Issue 15
D. Kytyr e ut the intern absorbed. T elationship b
t alii, Frattura e al structure he X-rays th etween input
d Integrità Strut . According at pass thro and output
turale, 15 (201 to the dens ugh are then intensity of m
1) 5-13; DOI: 10 ity and com captured an onochroma
.3221/IGF-ESIS.
15.01
µC spe out by
T provides cimen a frac put emission Beer-Lamber
detailed info tion of the X intensity I o t law:
rmation abo -ray beam is n detector. R
position of d represented tic X-ray is gi
the by ven
I e I
( ) E d
(4)
0
wh line
value of inpu n coefficient 3 4 Z ensity of abs lity is mainly er and the a surements ha ity reduction ound and be rams (3D ra econstructio
the specimen
ere I 0 is the ar attenuatio ere ρ is the d iograph qua source pow ibration mea inhomogene iation backgr rected radiog ect. For the r
t emission e :
mitted by th
e X-ray sour
ce, d is the t
hickness of
and µ(E) is
the
(5)
orbent mater given by the cquisition tim ve been perf across the am hardenin diation distr n Filtered Ba
ial, Z materia number of e. With dec ormed for th chip, dark cu g correction ibution in th ckprojection
l proton num photons con reasing num e noise reduc rrent correc to get absorb e 2D plane d (FBP) was u
ber and λ X tributing to t ber of photo tion. Flat fie tion (scannin ing characte etector) wer sed.
rays wavelen he image. Th ns the prop ld correction g with disco ristics [9, 10] e used for r
gth. is number is ortion of no (scanning w nnected sour , were perfor econstruction
wh Rad the Cal for rad cor obj
proportiona ise is increas ithout specim ce) to avoid med. The se of the scan
l to ing. en) the t of ned
Figure 9 : M
icrotomograp
hy device; pel
vic bone samp
le on the left,
X-ray source
on the right.
Figure 1 T imaging w libraries. Th
0 : Reconstruc ere visualiz e bone-ceme
ted acetabulum ed using µC nt interface b
from differe Tvis&model efore cyclic
nt views. ler software loading is sh
Pro Vis
jections obt ualization To
ained by µC olkit (VTK)
[12] based own in Fig. 1
on open sou 1a, the dama
rce ged
11
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