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Microscopic Profile Of Asbestos And Other Non-Opaque Particulates
Larger Than 5 Micrometers In Parenteral Drugs
` . by
. Leonora Auerbach
Food and Drug Administration Dept, of Health, Lducation, and Welfare 850 Third Avenue Brooklyn, N.Y. 11232
Presented at the 89th Annual Meeting of the Association of Official Analytical Chemists on October 15, 1975 in Washington, D.C.
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Abstract
This report describes a comparative microscopic study of
chrysotiie fibers utilizing three sequential optical systems:
plane polarized light (PL), phase-contrast ( P C ) a n d Nomarski v
differential interference-contrast (NDIC) for complementary
image analyses. The introduction of NDIC for qualitative
and quantitative determinations in this area of particulate
analyses resolves the problem of diffraction haloes encountered
in PC microscopy. High optical contrast, the instrumental
characteristic of the NDIC, is particularly useful of the
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detection of chrysotiie fibers at a magnification of 500X.
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Introduction! --------I -- . ------------- .----------------
/r In 1975, heightened awareness of the adverse clinical
significance of particulates in animal and human circulatory
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systems (1) resulted in official regulations regarding r
parentcrals. F.D.A, issued a directive restricting the use
of fiber-shedding asbestos and/or glass fiber filters in the
manufacture of parenteral drug dosage forms (2). The U.S.P.
XIX sets standards in terms of number and size limits for
particulate matter in large volume parenterals.
The purpose of this paper is to describe a microscopic
method, applicable to parenterals, for monitoring non-opaque
particulates in general, and fibers such as chrysotile asbestos
in particular. Animal studies reported in the literature appear
to indicate that the fibrous morphology and not the chemical
composition 'of chrysotile fibers is of pathological significance
"(4,5). This paper describes a method of sample preparation
and subsequent microscopic examination employing three optical
contrast systems: Plane Polarized Light (PL), Phase-Contrast
(PC), and Nomarksi Differential Interference-Contrast (NDIC) for qualitative and quantitative characterization of non-opaque
particulate matter.
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Expci~5mental
Atmospheric Conditions: All operations except microscopic examinations are conducted under Class 100 conditions (6).
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Clearing reagents; A 1:1 solution of diethyl oxalate and /'
dimethyl phthalate is filtered through a Millipore
Mitex filter, pore size 5 micrometers. For each ml. of the
solution 0.1 gram of white, ungridded mixed esters of
cellulose membrane material is added (7), The mixture is
stirred to dissolve the membrane material and set aside for
a.few days to eliminate air bubbles before use.
Microscopic Equipment: The standard ^JBIpolarizing microscope
was fitted with a revolving achromatic-aplanatic phase-contrast
and interference-contrast condenser, type VZ, with top lens * *
1.4 N/A. The condenser is equipped with six stops: one for
plane polari'zcd light., ,,two for phase-contrast, 16X-100X, and
"three positions for the planachromat objectives for the NDIC,
-viz,, 16X, 40X, and 100X. The NDIC requires an interference-
contrast slide which is inserted into the analyzer slot. The
9
revolving nose-piece accomodates five objectives. The eyepiece
contained a cross-hair micrometer.
Sample Prcpnrnt.i on: Isolate particulates on a white, gridded,
mixed esters of cellulose membrane filter (Millipore), pore size
0.45 micrometer as directed in the U.S.P. XIX, First Supplement (3).
As a final rinse, use 5 ml. of isobutyl alcohol which had
/.
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been previously filtered through a 0.22 micrometer MF filter.
The filter must be thoroughly dried before clearing. Drying
K M */
maybe accomplished by air (8 hrs) or by heating .on a^not
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bench at about 90 for approximately one hour..
Microscopic Examination: In the sample preparation area place
one drop of clearing reagent on a clean glass slide previously
rinsed with trichlorotrifluoroethane. Position the filter on
top of the drop so that only the entire lower surface is in
contact: with the reagent. Excess reagent should be avoid Q
so that the top of the filter is never flooded.. When the
filter is completely transparent, cover the'preparation with a
cl ean trichlorotrifluorethane-rinsed cover glass. The clearing
e reagent has a refractive index (N) of 1.46-1.47. The sample
should be examined within a few days because crystallization of
^the clearing reagent occurs within a week. The entire filter is
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examined in white light at a magnification of approximately 500X
using three optical systems sequentially in the following order:
PL, PC, NDIC. A darkened laboratory provides optimum conditions
for the microscopist.
Compnrat ive Microscopic Study of Chrysot.i 1c Fibers: For the
purpose of illustration, Canadian chrysotilc was mounted in
immersion oil having a refractive index (N) of 1.464. The same
microscopic, field was photographed in PL, PC, and NDIC. The
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focal plane in each system that exhibited the sharpest
contrast was selected.. ^^rt>a^3rf4-erj^4^n-^^s 200X and the
length of the principal bundle v.'as 175 um,-fbr--
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rounded massds on either side of the midpoint of
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the specimen are foreign crystals.
Figure 1.. Viewed in PL with uncrossed polars, chrysotile
fibers appear as a skein of transparent,
very
flexible parallel fibers with random waves, curls and twists.
Although the edge effects (diffraction, reflection, and
refraction) provide dark contrast, the fibers characteristically
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provide a blurred image due to the fact that the fibril bundle
does not lie in one focal plane. Glare and slight haloes de
grade th image. Chrysotile is dichroic anc* absorbs most
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strongly in the y index position, i^.je, the length of the
fiber parallel to the vibrational direction of the polarizer.
-In this position thick fibers may show green to blue-green
.*
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Colors and appear yellow-green to colorless in the a position.
Thin fibers exhibit no color, however, a slight change in
intensity is usually discernible with the fiber transparent
in the a position and somewhat opaque in the y position.
Figure 2. The chrysotile bundle is viewed in PL with
polars crossed and placed in the position of maximum brightness.
The birefringence of chrysotile is very low (0.004-0.016) and
O. T very thin fibers, ev'-a micrometer in diameter, arc invisible.'
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Khite to first order yellow is thc-maximum interference color
/angc for thick fibers. The extinction is parallel and the
sign of elongation is positive. The first order red compensator
can be used for the detection of^thin fibers that were invisible
9
with crossed polars, Fibers aligned parallel to the slow ray
of the compensator show second order blue color and exhibit
good contrast against the magenta background.
Figure 3 and
The chrysotile bundle in Figure 3 and
5
anthophyllite fiber in Figure $ are viewed in PC, Diffraction
haloes around the specimen and ghost images of particles above
and below the focal plane are in part instrumental characteristics
of PC. Note ghost images in the lower portion of the southwest
quadrant* of Figure 3. The large optical path discontinuities
9
between the refractive index of chrysotile and the surrounding
medium plus the wedge-edge effect of the combined haloes of the
'individual fiber bundles make halation a severe problem. In
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the microsopic field, only thin, well separated fibers are viewed
to advantage.
Fibers that did not present useful images when viewed with
the first order red plate are seen in good contrast in PC.
Thin fibers in positive PC arc seen as dark threads which
usually exhibit some terminal end-flair of the fibrils. Thick
chrysotile particles appear as opaque masses such as the dark mass
positioned at approximately three o'clock in Figure 3. Careful
focal studies of this particle (in PC) barely suggested iis tight
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fibrous mass. This particle, when well focused in the NDIC
s y s te m shows the topography of a fibrous mass.
The observations made in the discussion of the chrysotile
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fibers in Figupe 3 apply to the PC appearance of anthophyllite
in Figure ^
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Figure ^ and 6. The chrysotile bundle and authophyllite
fragment are viewed in NDIC. The sharp optical discontinuities
that produced halation in the PC image appear In dark and light
contrast, at the specimen-medium boundries. The chrysotile
fibers* are preceived by their shadow: cast slopes and appear
three dimensional. The specimen's variation in optical path
(Refractive Index x Thickness) across the width of the fiber
* -bundle is visually translated as elevations of various heights.
In NDIC microscopy, interfaces between media of different
.refractive index appear in relief, high relief for areas of higher
index and depressions for`the lower index. The topography of
the chrysotile bundle seen in the NDIC image reflects the
gradient of phase difference in the transverse direction which
is parallel to the direction of shear of the Nomarski prisms.
This contrast is differential interference-contrast. The diagonal,
north-east to south-west in the microscopic field is the direction
of shear. Specimens of chrysotile and amphiboles also effect a
"super-modulation" of the light to give amplitude-contrast (8)
when oriented perpendicularly to the direction of shear. Thus
the fibers are clearly delineated and appear of brighter intensity
I I
than the background.
A large fragment of anthophyllite
is seen in Figure 6.
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Microscopic differentiations between such amphiholes as
amosite, crocidolite, and anthophyllite could not be made.
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Discussion
The cleared membrane filter presents a background which
exhibits -some granulation#-o^^^n==poaife^is^-l Two other
clearing procedures suggested by the Millipore Corporation have
not been tested. They are the use of immersion oil (refractive
index (N) = 1..515) (9) and the transformation of the filter into
a transparent hard plastic (10). The principal problem encounted
on dissolution of the filter was due to residual moisture in the
filter.^ Faulty clearing is noticeable as a visible turbidity and
for such filters microscopie resolution is destroyed. An
additional uroblem was the friabilitv of thJinked grid markings. i
Excess oressurc in arriving the cover glass to the filter can
cause the opaque grid particles to migrate. Under these
circumstances a relatively large grid fragment can cause light
blockage and thus degrade the image of coincident or adjacent
particles in the field..
The sequential use of the three optical systems, PL, PC,
and NDIC provides maximum contrast and resolution for the
morphological identification and optical crystallographic
charnctcrization of non-opaque particulates in the fixed refractive
index (NT) medium of 1.46-1.47. The arrangement of these optical
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I systems on the standard polarizing microscope represents a
j /practical approach to the selection of a contrast technique
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which furnishes the most qualitative information concerning
a particulate. For the examination of ta microscopic field which
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may contain particles of various sizes and compositions, each
system provides some information and one system will exhibit
optimum contrast. Compare Figures 7_ and 8_. In Figure 7 one
focal plane in PC provides a good contrast image of the
diatomaccous earth fragment. The coincident chrysotile fiber
in this field cannot be sharply focused in any one plane.
On the other hand, Figure 8 shows the field of Figure 7 rotated
for optimum NDIC contrast. The image of the chrysotile
fiber is sharper and halation is negligible.
4 e
PC is very useful for phase objects having an optical path,
difference (Refractive Index x Thickness) of X/10- X/2.
'Larger differences introduced halation.. The majority of
particulates encountered in parenteral drug analyses are of a
higher refractive index than the medium and are seen in
dark contrast on a lighter background in the Zeiss positive PC. The NDIC is applicable in a broader path difference range
(X/10 -IX) and lias a very shallow depth of field which provides
sharp images free of spurious contrast above and below the focal
plane This instrumental characteristic is very useful for
optical sectioning of thick specimens and in instances of
ovcvlappi ng parti cuJat cs.
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Instrumental factors are significant and deserve some
comment. There are no instrumental drawbacks to the PL system.
Low and high power objectives can be used when the appropriate
condenser top lens element is employed* LenseS'With 0.63 - 1,4
N/A are available. The optical components of the PC system are
rotation-symmetric and specimen orientation in the field is not
significant. This is not the case in the NDIC system.. There
is a fixed orientation of the instrument; viz.., the specimen
may be oriented in a postion 90 with respect to the direction
of shear and then the stage is rotated so that the specimen
a
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is observed in a position parallel to the direction of shear.
There is an azimuth effect through this angle and some
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feature^ of a specimen may appear more pronounced in one f
position than another. Although the planachromat objectives
used the NDIC are not. centerable on the revolving multiple
,,nosepiece, a single centerable nosepiece is available from
* the Eels~s CojjnT for perfect centration of the objective.
The less than perfect centration of the specimen in the field
e
can be corrected during rotation by manual manipulation using
the' mechanical stage. In practice, for routine work, this
adjustment is often not: critical.
Sources of particulate contamination of parenteral drugs
can be broadly categorized. Algae, molds, insect fragments
and animal hairs are introduced under unsanitary conditions.
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Tyvek fibers (DuPont) from clean room garments and starch
grains from powdered gloves are possible laboratory contaminants.
Diatomaceous earth, glass wool, asbestos and cellulose fibers
may be residual particles from production line filters. Many
non-opaque particulates can be readily identified in the PL
system if encounted in a typical form. If however found in a
degraded state, identification becomes more difficult. Two
examples of particulates found in an atypical state are
hydrolyzed starchs grains and very fine shredded cellulosic
fibers. A hydrolyzed corn starch grain is isotxopic when
c
Viewed between crossed polars in PL, This grain when viewed
in NDIC clearly shows the depressed centric stellate helium
characteristic of corn starch. A shredded cellulosic fiber
1 micrometer in diameter often twists and curls, and may
........ A strongl)vresenlk*e chrysotile in the PL and PC systems, 'However,
when observed in the NDIC it does not effect a "super-
modulation" of the light and does not present the fibrillar,
cylindrical profile which is characteristic of chrysotile.
/ The method described was initially employed for the
detection of chrysotile and amphibole asbestos but was found
to be very useful for the examination of other non-opaque
particulates of 1ow birefringence. The inherent characteristics
of the NDIC system was found to enhance those aspects of the PL
and PC microscopic images which were deficient in contrast.
12
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Acknowlcdgment The author is grateful to Thomas Medwick, Science Advisor, Food and Drug Administration, New York District, and Professor of Pharmaceutical Chemistry, College of Pharmacy,
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Rutgers University, New Brunswick, N.J. for his invaluable assistance in the preparation of this manuscript.
I 33 References
3* United States Pharmacopeia (3975) 19th Rev., 1st Supplement,
`*
. Hack Publishing Co., Easton, PA., 56*-57
4. Gross, P., 8 Harley, Jr.., R.A. (1973) Arch. Environ. Health
27, 240-242
'
5.. Stanton, M.F. (1973) The. M I Record . (2) , 1 $ 6 6* United States Pharmacopeia (1975) 19th Rev.,"'(Note),
Hack Publishing Co., Easton, PA, p. 712
7.. .Edwards, G.H. , $ Lynch, J.R. (1968) Ann. Occup. Hyg. 11, 1-6
8. David, G.B., Williamson, B.S. (1971) Histochemistry 27, 1-20
9.. Anonymous (1975) Detection and Analysis of Particulate
4
'Contamination, ADM-30,- Millipre Corporation, Bedford, MA
01730, 16-17
! \ m*
10* Jones, E.J. (1975) Microscope 23, 93-101
I
14 -
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Legends For Figures
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j Figure 1. Canadian cbrysotile^at ^OX magnification;
principal bundle is 175 um in- length; plane polarized light.
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Figure 2. Canadian chrysotile^at^200X magnification; same
9
field as in Figure 1; plane polarized light with crossed
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polars.
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Figure 3. Canadian chrysotile,,at 200X magnification; same field as Figure 1; *---- ---
'phase contrast..
Figure Anthophy1lifeAat $00X magnification;^phase contrast.
--- -- '--
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Figured. Canadian chrysotile.at 200X magnification; same field
ii .* <
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as! in Figure 1, long axis of the fiber bundle oriented
*\
perpendicular to the direction of shear; Zeiss/Nomarksi
j
differential interference-contrast.
.
Figure <5. Antlwphyllj/^c^at^OOX magnification; long axis of
j
st
th-e large^ fragment (57 um) is oriented perpendicular to
the direction of shear; same field as in Figure 4; Zeiss/Nomarski f* o
differential interference-contrast.
Fjgure 1_. Coincident chrysotile fiber and diatomaceous earth
j* t' f^agmen't^at'500X magnification; phase contrast.
Eiiiure JS. Coincident chrysotile fiber and diatomaceous earth
fragment^at 50t)X magnification rotated for maximum contrast of
tile fiber; same field as in Figure 7; Zciss/K'omnrski differential
jntcvfcrence-contrast.