Gas-puff liner implosion in the configuration with helical current return rods

2013 ◽  
Vol 39 (2) ◽  
pp. 139-143 ◽  
Author(s):  
S. A. Sorokin
Author(s):  
Chris Lorenz

This introductory chapter assesses the role of theory in history and traces the developments in the discipline of history. Theoretical reflection about the ‘true nature’ of history fulfils three interrelated practical functions. First, theory legitimizes a specific historical practice—a specific way of ‘doing history’—as the best one from an epistemological and a methodological point of view. Second, theory sketches a specific programme of doing history. Third, theoretical reflections demarcate a specific way of ‘doing history’ from other ways of ‘doing history’, which are excluded or degraded. The chapter then considers three phases of theoretical changes from analytical to narrative philosophy of history, and then on to ‘history from below’ and the ‘presence’ of history, ultimately leading to the current return of fundamental ontological and normative questions concerning the status of history and history-writing.


2021 ◽  
Vol 63 (11) ◽  
pp. 115017
Author(s):  
Shuhao Li ◽  
Nengchao Wang ◽  
Yonghua Ding ◽  
Zebao Song ◽  
Yunfeng Liang ◽  
...  

IEEE Access ◽  
2019 ◽  
Vol 7 ◽  
pp. 96540-96548 ◽  
Author(s):  
Emilio Lorenzani ◽  
Giovanni Migliazza ◽  
Fabio Immovilli ◽  
Chris Gerada ◽  
He Zhang ◽  
...  

The instrument described is the outcome of conversations between the late Professor J. Viriamu Jones, F. R. S., and one of the authors (W. E. A.), on their return from the British Association Meeting held in Toronto in 1897. Its object was to determine “ the ampere ” as defined in the C. G. S. system, to an accuracy comparable with that attained in the absolute determination of the ohm by Lorenz’s apparatus, an account of which was given by Professors Ayrton and Jones at the Toronto Meeting. Professor Jones had previously developed a convenient formula for calculating the electromagnetic force between a helical current and a coaxial current sheet, viz., F = γ h γ (M 2 -M 1 ),† where γ h is the current in the helix, the γ current per unit length of the current sheet, and M 1 , M 2 the coefficients of mutual induction of the helix and the two ends of the current sheet respectively. By using coaxial coils with single layers of wire wound in screw-thread grooves, advantage could be taken of the above formula.


2014 ◽  
Vol 54 (6) ◽  
pp. 064016 ◽  
Author(s):  
M. Rack ◽  
L. Zeng ◽  
P. Denner ◽  
Y. Liang ◽  
A. Wingen ◽  
...  

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