Mechanical properties and cytocompatibility of oxygen-modified β-type Ti–Cr alloys for spinal fixation devices

2015 ◽  
Vol 12 ◽  
pp. 352-361 ◽  
Author(s):  
Huihong Liu ◽  
Mitsuo Niinomi ◽  
Masaaki Nakai ◽  
Ken Cho ◽  
Kengo Narita ◽  
...  
1993 ◽  
Vol 115 (1) ◽  
pp. 43-46 ◽  
Author(s):  
J. J. Crisco

Range of motion (ROM), the displacement between two limits, is one of the most common parameters used to describe joint kinematics. The ROM is a one-dimensional parameter, although the motion at many normal and pathological joints is three-dimensional. Certainly, the ROM yields vital information, but an overall measure of the three-dimensional mobility at a joint may also be useful. The volume of motion (VOM) is such a measure. The translational VOM is the volume defined by all possible ROMs of a point on a rigid body. The rotational VOM, although its interpretation is not as tangible as the translational VOM, is a measure of the three-dimensional rotational mobility of a rigid body. The magnitude of the VOM is proportional to mobility; the VOM is a scaler, which does not contain any directional information. Experimental determination of the VOM is not practical since it would require applying loads in an infinite number of directions. The mathematical derivation given here allows the VOM to be calculated, with the assumption of conservative elasticity, from the resultant displacements of three distinct load vectors of equal magnitude. An example of the VOM is presented in the comparison of the biomechanical stabilizing potential of various spinal fixation devices.


1996 ◽  
Vol 9 (3) ◽  
pp. 234???240 ◽  
Author(s):  
Antonius Rohlmann ◽  
Jorge Calisse ◽  
Georg Bergmann ◽  
Jens Radvan ◽  
Heinz-Michael Mayer

2001 ◽  
Vol IV.01.1 (0) ◽  
pp. 73-74
Author(s):  
Hiroki KAWASHIMA ◽  
Ko TAKANO ◽  
Kazuhiro HASEGAWA ◽  
Toshiaki HARA

1992 ◽  
Vol &NA; (284) ◽  
pp. 267???272 ◽  
Author(s):  
GORDON RUSSELL ◽  
GUY LAVOIE ◽  
ROBERT EVENSON ◽  
MARC MOREAU ◽  
DAVID BUDNEY ◽  
...  

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