Optimization of ultrasonic transducer horn geometry with vibrational-thermal performance improvement approach

Authors

1 Araku

2 araku

3 tafre

Abstract

The ultrasonic transducer transmits vibrations to the load carried by the piece called Horn. Depending on the application of the horn, vibrations can be concentrated or propagated. It is used in various applications such as ultrasonic welding. A limitation of this piece, the temperature rise during operation due to structural damping. Because this piece is vibrating at resonant frequency in the axial mode, the temperature increases and its mechanical properties change, the frequency of resonance and vibration efficiency decreases sharply. In this paper, a new optimized geometry is presented to reduce the horn temperature. The new geometry is optimal in terms of heat transfer and at the same time try to minimize lateral mode may be achieved. In order to improve this problem, a numerical model of the temperature rise for desired piece in steady-state is achieved. In addition, using the genetic algorithm, Horn thermal optimization is performed in two consecutive steps with the idea of fins. In the results section, the details of the new geometry are presented and discussed in detail in its various aspects.

Keywords


[2] P. Langevin, French Patents Nr. 575435 (1924).    
[3] Ando E, Kagawa Y (1992) Finite-element simulation of transient heat response in ultrasonic transducers. IEEE Trans Ultrason Ferroelectr Freq Control 39.                          
[4] Karnaukhov VG, Senchenkov IK, Mikhailenko VV, Dyachenko SM (1996) Numerical modeling of vibrational heating and thermal stresses in a Lagrangian piezoelectric rod transducer. Int Appl Mech 32.                                              
[5] Sherrit S, Dolgin BP, Bar-Cohen Y, Pal D, Kroh J, Peterson T (1999) Modeling of horns for sonic/ultrasonic applications. IEEE Int Ultrason Symp 647-651.
[6]Joo H, Lee C, Rho J, Jung H (2006) Analysis of temperature rise for piezoelectrictransformer using finite-element method. IEEE Trans Ultrason Ferroelectr Freq Control 53.                       
[7] Abdullah A, Shahini A, Pak A (2008) An approach to design a high power piezoelectric ultrasonic transducer. Electroceram 22: 369-382.                          
[8] Pak A, Abdullah A (2008) Correct prediction of the vibration behavior of a high power ultrasonictransducer by FEM simulation. Adv Manuf Technol 39: 21-28.                                                                        
[9] Gallego-Juárez JA, Rodriguez G, Acosta V, Riera E (2010) Power ultrasonic transducers with extensive radiators for industrial processing. Ultrason Sonochem 17: 953-964.                                                
[10] Ganesan R, Muthupandian A (2010) Simulation of heat generation from vibration in COMSOL multiphysics. Excerpt from the Proceedings of the COMSOL Conference India.
[11] Peshkovsky AS, Peshkovsky SL (2010) Acoustic cavitation theory and equipment design principles for industrial applications of high-intensity ultrasound. Nova Science Publishers.
 [12] Hosseni R, Ebrahimi Mamaghani A, Asa A (2013) An investigation into the effects of friction and anisotropy coefficients andwork hardening exponent on deep drawing with FEM. Adv Mater Process 1(2): 39-50.              
[13] Abdullah A, Malaki M (2013) On the damping of ultrasonic transducers’ components. Aerosp Sci Technol 28: 31-39.
[14] Rani MR, Prakasan K, Rudramoorthy R (2015) Studies on thermo-elastic heating of horns used in ultrasonic plastic welding. Ultrasonics 55: 123-132.
[15] Lu X, Hu J, Peng H, Wang Y (2017) A new topological structure for the Langevin-type ultrasonic transducer. Ultrasonics. 75: 1-8.
[16] Karafi MR, Khorasani F (2019) Evaluation of mechanical and electric power losses in a typical piezoelectric ultrasonic transducer. Sensor Actuat A-Phys 288: 156-164.
[2] P. Langevin, French Patents Nr. 575435 (1924).    
[3] Ando E, Kagawa Y (1992) Finite-element simulation of transient heat response in ultrasonic transducers. IEEE Trans Ultrason Ferroelectr Freq Control 39.                          
[4] Karnaukhov VG, Senchenkov IK, Mikhailenko VV, Dyachenko SM (1996) Numerical modeling of vibrational heating and thermal stresses in a Lagrangian piezoelectric rod transducer. Int Appl Mech 32.                                              
[5] Sherrit S, Dolgin BP, Bar-Cohen Y, Pal D, Kroh J, Peterson T (1999) Modeling of horns for sonic/ultrasonic applications. IEEE Int Ultrason Symp 647-651.
[6]Joo H, Lee C, Rho J, Jung H (2006) Analysis of temperature rise for piezoelectrictransformer using finite-element method. IEEE Trans Ultrason Ferroelectr Freq Control 53.                       
[7] Abdullah A, Shahini A, Pak A (2008) An approach to design a high power piezoelectric ultrasonic transducer. Electroceram 22: 369-382.                          
[8] Pak A, Abdullah A (2008) Correct prediction of the vibration behavior of a high power ultrasonictransducer by FEM simulation. Adv Manuf Technol 39: 21-28.                                                                        
[9] Gallego-Juárez JA, Rodriguez G, Acosta V, Riera E (2010) Power ultrasonic transducers with extensive radiators for industrial processing. Ultrason Sonochem 17: 953-964.                                                
[10] Ganesan R, Muthupandian A (2010) Simulation of heat generation from vibration in COMSOL multiphysics. Excerpt from the Proceedings of the COMSOL Conference India.
[11] Peshkovsky AS, Peshkovsky SL (2010) Acoustic cavitation theory and equipment design principles for industrial applications of high-intensity ultrasound. Nova Science Publishers.
 [12] Hosseni R, Ebrahimi Mamaghani A, Asa A (2013) An investigation into the effects of friction and anisotropy coefficients andwork hardening exponent on deep drawing with FEM. Adv Mater Process 1(2): 39-50.              
[13] Abdullah A, Malaki M (2013) On the damping of ultrasonic transducers’ components. Aerosp Sci Technol 28: 31-39.
[14] Rani MR, Prakasan K, Rudramoorthy R (2015) Studies on thermo-elastic heating of horns used in ultrasonic plastic welding. Ultrasonics 55: 123-132.
[15] Lu X, Hu J, Peng H, Wang Y (2017) A new topological structure for the Langevin-type ultrasonic transducer. Ultrasonics. 75: 1-8.
[16] Karafi MR, Khorasani F (2019) Evaluation of mechanical and electric power losses in a typical piezoelectric ultrasonic transducer. Sensor Actuat A-Phys 288: 156-164.