DRC-1998-001041 - 0901a06880805787

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NESIIAPS RADON FLIIX MEASUREME} T PROGRAM
White Mesa MiI1, 1998
Prepared for:
International Uranium (USA) Corporation
5425 S" Highway 191
Blanrling, Utah 845Ll-
Prepared by:
Tel1co Environmental
1231 N, 23 SE., Ste" 205
Grand .Tunetion, Colorado 81506
October 1-998
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NESHAPS RJADON FI,IIX MEAST}REMENT PROGRJN{
White Mesa MiII, L998
Prepared for:
International Uranium (USA) Corporation
6425 S. HighwaY 1-9L
Blanding, Utah 8451-1
PrePared bY:
Tel1co Envirorunental
l-23L N. 23 St-., Ste. 205
Grand ,function, Colorado 81505
Oct,ober 1998
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1.0
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Table of Contents
IN?RODUCTION
SITE DESCRIPTION
SAMPI,ER DESCRIPTION
FIEI,D OPERATIONS
4.L cenera1 Sit.e Specific Information
4.2 Sampler Placement
4.3 Sampler Retrieval
4.4 site Exit
4.5 Environmental Conditions During Measurement Periods
LABORATORY OPERATIONS
5.1 Introduction
5.2 Apparatus
5 .3 Analysis Procedure
5,4 Weighing and Background Counting
5.5 Receipt and weighing of Exposed Charcoal
5.6 Gamma Ray Counting
5.7 Quality Control Samples
5.8 Data Validation
5.9 Calculations
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6.O SAMPLE RESULTS/CAICULATIONS
Fi-gure 3-1, Large Area Activated CharcoaL Collector Diagram
APPENDICES:
A - Support Documents
B - Recount Data
C - Radon Flux Sample Laboratory Data and Field Bl-ank Data
D - Map PockeE, Figure 5-1
NESHAPS RADON FLIIX MEASUREMENT PROGRAM
International Uranium (USA) Corporation
White Mesa Mi1l
6425 S. Hwy. 191
B1anding, Utah 84511
1.0 INTRODUCTTON
Te1Ico Environmental L.L.C. (Tellco) provided support to International Uranium
(USA) Corporation (hereinafter, IUC) regarding their required National Emissj-on
Standards for Hazardous Air Pollutants (NESIAPs) Radon Flux Measurement effort on
Tailings Ce1ls 2 and 3 at the White Mesa Mi1l uranium processi-ng facility in
Blanding, Utah for the cal-endar year of 1998. These measurements are required of
IUC to show compliance with 40 Code of Federal Regulations, Part 51, Subpart W,
National Emission Standards for Radon Emissions from Operating Mi11 Tailings. At
present, there are no Subpart T uranlum mi1l tailings at this site. As required
by the regulations, the NESHAPs monj-toring for exi-sting mi1I tailings piles j-s a
flux standard that lj.mits the emission of radon from pi,les. The standard limits
the amount of radon that can be emitted per unit area (*') per unit of time (s).
This standard is not an average per facil-ity, but is an average per radon source.
According to subsection 51.252 Standard, (a) radon-222 emissions to ambient air
from an existing uranium mi1l tailings pile shall not exceed 20 pCi/m'?-s of radon-
222. Subsection 61-.253, Determining Compliance, states that: "Compliance with
the emission standard in this subpart shaLl be determined annually through the use
of Method 115 of Appendix B.'r
Te11co \4/as contracted to provide radon collectors, perform the field
placement/retrieval and sample analysi-s of the colLectors for calendar year 1998 -
This report addresses the procedures employed to obtain the resul-ts presented in
Section 5.0 of this report.
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)n SITE DESCRIPTION
The White Mesa Mi1l is located south of Blanding, Utah on Highway 191. The mi]l
began operations in 1980 for the purpose of extracti.ng uranium and. vanadium from
feed stocks. Processi-ng effluents from the operation are deposi-ted in four
ulined" cell-s which vary in depth. Cel"l-s 1and 4 are used solely for',liquor,,
storage, whi1e Ce1ls 2 and 3 are used for sand tailings/liquor deposition"
Ce1l 2 has a Eotal area of approximately 270,624 square meters (m'). This ce11
was comprised of two source regions that required NESHAPs radon monitoring:
approximately 233,095 m2 of the ce1I had a soil cover of varying thickness, wit.h
approximately 37 ,529 m2 of exposed tailings trbeaches". There was no significant
standi-ng liquid in ,,Iow" elevation areas within Ce]I 2.
Cel1 3 has a total area of 288,858 m2. This ce11 was comprised. of two source
regions that required NESHAPs radon monitoring: approximately 85,357 m'of the
cel1 had a soil cover of varying thickness, with approximately 40,396 m, of
exposed tailings 'rbeaches". The remai.ning approximately 163,105 m' was covered by
standi-ng 1j-quid in r\1ow', elevat,ion areas.
Due to worker health and safety concerns expressed by both rUC site personnel and
Te11co monitoring staff, a smaII portion of the areas of the wet beaches of Cell 2
and CeI1 3 were not sampled due to the extreme instabilit.y of wet tailings
beaches.
SAMPLER DESCRIPTTON
The Large Area Activated Charcoal Canist.ers (LAACC) used by Te11co personnel to
perform the required radon measurements were fabricated in conformance with "Radon
Flux Measurements on Gardinier and Royster PhosphogLpsum piles near Tampa and
Mulberry, Florida" (MIIS Document #PB85-1-51-8'1 4) as referenced in 40 CFR, part 51,
Method 115, Appendix B. This method of performing radon flux measurements
involves the adsorption of radon on activated charcoal in a large-area co]lector.
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The charged coll-ector is placed directly on the
and i-s allowed to col1ect radon for a given time
The radon collected on the acti-wated charcoal is
spectroscopy.
material surface to be measured
period (approximateTy 24 hours).
then measured by means of gamma
Each LAACC was constructed using a 10-inch diameter PVC end cap, spacer pads,
charcoal distribution grid, retainer screens, pads, and a steel retainer ring (see
Figure 3-1).
Prior to deployment, each collector was charged with 180 grams of baked charcoal
from sealed individual sample containers (reference Sectj-on 5.0 below for
laboratory procedures). After the 24 hour measurement period, the exposed
charcoal was transferred to the plastic sample containers, sealed ai-r-tight (with
tape), labeled as to sample identification along with exposure times/dates, and
transferred to the Tellco laboratory (Grand Junction, Colorado) facj-1ity for
analysis.
FTELD OPERATIONS
General Site Specific Information
Te11co personnel laid out baselines within the cover regions of Cel-1s 2 and 3, and
a grid coordinaLe locaLion system was developed to accommodate locatlng the
samplers in the fie1d.
The sampJ-i-ng effort commenced on Ehe morning of JuIy 21, 1998, after site specific
health and safety training was provided by IUC Health and Safety personnel on July
20, 1998. Te11co field technicians laid out the grid system on Ce1I 2 and CeIl 3
using a measurj-ng tape, pacing, and line-of-sighE markings. Boundary disEinctions
between the three source regions were establ-ished by vi-sual inspection and so
noted on the field maps. Tellco personnel placed a minimum,/maximum thermometer
within each of the two cel-ls, respectively, during samplingt, measuring ambient air
temperatures at the sj-te, to monitor compliance with the 35oF measurement
criterion.
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FIGURE 3_1
flGuRE 3-l Large-Area Radon Collector
I -in. Thick
Scrubber Pad
I /2.in- Thick
Scrubber Pad
I z2-in Ilrrcl Charcool
Support Grid
Retarnor
Spring
l0-in. dia
PVC End CaP
l/4-rn. Vent Holo
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Sampler Placement
Radon measurements were made in conformance with methods described in MIIS
Document #PBB6-1518'74 far each 100 sample measurement set for each source region.
In addition to the 100 samples, each sample set conslsted of 5t field bfanks. The
spacing distribution for each set of 100 measurements was determined by visual
means and a ',best fit., distribution pattern for each source region. Field
personnel safety was paramount in the distribution of samplers over "wet beach"
regions due to the loose, unconsolidated condi-tion of the saturated tailings,
which are simj-lar in consistency to "quicksand. "
Pl-acement/retrieval of colLectors was accomplished using vehicles where possible,
and by foot travel where vehicl-e travel was not feasible.
A collector was chosen and the retaining ring, screen and foam pad removed to
expose the charcoal support grid. A pre-measured charcoal charge was sefected
from a batch, opened and distributed evenly across the area of the support gri-d.
The collector was then re-assembled and gently pl-aced face down on the surface to
be measured. Care was exercised not to "push'r the device into the soil surface-
The col-lector rim was "sealed" to the surface using a berm of 1ocal borrow
material (either taillngs or soil) to reduce dj"lution due to air or wind currents
within the coll-ector.
A sample identification number was then asslgned to the collector. Sample numbers
utilized an alpha-numeric system composed of the charcoal batch l-etter (i.e., A,
B,C .) followed by a sequentj-aI number indicating the placement (i.e., 01,
02, . ) . This sample identification number was recorded on an adhesive labe1
and placed on the top of the coLlector. The sample ID, date, and time of
placement were recorded on a master data sheet for each set of measuremenLs.
During placemeut of charcoal flux collectors, five field blanks were collected.
The procedure for preparing a field blank was to charge a col]ector with charcoal,
and place it inside an air-tight container. The blank(s) remained in the sealed
collector for the 24-hour sample time period.
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4"3 SamIr1er Retrieval
Retrieval of the collectors followed the same pattern as placement. The
collectors were disassembled and the charged charcoal removed by pouring from the
collector into a large funnel suspended above a sample charge container. The
sample ID number was transferred to the charge container, which was sealed and
placed in a box for transport. The date and time of reLrieval were recorded on
the same data sheet as the sample placement information.
Each charged coflector was retriewed upon completion of the measurement time
peri-od (approximately 24 hours). Upon retrieval of the collectors, the field
blanks were retrieved and the charged charcoal returned to a container, sealed,
and labeled as such, and returned for analysis along with the measurement set.
Sample data sheets accompanied the shipment to the laboratory. During retrieval-
of LAACCs on Ce11 2 Beach region, one of the collectors (c13) was dropped while
the coll-ector was being handled, and the charcoal spilled, causing the sarq)le to
be 1ost.
The charcoal was inadvertentJ-y not loaded into one of the collectors (J04) that
was placed on the Ce11 3 Cover region. When the charcoal from the reErieved
collectors was being re-containerized, the collector J04 was identified as lacking
its charcoal load-
Te}]co personnel mainEained custody and assured timely deliwery of the samples to
the Te11co Grand Junctj-on laboratory for prompt analysj-s of the charcoal samples.
Site Exi-t
Tellco field personne)- and equipment were alpha scanned for possible contamination
resuJ-t.ing from fieldwork activities. A11 equipment. and field personnel were
surveyed and released for unrestr.icted use by IUC's HeaLth and Safety personnel'.
4.4
4.5 Environmental Conditions during Measurement Periods
Referencing 40 CFR, Part 51, Subpart W, Appendix B, Method 115 - Monitoring for
Radon-222 Emissions, Subsectiot 2.1.4 - Restrictions to Radon Flux MeasuremenEs,
,'the following restrictions are placed on making radon flux measuremenLs:
(a) Measurements shal1 not be initiated within 24 hours of a rainfall.
(b) If a rainfall occurs during the 24 hours measurement period, the
measurement is invalid if the seal- around the lip of the collector
has washed away or if the collector is surrounded by water.
(c) Measurements sha11 not be performed if the ambient temperaLure is
below 35oF or if the ground is frozen. "
Sitse Specific Diecussion
(a) Prior to commencement of any sampler placement, rainfall amounts (if
any) were ascerEained at the IUC weaLher staeion rain gauge and/or at
the rain gauge placed in the immediate area by Te11co field
personnel. A rainfall measuring 0.03" occurred during the 24-hour
period preceding placement of the collectors on the Ce11 3 Cover
region at the siLe. At the time that Lhe collectors were placed on
said ce1l 3 Cover region, the ground surface had completely dried
out, and IUC directed Tell-co personnel to proceed with placement of
the collectors on the region.
(b) The aforementioned rai,nfa11 measuring 0.03" occurred after the
collectors had been placed on the Ce]I 3 Beach region. A11 of the
col-lector seals from Ce11 3 Beach region remained intact, and none of
the collecLors were surrounded by water.
(c) During all 24-hour sample set placements, the minimum ambient air
temperature recorded by Te1lco at t.he site was 56"F, recorded
overnight Jvly 2a-22, 1998.
5.0 LABORATORY OPERATIONS
5.1 Introduction
Activated charcoal gas adsorption collectors are passive sampling devices used to
determine the flux rate of rador:-222 gas from a surface area. The charcoal
canister used consists of a 10-inch pVC cap containing a bed of 180 grams of
activated, granular charcoal pJ-aced in a distribution grid on top of a 1X inch
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thick layer
screen by a
of foam and secured under a % inch foam layer and a galvanized steel
retaining ring.
Sample collection is initiaEed by placing 180 grams of
sealed container into the above described canister
retai-ning ring, placing Lhe canisLer (open face down)
tested. Radon gas is adsorbed on the contaj-ned
radioactive decay of the entrained radon resulLs in the
lead-214 and bismuth-21-4 in the cani-ster.
Lead shielded counting well- approximately 4o
wal1s and a 7 cm thick base and 5 cm thick top'
NfST traceable aqueous sol-ution radium-225
activated charcoal calibration source.
unexposed charcoal from a
and, after securing the
onto the surface to be
charcoal and subsequent
occurrence of radioactive
cm deep with 5 cm thick lead
absorbed onto 180 grams of
These radon progeny isotopes emiL characteristic gamma photons which can be
detected. The original total activiEy of the adsorbed radon can be calculated
from these gamma ray measurements using empirical calibration factors derived from
cross-cali-bration of source standards containing a known total activity of radium-
226 in a geometry identical Eo the samples to be counted'
5.2 Apparatus
Single- or multi-channel pulse height analysis system, Ludlum Model 2200 with
a Teledyne 3't x 3" NaI(T1) detector.
5.3
ohaus Model C501 balance with 0-1 gram sensitivity.
Analvsis Procedure
Inapection of the Charcoal Container
Charcoal was received at the analytical laboratory in the sealed sanple
containers. Upon receipt, Lhe integrity of the container was verified by visual
i-nspecLj-on of t.he plastic container.
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Sam1>Ie Identificabion Nr:mbers
Each sample contai-ner had a
determined in the fieId, and
container.
un1que
written
sample
onto
idenLification number which was
a labef attached to the samPle
Drying and Recycling
AI1 charcoal was dri-ed before use in the field for
Procedures were the same for newly prepared charcoal
after field use. Charcoal was dried at approximately
were as follows:
radon flux measurements-
and for charcoal recYcled
110oC. Drying procedures
Oven temperature set to 1-10oC.
Charcoal placed in the oven i-n a metal baking tray'
Baked for 24 hours.
Immediately after the tray was removed, approximately 180 grams of charcoal
were transferred into clean sample containers and sealed with plastic tape'
5.4 weighing and Background Counting
Proper balance operation was verified daily by checking with a standard weight-
The balance readout should agree wit.h t.he known standard weight to wi-thin + 0.1t'
If a discrepant readout was obtained, the bal-ance was re-zeroed, the check weight
wiped with a soft, l-int-free cloth, and re-weighed. ff the discrepancy persisted'
the bal-ance would have been removed from service and tagged "out of Service ' " For
this project, the scale conformed for each day of use (see Appendix A, BaLalce
operation DailY Check form).
After acceptable balance checkout, each empty conEainer was individually placed orr
the balance and the Eare wei-ght of the container was documented to the nearest 0'1
grams on the }abe1. The scale was re-zeroed with the container on the balance'
Charcoal was carefully added to the container untsil the readout registered 180'0
grams. The 1id was immediately placed on the container and sealed with plastic
tape. The tape was stretched slightly while wrapping around the container' The
end of the tape was folded to form a tab for easy tape removal
checked for readout drj.ft between each container-weighing step.
The bal-ance was
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I Gamma ray counting system checkout was performed as described in Section 5.5. A
five-mj-nute background count was acqui.red for five containers seLected at random
to represenE the ,'batch.,' Each sealed container was placed individually in the
shielded counting well, with the bottom of the container centered on the detector.
Observed empty counting well background counts must fa11 wiEhin the average range
of approximately 123 to 176 cpm using the aforementioned Ludlum/Teledyne counting
system with shielded we1l. The background counE rate was then documented for the
five contai-ners, and subseguently documented on the respective "Radon Flux Field
Data SheeE', for that batch. If the background counts were too high to achieve a
suffj-ci-ent1y 1ow sensitiwity tevel- (Lower Level of Detection, LLD), the entire
batch was l-abeled non-conformi-ng and recycled through the drying process.
5 .5 Receipt and Weighing of Exposed Charcoaf
Containers of exposed charcoal were transported from the site and delivered to the
laboratory for analysis by Te11co personnel. The Te1lco laboratory staff was
responsible for weighing and inspecting the exposed canisters; inspecting the
documentation forms,. and entering the required data documentation to database
spreadsheets.
when the contai-ners were received, the following items were i-nspected:
o Container was c]osed and sealed with tape.
Contalner vras not damaged.
DaEa sheet was complete.
Discrepancj-es found during this inspection were documented on the data sheet.
Containers received open or damaged resulting in seal failure were considered void
and were not analyzed. A11 samples that were transported to the Te11co laboratory
were received there in good physicat condj-Eion; however, as previously mentioned,
one sample from Ce}I 2 Beach region and one sample from Cefl 3 Cover region were
lost i-n the fie1d.
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After receipt inspections, conforming containers were
nearest 0.1- gram and the gross weight was logged on
Sheet't under the appropriate column.
weighed on a balance to the
the "Radon Flux Field Data
5.6 Gamma Ray Counting
Source/Background Checks
The charcoal gamma ray counting system was subjected to performance checks daily
when used. These checks included background and radium-225 check source
measurements. (Appendix A of this report contains daily counting system
performance check records. )
Sauple Analyeis
e The length of count time was determined by the activity of the sample being
analyzed. A data quality objective establishing a mini-mum accruement of 1000
counts for any given sample was followed during sample analyses.
The sample container was placed in the counting well with the 1id si-de up and
the center on the NaI detector and the shielded well door was set into p1ace.
One sample count was accrued and the mid-sample counL tj-me and date was
documented on the field data sheet-
The sampLe counts were documented on the field data sheet for data reduction.
The above steps were repeated for each exposed sample collector.
. Approximatel-y 10t of the containers counted on a given date were selected for
recounting. These containers were recounted no sooner than 1 day and no
longer than 10 days following the original count.
5.7 Ouality Control Samples
Charcoal f L.rx measurement QC samples incl-uded the f o1J-owing intra-laboratory
analytlcal objectives as required in 4O CFR, Part 6a, Subpart W, Appendlx B,
MeEhod 115, 4.0 - Quality Assurance Procedures for Measuring Ra-222 Fh:x, D.:
. recounts, 10t, and
o field blanks, 5t.
2,
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5.8
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Data validation - Recounts/Blanks
A11 sample canister data were subjected to validation protocols. The following
presents the data validation results:
Forty-two recounL measurements were performed by conducting replicate analyses of
indiwidual field samples. These recount measurements comprised approximatsely L0t
of the toEal number of samples analyzed. The precision of a1I recount measure-
ments ranged from less than 1* to 8.7* with an overall average precision of
approximately 2.3*. This recount precision is weIl within the expected
variability of the analytical method.
Twenty-two field blanks were analyzed by measuring the radon progeny activi-ty in
samples subjected to all aspects of the measurement process, excepting exposure to
the source region. These blank sample measurements comprised approxi.mately 5* of
the fieLd measurements. The results of the blank sample analyses measured radon
flux rates, which ranged from 0.05 to 0.22 pCi/m2-s, with an arithmetic average
flux rate of O.10 pCi/m'z-s. This corresponds to approximately 0.58 of the
regulatory limit of 20 pCi/m'?-s.
The objective is 100 samples to
regulations. The following is
sampling program (EPA rules
objecti-ve):
be collected from each region, as specified by the
the actual completeness attained during Tellco's
and regulations specify an 85* completeness
100t completeness
99t completeness
99t completeness
1001 completeness
Ce11
Ce11
Ce11
Ce11
Cover - 100 samples
Beach - 99 samples
Cover - 99 samples
Beach - 100 samples
As presenged abowe, actual QC validation met the objective parameter requirements.
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5.9 CalcuLat.ions
Radon flux rates were cal-culated for charcoal collection samples using calibration
factors derived from cross-calibration to sources with known total activity with
identical geometry as Lhe charcoal containers. A yield efficiency factor was used
to calculate the total- activity of the sample charcoal containers "
In practice, radon fl-ux rates were calculated by a database computer program. The
algoriEhms utilized by the data base program were as follows:
Equation 5.1:
pci Rr'-22z/m,sec = tTS*A*b*:ffi1
where: N = net sample count rate, cpm under 220-662 keV peak
Ts = sample duration, seconds
b = instrument caLibration factor, cpm per pCi-; values used:
0.1660, for M-01/D-21 and
0.1711 , for M-02/D-2o
d = decay time, elapsed hours between sample mid-time and count
mid-time
A = area of the collector, m2
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Equatsion 5.2:
20error=2x
-/ "."=" =r*1.. "p- *" Sample count. t. min Bkgd count t. min
Net cPm (samPle concentratj-on)
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Equation 5.3:
2 -71 + (4.55) (S-)LLD =
where:. 2-77- =4.65 =
Ts=
b=
[Ts*A*b*O .5 (d/gr'zs) ]
constant
confidence interval factor
standard deviation of the background count rate
sample duration, seconds
instrument calibration factor, cpm per pCi-; values used:
0.1560 , for M-01-,/D-21 and
o . 1711, for M-02 /D-2o
decay time, elapsed hours between sample mid-time and count mid-time
area of Ehe co11ect.or, m2
d=
A=
6.0 SAMPLE RESIILTS / CAISULA'TIONS
Referencing 40 CFR, Part 51, Subpart W, Appendix B, Method 115 - Monitoring for
Radon-222 Emissj.ons, SubsecLion 2.1.7 - Calculations, "the mean radon flux for
each region of the pile and for the toLal pile sha11 be calculated and reported as
follows:
The individual radon flux calculati-ons shal1 be made as provided in
Appendi-x A EPA 85 (1) . The mean radon flux for each region of the
pile sha1l be calculated by summing all individual flux measurements
for the region and dividing by the toEal number of flux measurements
for the region.
The mean radon flux for the total uranium miII tailings pile shal1 be
calculated as follows:
- JrAr + JrA, [+l J,At"\
(a)
(b)
Where: J" =
T_uI -
l_nl-
4=
Mean flux for the total pile (pCi,im'?-s)
Mean flux measured in region i (pci/m'?-s)
Area of region i (m2)
Total area of the pile (m'?)
2-1.8 Reporting. The resuLts of individual flux measurements, Ehe
approximate locations on the pile, and the mean radon flux for each
region and the mean radon flux for the total stack [pile] shal1 be
included in Ehe emissj-on tesL report. Any condit.ion or unusuaL event
that occurred during the measurements that coul-d significantly affect
the results should be reported. "
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Site Specific Sa:qrle ReauIUs (reference Figure 5-1)
(a) The mean radon flux for each region within each ce11 is as follows:
CelI2-CoverArea
- Beach Areas
= 9.8 pCi/m2-s (based on 233,095 m2 area)
= 4L.9 pCi/m'?-s (based on 37,529 m2 area)
Cell 3 - Cover Area = 23.g pCi/m'z-s (based on 85,35? m2 area)
- Beach Areas = 55.4 pCi/m'?-s (based on 40,395 m2 area)
- Standing Liquid Areas = 0 pCi/m'?-s (based on 163,105 m2 area)
Note: Reference Appendix B of this report for entire summary for
individual measurement resul-ts and specific sample regi-on maps.
(b) Using the data presented above, we have calculated the total mean radon flux
for each pile (ce11) as follows:
Ce11 2 = 1,4.3pCi/m'?-s
(9. 8) (233 . 095) + (41.9) (37. 529)
27 0 ,624
CeI13= t4.9pCi/m'?-s
(23.8) (85.357) + (56.4) (40.396) + (0) (163.105)
288, 858
15
APPENDIX
SupporL Documents
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BALANCE OPERATION DAILY CHECK
Balance Model . Ofl4U5 ForJ - o - a,,-a,^ sev'4 t2-3o1
I st andard wei ght ( g ) : -
3oo' O
t Date pre-check (9) post-check (s) o.K. r o. tx By
3d9 _O
_=============
t/q
- 7r----ba-1tz je-o
TltnlqR Joo, o 30o, o Ye-3 4r
7l*drr 3 o,t, o 3oo' a /c-S t ar
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CHARCOAL CANISTER ANALYSIS SYSTEM
T<l( ,,> L",b
Tnt t rv,,a*' r 6a o'l Llvaq, wr-^
SITE LOCATION:
CLIENT:
I
t
System ID: IvtO D--z
Scaler SA.I: g l51Z L Mo D
DetectorS/N: o41533 COz f)
Calibration Check Log
CalibrationDate: Z I V ( q g
HighVoltage: lO 5O Window:
Source ID/SN: 1o,2-zl. Gt- o&
-tDueDate: >[blg1
*'4-> Thrshld: 7-7o
Blank Canister Bkgd. Range, cpm: 2 o -tz1 ,o La) :o= LIJ to L b.Z
Gross Source Range, cpm:2c: q4qV to 7o341 36= nZ-b4 to
rechnician: \>/ Cf--
Source Activity: 59 '3 K f ci
^--to9> f
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14
7fe
Po
Pt'ctb:l
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y/n: y -- average background and source cpm falls within the control limits.
n: average background and source cpm does not fall within the control limits.
The acceptable ranges were determined from prior background and source check data.
All counts times are one minute.
DATE BY BKG
#t
BKG
#2
BKG
#3
BKG
AVG
SOURCE
#l
SOURCE
#2
SOURCE
#3
SOURCE
AVG.
ok'l
ylr.
1 lLv lm 41,(-17t 145 rt9 rt)loo t+4 16oG root'b aa44 Yt tc-olaQ Dtl 5L t4l tLn t+r qol'LD qq'a \99t"L qq \1 v
7tL7t 19 c,ir )€L t<{/{o , -r,7 b;3 /i.1 0t /Dt t../ilrt,) {/y
'7 l)11 gq qF tl^l ,4'7 ,l-7 15-lo t o 6 to3to ta at .l /0 , Dt Y
7ltK17'nqr I LO tvo t;7 ,i3 /Dlb8 lo33 6 /o t r;-,8 lo ats7 v
TltelEx WD t 3Ll I.J .L '1,\o / 5.r-/o 3C.,..t D Aq-r /0t8-f in)y4/
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CHARCOAL CANISTER ANALYSIS SYSTEM
a-(t(.-, L.,bSITE LOCATION:
CLIENT:f nkrnerl)o^ c- | l)r'a 't iq r-t
L*) z-zoo [^t 4d-2ocalibration check l-og
System ,r,
*- twot I Drl calibrarion ou"' 5lv lq?, DucDare:,;la{qg
scalersN: sr5f z CVr oD Highvortage: loSD Wirrtlow: 4' 4 2 't'lrrshltl: 2'z o
DetectorstN,o4t133LDl.D,o,,..ID/SN:WSourccActir,ity.57:}lLf{1
3o= lt4 to tBOBlenk Canister Bkgd. Range, cpm: 2 o = I 21
Gross Source Range, cpm:2o= q b1'7-t"= 453t,o rD3ll
b t1 b
ro loLnI
p,<-
(*)
?r-
P"5
P j-e
fctl
Technician:
yln: y = average background and sourcc cpm falls within thc control linrits.
n = average background and source cprn does not fall within the cortnol lintits.
The acceptable ranges were determincd from priorbackground and source check drta.
All counts times arc one minute.
DATE BY BKC
#t
I]KG
#2
I]KG
#3
BK(;
AVC
SOUITCE
#l
S()URCE SOURCI'
tt3
SOTIRCT:
AVG.
ok'.)
yitr
i lzblqo uyk-t 5-)('>-)t3 r->141 q Lrlc g-r 5f tor r(?.Bt r tl
1l2r'lqb 9tzz rf4 tvb t1l-t5')-loocaL)t)(fL't Q tlol o)9ab v
tlrzli\1 aT t.{L , L3 l.fo / CLI t009</acqg lD) L/)/ t)/'1 {/Y
1 l?7 111 A-r tl. I r17 /t,,{9 t )o 23 tn n7O /a)\o /Oi/-;vl ltsls t *Ld It^o t40 -;1 /ot&1 r Dl9L /Dt9y raL9l 1/
1 lt tnt t4>T t Ttl /./ )150 /Js t Dotb / o o '18 tolTD /nn8,f {u
LwJ.zzoo f uul- 47-to calibration check I os
system to,**-lul o> f D Zo caribratio[ Date: 5lvlaO DueDarc: 5 | t"loot
Detecror Srr.r, o 41 532- clzo) source rD/SN ,wr_b 95' o+
2o= lL3 o tQ4
zo= qqBO ro
Technician: ../t
yln: y : average background and source cpnr lalls wrthin tlrc conrrol linrirs.
n = average background and sourcc cpm does not lirll ivithin the conrrol liurits.
The accepuble rangcs wcre determined lionr prior background and sourcc clrcck dara.
lo=- I lJ.-rn
3o= q166
t1+
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Pos
CHARCOAL CANISTEIT ANALYSIS SYS'I'EM
srrElocArroN:-
- 1zlt"u Lo$-
CLIENT:T n ttt-Aq*,o^a \ Ur^A'tv( Y4
5'5b3 High Volrage: j7_q 9 Window: 4'+L t'lrrslrld: '2,2O
Blank Canister Bkgd. Range, cpm:
Gross Source Range, cpm:u'' I \O4 I
All counts times arc onc minute.
DATE BY UKU
#t
BKG
#2
I]KC
il)
T]KC
AVC
sot.ll{ct:
itI
soL lt((:li
il2
s()t ,l{('t
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okl)
y/n
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7 ^7'119 AF I.CL lrl<i3q ro L00 / 0/,8 5 tO-i.9,/o l, )A1rqlg(6-r , <o l,to t 3-7 ),1 L roA2l /oetl ta.'t ? L /0? f t Y1lt*ls x t7 t<l /..E r1 /40 t-{o j 0 e,J7 I oTot tDLoT /0Ly-7 Yv
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CHARCOAL CANISTER ANALYSIS SYSTEM
a< t(c., LabSITE LOCATION:
CLIENT:f tfe r nalioa 4 t lArqut r * 11
f.
frs
L,,^,l.zzoo / Lud.i+-"D calibration check Log
Sysremn,-iOz / p'Zo catibrationgor"' 5fblq8 ,urorr"' ;lt lgos
scatcrsN: ft5Uf (moz-) HighVolragc: -Jt9* wi,dorv: *4'+l- I'hrsSttl: z,Zo
Detectorsn-t, O4t5 SZ (Dzo) SourceID/SN t ?a-tb G9o5 SourccAcririry: 5q3 *PL;
Blank Canistcr Bkgd. Range, cpm: 2 o = \ Z*n lva 3o--.t16 o-r13
Gross Source Range, cpm:2o= t@ol _ro-tO"l43 to= ltst{
Techniciarr: Z/k
yln: y = avcrage background attd s6urr:c cpm talls within thc colltlul linlils.
n - average background and sourcc cpm does not tall within thc cotttrol lintits.
The acceptable langes were dctermined from prior background and source chcck data.
Pre
All couns times are one minute.
APPENDIX
Recount Data
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