THE
JOURNAL
Copyright
OF
HI5TOCHEMISTRY
@ 1976 by The
AND
Society.
LASER
TECHNIQUE
FOR
of Pathology,
CELL
Squamous
cells
in fluid
Fluid
flow
utilization
systems
rapid
transport
recording wavelengths cellular nation phologic lation
of
Most
cell
cells. laminar into
through
sheath.
the
axial
beam
serves
to
air
may
and,
This
paper
nozzle
in some
cases,
The
cells
tation
in flow of
Several
sheath near the
case
for
spherical at spatial thelial present essing
light
images
field
is
scatter
cells,
because
a unique
This
of
challenge utilizing
cells
pass
work
was
cells
the
their
supported
on
pho-
flow.
(index
vented systems.
Conference Calif., 1975.
shuttered
The
beam
contrast
prove
thickness
‘ania-
variations) the
in cells. in
a
discipline used
filtering
in
operation.
The
a phase
shift.
the
optical
configuration.
continuous off’ and
on
spatially
a fluid-filled
265
Downloaded from jhc.sagepub.com at GEORGIAN COURT UNIV on March 18, 2015
from an argon ion fluorescence mealaser
beam
flow
by
by
as this
9% of its high con-
with
a strobed
is then
Fourier
known
technique
is derived used for cell
The
and through
along
illumination normally into
Nemarski.
is attenuated to thereby providing
1 depicts
surements.
the
to plane
images,
transmit-
implemented The
Figure Laser laser.
optical
to Bright
whereas
modulation
processing.
Epi-
from
flow
belongs
utilized
visualizing
thickness is
illumination amplitude,
excitation
a contract
and
is a Fourier
illumination.
laser
and
optical
trast
for
contrast
are specimens.
a cell.
visualizing
study
proc-
Presented at the Engineering Foundation on Automated Cytology, Pacific Grove,
in
biological
in
direct original
in automated
NO1CB33862. Slit-scan
orien-
representative
techniques
of
non-
measurements the cell size.
shape,
the
tech-
cell
TECHNIQUES
and
for
plane
the
flattened
by DB:
mea-
is certainly
slit-scan
through
National Cancer Institute, 2 Wheeless LL, Kay
affect
measurements fluorescence less than
for
in flow.
optical
cells
satisfactory
valuable Phase
cells and resolutions
systems
Should I
of the
This
technique
orientation
presents
microscopic
provide
tions
orientation
performed.
and
EXPERIMENTAL
measurement.
being
system
recording
gynecologic
assure
surement
forces
in a flow
coherent
tographs
ever,
greatly
the
a
cell
describes
solution. of
important,
on
orientation.
complex
orientation
for photographically
utiliza-
slit-measuring orientation
cell
less
to
slit-scan
is the
of
a
niques
contrast
may
is parallel
understanding
equally
phase
orientation
cell
solution
or visualizing
variations
Cell
The
measured
Control
an
tance
desired
the
One
to cell
recording
tube
of the
provide
requires
contributing
to
plane beam,
slit.
of the flow stream, forcing passage of’ the through the desired geometrical position the detector assembly. It does not. howthe
technique.
of
one
however,
8).
the
(2).
maintain
set
center cells within during
14642
intersects
from or,
into
York
three orthogonal to provide acceptable cell a
least
This
by a coaxial
laser
the
of the is af’f’ected.
of’
beams
The
specimen
plane
(5)
(7,
stream.
such
the
at
corre-
technique
flow
as it emerges
emerges
New
stroboscopic
that
slit
tion
cellular
enveloped
chamber2
stream
technique
flow
an
A focused
stream
a fluid-filled
as
specific cytoplasm)
the
are
permits
or
a sheath
assembly,
coaxial
and
with
within
FLOW’
Rochester,
a laser
contour
illumimor-
use
entering
allowing Detectors
(4. 6). Use of’ slit provides low resolution
position
in a nozzle
the
or more specific
nucleus
systems
control
for
optics,
on cells
(i.e.,
IN JR.
Center,
using
increased
at one on
fluorescence
structures
gaining
from cells information
information
L. WHEELESS, Medical
photographed
parameters.
fluorescence provide components techniques
are
STUDIES
dark field or phase contrast multiple images of a cell on a single permitted by the thickness of the cell stream. Cell orientation, are obtained from these photographs for evaluation of flow sys-
past
of cellular
LEON
AND
of Rochester
cytopathology
of’ cells
quantitation
the
are
in automated
B. KAY
flow
1. pp. 265-268, 1976 Printedin (‘.S..4.
PHOTOGRAPHY
ORIENTATION
University
technique provides either frame of film at resolutions velocity and acceleration tern performance.
24, No.
Inc.
STROBOSCOPIC
DAVID Department
Vol.
CYTOcHEMISTRY
Histochemical
source a chopper
computer filtered
chamber
is conwheel
control. and into
ficused a Fou-
266
KAY,
rier
plane
where
lenses
behind
a film
plane.
plane
exposure
a frame
the
the
after
of
laser
a single
cell
passes
shutter.
the
strobed
flow stream of’ the film.
surement
region
laser
flow
and
to
The
computer
the
scatter
for
through
the
the the
closes
as
ar’
of
time
the
an
paid
the
coaxial
an
exit
by
a quiescent
recording
A from
capillary.
This
interface
flow
chamber
gap
volume
strong
optical
thereby and
TO
THE
where
the
and
measurement
delay the
a
region exposure
may
is
short.
a
elimi-
accumulate
d
2, A-E
lO-jisec
gion the
axis
the
ing
the
delay
beam
at 2A
1. Optical
system
for
and
A is the
may be recontime for analysis
obtained
cells
flowing
at
chopped
to
tech-
10 cm/ produce
repetition
a superficial
The
edge cell
of the
Figure
always,
2E
squamous
noise and
photography.
Downloaded from jhc.sagepub.com at GEORGIAN COURT UNIV on March 18, 2015
a cell edgewise
is present shows
in Figure rotated
depicts
region
Coherent
cell
is partially
measurement
stroboscopic
the
a 2000-pulses/sec shows
the
of flow.
as
using
with gynecologic of superficial and
camera and Figure 2B shows an squamous cell. Figure 2C depicts flowing through the measurement reand
camera. ages,
laser
d2/ holo-
z
Fraunhofen
DISCUSSION
was
FLOW CHAMBER
FIG.
the
the
together.
laser
if’ the
a distance
diameter
AND
was
pulses
is curled
.
are
and
collimated light A photographic
described images are
laser
Figure
the
hack-
cell
squamous
The
into
large
Filters
orientation.
rate.
works spec-
cell
A
where
cell facing intermediate two cells
opening of
at
in-line
intermediate sec.
minimizing
technique concentrated
between
entrance
pattern
the
of
the flow chamber is by the cell then inter-
is an
Figure
TECHNIQUE
The previously described very well with a moderately
plane
this
nique previously specimens. The
is surrounded
of water, interfaces
(1).
cell is
to
three-dimen-
needed
preceding scattered
RESULTS
aberration.
shutter
of
modified
Fourier
the
cell
of
nozzle into pass through
region
lens Light
is
environment.
The
the
in
holograms
and
laser wavelength. The hologram structed and viewed at a later
inter-
in a fluid-filled
EXTENSIONS
ground
pass
then
imaging
wherein cells emerge from the flow gap measurement region and then
imen
to
builds
cells.
in-line
is
from
measure-
however, a signal levels
be easily
of focus
information
eliminated
Strong
if’ cell
depth
to shutter
the
of
may
imagscatter
exposure
feres with the unscattened forming an interference pattern.
situation.
stream
in an air is solved
system
sional
sense
and
used
enters
exposure
if large
cell the
is then
selection
system
alternate
for
generate
signal.
to optical
imaging
to
a cell
preferential
multiple
gram, was
when
An
one
No background
optical
cells
and aberrations of’ the laser beam for example. at the air-water hound-
attempted
nating
cell
in
provide
shutter.
with
problem
for
long.
converging removed.
of the
of’ measurement
9O
signal
on
region.
too
lasers,
to the images
a sense
receipt
required
attention
refractions will occur,
as
upon
region
laser
Careful faces
detector
delays,
at
scatter
laser
The
scatters both cell
other
The
result
illumi-
chamber
is
two
the images with this approach; problem may occur if the scatter
and begins a background A cell entering the mea-
of’ the
arrives
the
first
ment
the
light
and
the
to block
through
cell
employs
signal.
re-
chamber. The Upon opening
out of the illuminating beam plane to form the stroboscopic
signal.
a
approach
to
are
is used
the
light film
before
cell
a cell
shutter
region of’ the flow of’ events is as follows.
nates the exposure
the
plane (Figure 1). To prevent of’ more than one cell in
measurement sequence laser
Objective
image
images
film images
of film,
beam
occurs.
Fourier
ing
Multiple corded at overlapping the
filtering
the
WHEELESS
up
in as
2D about
traversto
the
the
im-
assorted
LASER
STROBOSCOPIC
267
PHOTOGRAPHY
E FIG.
fringe
on
traceable elements.
patterns
the
2.
optical
at the top of the images tion from the ends ofthe Resolution matel the
in
4
the
stroboscopic
to dust and The horizontal
images
is
x5
50-ji
low
Only
shape,
outline
fore.
should
difficulty
be
specimen and
gleaned
in obtaining images is
of a result
nuclear from rotated
of
applying
diffrac(approxi-
of gynecologic
sional
depth
aperture of the cells
position,
there-
easily
images.
The
cell
obtained
multiple
acceleration
away
from
the
cell
a
two-dimen-
be obtained
using
through
the
measurement
and
acceleration
a single
spacings
obtained
Downloaded from jhc.sagepub.com at GEORGIAN COURT UNIV on March 18, 2015
holoregion
may
photograph.
carry
the
since
the
Cell from
the
earlier.
velocity
is constant. be
a three-dimensional
discussed
information
images also
to
filtering operations are on cell orientation. High images wit h good
from
image
ion
may
may
rotation with
inf’ormat
in flow.
technique
technique
Cell along
cells
Fourier plane for the face three-dimensional
of field
graphic
depth.
the
imaging
cell. The best suited resolution
stream
morphologic
cells
photographs
scratches fringes
are caused by capillary tubes.
due to the low numerical objective used to image the
camera
laser
ji)
throughout
from
A-E,
velocity
time
rotational cell
rotation
he
The and
between velocity between
268
KAY,
images. for
Cell
stability
slit-scan
noted
and
in
all
of
however,
a
the
of’ the
plane
these
cell
images.
image
is
cell
affect
measurement
cell
Current
efforts
of
cell
flow
capillary flow
are
one
will
be
future
an
Laser
utilized
to
attempt
to
the
assess
flow
fluid-filled
force
alignment
stroboscopic
photography
the
success
of
desirable
potential
exists
cell
orientation
for
using
techniques
tion
two-dimensional
flow
system
this
and
at
occurring
one
at
orthogonally laser
transferred
flow.
primary
slit-scan
measurement
and
flow.
a high
strobe
The in
flow or
A cell speed
A is
illumination
stations
the
wavelengths
to
in
stations
other.
of
resolu-
measurement
positioned
direction
photo-
moderate
two
station
the
achieved,
strobe
information
the
occurring
separate
to obtain
with
envisioned,
be laser
could stream
vidicon,
be
along
8.
would
be
linear
ar-
at
additional from
prescreening
an on
the
second
Processing morphologic image
which
cell
classification
sta-
would inforwould
be (3).
CITED
1. Boettner EA, Thompson BJ: Multiple exposure holography of moving fibrous particulate matter in the respiratory range. Optical Engineering: March/April, 1973. 2. Bonner WA, Hullett HR, Sweet RG, Herzenberg LA: Fluorescence activated cell sorting. Rev Sci Instrum 43:404, 1972 3. Cambier JL, Wheeless LL: The binucleate cell: Implications for automated cytopathology. Acta Cytol 19:281, 1975 4. Crissman H, Mullaney P, Steinkamp J: Methods and applications of flow systems for analysis and sorting of mammalian cells, Methods for Cell Biology. Edited by DM Prescott. Academic Press, New York, 1974 5. Goldsmith HL: Red cell motions and wall interactions in tube flow. Fed Proc 30:1578, 1971 6. Wheeless LL, Hardy JA, Balasubramanian N: Slit-scan flow system for automated cytopathology. Acta Cytol 19:45, 1975 7.
using
separated
image
in
array
processing.
LITERATURE
shaping
elliptical
in
to derive available
should greatly
achieving
proper
detector
image
used
useful
performed.
toward An
flow.
other
for
mation
modifications.
graphic
the
directed
incorporated in
Should the
being
through
plane.
and may
on
be
indicates to the
geometry.
chamber
to
which
unstable as it
orientation
is being
Occasionally,
seen
is usually possible,
chamber
ray
tion
are
is perpendicular
if
the
orientations
measurements
This orientation be prevented,
desired
favorable
fluorescence
WHEELESS
Wheeless
LL, Patten SF: Slit-scan cytofluorometry. Acta Cytol 17:333, 1973 Wheeless LL, Patten SF, Onderdonk MA: Slitscan cytofluorometry: data base for automated cytopathology. Acta Cytol, in press
Downloaded from jhc.sagepub.com at GEORGIAN COURT UNIV on March 18, 2015