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Applied and Environmental Microbiology, April 2003, p. 1898-1903, Vol. 69, No. 4
0099-2240/03/$08.00+0 DOI: 10.1128/AEM.69.4.1898-1903.2003
Copyright © 2003, American Society for Microbiology. All Rights Reserved.
Effect of Particles on the Recovery of Cryptosporidium Oocysts from Source Water Samples of Various Turbidities
Yao Yu Feng, Say Leong Ong,* Jiang Yong Hu, Lian Fa Song, Xiao Lan Tan, and Wun Jern Ng
Center for Water Research, Department of Civil Engineering, National University of Singapore, Singapore 119260, Singapore
Received 19 August 2002/
Accepted 6 January 2003

ABSTRACT
Cryptosporidium parvum can be found in both source and drinking
water and has been reported to cause serious waterborne outbreaks
which threaten public health safety. The U.S. Environmental
Protection Agency has developed method 1622 for detection of
Cryptosporidium oocysts present in water. Method 1622 involves
four key processing steps: filtration, immunomagnetic separation
(IMS), fluorescent-antibody (FA) staining, and microscopic evaluation.
The individual performance of each of these four steps was evaluated
in this study. We found that the levels of recovery of
C. parvum oocysts at the IMS-FA and FA staining stages were high, averaging
more than 95%. In contrast, the level of recovery declined significantly,
to 14.4%, when the filtration step was incorporated with tap
water as a spiking medium. This observation suggested that a
significant fraction of
C. parvum oocysts was lost during the
filtration step. When
C. parvum oocysts were spiked into reclaimed
water, tap water, microfiltration filtrate, and reservoir water,
the highest mean level of recovery of (85.0% ± 5.2% [mean
± standard deviation]) was obtained for the relatively
turbid reservoir water. Further studies indicated that it was
the suspended particles present in the reservoir water that
contributed to the enhanced
C. parvum oocyst recovery. The levels
of
C. parvum oocyst recovery from spiked reservoir water with
different turbidities indicated that particle size and concentration
could affect oocyst recovery. Similar observations were also
made when silica particles of different sizes and masses were
added to seeded tap water. The optimal particle size was determined
to be in the range from 5 to 40 µm, and the corresponding
optimal concentration of suspended particles was 1.42 g for
10 liters of tap water.

INTRODUCTION
Cryptosporidium parvum remains a potential risk for drinking
water consumers in spite of the considerable efforts made by
water providers and the U.S. Environmental Protection Agency
(USEPA) (
6,
10,
14,
15,
16).
Cryptosporidium has a long survival
time in water and a low infectious dose. As there is no cure
for cryptosporidiosis at this time,
Cryptosporidium poses considerable
danger to the public. It has been reported that cryptosporidiosis
is life threatening to immunosuppressed patients and children
who are less than 1 year old (
3,
9).
Cryptosporidium oocysts
are known to be resistant to chlorine disinfection due to their
thick cell walls (
5,
7,
18). At present, physical removal by
filtration is the primary means for removing the oocysts from
source waters. However, there is a possibility that oocysts
could penetrate the treatment system and cause disease outbreaks,
such as the 1993 Milwaukee cryptosporidiosis outbreak in which
403,000 people were infected and 110 deaths occurred (
8). This
incident resulted in considerable attention being paid to the
detection and removal of
Cryptosporidium in water treatment
plants, as well as monitoring for this pathogen in source waters.
Detection of Cryptosporidium oocysts in raw water sources is considered an important component in the control of Cryptosporidium in drinking water supplies. Various methods have been developed to detect C. parvum in both raw source waters and finished drinking waters. For example, the USEPA has established an Information Collection Requirement Rule (ICR) method to detect Cryptosporidium oocysts present in source waters (15). The ICR method, which replaced the American Society for Testing and Materials P229 method, has been criticized for being difficult to perform, yielding highly variable results, and providing different responses in a variety of water matrices (17). With the Safe Drinking Water Act Amendments of 1996, the USEPA revised the ICR method and proposed draft method 1622. This proposed method was validated in January 1999. Method 1622 includes the following main steps: (i) oocyst capture and concentration from a volume of water by filtration, elution, and centrifugation; (ii) oocyst purification by immunomagnetic separation (IMS); (iii) staining of the IMS product by fluorescent-antibody (FA) staining and 4',6-diamidino-2-phenylindole (DAPI) counterstaining; and (iv) examination and confirmation of oocysts by epifluorescence and differential interference contrast microscopy (16).
Although USEPA method 1622 is a widely used assay for detection of Cryptosporidium oocysts, this method still has drawbacks, such as low levels of oocyst recovery and extremely variable results (1, 2, 11, 12). Connell et al. (4) studied oocyst recovery from 430 samples collected from 87 source waters. They noted that the levels of oocyst recovery from 97.5% of spiked water samples ranged from less than 10% to as high as 80%. They further noted that the chances of obtaining levels of oocyst recovery in the range from 20 to 70% were almost equal. Turbidity was among the possible factors which affected oocyst recovery in the IMS procedure. However, there has not been unanimous agreement concerning turbidity as some studies have shown that turbidity has little effect on oocyst recovery in the IMS procedure (11), while other studies have indicated that samples with high turbidity can result in low levels of oocyst recovery (2, 13). It has even been reported there was an optimum turbidity of 500 nephelometric turbidity units (NTU) which could result in the highest level of oocyst recovery (1). Despite the many studies that have been conducted on method 1622, the effects of turbidity are still not well understood. By comparing the levels of oocyst recovery from surface water and reagent water with an Envirocheck capsule filter (Pall Gelman Sciences, Ann Arbor, Mich.) as recommended in method 1622, Simmons et al. (12) found that the rates of recovery of oocysts from surface water were significantly lower and also more variable than the rates of recovery from reagent water. They also found that the rates of recovery of oocysts from surface water increased significantly when another kind of filter from their laboratory was employed instead of the Envirocheck capsule filter. The findings of these authors suggested that turbidity might affect the performance of method 1622 by affecting the filtration procedure. In view of uncertainties concerning the impact of turbidity on method 1622, the objectives of this study were to identify the critical steps of method 1622 and to determine whether turbidity does indeed have an effect on oocyst recovery.

MATERIALS AND METHODS
Sources of oocyst suspensions.
C. parvum oocysts were obtained from Waterborne Inc. (New Orleans,
La.). These oocysts were isolated from infected calves and are
referred to as the Iowa strain. The feces of experimentally
infected calves were collected and clarified by using sucrose
and Percoll density gradient centrifugation after initial extraction
of the feces with diethyl ether. Purified oocysts were stored
in a solution containing phosphate-buffered saline supplemented
with 1,000 U of penicillin per ml and 1,000 µg of streptomycin
per ml at 4°C. The age of the oocysts used in this study
was less than 2 months.
Enumeration of oocyst stock suspensions.
The suspensions of C. parvum oocysts were enumerated by placing 10 replicates of 10-µl aliquots on glass well microscope slides and staining the preparations with fluorescein isothiocyanate (FITC)-conjugated anti-Cryptosporidium sp. monoclonal antibody (MAb) (Waterborne). The slides were then examined by using an epifluorescence microscope as described in USEPA method 1622.
Water matrices used to assess C. parvum oocyst recovery following FA staining, IMS, centrifugation, and filtration.
Ten-microliter portions of an oocyst suspension were used to spike the solutions for each step employed in method 1622 to investigate which steps were the crucial steps that could affect oocyst recovery. To recover seeded oocysts following IMS, 10 ml of reagent water was used. For the recovery studies with seeded oocysts following filtration, 10-liter portions of different water matrices were used. These matrices included reservoir water, reclaimed water, microfiltration (MF) filtrate, and tap water. The tap water was obtained from the laboratory. The reclaimed water and MF filtrate were collected from a dual-membrane-based water reclamation facility in which secondary effluent from a domestic wastewater treatment plant was further treated by chlorination, MF, reverse osmosis, and UV disinfection. The reservoir water was collected from a local freshwater reservoir, and all reservoir water samples were grab samples. The turbidities of all samples were measured before use with a HACH 2100P turbidimeter (Hach Co., Loveland, Colo.). To study the effect of reservoir water suspended particles, particles were obtained by filtering 10 liters of reservoir water through an Envirochek capsule filter (Pall Gelman Sciences). The trapped particles were then eluted with elution buffer and dried in an oven at 100°C. The dried particles were then added into 10-liter tap water samples to produce particle-spiked tap water. Other types of water matrices were also prepared by adding different sizes and masses of Silica Gel 60 (Merck, Darmstadt, Germany) to tap water to generate various levels of turbidity.
Filtration, IMS, and FA staining of seeded oocysts.
Ten-liter water samples were filtered at a flow rate of 2.0 liters/min through Envirochek capsule filters (Pall Gelman Sciences). Oocysts were eluted from the capsule filters with elution buffer and wrist action agitation, as specified in method 1622. Eluants were collected in 250-ml conical-bottom centrifuge tubes, and the oocysts were concentrated by centrifugation at 1,500 x g for 15 min (Eppendorf 5810; Eppendorf, Hamburg, Germany). The resulting pellet volumes were recorded. Supernatant was carefully aspirated from each tube until the volume above the pellet was 5 ml. Reagent water was then added so that the pellet volume was 5% or less in the 10-ml samples subjected to IMS. An anti-Cryptosporidium IMS kit (Dynal Inc., Lake Success, N.Y.) was utilized to separate the oocysts from other interfering particulate matter by the IMS protocol as described in method 1622. Samples were transferred to well slides (Waterborne) and stained with FITC-conjugated anti-Cryptosporidium sp. MAb (Waterborne). The slides were then examined by using an epifluorescence microscope as described in method 1622.
Epifluorescence microscopy.
An Olympus BX51 fluorescence microscope equipped with a blue filter block (excitation wavelength, 490 nm; emission wavelength, 510 nm) was used to detect FITC-conjugated MAb-labeled oocysts at a magnification of x200. The presence of oocysts was confirmed at a magnification of x400 by using a UV filter block (excitation wavelength, 400 nm; emission wavelength, 420 nm) for visualization of DAPI, and the internal morphology of oocysts was determined by Nomarski differential interference contrast microscopy.
Measurement of particle size distribution.
An LS 230 particle size analyzer with a Small Volume Module Plus and Coulter LS control software (Coulter, Miami, Fla.) was used to measure the particle size distribution in reservoir water. The particle size range analyzed was from 0.04 to 2,000 µm.

RESULTS
Effect of each method 1622 step on oocyst recovery.
A 10-µl oocyst stock suspension was spiked into 10 liters
of tap water, and then filtration, IMS, and FA staining were
performed. Alternatively, a 10-µl oocyst stock suspension
was spiked into 10 ml of reagent water and then IMS and FA staining
were performed, or a 10-µl oocyst stock suspension was
stained with FA directly (spike dose, 2,010 ± 111.1 oocysts/10
µl;
n = 10). The levels of oocyst recovery following the
different treatments were as follows: level after FA staining,
98.3% ± 2.1% (mean ± standard deviation;
n = 3);
level after IMS and FA staining, 95.1% ± 3.4%; and level
after filtration, IMS, and FA staining, 14.4% ± 7.5%.
The levels of recovery following FA staining ranged from 96.0
to 100.0%, while the levels of recovery following IMS and FA
staining ranged from 92.4 to 99.0%. When the data were analyzed
by using a two-sample
t test (based on the assumption that data
for both populations were normally distributed and the assumption
that the population standard deviations for the two treatments
were the same), no significant differences in oocyst recovery
for these two populations were detected (
P = 0.240). The high
levels of recovery following IMS and FA staining showed that
these two procedures could be easily performed with good accuracy
and could provide stable results. However, when the filtration
step was added, the levels of recovery decreased significantly
(
P < 0.001, as determined by a
t test) to 9.0 to 22.9%. This
suggested that the greatest loss occurred at the filtration
stage. The filtration stage included filtration, elution, and
centrifugation. As shown by the data given above, recovery of
oocysts by using a Dynal anti-
Cryptosporidium IMS kit yielded
excellent results, and the average level of recovery was 95.1%
(standard deviation, ±3.4%). Using the same type of kit,
Bukhari et al. (
1) found that the levels of oocyst recovery
ranged from 68 to 83% for deionized water, while Stanfield et
al. (
13) reported a mean level of recovery of 96.1% for treated
water. The manufacturer-stated levels of recovery fell within
the range from 60 to >95% for treated and raw waters. The
IMS values obtained in this study were therefore within the
reported range. However, if the filtration step was included,
the mean level of recovery decreased significantly to only 14.4%
(standard deviation, ±7.5%) for seeded tap water. This
was much lower than the values reported by Simmons et al. (
12)
and Stanfield et al. (
13), who obtained levels of oocyst recovery
of 46% (standard deviation, ±18%) and 58.1% (standard
deviation, ±23.8%) for seeded reagent water and treated
water, respectively.
Effect of water matrices on oocyst recovery.
In order to study whether the water matrix had an effect on oocyst recovery, 10-liter portions of various water samples were spiked with predetermined numbers of oocysts. Preliminary studies had shown that none of the water matrices used contained Cryptosporidium oocysts before spiking. The results obtained in this series of studies are summarized in Table 1. The levels of recovery ranged from 8.4 to 16.2%, from 9.0 to 22.9%, and from 13.4 to 22.0% for the reclaimed water, tap water, and MF filtrate, respectively. These values were not significantly different from one another (P > 0.271, as determined by a t test). However, the levels of recovery from the most turbid reservoir water samples (range, 79.8 to 92.0%; mean, 85.0%) were much higher than those from the reclaimed water, tap water, and MF filtrate. The t test indicated that the levels of recovery from reservoir water were significantly higher than the levels of recovery from the three other water matrices (P < 0.001). The high levels of recovery from reservoir water samples were obtained with samples that had relatively high turbidity. As discussed above, filtration had an adverse effect on oocyst recovery. This suggested that recovery of oocysts associated with the filtration stage might be influenced by the turbidity of the water matrix.
Effect of particles on oocyst recovery in reservoir water.
Experiments were carried out to investigate if suspended particles
could be responsible for the high levels of recovery from reservoir
water samples. To facilitate this study, similar quantities
of oocysts were spiked into four different water matrices. The
first matrix was the actual reservoir water, while the second
was prepared by filtering reservoir water through the capsule
filter recommended in method 1622. The third matrix was tap
water, which served as the control, while the last matrix was
tap water spiked with particles obtained from the capsule filter
used to filter the reservoir water. Table
2 summarizes the average
results. After the particles were removed from the reservoir
water, the mean level of oocyst recovery was found to decrease
drastically from 82.4 to 16.4%. This observation suggested that
the suspended particles present in the reservoir water contributed
to the high level of oocyst recovery associated with reservoir
water. This was verified by the increase in the level of oocyst
recovery from 15.9% in tap water to 70.8% when the extracted
particles (obtained from reservoir water) were added to tap
water. Possibly because of a loss of particles during preparation,
the spiked tap water had a turbidity of 4.5 NTU, compared to
the turbidity of 5 NTU for the original reservoir water. The
lower turbidity could have contributed to the slightly lower
level of recovery from the former sample.
Effect of turbidity on oocyst recovery from reservoir water samples.
It was observed that the turbidities of reservoir water samples
were different for different collections, ranging from 1.8 to
40 NTU. Rain was found to be the key factor causing high turbidity,
and this was especially true for the sample with a turbidity
of 40 NTU. The effect of turbidity on oocyst recovery from reservoir
water samples was investigated, and the results are summarized
in Table
3. A
t test indicated that the levels of recovery from
reservoir water samples with turbidities other than 40 NTU were
significantly higher than the levels of recovery from tap water
(
P < 0.005). However, no significant difference between the
level of recovery from reservoir water with a turbidity of 40
NTU and the level of recovery from tap water (
P = 0.182) was
found. As the turbidity of reservoir water increased from 1.8
to 5 NTU, the level of oocyst recovery increased significantly,
from 63.3% (standard deviation, ±8.1) to 85.0% (standard
deviation, ±5.2%) (
P = 0.008, as determined by a
t test),
although the difference between the levels of recovery from
samples with turbidities of 1.8 and 3.0 NTU was not significant
(
P = 0.344, as determined by a
t test). When the turbidity increased
further from 5 to 40 NTU, the level of oocyst recovery decreased
significantly, from 85.0% (standard deviation, ±5.2%)
to 24.9% (standard deviation, ±8.4%) (
P < 0.001, as
determined by a
t test). The highest mean level of recovery
was obtained at a turbidity of 5 NTU, and the value was significantly
higher than the levels of recovery for all the other turbidities
investigated (
P < 0.025, as determined by a
t test). This
finding suggested that a moderate degree of turbidity enhances
oocyst recovery. However, increasing the turbidity beyond the
threshold value caused the efficiency of recovery to decline.
This finding agreed with previous findings which showed that
high turbidity was not conducive for oocyst detection (
12).
The results obtained in this study also suggested that a moderate
amount of suspended particles (i.e., a moderate degree of turbidity)
enhanced oocyst recovery, probably because the oocysts adhered
to the suspended particles, making them easy to capture.
Experimental verification of the particle effect.
As the suspended particles present in the reservoir water were
likely to consist of a mixture of particles of various sizes,
it was useful to investigate if particle size and particle size
distribution affected the efficiency of recovery. The particle
size distribution in reservoir water with a turbidity of 5 NTU
is shown in Fig.
1. We found that most of the suspended particles
were in size range from 1 to 400 µm. However, the relative
volumetric fractions varied considerably with respect to particle
sizes.
To study the effect of particle size, silica gel particles in
four size ranges from 5 to 400 µm were introduced into
different tap water samples. The results obtained are shown
in Table
4. We found that the level of recovery decreased as
the size of the added particles increased. A
t test indicated
that the levels of recovery from samples with particles that
were not larger than 63 µm were significantly higher than
the levels of recovery from tap water (
P < 0.011). However,
no significant differences were detected for the levels of recovery
from samples containing silica particles larger than 63 µm
(
P > 0.158). The highest mean level of recovery was 51.5%
(standard deviation, ±6.5%), when the size of the added
silica particles was in the range from 5 to 40 µm. This
value was significantly higher than the levels of recovery associated
with the other silica particle sizes (
P < 0.005, as determined
by a
t test). Figure
1 shows that although the volumetric fraction
of particles in the size range from 5 to 40 µm was low,
the particle count for this fraction accounted for 70 to 80%
of all the particles present (after calculation). Table
4 shows
that in order to obtain a turbidity of 5 NTU, the masses needed
for the different size ranges of silica were quite different.
For example, only 0.71 g of silica particles in the size range
from 5 to 40 µm was needed to obtain a turbidity of 5
NTU in 10 liters of tap water, while 10.4 g or more of silica
particles was needed when larger particles were used.
In order to study the effect of particle concentration on oocyst
recovery, different masses of silica particles in the size range
from 5 to 40 µm were added to 10-liter tap water samples
to obtain different concentrations of particles in the water
samples. The results obtained are summarized in Table
5. The
levels of recovery from samples spiked with silica particles
were significantly higher than the levels of recovery from tap
water samples (
P < 0.004, as determined by a
t test). The
efficiency of recovery improved from 37.4% (standard deviation,
±3.0%) to 90.6% (standard deviation, ±3.7%) when
the amount of silica added was increased from 0.35 to 1.42 g,
and this increase was statistically significant (
P < 0.013,
as determined by a
t test). However, the efficiency of recovery
deteriorated significantly when 2.16 g or more of silica particles
was added to a 10-liter tap water sample (
P < 0.021, as determined
by a
t test). This suggested that while a moderate amount of
silica particles enhanced oocyst recovery, there was a threshold
concentration above which the recovery efficiency was adversely
affected. The highest level of recovery was obtained when 1.42
g of silica was added to 10 liters of tap water, and the corresponding
water turbidity was 10 NTU.

DISCUSSION
We noted that the filtration step resulted in a significant
decrease in the level of oocyst recovery. We found that of the
different water matrices investigated, reservoir water gave
the highest average level of recovery, 85.0% (standard deviation,
±5.2%). We suggest that the suspended particles present
in the reservoir water enhanced oocyst recovery. A turbidity
of 5 NTU for the reservoir water resulted in the highest level
of oocyst recovery. As reservoir water samples with different
turbidities have distinct particle size distributions, it is
reasonable to believe that particle size and concentration could
be the key factors affecting oocyst recovery. Using silica to
verify this hypothesis, we found that addition of particles
in the size range from 5 to 40 µm to obtain a turbidity
of 10 NTU resulted in the highest level of oocyst recovery.
This size range corresponded to the major particle count fraction
of suspended particles identified in reservoir water samples.
When different amounts of silica particles in the size range
from 5 to 40 µm were added to 10-liter tap water samples,
the sample with a turbidity of 10 NTU yielded a higher level
of recovery than the water samples with turbidities ranging
from 2.5 to 7.5 NTU. Further increases in the amount of silica
particles added (i.e., increases in the turbidity to 15 to 20
NTU) led to decreases in the levels of oocyst recovery. This
confirmed that particle size distribution and particle concentration
affected oocyst recovery.
The filtration stage includes filtration, elution, and centrifugation. It is possible that oocysts could adhere to particles which are larger than the oocysts (diameter, 4 to 6 µm). Because of this attachment, oocysts could then be more readily retained by the filter and therefore could subsequently be recovered during the elution and centrifugation steps. Pellets resulting from centrifugation were easily obtained when silica was added to tap water, while this was not true when no silica was added. However, when there were too many particles or the particles were too big, it was not easy to elute the particles from the filter. Consequently, some particles were retained on the filter, thereby reducing the recovery efficiency of the elution process. We found in this study that when silica particles in the size range from 5 to 40 µm were added to tap water to increase the turbidity to more than 10 NTU or when particles larger than 40 µm were added to tap water to obtain a turbidity of 5 NTU, various amounts of particles remained on the filter after the elution process. Furthermore, a large amount of particles may also affect the IMS step, as reported by Stanfield et al. (13) and Campbell and Smith (2). This was also noted from microscopic observations made in this study. We also noticed that most of the oocysts were entrapped on the background debris (from reservoir water or water to which silica was added) present on the slides (Fig. 2 and 3). In contrast, background debris was not present on the slides when tap water was used. As observed in this study, when silica particles in the size range from 5 to 40 µm were added to tap water to increase the turbidity to a level that did not exceed 15 NTU, the typical image of FITC staining appeared, as shown in Fig. 3, and we found that the oocysts could be embedded in a thin layer of background debris present on a slide. However, the oocysts were not blocked by the background. A similar phenomenon also occurred with DAPI-stained preparations. In contrast, when silica particles in the size range from 5 to 40 µm were added to tap water to increase the turbidity to more than 20 NTU or when particles larger than 40 µm were added to tap water to obtain a turbidity of 5 NTU, the corresponding background particles were present in large thick clumps, oocysts were found to be embedded within the clumps, and weak fluorescence from FITC and DAPI staining could be observed behind the clumps. It is therefore reasonable to believe that some of the oocysts were blocked from view and therefore could not be counted.
In this study, high levels of recovery (95.1% ± 3.4%)
following the IMS step were obtained for spiked reagent water.
Similar experiments were performed by Bukhari et al. (
1), as
well as by Campbell and Smith (
2). These authors reported levels
of recovery of 77.4% ± 5.6% for deionized water (data
after calculation) and 89.2% ± 30.4% for water with no
turbidity (data after calculation), respectively. The values
obtained in this study were, however, higher and more stable.
We also noted in this study that there was an optimal turbidity
in terms of oocyst recovery when silica particles in the size
range from 5 to 40 µm were added to tap water samples.
Deviating from this optimal turbidity led to a decrease in the
efficiency of recovery in the filtration step and possibly also
in the IMS step. The turbidities of the IMS concentrate increased
from 2,520 to 5,400 and 7,200 NTU when the turbidities of the
water were increased from 2.5 to 10 and 20 NTU, respectively.
The highest level of oocyst recovery was obtained when the water
turbidity was 10 NTU. It was possible that when the turbidity
of the water was more than 10 NTU, the recovery following both
the filtration stage and IMS was affected. Stanfield et al.
(
13) reported that the levels of recovery following IMS for
treated water were 96.1% ± 9.5%, while for raw water
they were only 48.9% ± 14.2%. Campbell and Smith (
2)
noted that an increase in turbidity from 0 to 60 NTU caused
the levels of recovery following IMS to decrease from 89.2%
± 30.4% to 62.4% ± 32.4%. A further increase in
turbidity to 611 NTU caused the levels of recovery following
IMS to decrease drastically to 29.0% ± 34.1%. However,
it should be pointed out that the negative effect of higher
turbidity in nature on IMS is still speculative as contradictory
conclusions have been reported. For example, Rochelle et al.
(
11) reported that the levels of recovery following IMS were
79.1% ± 12.4% when the turbidities of water concentrate
samples were between 210 and 11,480 NTU.
In this study, silica particles were used to adjust the water turbidity because they could readily represent the turbidity caused by inorganic particles. In addition, they could also simulate the effects of particles present in reservoir water conveniently since a full range of silica particles of the sizes typically present in reservoir water was easily obtainable.
In conclusion, results obtained in this study indicated that filtration was the most important step in terms of oocyst recovery and that suspended particles present in reservoir water could help improve oocyst recovery. In addition, we found that the recovery was affected by particle size and particle concentration. We propose that adding particles to a water matrix is a possible approach to improve oocyst recovery when method 1622 is used for oocyst detection.

FOOTNOTES
* Corresponding author. Mailing address: Centre for Water Research, Department of Civil Engineering, National University of Singapore, 10 Kent Ridge Crescent, Singapore 119260, Singapore. Phone: (65) 68742890. Fax: (65) 68742890. E-mail:
CVEONGSL{at}nus.edu.sg.


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Applied and Environmental Microbiology, April 2003, p. 1898-1903, Vol. 69, No. 4
0099-2240/03/$08.00+0 DOI: 10.1128/AEM.69.4.1898-1903.2003
Copyright © 2003, American Society for Microbiology. All Rights Reserved.
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