tripanagnostopoulos Y.: Air-cooled PV/T solar collectors with low cost performance improvements. Sol. Energy 81(2007), 4, 498–511.
[7] Kaiser A.S., Zamora B., Mazón R., García J.R., Vera F.: Experimental study of cooling BIPV modules by forced convection in the air channel. Appl. Energ. 135(2014), 88–97.
[8] Choubineh N., Jannesari H., Kasaeian A.: Experimental study of the effect of using phase change materials on the performance of an air-cooled photovoltaic system. Renew.Sust. Energ. Rev. 101(2019), 103–111.
[9] Du B., Hu E., Kolhe M.: Performance Analysis of Water Cooled Concentrated Photovoltaic (CPV) System. Renew. Sust. Energ. Rev. 16(2012), 9, 6732–6736.
[10] Abdolzadeh M., Ameri M.: Improving the effectiveness of a photovoltaic water pumping system by spraying water over the front of photovoltaic cells. Renew. Energ. 34(2009), 1, 91–96.
[11] Bahaidarah H., Subhan A., Gandhidasan P., Rehman S.: Performance evaluation of a PV (photovoltaic) module by back surface water cooling for hot climatic conditions. Energy 59(2013), 445–453.
[12] Najafi H., Woodbury K.A.: Optimization of a cooling system based on Peltier effect for photovoltaic cells. Sol. Energy 91(2013), 152–160.
[13] Rahimi M., Sheyda P.V.E., Parsamoghadam M.A., Masahi M.M., Alsairafi A.A.: Design of a self-adjusted jet impingement system for cooling of photovoltaic cells. Energ. Convers. Manage. 83(2014), 48–57.
[14] Nižetic S., Coko D., Yadav A., Grubišic-Cabo F.: Water spray cooling technique applied on a photovoltaic panel: The performance response. Energ. Convers. Manage. 108(2016), 287–296.
[15] Otmani A., Mzad H., Bey K.: A thermal parametric study of non-evaporative spray cooling process. MATEC Web of Conferences 240(2018), 01030.
[16] Otmani A., Mzad H.: Parametric study of non-evaporative spray cooling on aluminum plate: Simulation and analysis. Therm. Sci. 23(2019), 4, S1393–S1402.
[17] Mikielewicz D., Muszynski T., Mikielewicz J.: Model of heat transfer in the stagnation point of rapidly evaporating microjet. Archives of Thermodynamics 33(2012), 1, 139–152.
[18] Rusowicz A., Leszczynski M., Grzebielec A., Laskowski R.: Experimental investigation of single-phase microjet cooling of microelectronics. Archives of Thermodynamics 36(2015), 3, 139–147.
[19] Tebbal M., Mzad H.: An hydrodynamic study of a water jet dispersion beneath liquid sprayers. Forsch. Ingenieurwes. 68(2004), 3, 126–132.
[20] Mzad H., Tebbal M.: Thermal diagnostics of highly heated surfaces using waterspray cooling. Heat Mass Transfer 45(2009), 3, 287–295.
[21] https://www.comsol.com/release/5.2 (accessed: 08 Feb. 2020).
[22] Byron Bird R., Stewart Warren E., Lightfoot Edwin N.: Transport Phenomena. John Wiley & Sons, New York 1966.
[23] White Frank M.: Fluid Mechanics. McGraw-Hill, 1999.
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Authors and Affiliations

Hocine Mzad
1
Abdessalam Otmani
1

  1. Mechanical Engineering Department, Badji Mokhtar University of Annaba, P.O. Box 12, DZ-23000, Algeria
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Abstract

The two-dimensional distribution of gas-solid flow parameters is a great research significance to reflect the actual situation in industry. The commonly used method is the ultrasonic tomography method, in which multiple probes are arranged at various angles, or the measurement device is rotated as that in medicine, but in most industrial situations, it is impossible to install probes at all angles or rotate the measured pipe. The backscattering method, however, uses only one transducer to both transmit and receive signals, and the twodimensional information is obtained by only rotating the transducer. Ultrasound attenuates greatly in the air, and the attenuation changes with frequency. Therefore, COMSOL is used to study the reflection of particles with different radii in the air to ultrasound with various frequencies. It is found that the backscattering equivalent voltage is the largest when the product of ultrasonic frequency and particle radius is about 27.78 Hz �� m, and the particle concentration of 30% causes the strongest backscattering. The simulated results are in good agreement with the Faran backscattering model, which can provide references for selecting the appropriate frequency and obtaining the concentration when measuring gas-solid two-phase flow with the ultrasonic backscattering method.
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Authors and Affiliations

Jinhui Fan
1
Fei Wang
1

  1. State Key Laboratory of Clean Energy Utilization, Zhejiang University, Hangzhou, 310027, China
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Abstract

Finite Element Method FEM via commercially available software has been used for numerical simulation of the compaction process of bentonite-bonded sand mould. The mathematical model of soil plasticity which involved Drucker-Prager model match with Mohr-Coulomb model was selected. The individual parameters which required for the simulation process were determined through direct shear test based on the variation of sand compactability. The novelty of this research work is that the individual micro-mechanical parameters were adopted depend on its directly proportional to the change of sand density during the compaction process. Boundary conditions of the applied load, roller and fixed constraint were specified. An extremely coarse mesh was used and the solution by time-dependent study was done for investigation of material-dependent behaviour of green sand during the compaction process. The research implemented also simulation of the desired points in sand mould to predict behaviour of moulding process, and prevent failure of the sand mould. Distance-dependent displacement and distance-dependent pressure have been determined to investigate the effective moulding parameters without spent further energy and cost for obtaining green sand mould. The obtained numerical results of the sand displacement show good agreement with the practical results.
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Bibliography

[1] Naeimi, K., Baradaran, H., Ahmadi, R. & Shekari, M. (2015). Study and simulation of the effective factors on soil compaction by tractors wheels using the finite element method. Journal of Computational Applied Mechanics. 46(2), 107-115. DOI: 10.22059/jcamech.2015.55093.
[2] Soane, B. (1990). The role of organic matter in soil compatibility: A review of some practical aspects. Soil & Tillage Research. 16(1-2), 179-201. DOI: https://doi.org/ 10.1016/0167-1987(90)90029-D.
[3] Minaei, S. (1984). Multi pass effects of wheel and track- type vehicles on soil compaction. MS Thesis, Virginia Polytechnic Institute and State University.
[4] Chen, Y. Tessier, Y. & Rauffignat, S. (1998). Soil bulk density estimation for tillage systems and soil texture. Transactions of the American Society of Agricultural and Biological Engineers. 41(4), 1601-1610.
[5] Wenzhen, L. & Junjiao, W. (2007). Numerical Simulation of Compacting Process of Green Sand Molding Based on Sand Filling. Materials Science Forum. 561-565, 879-1882. DOI: https://doi.org/10.4028/www.scientific.net/MSF.561-565.1879.
[6] Hovad, E., Larsen, P., Walther, J., Thorborg, J. & Hattel,. J.H. (2015). Flow Dynamics of green sand in the DISAMATIC moulding process using Discrete element method (DEM). IOP Conference Series Materials Science and Engineering. 84(1) 1-8. DOI: 10.1088/1757-899X/84/1/012023.
[7] Hua, L., Junjiao, W., Tianyou, H. & Hiroyasu, M. (2011). A new numerical simulation model for high pressure squeezing moulding. China foundry. 8(1) 25-29. ID: 1672-6421(2011)01-025-05.
[8] Schijndel, van, A.W.M.(2007). Integrated heat air and moisture modeling and simulation. Doctoral dissertation, Eindhoven University of Technology. https://doi.org/ 10.6100/IR622370.
[9] Terzaghi, K. (1976). Earthwork mechanics based on soil physics (in German). G. Gistel & Cie. GmbH, Wien.
[10] Tomas, J. (1991). Modeling of the flow behavior of bulk solids on the basis of the interaction forces between the particles and applications in the design of bunkers (in German). Habilitation thesis, TU Bergakademie Freiberg.
[11] Inoue, Y., Motoyama, Y., Takahashi, H., Shinji, K. & Yoshida, M. (2013). Effect of sand mold models on the simulated mold restraint force and the contraction of the casting during cooling in green sand molds. Journal of Materials Processing Technology. 213(7), 1157-1165. https://doi.org/10.1016/j.jmatprotec.2013.01.011.
[12] Kadauw, A. (2006). Mathematical modeling of the moulding material processes (in German). Doctoral dissertation, TU- Bergakademie Freiberg.
[13] Lang, H.-J., Huder, J., Amann, P., Puzrin, A.M. (1996). Soil mechanics and foundation (in German). Springer, Berlin Heidelberg.
[14] Suroso, P., Samang, L., Tjaronge, W. & Muhammad Ramli. (2016). Estimates of Elasticity and Compressive Strenght in Soil Cement Mixed With Ijuk-Aren, International Journal of Innovative Research in Advanced Engineering (IJIRAE), 3(4), 21-26.
[15] Nujid, M.M. & Taha, M.R. (2016). Soil Plasticity Model for Analysis of Collapse Load on Layers Soil. EDP Sciences, MATEC Web of Conferences. 47(03020) 1-6. DOI: 10.1051/matecconf/ 20164703020.
[16] Chen, W.F. Mizuno, E. (1990). Nonlinear Analysis in Soil Mechanics: Theory and Implementation, Elsevier Science Publishers B. V., ISBN 978-0444430434, 5-36.
[17] Bast, J., Kadauw, A. (2004). 3D-Numerical Simulation of Squeeze Moulding with the Finite element Method. Proceeding of 66th World Foundry Congress Istanbul, 247 - 258.
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Authors and Affiliations

Dheya Abdulamer
ORCID: ORCID
A. Kadauw
1 2

  1. IMKF. TU - Bergakademie Freiberg, Germany
  2. Salahddin University-Erbil, Iraq
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Abstract

The paper presents a numerical model of the novel design of the axial magnetic bearing with six cylindrical poles. The motivation behind this idea was to eliminate vibrations in rotating machinery due to the axial load. Common conception of such a bearing provides a single component of the electromagnetic force, which is not enough to reduce transverse and lateral vibrations of the armature. The proposed design allows for avoiding wobbling of the disc with the use of a few axial force components that are able to actively compensate the axial load and stabilise the disc in a balanced position. Before a real device is manufactured, a virtual prototype should be prepared. The accurate numerical model will provide essential knowledge about the performance of the axial magnetic bearing.

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Authors and Affiliations

Bartłomiej Marian Sikora
Adam Krzysztof Pilat
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Abstract

To improve the welding performance of aluminum alloys, a thermal source model of an irregular weld seam was established. COMSOL software was used for numerical simulation of the weld seam geometry effect on the temperature and stress fields in laser welding, which results were experimentally validated. The results show that the ellipsoidal laser welding melted micropool exhibited quasi-steady-state temperature field characteristics. The temperature gradient and thermal stress showed an increase followed by a decline. The temperature fluctuation amplitude of the square-tooth-shaped weld seam exceeded that of the arc-toothshaped one. The temperature evolution of the broken line tooth-shaped weld seam showed a slightly increasing trend, except for the inflection point. The experimental average tensile strength of the weld seam was the highest, reaching about 210 MPa, i.e., roughly 85% of the base material (245 MPa), which coincided with the COMSOL-based temperature field simulation results. With increasing deformation amplitude and transition radius, the maximum tensile force, tensile strength, and elongation at fracture showed an increasing trend. However, the deformation amplitude should be below a certain limit because its increase elongates the welding path and reduces the distance between weld seams, resulting in serious heat accumulation. The tensile fracture morphology of the 6063-T6 base material was curved shear, with shallow toughness pits, small tearing edges at the edges, and small granular objects, indicating small plastic deformation during the fracture process. The tensile fracture of the welded part spanned the weld seam and the base material, and the fracture occurred along the tangent direction of the weld seam. The fracture surface was smooth, the tearing edges at the edge of the toughness pit shifted along the weld seam direction, forming many co-directional slip bands, with highly pronounced plastic deformation.
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Authors and Affiliations

Aiyong Cui
1
ORCID: ORCID
Haodong Liu
1
ORCID: ORCID
Shaodong Gao
2
ORCID: ORCID
Huakai Wei
1
ORCID: ORCID
Jialei Zhao
2
ORCID: ORCID

  1. Naval Aeronautical University, Qingdao, 266041, China
  2. Liaoning University of Technology, Jinzhou, 121001, China

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