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Embryonic Stem (ES) cells are cell lines derived directly from the pre-implantation embryo. The generation of pure populations of neural progenitors from ES cells and their further differentiation into neurons, astrocytes and oligodendrocytes allows the potential use of these cells for the cure of neurodegenerative diseases and for neural drugs testing. An integrated device based on magnetophoresis, including microfluidic channels and incorporated high magnetic field gradients, was used to control the motion of cells, labeled with magnetic particles (MPs), through a biochip. This will result in a device capable of high-throughput separation at low cost. The separator was fabricated in polydimethylsiloxane (PDMS) comprising an inlet channel for cells 200 μm wide and inlet channel for buffer solution 700 μm wide. This device allows high separation efficiency of MP’s even when using inlet laminar fluid velocities up to 30 mm/s, by using a 15 mm wide and 60 μm thick separation chamber. The permanent magnet used was the W-12-Nfrom Supermagnete® made from an alloy of neodymium, iron and boron (Nd2Fe14B).In this work, the magnetophoretic device has been used for depletion of tumorogenic pluripotent stem cells from 46C mouse ES cell cultures by the specific recognition and labeling of the stage specific embryonic antigen 1 (SSEA-1). Purity degrees ranging from 95% to 99% were obtained and determined by flow cytometry analysis. These results raise the possibility of using this micro-device for the purification of human neural progenitor cultures from tumurogenic pluripotent stem cells.
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1
Magnetic Separation of Undifferentiated Mouse Embryonic Stem (ES) Cells from Neural Progenitor Cultures using a microfluidic
device.
Sousa, A.F.1,2,3, Diogo, M.M.2,3, Freitas, P.P1,3. 1INESC-MN, 2BERG-IBB, 3Instituto Superior Técnico
ABSTRACT
Embryonic Stem (ES) cells are cell lines derived directly from the pre-implantation embryo. The generation of pure populations of neural
progenitors from ES cells and their further differentiation into neurons, astrocytes and oligodendrocytes allows the potential use of these
cells for the cure of neurodegenerative diseases and for neural drugs testing. An integrated device based on magnetophoresis, including
microfluidic channels and incorporated high magnetic field gradients, was used to control the motion of cells, labeled with magnetic
particles (MPs), through a biochip. This will result in a device capable of high-throughput separation at low cost. The separator was
fabricated in polydimethylsiloxane (PDMS) comprising an inlet channel for cells 200 µm wide and inlet channel for buffer solution 700 µm
wide. This device allows high separation efficiency of MP’s even when using inlet laminar fluid velocities up to 30 mm/s, by using a 15 mm
wide and 60 µm thick separation chamber. The permanent magnet used was the W-12-Nfrom Supermagnete® made from an alloy of
neodymium, iron and boron (Nd2Fe14B).In this work, the magnetophoretic device has been used for depletion of tumorogenic pluripotent
stem cells from 46C mouse ES cell cultures by the specific recognition and labeling of the stage specific embryonic antigen 1 (SSEA-1).
Purity degrees ranging from 95% to 99% were obtained and determined by flow cytometry analysis. These results raise the possibility of
using this micro-device for the purification of human neural progenitor cultures from tumurogenic pluripotent stem cells.
Key words: Magnetophoresis, Magnetization, Microfluids, ES cells, Flow Cytometry, SSEA-1.
1. INTRODUCTION
he miniaturization of analytical and practical
techniques has become today a leading area of
investigation [1]. This trend encloses various fields
since many laboratories are interested in creating
novel microfabricated structures. This interest is
driven by the need to reduce costs by reducing
consumption of expensive reagents and by the high
throughput analysis that can be achieved.
Generally, microfluidics refers to devices or flow
configurations that have the smallest design feature
on the scale of a micron or smaller. Frequently, this
means rectangular channels with cross-sectional
dimensions on the order of tens or hundreds of
microns [2]. Besides the traditional advantages
conferred by the miniaturization described above,
the understanding of the microscale phenomena,
can be used to perform techniques and
experiments not possible on the macroscale,
allowing new functionality and experimental
paradigms [3]. Some examples of devices
considered microfluidic are gene chips, chip based
capillary electrophoresis and magnetophoresis cell
sorters [4-6]. The latter is the main concern of this
paper.
Flow (Q) is the quantity of material passing a given
area in a unit period time. Regardless of the scale
(macroscopic or microscopic) working with, a fluid
flow is said to be laminar whenever the viscous
forces dominate inertia [7]. The laminar flow
regime is characterized by high moment diffusion
and low momentum convection. For pipe flow, the
critical Reynolds number above which turbulence
may exist is about 2000 [8]. Such flow regimes are
important for the purpose of this work since a
controlled environment with defined microfluidic
fluid flows is required, as explained next.
T
2
1.1. MAGNETOPHORESIS
Free-flow Magnetophoresis is a method that allows
the separation of magnetic particles (MPs) in
continuous flow. It consists in a microfluidic device
with a separation chamber in which laminar flow is
generated in the x-direction. Perpendicularly to the
laminar flow, that is in the y-direction a magnetic
field gradient is applied (figure, 2). By doing so,
superparamagnetic particles usually composed by
iron oxide material are deflected from their
trajectory. Magnetophoresis can be used to control
the motion of labeled cells with MP’s [9]. This is
obtained by labeling the cells with specific
antibodies that are previously immobilized in
magnetic particles with different sizes, and so
different magnetic momentum – this allows
for immunomagnetic separation of different cells in
an heterogeneous population [10]
Magnetophoresis in lab-on-a-chip devices is
currently undergoing a rapid development, being a
strong tool for biological research. Most of the
biological samples under study are non-magnetic
and are neither affected nor destroyed by the
presence of a weak magnetic field gradient.
Labeling those species with MP’s provides a
versatile physical handle for manipulation of
biological samples.
Superparamagnetic particles are available with
carboxyl groups or amino groups on their surface.
Biomolecules such as DNA strands or antibodies can
then easily be attached to the particle surface [11].
When coated with, for example, an antibody, the
particles can attach themselves to particular
targeted cells (figure, 3).
Depending on their magnetic susceptibility
magnetic particles are deflected from the path, in
the presence of a permanent magnet. Non
susceptible cells keep their trajectory. The
deflection of the magnetic particles can be
described as the sum of two vectorial components.
The magnetically induced flow, umag, is the ratio of
the magnetic force, Fmag (in N), exerted on the
particle by the magnetic field to the viscous drag
force:
where η is the viscosity of the medium (in kg/m/s)
Cell
Fig. 3 - Diagram of an immunomagnetically labeled cell. Note that the monoclonal antibodies are binding only to the specifically targeted cell surface molecules (antigens).
Fig. 2 – Concept of free-flow magnetophoresis. A heterogeneous population of non-labbeled and labbeled cells with MP are pumped into a laminar flow chamber; a magnetic field is applied perpendicular to the direction of flow. Cells deviate from the direction of laminar flow according to their magnetic susceptibility and are thus separated from each other and from nonmagnetic material.
Fig. 1 - Fluid flowing through microfluidic channels. a) Low velocity profile induces laminar fluid flow even in a presence of an obstacle. b) As the velocity increases, and so the Reynolds number, the flow becomes turbulent and the creeping fluid flow regime is achieved.
3
a)
b) Fig. 4 – Sparation system using a permanent magnet of 500 mT.
There are two inlets converging to a PDMS separation chamber where cells labeled with MPs from inlet 1 are deflected by magnetic attraction into outlet 2. a) top view of the microfluidic device in the presence of the permanent magnet. b) Perspective view of the structure comparing the dimension of the permanent magnet with the PDMS channels.
and r the particle radius (in m). The magnetic force,
is proportional to the magnetic flux density, B (in
tesla) and the gradient of the magnetic field,
(in tesla m-1
) of the externally applied field. The
magnetic force is proportional to the particle
volume Vp (m3) and the difference in magnetically
susceptibility between the particle and the fluid, ∆χ
(dimensionless):
where μ0 is the permeability of a vacuum (in H m-1).
When inserting eq. 3 into eq. 2, it can be seen that,
for a given magnetic field and a given viscosity, the
magnetic velocity, umag, is dependent on the size
and the magnetic characteristics of the particle. It is
proportional to the square of the particle radius and
to the magnetic susceptibility of the particle:
,
So, when having a heterogeneous culture of cells on
which some are labeled with MPs, these will be
defected from their initial trajectory and will then
be separated from the rest of the culture, allowing
the purification of a given sample.
2. MATERIALS AND METHODS
utoCad, a software that allows the design of
microfluidic structures, was used in this work.
Microfluidic structure was designed in order to have
a large separation chamber with enough height so
cells could pass freely without colliding with the
Polydimethylsiloxane (PDMS) walls. The chamber
was also designed to have two inlets; one for the
solution containing the cells and the other one to a
buffer solution of PBS 0,1 M, pH 7.3. After several
designs (see annex I), a final microfluidic structure
was designed with a separation chamber 2mm
wide, a inlet for the cell solution 200μm wide and a
buffer solution inlet channel 700μm wide. The
whole structure had 60μm thickness and it is
represented in figure 4. Such a big microfluidic
structure represents several advantages as:
- Lower cell aggregation, allowing much more
efficient separation;
- By using a separation chamber with 60 μm
thickness the cells will more probably be located in
the central part of the channel and won’t get so
easily stuck in the walls lowering the percentage of
cell loss.
- Higher flow rates at the inlets, while maintaining
low velocities in the separation chamber, around
4mm/s. This way, the magnetic field gradient used
will be sufficient to deviate the magnetically
susceptible cells in order to be collected in the
outlet 2. This is an important characteristic of such a
device, since it may be necessary to process
solutions of cells in the range of milliliters.
2.1. THE PROCESS FOR FABRICATION OT THE
MICROFLUIDIC DEVICE
The microfluidic structure was made of PDMS. This
polymeric organosilicon compound presents many
A
4
Fig. 5 – Schematic representation of the entire PDMS structure fabrication process.
advantages, namely the easiness of fabrication,
good physical properties and the low price of this
material [12]. PDMS is optically clear, non-toxic,
non-flammable and inert material, and it is known
for its unusual rheological (or flow) properties.
There are many methods for the fabrication of
PDMS based microfluidic devices. The method used
during this work is the most commonly used and is
schematically represented in figure 5. All this
process is presumed to be done in a clean
environment.
2.2. CELL LINE
For this work, the 46C mouse ES cell line [13],
established at the laboratory of Professor Austin
Smith, Wellcome Trust Centre for Stem Cell
Research, University of Cambridge, England, UK,
was used as the model cells. This cell line can be
induced to undergo neural commitment in serum
free conditions [14]. 46C mouse ES cells were kept
cryopreserved in liquid nitrogen until further use.
2.3. SSEA-1 EXPRESSION DETERMINATION BY
FLOW CYTOMETRY
After in vitro expansion of 46C ES cells, the
percentage of SSEA-1+ cells was evaluated by flow
cytometry. The same procedure was used after cell
separation using the different procedures (batch
and microfluidic-based). For that purpose, cells
were collected and ressuspended in 100 μL of PBS.
The antibody was then added to the cell suspension
(IgM, PE mouse/human monoclonal conjugated
anti-SSEA1 (BD), 1:10 dilution in PBS), followed by
incubation for 15 min at room temperature in the
dark. Negative Isotype controls (γ1- PE) were used
in every experiment in order to exclude non-specific
binding of the antibody to the cells surface.
2.4. BSA BLOCKING STEP AND CALCULATION
OF NON-SPECIFIC ADSORPTION OF CELLS TO
MP’S
A first experiment was designed in order to
evaluate the degree of non-specific adsorption (non
antibody-based) of cells to these MP’ and in order
to test the feasibility of using an incubation with
bovine serum albumin (BSA) to block this
adsorption. For that purpose, approximately 7×108
MP’s were added to a 100 µL solution of PBS 0,1M
pH 7.2 and incubated with 5×105 46C ES cells
containing 76,9% of SSEA-1+ cells. The mixture
containing the cells and MP’s was then left to
incubate for one hour at room temperature with
constant mixing. Three different studies were
performed in parallel with increasing BSA
concentrations (%w/v) of 1%, 2% and 5%. The cell–
MP complex pellet was then isolated from the
supernatant by placing the eppendorfs near a
magnet in a magnetic particle separator Magna-
SepTM
. The remaining pellet of cells-MPs complex
was ressuspended in 100µL of PBS 0,1M. The
number of cells in each one of the phases
(supernatant and pellet) was then counted using a
5
Fig. 6 - Experimental setup for the separation in microfluidic device. a) Cubic Permanent Magnet. b) Inlet 2 for buffer solution c) Inlet 1 for cells-MPs complex containing solution d) microfluidic separation chamber e) glass surface f) fluorescence microscope ocular g) outlet 2 for SSEA-1+ cells h) outlet 1 for SSEA-1- cells. Note that the entire structure is mounted in an inverted position due to technical properties of the microscope.
hemocytometer. The percentage of cells that were
adsorbed to the MP’s by non-specific adsorption
(NSA) (non-based in antibody interaction) was
calculated as shown below:
ells dsorbed of cells pellet
of total cells pellet supernatant)
2.6. SEPARATION OF CELLS USING IGM,
BIOTIN ANTI-MOUSE/HUMAN SSEA-1
ANTIBODY IN BATCH PROCEDURE
The main purpose was to place a magnet near the
eppendorfs and once the magnetically susceptible
cells were attracted to the eppendorfs walls, the
supernatant was decanted to new eppendorfs and
the number of cells were counted again. In this
case, 2 µL of 3 nm MP’s were added to a 100µL
solution of PBS 0,1 M pH 7.2, containing final
antibody concentrations of 0,125µg/mL 0,25µg/mL
and 0,375µg/mL in different eppendorfs. A negative
control run with no antibody added was also
performed. The number of cells in each eppendorf
varied between 1,4×105 - 3,5×10
5 since it was not
possible to collect the same number of cells from
the initial cell suspension.
2.7. SEPARATION OF CELLS USING
MICROFLUIDIC DEVICE
The fabricated microfluidic device was used for the
negative separation of SSEA-1+ cells from of a
heterogeneous mixture of 46C ES cells containing
both SSEA-1+ and SSEA-1
- cells. For that purpose,
2µL of 3 nm MP’s particles were added to 3 µL
of PBS 0,1M pH 7.2, with antibody at final
concentrations of 0,250µg/mL 0,375µg/mL and
0,625µg/mL in different eppendorfs.
A negative control run with no antibody was also
performed. All the mixtures were left to incubate
for one hour. The 300µL solution was then
ressuspended in the same volume of BSA blocking
solution 2%(w/v) and left to incubate for one hour
at room temperature. To each eppendorf, a
heterogeneous mixture of 3×105 46C ES cells
containing both SSEA-1+ and SSEA-1
-cells was added
and again left for incubation for one hour at room
temperature. The total solution in each eppendorf
was ressuspended in 300μL of PBS 0,1 M, ph 7.3
solution and fed into a 1mL syringe located in the
NE-1000 Programmable Syringe Pump from NAI –
Wis Biomed with a constant fluid flow of 20μL/min
in inlet 1. The buffer solution was injected into inlet
2 with a constant fluid flow of 100μL/min. Each run
was performed during 15min approximately. The
outlets fluid flows were finally collected in
eppendorfs connected to the separation chamber
by polymer tubes. In order to differentiate fluid
flows through inlet 1 and 2 during the separation,
FITC diluted 1:1000 was added to the buffer
solution and visualized under a fluorescence
microscope (figure, 6). Prior to the injection of the
cells, the entire microfluidic device as well a s all the
accessories such as syringes, microfluidic tubes and
eppendorfs that would contact with the cells-MP’s
complex were coated with a blocking solution
containing 2% (w/v) BSA. The percentage of SSEA-1+
negatively selected cells in the microfluidic device is
calculated as:
6
Separation cells in 2
cells total
Being Ncells total, the sum of the number of cells
counted in outlet 1 and outlet 2.
3. RESULTS AND DISCUSSION
3.1. SEPARATION OF CELLS USING IGM,
BIOTIN ANTI-MOUSE/HUMAN SSEA-1
ANTIBODY IN BATCH PROCEDURE
After the results presented in previous works (data
not shown) several considerations were taken in
account and it was decided to perform the batch
procedure using an antibody already biotinylated –
IgM biotin anti-mouse/human SSEA-1. In this case,
the biotin group is labeled to the antibody in a
different area than the antigen binding-site (Fab
Region), this way the specific recognition of the
SSEA-1+ cells by the antibody is not affected. Since
this antibody is concentrated, each run will have a
low cost because a low monoclonal antibody
volume is used. In order to perform this
experiment, 3×105 46C ES cells containing 53,4% of
SSEA-1+ cells were used.
As can be observed in figure 7, an increasing
percentage of captured cells were obtained when
increasing the concentration of biotinylated
antibody. The maximum percentage of captured
cells (91,1%) was obtained when using a
concentration of 0,375ug/mL of the biotinylated
antibody. However, from the control run (no
antibody used) results it can be concluded that a
high percentage of cells (42,4%) was captured due
to non-specific adsorption.
In order to evaluate the efficiency of this batch
system concerning the capture of SSEA-1+ cells, the
percentage of SSEA-1+ cells, in the supernatant was
determined by flow cytometry analysis (figure, 8).
Only after this analysis it will be possible to evaluate
if the antibody-MP’s complex is efficiently binding
to the specif ic antigen in the cells surface. The first
plot [figure 8, a)] represents the negative control of
the flow cytometry analysis by using an IgG γ1
antibody with a linked fluorophore – PE – but
without a specific affinity for the ES cells.
This negative control is used namely to account for
the non-specific adsorption of the fluorophore to
the ES cells.
By making this negative control run it is possible to
define a peak with fluorescence between 100 and
101 of the PE fluorescence (FL2-H intensity scale).
This way, only ES cells with fluorescence intensity
(FL2-H) higher than 101 will be considered to
express the SSEA-1 antigen. After performing the
negative control run, the percentage of SSEA-1+
cells was determined in 46C ES cells feed to the
batch system, before purification, using the SSEA1
antimouse/human IgM PE antibody [figure 8, b)].
Next, in figures 8, c), d), e) and f) it is possible to
observe the flow cytometry analysis of the
supernatants after the batch procedure when
antibody concentrations of 0 μg/mL, 0,25 μg/mL,
0,25 μg/mL, 0,375 μg/mL were used. As can be
observed in figure 8, c), when no antibody was used
in the batch separation procedure, a percentage of
36,4% of SSEA-1+ cells was obtained in the
supernatant. Looking at the separation value of
42,4% [figure 7, Control run with no antibody used]
75,5
90,7 91,1
42,4
30
40
50
60
70
80
90
100
, 25μg/mL ,25μg/mL ,375μg/mL control
Sep
arat
ion
Pe
rce
nta
ge
Antibody concentration
Capture of Cells
Fig. 7 - Results for the capture percentage of 46C ES cells labeled with a specific biotinylated antibody (in different concentrations) immobilized into MPs and using the batch procedure.
7
6,1%
53,4%
36,4%
15,6%
4,1%
1,2%
Fig. 8 – Flow cytometry analysis of SSEA-1 positive 46C ES cells when using the batch procedure: a) Flow cytometry negative control run, b) %SSEA-1 positive cells before separation; c) Control run, where no antibody was used for the selective separation of cells. %SSEA-1 positive cells in the supernatant after the batch procedure while using d) , 25μg/mL, e) , 25μg/mL and f) ,375μg/mL of SSEA1 specific antibody.
a)
b)
c)
d)
f)
e)
it is possible to say that some of the non-specific
interaction of the antibody-MPs complex with the
cells is promoting depletion of SSEA-1+ cells from
the 46C ES cells heterogeneous population.
Next, after the separation protocol using 0,125μ/mL
of antibody, the percentage of 46C ES cells
expressing the SSEA-1 antigen was also determined
by flow cytometry. The M region denotes the
percentage of ES cells expressing SSEA-1 antigen,
and for this run that percentage decreased to 15,6%
[figure 8, d)] leading to conclude that the separation
protocol while using specific antibodies was
purifying the initial solution of 46C ES cells. Once
increasing the antibody concentration to 0,250
μg/mL and 0,375 μg/mL, the percentage of cells
expressing the SSEA-1 antigen in the supernatant
decreased to 4,1% and 1,2% respectively [figure 8,
e) and f)]. After performing flow cytometry analysis
it was possible to calculate the purity degree of the
supernatant after the batch procedure (Table 1) is:
Purity Degree = 100% - % SSEA-1 positive cells in the
supernatant
It is important to notice that although the obtained
purity degree is high (table 1), the loss of cells is
also high (see figure 9). Since the percentage of cells
expressing the SSEA-1 antigen before the batch
separation is 53,4% the number of cells that are
attracted to the magnet in the batch procedure
should not overcome that value, otherwise this
separation is not only based on specific cell-
antibody interactions. Since the separation
percentages are higher than that value (as can be
seen in figure 7) this means that cells are being
attracted to the magnet placed near the eppendorf
by non-specific interactions. The percentages of cell
loss (SSEA-1- cells non-specifically attracted to the
magnet) have values around 60-70% (figure 9). In
this figure the white areas should maintain the
same values after batch separation since they
represent the number of SSEA-1- cells before
(columns on the left of each cluster) and after
(columns on the right of each cluster) the
separation in batch procedure.
Thus, the first conclusion that can be taken from
this study is that the batch procedure for the
separation of SSEA-1+ 46C ES cells is promoting high
levels of non-specific interactions either between
cells and between cells and the eppendorfs, during
8
Separation of cells in outlet 2 cells in 2
cells total
the time the solution remains in batch. Perhaps the
formation of aggregates between the antibody-MP-
cell is contributing for the non-specific adsorption
of cells. However, more studies about this aspect
would be needed to understand this phenomena.
Taking these results into consideration, a different
method for the depletion of SSEA-1+ cells from 46C
ES cells should be attempted.
3.2. SEPARATION OF SSEA-1+ 46C ES
CELLS USING THE MICROFLUIDIC DEVICE
After performing SSEA-1+ cell separation using the
batch procedure, the protocol was adapted for the
separation in the microfluidic device. Looking at the
microfabricated structure, there are two inlets, one
for the solution containing the cells (inlet1) and the
other for the buffer solution of PBS 0,1M pH 7.3.
The presence of the permanent magnet will induce
cells labeled with MPs to deviate from their path to
outlet 2, while non-susceptible cells will continue
along their path to outlet 1. Three different
concentrations of antibody were again evaluated,
and a control run where no antibody was used was
also performed. The separation percentage is given
by a similar formula to that presented before:
Where Ncells total, is the total number of cells
counted in outlet 1 and outlet 2. Cells that went
through outlet 2 are magnetically susceptible and
presumed to be labeled with the 300nm particles
from Ademtech®. The percentage of separation
using the microfluidic procedure is lower than that
obtained in batch procedure. One important result
is the one of the control run, where no antibody
was used.
Indeed, in this case, only 10,3% of the 46C ES cells
were attracted to O2 via non-specific interactions
(figure, 10). This value is much lower than the
obtained in the batch procedure which presents a
major advantage of the microfluidic
procedure.Indeed, in this case, all the cells in the
separation device are in constant motion due to the
fluid flow, decreasing the amount of interaction
between all the species and preventing cells from
forming aggregates. In fact, cell aggregates are
more difficult to separate based on the expression
of surface antigens. The cells labeled with MPs are
in constant movement, while in the separation
chamber they get subjected to the magnetic field
generated by the permanent magnet. This exposure
to the magnetic field occurs for only a few seconds
Table 1 - Resume table for the purity degree of each solution after the separation procedure.
Fig. 9 - Four different clusters of results, each one representing the use of a different antibody concentration during batch separation. In each cluster, the left column represents the total number of cells prior to the separation, and the right column represents the total number of cells in the supernatant after the separation. In blue is the number of ES cells expressing the SSEA-1 antigen.
39,4 42,0 42,9
10,3
0
10
20
30
40
50
,25μg/mL ,375μg/mL ,625μg/mL control
Pe
rce
nta
ge o
f Se
par
aio
n
Antibody concentration
Cell separation Outlet 2
Fig. 10 – Results for the capture percentage of cells labeled with specific antibody biotinylated (in different concentrations) immobilized into MPs in the microfluidic structure.
9
Table 2 - Resume table for the purity degree of each 46C ES cells solution after the separation procedure in the microfluidic structure.
Fig. 12 - Four different clusters of results, each one representing the use of a different antibody concentration. In each cluster, the left column represents the total number of cells prior to the separation, and the right column represents the total number of cells out of outlet 1 after the separation. In blue is the number of ES cells expressing the SSEA-1 antigen.
≈4 sec, as they travel at ≈4mm/s and the
separation chamber is 15mm wide), and that is
sufficient to alter the cells trajectory according to
results shown in figure 10.
In these experiments, the microfluidic system was
injected with a cell suspension containing 42,4% of
cells expressing the SSEA-1 antigen [figure 11, b)].
However, as can be seen in figure 11, c) and in
opposition to the batch procedure [fig ure 7, c)], the
separation of cells by non-specific adsorption in this
dynamic protocol is negligible, which means that a
high specificity is achieved in cell binding to MP’s-
antibody complex. Besides that, the M region on
the graphics decreases as the antibody
concentration gets higher [figure 11, d) e) and f)],
denoting again that the antibody is recognizing the
cells to be deviated from their path with the use of
the permanent magnet. By other words, most of
the SSEA-1+ ES cells (and not other cells) which we
want to deplete from the initial cell solution are
exiting the structure through outlet 2, resulting in a
negative selection separation procedure in a novel
working microfluidic structure with low cost per
run. Another aspect is the purity degree that was
obtained using this microfluidic procedure. The
results obtained are presented in table 2. The purity
degree is not as high as in the batch procedure,
however it is highly comparable, once standard
errors are considered. The advantages of using a
microfluidic device, is the ease and low cost of the
procedure. Besides, in this case, each solution of
cells can be injected more than once into the
separation device. In a better look, cell loss values
obtained was around 1%-5% (figure, 12), better
than in batch procedure. The results achieved here
could potentially be improved by passing the
42,4%
44,6%
10,3%
5%
3,7%
1,25%
Fig. 11 – Flow cytometry analysis of SSEA-1 positive 46C ES cells when using the microfluidic separation device: a) Flow cytometry negative control run, b) %SSEA-1 positive cells before separation; c) Control run, where no antibody was used for the selective separation of cells. %SSEA-1 positive cells in the supernatant after the batch procedure while using d) , 25μg/mL, e) , 25μg/mL and f) ,375μg/mL of SSE specific antibody.
a)
b)
c)
d)
f)
e)
10
solution of cells several times in the microfluidic
device since this would enhance the final purity
degree [16]. However, in this case, clearance rates
for undifferentiated ES cells would decrease with
decreasing amounts of undifferentiated SSEA-1+ ES
cells [16].
4. CONCLUSIONS AND FUTURE WORK
Before using the microfluidic device for the
magnetophoresis based separation all the biological
protocols needed optimization. The immobilization
of the 300nm particles from Ademtech® to the
specific antibodies used, needed to be engineered
from the beginning with constant improvements
and changes. The final protocols were adequate for
the specific and correct labeling of SSEA-1+ cells.
The batch procedures performed lead ultimately to
good results for the purification of a heterogeneous
population of cells. Final purity degrees obtained in
batch separation ranged from 96,9% to 99,5% while
using well defined concentrations of IgM, Biotin anti
mouse/human SSEA1 antibody. However, the
values for the cells loss percentage were also high
and observed between 60% and 70%.
As for the magnetophoresis in a dynamic
microfluidic device the use of a permanent magnet,
the W-12-N: Cube 12mm from Supermagnete®
made from an alloy of neodymium, iron and boron
to form the Nd2Fe14B proved to be sufficient for the
deviation of labeled SSEA-1+ cells with 300nm
particles from Ademtech®. The final purification
degrees obtained in this procedure ranged from
92,3% to 98,5% in a single step run which in terms
of results is comparable to those obtained in the
batch procedure if laboratorial errors are taken in
account. As for the percentages of cells loss, while
using the microfluidic device, the values obtained
were at most, 5%. This characteristic leads to
conclude that this procedure of purification can be
repeated several times in order to obtain higher
final purity degrees. Each run can be performed in
less than 8 hours using a simple protocol.
The microfluidic device was used for the
purification of a population of mES cells from cells
expressing the SSEA-1 antigen, a marker for
pluripotent and tumorogenic cells. Such model can
be used as a proof of concept of this technology for
the direct application in the purification of a neural
progenitors population of cells from tumorogenic
cells. A high-throughput separation system with low
cost per run was developed in this MSc project.
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