Biomedical Engineering Reference
In-Depth Information
þ1
R
nV;
ð j
g
ice
50%;
g
water
10%
dV
0
PIIF
det ect
ðÞ¼
;
ð
17
Þ
N
tot
where g
water
ðÞ¼
V
ice
ðÞþ
V
water
ðÞ
V
ðÞ
is the fraction of water (solid plus liquid) inside any
single size class of the cell population. This way, iced-up cells are assumed to be
experimentally detectable by human eye looking at a microscope if the ice volume
fraction reaches the value of 0.5 (i.e. g
ice
C 0.5), whilst a relatively small content
of intra-cellular liquid water equal to 10% vol. is maintained (i.e. g
water
C 0.1).
Accordingly, the PIIF
detect
is evaluated at each temperature level as the fraction of
frozen cells at that temperature containing a minimum amount of water (thresh-
old). The choice of a specific threshold value for g
water
in order to detect ice
formation is quite reasonable. Indeed, the volumetric content of total water
(V
water
? V
ice
) inside the cells may be relatively small with respect to the inactive
volume V
b
and/or CPA volume V
CPA
in Eq.
1
. Therefore, ice formation may not be
experimentally detectable through the darkening/flashing of the cell commonly
used in cryomicroscopy, even if the liquid water contained in the cell is completely
turned into ice (i.e. g
ice
? 1 and V
water
? 0). On the basis of the chosen
thresholds for g
ice
and g
water
, in general the size distribution of the cell population
may be divided in three adjacent portions, for which different fates are assumed:
unfrozen cells characterised by g
ice
\ 0.5; iced-up cells with a small, innocuous
amount of water when g
ice
C 0.5 and g
water
\ 0.1; iced-up cells with a large, lethal
amount of water when g
ice
C 0.5 and g
water
C 0.1.
Alternatively, as very recently proposed in the literature [
37
], IIF may
be measured by means of a high-speed (8000 fps) video cryomicroscopy system.
This way, cells at the initial stage of ice formation (before flashing takes place)
may be numbered and a cumulative incidence of initial IIF (PIIF
init
) may be
experimentally determined. This new cumulative fraction of cells with an initial
ice formation (i.e. when g
ice
becomes greater than zero, g
ice
[ 0) is defined as:
þ1
R
nV;
ð j
g
ice
[ 0
dV
N
tot
0
PIIF
init
ðÞ¼
ð
18
Þ
3 Results and Discussion
3.1 Experimental Validation of the Model
The most relevant aspect of the mathematical modelling of cryopreservation based
on PBM is that the different IIF temperatures experimentally evidenced for a pool
of a given cell lineage is not ascribed to statistical variations but is explained
through a deterministic criterion: the size distribution of the cell population.
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