Formation of Nanosize Apatite Crystals in Sediment for Containment and Stabilization of Contaminants

Author(s):  
Robert C. Moore ◽  
Jim Szecsody ◽  
Michael J. Truex ◽  
Katheryn B. Helean ◽  
Ranko Bontchev ◽  
...  
Keyword(s):  
1963 ◽  
Vol 101 (2) ◽  
pp. 215-224 ◽  
Author(s):  
W.F. Neuman ◽  
R. Bjornerstedt ◽  
B.J. Mulryan

2006 ◽  
Vol 41 (3) ◽  
pp. 268-275 ◽  
Author(s):  
S. N. Danilchenko ◽  
A. V. Koropov ◽  
I. Yu. Protsenko ◽  
B. Sulkio-Cleff ◽  
L. F. Sukhodub

2017 ◽  
Vol 26 (4) ◽  
pp. 399-404
Author(s):  
Hiroyuki Mishima ◽  
Mitsuo Kakei ◽  
Ichiro Sasagawa ◽  
Yasuo Miake
Keyword(s):  

1991 ◽  
Vol 71 (5) ◽  
pp. 943-945
Author(s):  
Kh. Murtazaev ◽  
V. P. Perelygin ◽  
R. I. Petrova ◽  
S. G. Stetsenko

1980 ◽  
Vol 13 (8) ◽  
pp. 725-729 ◽  
Author(s):  
G.E. Bacon ◽  
P.J. Bacon ◽  
R.K. Griffiths

Author(s):  
Justin M. Deuerling ◽  
Weimin Yue ◽  
Alejandro A. Espinoza ◽  
Ryan K. Roeder

The elastic constants of cortical bone are orthotropic or transversely isotropic depending on the anatomic origin of the tissue. Micromechanical models have been developed to predict anisotropic elastic properties from structural information. Many have utilized microstructural features such as osteons, cement lines and Haversian canals to model the tissue properties [1]. Others have utilized nanoscale features to model the mineralized collagen fibril [2]. Quantitative texture analysis using x-ray diffraction techniques has shown that elongated apatite crystals exhibit a preferred orientation in the longitudinal axis of the bone [3]. The orientation distribution of apatite crystals provides fundamental information influencing the anisotropy of the extracellular matrix (ECM) but has not been utilized in existing micromechanical models.


Bone ◽  
2020 ◽  
Vol 135 ◽  
pp. 115304 ◽  
Author(s):  
H.P. Schwarcz ◽  
D.M. Binkley ◽  
L. Luo ◽  
K. Grandfield

1974 ◽  
Vol 29 (6) ◽  
pp. 897-900 ◽  
Author(s):  
A. Lodding ◽  
J.-M. Gourgout ◽  
L. G. Petersson ◽  
G. Frostell

In studies of F concentrations in apatite crystals by means of secondary ion micro-analysis, it is found that even in a sample with a known and constant F/Ca ratio the recorded ratios of the F and Ca secondary ion currents can vary widely, depending on the experimental conditions of primary bombardment. An attempt has been to explain this behaviour and to devise a way to obtain quantitative atomic F to Ca ratios independent on measuring conditions. Simultaneous recording of the mass peaks of F+, Ca+ and another matrix ion (P+ or C++) appears to offer a solution of the reproducibility problem. This is demonstrated by ion probe measurements under varied conditions in three groups of materials where the F concentrations had previously been determined by macroscopic methods: apatite crystals with about 3% F, whale teeth of about 10-1 % F, and human enamel ob about 10-2 % F.


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