Transient structure current generated by the activation of a squib device

Author(s):  
P. Leung ◽  
Tien Nguyen
Keyword(s):  
Soft Matter ◽  
2016 ◽  
Vol 12 (1) ◽  
pp. 171-180 ◽  
Author(s):  
Fabian Westermeier ◽  
David Pennicard ◽  
Helmut Hirsemann ◽  
Ulrich H. Wagner ◽  
Christoph Rau ◽  
...  

Simultaneous coherent X-ray and rheology experiments provide access to the transient structure, dynamics and viscoelastic behavior in repulsive colloidal suspensions.


Biochemistry ◽  
2014 ◽  
Vol 53 (46) ◽  
pp. 7170-7183 ◽  
Author(s):  
Jane R. Allison ◽  
Robert C. Rivers ◽  
John C. Christodoulou ◽  
Michele Vendruscolo ◽  
Christopher M. Dobson
Keyword(s):  

2016 ◽  
Vol 19 (3) ◽  
pp. 337-341 ◽  
Author(s):  
Liyin Wu ◽  
Zhen-guo Wang ◽  
Qinglian Li ◽  
Chun Li

2002 ◽  
Vol 12 (9) ◽  
pp. 181-182
Author(s):  
H. Requardt ◽  
D. Rideau ◽  
R. Danneau ◽  
A. Ayari ◽  
F. Ya Nad ◽  
...  

We present high resolution X-ray diffraction measurements on NbSe3 of the charge-density-wave (CDW) relaxation from the deformation created by the sliding of the CDW. The data are taken in the temperature range 75 K < T < 105 K in the upper-CDW phase of NbSe, and cover spatial positions up to $8OO~\mu$m from the current contact. Convenient fits to the data are obtained by a stretched exponential decay profile yielding exponents μ in the range of 0.4–0.7 and relaxation time-scales τ of the order of 1–150 ms. becoming faster with increasing sample temperature and slowing down with increasing distance from the current contact.


2019 ◽  
Vol 73 (6-7) ◽  
pp. 305-317 ◽  
Author(s):  
Christoph Hartlmüller ◽  
Emil Spreitzer ◽  
Christoph Göbl ◽  
Fabio Falsone ◽  
Tobias Madl

1997 ◽  
Vol 3 (S2) ◽  
pp. 177-178
Author(s):  
M. Monteagudo de la Rosa ◽  
M. González-Santander Martínez ◽  
G. Martinez Cuadrado ◽  
R. González Santander

Just after neural fold fusion to form the neural tube, neural crest cells detach from the neural crest, a transient structure located in the dorsal region of the neural tube. Neural crest cells migrate and differentiate into many structures and cells. But the underlying controls of this detachment and initiation of emigration are unknown. Neural crest cells are usually not morphologically distinct from the adjacent neural epithelium (neural tube) and epidermal ectoderm (epiblast) flanking them. We are combining morphological and immunohistochemical approaches to study neural crest cells in their early stage of detachment from the neural crest.Hamburger and Hamilton (1951) stages 9 to 12 White Leghorn chick embryos. Fixation in 2.5% glutaraldehyde - 0.5% tanic acid and postfixation in 1% osmium tetroxide. Embryos contrasted in bloc using uranyl acetate and embedded in araldite. Semithin transversal sections stained with toluidine blue for light microscopy. Ultrathin sections contrasted with lead citrate.


2020 ◽  
Vol 118 (3) ◽  
pp. 216a
Author(s):  
Reinhard Klement ◽  
Timo Graen ◽  
Asaf Grupi ◽  
Elisha Haas ◽  
Helmut Grubmueller

2012 ◽  
Vol 40 (13) ◽  
pp. 6353-6366 ◽  
Author(s):  
Cecilia Andresen ◽  
Sara Helander ◽  
Alexander Lemak ◽  
Christophe Farès ◽  
Veronika Csizmok ◽  
...  

1989 ◽  
Vol 62 (5) ◽  
pp. 838-849 ◽  
Author(s):  
L. C. Burton ◽  
K. Hwang ◽  
T. Zhang

Abstract 1. Low-frequency resistance can be dominated by contacts. It was found that silver paint contacts were roughly equivalent to metal contacts bonded during vulcanization. 2. Three electrical regimes are clearly evident, determined by loading: dielectric, percolation, and conducting. 3. Resistance and dielectric constant dispersion for loading above 30 phr agree with Kawamoto's model. 4. Each carbon-black loading results in a distinctive dispersion signature. 5. Dynamic conductivity can be used to delineate persistent and transient carbon-black-structure changes versus composition, DSA, frequency, and potentially other parameters (temperature, stress waveform, etc.). 6. The remaining conductive network during stress is represented by gmin; Δg is determined by network fracture and reformation; gmin−gα is proportional to the amount of remaining transient structure; g0−gα is proportional to the total transient structure; normalized conductivity Z is the remaining-to-total transient-structure ratio. 7. The Δgm=0.525(g0−gα) relation indicates that maximum reformation occurs when approximately half the transient structure is broken down and confirms the correlation between conductivity parameters and transient carbon-black structure.


2010 ◽  
Author(s):  
Klaus Sokolowski-Tinten ◽  
Anton Barty ◽  
Sebastien Boutet ◽  
Uladzimir Shymanovich ◽  
Henry Chapman ◽  
...  

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