scholarly journals Design and Fabrication of a Single-Aperture 11 T ${\rm Nb}_{3}{\rm Sn}$ Dipole Model for LHC Upgrades

2012 ◽  
Vol 22 (3) ◽  
pp. 4001705-4001705 ◽  
Author(s):  
A. V. Zlobin ◽  
N. Andreev ◽  
G. Apollinari ◽  
B. Auchmann ◽  
E. Barzi ◽  
...  
Keyword(s):  
Dipole Model ◽  
Single Aperture

Test results of a single aperture dipole model magnet for LHC

1999 ◽  
Vol 9 (2) ◽  
pp. 467-470 ◽  
Author(s):  
T. Shintomi ◽  
T. Nakamoto ◽  
N. Higashi ◽  
N. Kimura ◽  
T. Ogitsu ◽  
...  
Keyword(s):  
Dipole Model ◽  
Test Results ◽  
Single Aperture

scholarly journals Quench Performance of a 1 m Long Single-Aperture 11 T $ \hbox{Nb}_{3}\hbox{Sn}$ Dipole Model for LHC Upgrades

2014 ◽  
Vol 24 (3) ◽  
pp. 1-5 ◽  
Author(s):  
A. V. Zlobin ◽  
N. Andreev ◽  
G. Apollinari ◽  
B. Auchmann ◽  
H. Bajas ◽  
...  
Keyword(s):  
Dipole Model ◽  
Single Aperture

scholarly journals Field Quality Study of a 1-m-Long Single-Aperture 11-T $\hbox{Nb}_{3}\hbox{Sn}$ Dipole Model for LHC Upgrades

2014 ◽  
Vol 24 (3) ◽  
pp. 1-5 ◽  
Author(s):  
G. Chlachidze ◽  
J. DiMarco ◽  
N. Andreev ◽  
G. Apollinari ◽  
B. Auchmann ◽  
...  
Keyword(s):  
Dipole Model ◽  
Field Quality ◽  
Single Aperture ◽  
Quality Study

scholarly journals Test results of a single aperture 10 tesla dipole model magnet for the Large Hadron Collider

1996 ◽  
Vol 32 (4) ◽  
pp. 2116-2119 ◽  
Author(s):  
A. Yamamoto ◽  
T. Shintomi ◽  
N. Kimura ◽  
Y. Doi ◽  
T. Haruyama ◽  
...  
Keyword(s):  
Large Hadron Collider ◽  
Hadron Collider ◽  
Dipole Model ◽  
Test Results ◽  
Single Aperture

A New Defect in Polyethylene Single Crystals

1973 ◽  
Vol 31 ◽  
pp. 70-71
Author(s):  
E. L. Thomas ◽  
S. L. Sass
Keyword(s):  
Single Crystals ◽  
Screw Dislocation ◽  
Small Distance ◽  
Dipole Model ◽  
Dislocation Dipole ◽  
Chain Folding ◽  
Black And White ◽  
Polymer Crystal ◽  
Different Types

In polyethylene single crystals pairs of black and white lines spaced 700-3,000Å apart, parallel to the [100] and [010] directions, have been identified as microsector boundaries. A microsector is formed when the plane of chain folding changes over a small distance within a polymer crystal. In order for the different types of folds to accommodate at the boundary between the 2 fold domains, a staggering along the chain direction and a rotation of the chains in the plane of the boundary occurs. The black-white contrast from a microsector boundary can be explained in terms of these chain rotations. We demonstrate that microsectors can terminate within the crystal and interpret the observed terminal strain contrast in terms of a screw dislocation dipole model.

scholarly journals Space Charge Property of Polyethylene/Silica Nanocomposites at Different Elongations

2015 ◽  
Vol 2015 ◽  
pp. 1-14 ◽  
Author(s):  
Can Wang ◽  
Youyuan Wang ◽  
Peng Fan ◽  
Ruijin Liao
Keyword(s):  
Particle Size ◽  
Space Charge ◽  
Dipole Model ◽  
Particle Sizes ◽  
Test Results ◽  
Silica Nanocomposites ◽  
Induced Dipole ◽  
Interface Characteristics ◽  
Space Charge Distribution ◽  
Charge Property

This paper prepares polyethylene/silica nanocomposites with concentrations of 3 wt% and 5 wt% by using silicon dioxide (SiO2) nanopowder (nanosilica) with particle sizes of 15 and 50 nm. Samples whose elongations are 3%, 6%, and 10% are prepared. Pulsed electroacoustic technique is applied to evaluate the space charge distribution in samples. Test results show that homocharge near electrodes is generated in the polyethylene/silica nanocomposites. Nanocomposites with a nanoparticle concentration of 3 wt% and particle size of 15 nm suppress the accumulation of space charge effectively. The amount of space charge in the samples increases with the increase in elongation. At an elongation of 10%, packet-like space charge is generated in polyethylene/silica nanocomposites with the concentration of 5 wt% and particle sizes of 15 and 50 nm. The packet-like space charge in nanocomposites whose particle size is 50 nm is more obvious than that in nanocomposites whose particle size is 15 nm. The experiment results are explained by applying interface characteristics, dipole model, and induced dipole model.

Sign in / Sign up

Export Citation Format

Share Document