STUDY OF ENERGY TRANSFER ON PENDULUM-TYPE WAVES PROPAGATION IN BLOCK-ROCK MASS

Author(s):  
Kaixing WANG ◽  
Yishan PAN ◽  
Linming DOU
1991 ◽  
Vol 27 (4) ◽  
pp. 363-367
Author(s):  
V. Yu. Veksler ◽  
Yu. S. Gurevich ◽  
A. G. Egorov

2009 ◽  
Vol 19 (6) ◽  
pp. 699-708
Author(s):  
Hao WU ◽  
Qin FANG ◽  
Ya-dong ZHANG ◽  
Jin-chun LIU ◽  
Zi-ming GONG

2006 ◽  
Vol 42 (5) ◽  
pp. 468-475 ◽  
Author(s):  
N. I. Aleksandrova ◽  
A. G. Chernikov ◽  
E. N. Sher
Keyword(s):  

2009 ◽  
Vol 19 (4) ◽  
pp. 409-419 ◽  
Author(s):  
Hao WU ◽  
Qin FANG ◽  
Ya-dong ZHANG ◽  
Yu-sheng LU ◽  
Jin-chun LIU

2014 ◽  
Vol 651-653 ◽  
pp. 988-991 ◽  
Author(s):  
Nan Zhao ◽  
Li Wei Song

Full face rock tunnel boring machine in construction process, disc cutter put pressure on rock breaking, actually belongs to the process of energy transfer, from the point of view of energy analysis the energy transfer rules in the process of disc cutter rock breaking, based on CSM force prediction model, analysis disc cutter energy input and rock mass energy output efficiency ratio, for excavation with minimum energy efficiency. Taking S-536 Hong Kong water tunnel TBM as an example, When the penetration is 10mm, based on the energy efficiency ratio the optimal disc cutter spacing should be less than 70mm, than the actual average disc cutter spacing is small 2mm, rock mass as a reference the disc cutter rock breaking efficiency mechanism provides certain reference value for the cutter layout.


Author(s):  
Kuan Jiang ◽  
Cheng-zhi Qi ◽  
Shou-dong Zhu ◽  
Tian-wei Jin

Author(s):  
R.D. Leapman ◽  
P. Rez ◽  
D.F. Mayers

Microanalysis by EELS has been developing rapidly and though the general form of the spectrum is now understood there is a need to put the technique on a more quantitative basis (1,2). Certain aspects important for microanalysis include: (i) accurate determination of the partial cross sections, σx(α,ΔE) for core excitation when scattering lies inside collection angle a and energy range ΔE above the edge, (ii) behavior of the background intensity due to excitation of less strongly bound electrons, necessary for extrapolation beneath the signal of interest, (iii) departures from the simple hydrogenic K-edge seen in L and M losses, effecting σx and complicating microanalysis. Such problems might be approached empirically but here we describe how computation can elucidate the spectrum shape.The inelastic cross section differential with respect to energy transfer E and momentum transfer q for electrons of energy E0 and velocity v can be written as


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