U.S. TAG for ISO/TC108 Mechanical Vibration and Shock (Minutes of the Accredited Standards Committee on Mechanical Shock and Vibration, S2)

1991 ◽  
Author(s):  
ACOUSTICAL SOCIETY OF AMERICA NEW YORK
2003 ◽  
Vol 56 (5) ◽  
pp. B67-B68 ◽  
Author(s):  
C Lalanne, ◽  
C Cetinkaya,

2013 ◽  
Vol 2013 (1) ◽  
pp. 000200-000207
Author(s):  
Hoang-Vu Nguyen ◽  
Knut E. Aasmundtveit ◽  
Helge Kristiansen ◽  
Tore Helland

Novel isotropic conductive adhesives (ICAs) filled with metal-coated polymer spheres (MPS) have been introduced in order to improve the mechanical performance, and hence the reliability, compared to conventional ICAs filled with solid silver (Ag) particles. This paper summarizes a number of characterization studies on the electrical, the mechanical and the rheological properties, as well as a study on the reliability, of MPS-based ICAs. The feasibility of the ICAs filled with MPS has been demonstrated in terms of potential processing capabilities, improved mechanical performance and competitive electrical properties (compared to conventional ICAs with Ag flakes). Therefore, the MPS-based ICAs have a good potential for demanding environment applications, in which electronic products (e.g., hand held devices) are subjected to thermal shock and thermal cycling, mechanical vibration and mechanical shock.


2018 ◽  
Author(s):  
Katherine Marczenko ◽  
James Goettel ◽  
Gary Schrobilgen

Oxygen coordination to the Xe(VI) atom of XeO<sub>3</sub> was observed in its adducts with triphenylphosphine oxide, dimethylsulfoxide, pyridine-N-oxide, and acetone. The crystalline adducts were characterized by low-temperature, single-crystal X-ray diffraction and Raman spectroscopy. Unlike solid XeO<sub>3</sub>, which detonates when mechanically or thermally shocked, the solid [(C<sub>6</sub>H<sub>5</sub>)<sub>3</sub>PO]<sub>2</sub>XeO<sub>3</sub>, [(CH<sub>3</sub>)<sub>2</sub>SO]<sub>3</sub>(XeO<sub>3</sub>)<sub>2</sub>,<sub> </sub>and (C<sub>5</sub>H<sub>5</sub>NO)<sub>3</sub>(XeO<sub>3</sub>)<sub>2</sub> adducts are insensitive to mechanical shock, but undergo rapid deflagration when ignited by a flame. Both [(C<sub>6</sub>H<sub>5</sub>)<sub>3</sub>PO]<sub>2</sub>XeO<sub>3 </sub>and (C<sub>5</sub>H<sub>5</sub>NO)<sub>3</sub>(XeO<sub>3</sub>)<sub>2</sub> are air-stable whereas [(CH<sub>3</sub>)<sub>2</sub>SO]<sub>3</sub>(XeO<sub>3</sub>)<sub>2</sub> slowly decomposes over several days and [(CH<sub>3</sub>)<sub>2</sub>CO]<sub>3</sub>XeO<sub>3</sub> undergoes adduct dissociation at room temperature. The xenon coordination sphere of [(C<sub>6</sub>H<sub>5</sub>)<sub>3</sub>PO]<sub>2</sub>XeO<sub>3</sub> is a distorted square pyramid which provides the first example of a five-coordinate XeO<sub>3</sub> adduct. The xenon coordination spheres of the remaining adducts are distorted octahedra comprised of three Xe---O secondary contacts that are approximately trans to the primary Xe–O bonds of XeO<sub>3</sub>. Quantum-chemical calculations were used to assess the Xe---O adduct bonds, which are predominantly electrostatic σ-hole bonds between the nucleophilic oxygen atoms of the bases and the σ-holes of the xenon atoms.


Author(s):  
DANILO CESAR DE AZEVEDO MONTEIRO ◽  
Tatiane de Campos Chuvas ◽  
Maria Cindra Fonseca

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