scholarly journals Mechanical dissipation in MoRe superconducting metal drums

2017 ◽  
Vol 110 (8) ◽  
pp. 083103 ◽  
Author(s):  
S. Yanai ◽  
V. Singh ◽  
M. Yuan ◽  
M. F. Gely ◽  
S. J. Bosman ◽  
...  
2021 ◽  
Vol 15 (2) ◽  
Author(s):  
Yingchun Leng ◽  
Rui Li ◽  
Xi Kong ◽  
Han Xie ◽  
Di Zheng ◽  
...  

2013 ◽  
Vol 12 (11) ◽  
pp. 1019-1023 ◽  
Author(s):  
M. P. M. Dean ◽  
G. Dellea ◽  
R. S. Springell ◽  
F. Yakhou-Harris ◽  
K. Kummer ◽  
...  

Author(s):  
Thuy Linh Pham ◽  
Jean Balcaen ◽  
Sambor Chhay ◽  
Yves Bereaux ◽  
Jean-Yves Charmeau

In injection moulding or in extrusion, plastication is the step during which polymer pellets are melted by the means of mechanical dissipation provided by a rotating screw and by thermal conduction coming from a heated metallic barrel. This step is crucial for melt thermal homogeneity, charge dispersion and fibre length preservation. Although there have been a large number of theoretical and experimental studies of plastication during the past decades, mostly on extrusion and mostly using the screw extraction technique, extremely few of them have dealt with trying to visualise plastication, let alone measuring the plastication profile in real-time. As a matter of fact, designing such an equipment is an arduous task. We designed an industry-sized metallic barrel, featuring 3 optical glass windows; each window possessing 3 plane faces itself to allow for visualisation and record by synchronised cameras and lightening by lasers. The images recorded can be further analysed by digital image processing. Preliminary results confirm the plastication theory and show a compacted solid bed and a melt pool side by side. The total plastication length is a direct function of screw rotation frequency as it is obvious from results on the melt pool width, which increases when the screw rotation frequency decreases. However, some evidence of solid bed breakage has been recorded, whereby the solid bed does not diminish continuously along the screw but is fractured in the compression zone.


2009 ◽  
Vol 26 (15) ◽  
pp. 155012 ◽  
Author(s):  
I W Martin ◽  
E Chalkley ◽  
R Nawrodt ◽  
H Armandula ◽  
R Bassiri ◽  
...  

1973 ◽  
pp. 341-353 ◽  
Author(s):  
Juana V. Acrivos ◽  
S. F. Meyer ◽  
T. H. Geballe

1988 ◽  
Vol 121 ◽  
Author(s):  
Mariquita A. Accibal ◽  
Jonathan W. Draxton ◽  
Allen H. Gabor ◽  
Wayne L. Gladfelter ◽  
Beth Anne Hassler ◽  
...  

ABSTRACTA comparison of the use of three different coordination compounds of copper as precursors for the sol-gel synthesis of YBa2Cu3O7-δ has been made. For yttrium, the tris(isopropoxide) was used exclusively, while the use of both Ba(O-i-Pr)2 and Ba(OCH2CH2OEt)2 (prepared in situ from Ba metal) as sources for Ba were studied. After dissolving Y(O-i-pr)3, a Ba source, and the copper(I) alkoxide, [Cu(O-i-Bu)]4, hydrolysis led immediately to an orange gelatinous solid which yielded YBa2Cu3O7-δ upon firing in oxygen. Copper(II) acetate was found to give heterogeneous mixtures under our conditions and was not further studied. Copper(II) acac (acac = acetylacetonate) yielded the best results. Partially hydrolyzed solutions of Cu(acac)2, Ba(OCH2CH2OEt)2, and Y(O-i-pr)3 were spin coated on SrTi03 (100) and fired under oxygen to give oriented (b axis normal to the surface) thin films of YBa2Cu3O7-δ. The onset of superconductivity for the films was 92 K, but they did not reach zero resistance until much lower temperatures.


2020 ◽  
Vol 32 (11) ◽  
pp. 1906046 ◽  
Author(s):  
Nitesh Kumar ◽  
Mengyu Yao ◽  
Jayita Nayak ◽  
Maia G. Vergniory ◽  
Jörn Bannies ◽  
...  

Author(s):  
Georg Anetsberger ◽  
Albert Schliesser ◽  
Remi Riviere ◽  
Olivier Arcizet ◽  
T. J. Kippenberg

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