void interaction
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Author(s):  
Daniel Franke ◽  
Michael Zinn ◽  
Shiva Rudraraju ◽  
Frank E. Pfefferkorn

Abstract The goal of this research was to examine how altering the amount of friction stir tool eccentricity while controlling the amount of slant in the tool shoulder (drivers of oscillatory process forces) effects the generation of process force transients during sub-surface void interaction. The knowledge gained will help improve the accuracy of force-based void monitoring methods that have the potential to reduce the need for post-weld inspection. Process force transients during sub-surface void formation were examined for multiple tools with varying magnitudes of kinematic runout. The eccentric motion of the tool produced oscillations in the process forces at the tools rotational frequency that became distorted when features (flats) on the tool probe interacted with voided volumes, generating an amplitude in the force signals at three times the tool rotational frequency (for three flat tools). A larger tool eccentricity generates a larger amplitude in the force signals at the tool’s rotational frequency that holds a larger potential to create a distortion during void interaction. It was determined that once void becomes large enough to produce an interaction that generates an amplitude at the third harmonic larger than 30% of the amplitude at the rotational frequency in a weld with no interaction (amplitude solely at rotational frequency), the trailing edge of the tool shoulder cannot fully consolidate the void, i.e., it will remain in the final weld. Additionally, once the void exceeds a certain size, the amplitudes of the third harmonics saturate at 70% of the amplitude at the rotational frequency during full consolidation. The interaction between the eccentric probe and sub-surface void was isolated by ensuring any geometric imperfection in the shoulder (slant) with respect to the rotational axis was removed. The results suggest that geometric imperfections (eccentricity and slant) with respect to the tool’s rotational axis must be known when developing a void monitoring method from force transients of this nature.


Author(s):  
Daniel Franke ◽  
Michael R. Zinn ◽  
Shiva Rudraraju ◽  
Frank E. Pfefferkorn

Abstract The goal of this research is to examine how altering the amount of friction stir tool eccentricity while controlling the amount of slant in the tool shoulder (drivers of oscillatory process forces) effects the generation of process force transients during sub-surface void interaction. The knowledge gained will help improve the accuracy of force-based void monitoring methods that have the potential to reduce the need for post-weld inspection. The eccentric motion of the tool produces oscillations in the process forces at the tool's rotational frequency, which becomes distorted when features on the probe interact with voids, generating an amplitude in the force signals at three times the tool rotational frequency (for three flat tools). A larger tool eccentricity generates a larger amplitude in the force signals at the tool's rotational frequency, which has a greater potential to create a distortion during void interaction. Once a void becomes large enough to produce amplitude at the third harmonic larger than 30% of the amplitude at the rotational frequency, the trailing edge of the tool shoulder cannot fully consolidate the void. The interaction between the eccentric probe and sub-surface void is isolated by ensuring any geometric imperfection in the shoulder (slant) is removed. The results suggest that geometric imperfections (eccentricity and slant) with respect to the tool's rotational axis must be known when developing a void monitoring method from force transients of this nature.


2018 ◽  
Vol 123 (24) ◽  
pp. 245101 ◽  
Author(s):  
Kai Zhao ◽  
Jianying He ◽  
Inga Gudem Ringdalen ◽  
Zhiliang Zhang

2018 ◽  
Author(s):  
Sagar Chandra ◽  
M. K. Samal ◽  
V. M. Chavan ◽  
S. Raghunathan

2017 ◽  
Vol 97 (12) ◽  
pp. 504-514 ◽  
Author(s):  
S. Chandra ◽  
M. K. Samal ◽  
N. N. Kumar ◽  
V. M. Chavan ◽  
S. Raghunathan

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