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JOURNAL OF APPLIED SCIENCES RESEARCH
Copyright © 2014, American-Eurasian Network for Scientific Information publisher JOURNAL OF APPLIED SCIENCES RESEARCH JOURNAL home page: http://www.aensiweb.com/JASR. 2014 May; 10(5): pages 523-527. Published Online 2 2 June 2014. Research Article Finite-element simulation of explosive welding process by ansys software and UT process Ali Moarrefzadeh Department of Mechanical Engineering, College of Mechanics, Mahshahr Branch, Islamic Azad University, Mahshahr, Iran. Received: 15 April 2014; Revised: 2 0 May, 2014; Accepted: 25 May 2014 © 2014 AENSI PUBLISHER All rights reserved ABSTRACT The origins of explosion welding go back to World War II, when it was observed that pieces of shrapnel were not only embedded into armor plating but also being clad, or welded, to the metal. Since there was none of the extreme heat involved in other forms of welding, it was determined that the weld was caused by the explosive forces. Explosive welding is a process which uses explosive detonation to propel the flyer plate material into the base material to produce a sound joint. The factors which cause localized heat gain and control the process. The approach to model metal surfaces is an example of a problem dealing with the influence of the finite element method has been used. AUTODYNE purpose of the program is that the dynamic model is used ANSYS software. In the second part, the first part is actually complementary. In this study, all the experiments carried out were simulated using the finite element method. The Williamsburg equations of state were used to describe the behavior of explosive. The Williamsburg equations of state have been previously developed for low explosive mixture. These equations were coded into the FEM software. This paper describes work carried out to numerically analyze a two plate welding process using a finite element method (FEM) and the verification of the results using experimental data. Key words: Explosive Welding, UT, Numerical Simulation, Optimization, metal, Ansys INTRODUCTION The explosion welding process begins with only the highest-quality materials from the most reputable manufacturers around the world, that meet our clients’ expectations and our own exacting specifications. Let’s look at the explosion welding of two plates as an example. When two plates are being clad, the mating surfaces of both metals (the surfaces facing each other) are ground flat to achieve a smooth finish and prepare the surfaces for the explosion. The plates are then ready to be assembled into the pack, which locks the plates into position. To build a pack, the base metal, which is the stronger and thicker of the plates, is laid face up. Then the cladding metal, which is the thinner of the two plates, is placed on top. A small gap is left between the base metal and cladding metal. Next, explosive powder is evenly spread on the cladding (alloy) plate. The amount and exact formulation of the powder are always matched to the types of metal involved. The explosion is detonated from one edge of the cladding plate and moves across the top of the pack at a uniform speed, which results in a high-pressure collision of the metals. Oxides and impurities are expelled, leaving the plate surfaces metallurgically pure and creating a metallurgical weld between the two metals. After this process is performed, the newly formed clad is flattened out by a press or, for thinner clad, a series of rollers known as levelers(fig.1). Corresponding Author: Ali Moarrefzadeh, Department of Mechanical Engineering, College of Mechanics, Mahshahr Branch, Islamic Azad University, Mahshahr, Iran. E-mail: [email protected] 524 Ali Moarrefzadeh, 2014 /Journal Of Applied Sciences Research 10(5), May, Pages: 523-527 Fig. 1: Explosion welding (EXW) process General Specifications: Experimental tests have been performed to explosively welded aluminum 5056, aluminum 1015 and stainless steel 304 tubes in one step. The welded tubes had an external diameter of 135mm and internal diameter of 113mm. The outer layer was made of 304-stainless steel, with the external diameter of 135 and thickness of 4.5mm. The middle tube was made of Al-1015 and its thickness was 1.5mm. The inner tube was made of Al-5056 with 5mm thickness. The tests have been carried out using various stand-off distances and explosive ratios. Various interface geometries have been obtained from these Basic Principles of Ultrasonic Testing: In the explosive welding process, the metal plates are made to collide obliquely with each other at a high velocity with the use of explosive. The impact causes the two metals to come into intimate contact such that metallurgical bonding takes place across the interface. As the detonation of the explosive proceeds, a scavenging action occurs experiments. The explosive material was positioned inside the inner tube. In this study, all the experiments were simulated using the finite element method. The Williamsburg equations of state were used to describe the behavior of explosive. The Williamsburg equations of state have been previously developed for low explosive mixture10 These equations were coded into the FEM software. The Johnson-Cook constitutive equations were used to model the behavior of tubes. The Johnson-Cook equations were described as: ( A B n )(1 C ln p )(1 Tm ) between the two mating surfaces, due to jetting. The jet formation aids metallurgical bonding in two ways: first, it causes the breakup of the contaminant surface film and expels it from the point of collision and it exposes virgin surfaces, which are brought into close contact as a result of collision. Ultrasonic Testing method: 525 Ali Moarrefzadeh, 2014 /Journal Of Applied Sciences Research 10(5), May, Pages: 523-527 Ultrasonic Testing (UT) uses high frequency sound energy to conduct examinations and make measurements. Ultrasonic inspection can be used for flaw detection/evaluation, dimensional measurements, material characterization, and more. To illustrate the general inspection principle, a typical pulse/echo inspection configuration as illustrated below will be used. A typical UT inspection system consists of several functional units, such as the pulser/receiver, transducer, and display devices. A pulser/receiver is an electronic device that can produce high voltage electrical pulses. Driven by the pulser, the transducer generates high frequency ultrasonic energy. The sound energy is introduced and propagates through the materials in the form of waves. When there is a discontinuity (such as a crack) in the wave path, part of the energy will be reflected back from the flaw surface. The reflected wave signal is transformed into an electrical signal by the transducer and is displayed on a screen. In the applet below, the reflected signal strength is displayed versus the time from signal generation to when a echo was received. Signal travel time can be directly related to the distance that the signal traveled. From the signal, information about the reflector location, size, orientation and other features can sometimes be gained. Manual ultrasonic weld inspections are performed using a single probe, which the operator “rasters” back and forth to cover the weld area. Many automated weld inspection systems use a similar approach (see Figure 2a), with a single probe scanned back and forth over the weld area. This is time consuming, since the system has dead zones at the start and finish of the raster. Fig. 2: Scanninig in ultrasonic testing process Ultrasonic Inspection is a very useful and versatile NDT method. Some of the advantages of ultrasonic inspection that are often cited include: It is sensitive to both surface and subsurface discontinuities. Result And Discussions Hydraulic turbulence phenomena appear in a large variety of industrial pipe flows. They introduce some errors in the ultrasonic flowmeter measurements. In this study, we have described a numerical procedure toquantify the transit-time flowmeter uncertainties causedby the deviation of the acoustical The depth of penetration for flaw detection or measurement is superior to other NDT methods. Only single-sided access is needed when the pulse-echo technique is used. It is highly accurate in determining reflector position and estimating size and shape. paths from the straightlines. In our simplified configuration, we have foundthat the flow rate is overestimed of 0.35% due to theeffects of the mean velocity profile, and that the meanthermal field has a negligible influence. In the second part, the first part is actually complementary. Ways to try to generate heat and increase the impact of the collision and impact force and the results of the survey analysis software 526 Ali Moarrefzadeh, 2014 /Journal Of Applied Sciences Research 10(5), May, Pages: 523-527 environment used to increase weld quality and productivity. Finally, optimal results in terms of mechanical and metallurgical weld ultrasonic testing method for controlling the size and quality of weld to be examined. Ultrasonic A-scan examination was found to be very precise in detecting the presence of delamination in the weld joints. This has also been imaged and confirmed using C-scan technique(fig. 3). Fig. 3: result of C-scan Conclusion: The simulations showed that the temperature at the collision point was not reached to the material melting point. But, it was high enough for phase transformation to occur. Therefore, this study supports the idea that the explosive welding process is a solid state process. This study suggests that the minimum plastic strain may be required to bonding take place. The results showed that the shear strain profiles at the surfaces of the tubes bonded had opposite sign at the collision points. Acknowledgments This paper was extracted from a research project entitled Study of weld quality in explosive welding process by finite-element method and ultrasonic testing. financial assistance from Islamic Azad University, Mahshahr Branch is gratefully acknowledged. References Blazynski, T.Z., 1983. Explosive Welding, Forming and Compaction, Applied Science, London. Cowan, G.R. and A.H. Holtzman, 1963. “Flow Configuration in Colliding Plates: Explosive Bonding”, J. Appl. Phys., 34: 928-939. Wylie, H.K., P.E.G. Williams and B. Crossland, 1970. “Further Experimental Investigation of Explosive Welding Parameters”, Proc. 1stInt. Sym. on Use of New Properties and Possibilities of Application thereof in the Chemical Industry, pp: 4570. Szecket, A., 1979. “An Experimental Study of the Explosive Welding Window”, Ph.D. Thesis. Wittman, R.H., 1973. “The Influence of Collision Parameters on the Strength and Microstructure of an Explosion Welded Aluminum Alloy”, Proc. 2ndSym. on Use of Explosive Energy in Manufacturing Metallic Materials of New Properties and Possibilities of Application thereof in the Chemical Industry, pp: 153-168. Deribas, A.A., V.A. Simonov and I.D. Zakharenko, 1975. “Investigation of Explosive Welding Parameters for Arbitrary Combinations of Metals and Alloys”, Proc. 5th Int. Conf. on High Energy Rate Fabrication, 4.1.1-4.1.24. Lazari, G.L. and S.T.S. Al-Hassani, 1984. “Solid Mechanics Approach Explosive Welding Composite, Proc. 8th Int. Conf. on High Energy Rate Fabrication, San Antonio. Oberg, A., J.A. Schweitz and H. Olfsson, 1984. “Modeling of the Explosive Welding Process, Proc. 8thInt. Conf. on High Energy Rate Fabrication, pp: 75-84. Akihisa, A.B.E., 1997. “Numerical study of the mechanism of a wavy interface generation in 527 Ali Moarrefzadeh, 2014 /Journal Of Applied Sciences Research 10(5), May, Pages: 523-527 explosive welding”, JSME Int. J., Series , 40(3): 395401. Akbari Mousavi, S.J. Burley and S.T.S. AlHassani, 2004. “Simulation of Explosive Welding with Anfo Mixtures”, Propellants, Explosives, Pyrotechnics, 29(3): 188-196.