scholarly journals Diameter Effect Curve and Detonation Front Curvature Measurements for ANFO

2002 ◽  
Author(s):  
R. A. Catanach
Keyword(s):  
Detonation Front ◽  
Effect Curve ◽  
Curvature Measurements ◽  
Front Curvature ◽  
Diameter Effect

Effect of Deuteration on the Diameter-Effect Curve of Liquid Nitromethane

2006 ◽  
Vol 110 (24) ◽  
pp. 7744-7748 ◽  
Author(s):  
Ray Engelke ◽  
Stephen A. Sheffield ◽  
Howard L. Stacy
Keyword(s):  
Effect Curve ◽  
Diameter Effect

Experimental Determination of the Detonation Front Curvature of Non-Ideal Explosive ANFO

2004 ◽  
Vol 465-466 ◽  
pp. 181-184 ◽  
Author(s):  
Atsumi Miyake ◽  
Yuji Ohtagaki ◽  
Takayuki Abe ◽  
Yuji Wada ◽  
Yoshio Nakayama ◽  
...  
Keyword(s):  
Experimental Determination ◽  
Detonation Front ◽  
Front Curvature

scholarly journals OPTIMEX: Measurement of Detonation Front Curvature with a Passive Fiber Optical System

2016 ◽  
Vol 13 (4) ◽  
pp. 807-820 ◽  
Author(s):  
Jiri Pachman ◽  
Martin Künzel ◽  
Karel Kubát ◽  
Jakub Selesovsky ◽  
Roman Maršálek ◽  
...  
Keyword(s):  
Optical System ◽  
Detonation Front ◽  
Passive Fiber ◽  
Fiber Optical ◽  
Front Curvature

STUDY OF THE PIPE DIAMETER EFFECT ON HORIZONTAL AIR-WATER TWO-PHASE FLOW

2017 ◽  
Author(s):  
Guilherme Gonçalves da Silva ◽  
Saon Vieira ◽  
Marcelo Souza de Castro ◽  
Felipe Jaloretto da Silva
Keyword(s):  
Two Phase Flow ◽  
Pipe Diameter ◽  
Phase Flow ◽  
Two Phase ◽  
Diameter Effect

scholarly journals The measurement of the energy of cosmic rays - II—The curvature measurements and the energy spectrum

1936 ◽  
Vol 154 (883) ◽  
pp. 573-587 ◽  
Keyword(s):  
Magnetic Field ◽  
Energy Spectrum ◽  
Cosmic Rays ◽  
Magnetic Fields ◽  
Strong Magnetic Fields ◽  
The Earth ◽  
Primary Particles ◽  
Curvature Measurements

Both the penetrating power of the cosmic rays through material ab­sorbers and their ability to reach the earth in spite of its magnetic field, make it certain that the energy of many of the primary particles must reach at least 10 11 e-volts. However, the energy measurements by Kunze, and by Anderson, using cloud chambers in strong magnetic fields, have extended only to about 5 x 10 9 e-volts. Particles of greater energy were reported, but the curvature of their tracks was too small to be measured with certainty. We have extended these energy measurements to somewhat higher energies, using a large electro-magnet specially built for the purpose and described in Part I. As used in these experiments, the magnet allowed the photography of tracks 17 cm long in a field of about 14,000 gauss. The magnet weighed about 11,000 kilos and used a power of 25 kilowatts.

Sign in / Sign up

Export Citation Format

Share Document