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Measurement Parameters of Ultrasonic Oscillatory System during ...

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4MEASUREMENT PARAMETERS OF ULTRASONIC OSCILLATORY SYSTEM DURING WELDINGTHERMOPLASTICS2. Value <strong>of</strong> a current on oscillatory system.3. Oscilation frequency UOS.4. A phase difference <strong>of</strong> a voltage and a current onoscillatory system.5. A phase difference between two any periodic signals(from the basic generator, a feedback, a current or avoltage on oscillatory system).For management <strong>of</strong> job <strong>of</strong> the measuring complex andas recordings and processings <strong>of</strong> the measuredinformation the personal computer is used.Communication is carried out by means <strong>of</strong> protocol RS-232.During ultrasonic welding continuous measurement <strong>of</strong>amplitude current <strong>of</strong> mechanical branch UOS I,amplitudes <strong>of</strong> electric voltage U, a phase angle between avoltage and current φ(I, U), a phase angle between avoltage on oscillatory system and feedback signal φ(I,Os), a phase angle between a voltage and a signal basicfrequencies φ(I, Op) was made (figure 2).In figure 2 dependences <strong>of</strong> electric parameters UOS atan absent material are presented (radiation to air).During welding at an absent material value <strong>of</strong> currentI, voltage U and phase angles φ (I, U), φ (I, Op), φ (I,Os) are saved by constants <strong>during</strong> all period <strong>of</strong> ultrasonicaffecting. In this case parameters UOS remain toconstants, because <strong>of</strong> absence <strong>of</strong> effect on oscillatorysystem, changing properties <strong>of</strong> a welded material <strong>during</strong>welding.Dependences presented in figure 3 illustrate effect <strong>of</strong>changing properties <strong>of</strong> a welded material in a weld zone(a s<strong>of</strong>tening <strong>of</strong> a polymeric material and transition in a isviscous-plastic condition) on electric parametersoscillatory system. There is a change <strong>of</strong> followingmagnitudes: I, U, φ(I, U), φ(I, Os) and φ(I,Op).From dependences presented in figure 3 follows thatprocess <strong>of</strong> welding can be broken into 3 stages:1. Change <strong>of</strong> a welded material from a solid conditionin is viscous-plastic. At this stage there is a decrease <strong>of</strong>value <strong>of</strong> current I and voltage U on oscillatory system,increase in a phase angle between a voltage and a currentφ(I,U), and values <strong>of</strong> phase angles φ(I,Os) and φ(I,Op)remain practically constant.2. The Is viscous-plastic condition. At this stage thereis maximum damping oscillatory system. Values <strong>of</strong>current I and voltage U attain the minimal value, andmagnitude <strong>of</strong> a phase angle between a voltage and acurrent φ(I,U) on oscillatory system attains the maximumvalue.3. Change <strong>of</strong> a welded material from a is viscousplasticcondition in is viscous-fluid. At this stage there isan intensive smelting a material in a weld zone. Excesses<strong>of</strong> the fused material start to be extruded from a weld zonethat reduces welding pressure on oscillatory system. Thereis an increase in value <strong>of</strong> current I and voltage U onoscillatory system, decrease <strong>of</strong> a phase angle between avoltage and current φ(I, U).One <strong>of</strong> key parameters <strong>of</strong> ultrasonic welding is weldingpressure.In figure 4 some dependences <strong>of</strong> the current flowingthrough piezoceramic elements oscillatory system atwelding <strong>of</strong> equal specimens on thickness frompolypropylene at changing welding pressure on a materialare presented.From the presented dependences follows, that, atwelding equal specimens on thickness, curves <strong>of</strong> a currentcan differ essentially from each other. It is connected, first<strong>of</strong> all, with various force <strong>of</strong> welding pressures on weldedmaterials, both <strong>during</strong> the initial moment, and <strong>during</strong> allprocess <strong>of</strong> welding.Carried out researches have shown, that at effect <strong>of</strong> bigwelding pressures there is strong damping UOS owing towhat it is not formed a qualitative welded joint. On theother hand at small welding pressure also it is not formeda qualitative welded joint, owing to insufficient energyforwarded in a weld zone.Thus, for implementation <strong>of</strong> the qualitative joint <strong>of</strong>materials it is necessary to expel effect <strong>of</strong> instabilitywelding pressures at ultrasonic welding, i.e. to expeldistortions <strong>of</strong> curves <strong>of</strong> a current.From the gained results necessity <strong>of</strong> search optimumwelding pressures <strong>during</strong> ultrasonic welding follows.The further jobs will be directed on search <strong>of</strong> optimumparameters <strong>of</strong> ultrasonic welding thermoplastic materials.IV. CONCLUSIONAs a result <strong>of</strong> the spent researches have been solvedfollowing individual problems:1. <strong>Measurement</strong>s <strong>of</strong> electric parameters UOS <strong>during</strong>ultrasonic welding are carried out;2. Effect, changing properties <strong>of</strong> welded materials onparameters UOS is determine;3. Eeffect welding pressures on electric parametersUOS Is researched;4. Optimum regimes for implementation <strong>of</strong> ultrasonicwelding with the maximum effect are installed.5. Criteria <strong>of</strong> automatic determination <strong>of</strong> optimumregimes <strong>of</strong> ultrasonic welding <strong>of</strong> various materials invarious conditions are determined.REFERENCES[1] Volkov S.S., Cherniak B.J. Welding <strong>of</strong> plastic usingultrasound, Chemistry.[2] Volkov S.S., Orlov U.N., Astahova R.N. Weldingand agglutination <strong>of</strong> plastic. М., «Machinery», 1972,128 с .[3] Zaysev K.I., Matsuk L.N. Welding plastic. М.,«Machinery», 1978.[4] Holopov JU.V. <strong>Ultrasonic</strong> welding <strong>of</strong> plastic andmetals. "Mechanical engineering", 1988.[5] Khmelev V.N., Slivin A.N., Barsukov R.V.,Tsyganok S.N., Savin I.I., Shalunov A.V., LevinS.V., Abramov A.D. "Development <strong>of</strong> the New

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