On the estimation of dynamic mass density of random composites

2012 ◽  
Vol 132 (2) ◽  
pp. 615-620 ◽  
Author(s):  
Congrui Jin
2017 ◽  
Vol 142 (2) ◽  
pp. 890-901 ◽  
Author(s):  
Guy Bonnet ◽  
Vincent Monchiet
Keyword(s):  

Author(s):  
Jun Mei ◽  
Guancong Ma ◽  
Min Yang ◽  
Jason Yang ◽  
Ping Sheng

2007 ◽  
Vol 394 (2) ◽  
pp. 256-261 ◽  
Author(s):  
Ping Sheng ◽  
Jun Mei ◽  
Zhengyou Liu ◽  
Weijia Wen

2016 ◽  
Vol 06 (04) ◽  
pp. 83-90
Author(s):  
广浩 王

2012 ◽  
Vol 407 (20) ◽  
pp. 4093-4096 ◽  
Author(s):  
Ying Wu ◽  
Jun Mei ◽  
Ping Sheng

2010 ◽  
Vol 128 (2) ◽  
pp. 571-577 ◽  
Author(s):  
P. A. Martin ◽  
A. Maurel ◽  
W. J. Parnell

2007 ◽  
Vol 76 (13) ◽  
Author(s):  
Jun Mei ◽  
Zhengyou Liu ◽  
Weijia Wen ◽  
Ping Sheng

Author(s):  
M. K. Lamvik ◽  
A. V. Crewe

If a molecule or atom of material has molecular weight A, the number density of such units is given by n=Nρ/A, where N is Avogadro's number and ρ is the mass density of the material. The amount of scattering from each unit can be written by assigning an imaginary cross-sectional area σ to each unit. If the current I0 is incident on a thin slice of material of thickness z and the current I remains unscattered, then the scattering cross-section σ is defined by I=IOnσz. For a specimen that is not thin, the definition must be applied to each imaginary thin slice and the result I/I0 =exp(-nσz) is obtained by integrating over the whole thickness. It is useful to separate the variable mass-thickness w=ρz from the other factors to yield I/I0 =exp(-sw), where s=Nσ/A is the scattering cross-section per unit mass.


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