Contents
CONTENTS ...1
1 INTRODUCTION ...2
2 MATERIAL AND METHODS...6
2.1 X-RAY ...6
2.1.1 Angiographic procedures ...6
2.1.2 Computed tomography...8
2.2 NUCLEAR MEDICINE...9
2.2.1 External irradiation ...9
2.2.2 Internal irradiation ...10
3 RESULTS AND DISCUSSION...12
3.1 X-RAY...12
3.1.1 Angiographic procedures...12
3.1.2 Computed tomography procedures ...16
3.2 NUCLEAR MEDICINE ...16
3.2.1 External irradiation ...18
3.2.2 Internal irradiation ...19
4 CONCLUSION ...24
5 ACNOWLEDGEMENTS ...26
6 REFERENCES ...27
1 INTRODUCTION
The use of ionizing radiation in medicine is of special concern when applied to women in fertile age, due to the possible irradiation of a foetus. In diagnostic medicine this applies especially to female patients undergoing examinations or interventions using X- rays or radionuclides, as well as to pregnant staff involved in such procedures. Patient examinations are governed by the ALARA principle. It states that all examinations that involve ionizing radiation should be optimized. Naturally, only examinations that are considered justified for obtaining relevant and necessary diagnostic information of the patient should be performed. In addition, special regulations apply to women in fertile age who undergo examinations involving irradiation of the lower trunk and/or pelvis region. Provided these guidelines for patients are properly taken into account, there are very few situations in diagnostic medicine in which the absorbed dose to the foetus will exceed 100 mGy, considered a relevant abortion indication level (ICRP Publication 84 (2000)). With female medical staff, the problem of foetus irradiation becomes more complex, as in this case the unborn child is treated like a member of the general public, with a dose limit of 1 mSv (effective dose) during the gestational period (ICRP Publication 84 (2000)).
The protection of the unborn child from radiation is indeed very important because the foetus is particularly sensitive to its harmful effects (ICRP Publication 84 (2000)). The type of effect will depend on the gestational age of the embryo at the time of irradiation.
The post conception period can be divided into three major phases. These are 1) the preimplantation phase, 2) phase of major organogenesis (3rd to 8th week post- conception), and 3)foetal development (9th week until birth) (ICRP Publication 84 (2000)). The last phase includes the development of the central nervous system (CNS).
Radiation risks are most significant during organogenesis and early foetal period, somewhat less in the second trimester and least in the third trimester (ICRP Publication 84 (2000)). The most severe deterministic effects of prenatal exposure to ionizing radiation are intrauterine mortality (IU), organ malformations, and mental impairment.
Stochastic effects (leukaemia, solid tumours, and genetic anomalies) are also included
in the list of possible radiation induced effects from foetal exposure. The radiation risks at different gestational age of the foetus have been summarized by Fattibiene et a1 (1999), see table 1.
Table 1
Major effects of prenatal irradiation during different gestational periods [3].
Embryonic or
foetal age (wk) Development stage Effects 0 -2 Pre- implantation;
implantation Abortion
3 - 7 Early organogenesis IU mortality
Organ malformation 8 - 15 Brain development
stage I
IU mortality SMR Epilepsy attack
Decreased IQ 16-25 Brain development
stage II IU mortality
SMR
>25 IU mortality
Whole pregnancy Child. fatal cancers
IU - intrauterine mortality SMR – sever mental retardation IQ - Intelligence Quotient
Based on a national survey carried out by ISPESL (National Institute for Occupational Safety and Prevention, Italy), Parisi et al (1994), reported that 30% of hospital female staff working with nuclear medicine and X-rays were exposed to effective doses higher than 1 mSv during one year1. For comparison, in 2004 and 2005 approximately 60% of nuclear medicine staff (nurses) at Karolinska University Hospital/Site Solna was exposed to yearly effective doses of at least 1mSv.
Although radiation doses to occupationally exposed staff working with radiological equipment are generally low, the results presented by the Italian research group indicate that the situation with a pregnant female staff requires special attention, especially as there is no threshold dose under which stochastic effects are not believed to be operative
1 In case of homogeneous, whole body, gamma and X-ray exposures, the effective dose (mSv) can be considered equal to the absorbed dose to any organ in the body.
under the concept of the LNT-model (LNT=Linear No Threshold; ICRP Publication 84 (2000)).
The aim of this work was to define guidelines on how to interpret the dosimeter readings for staff involved in high-dose procedures in X-ray and nuclear medicine applications, such that the foetal dose for pregnant staff will not exceed the limit of 1 mSv. The absorbed dose to the foetus depends on several factors. In X-rays the main factors that influence (staff) foetal dose are type of equipment, exposure parameters (incident beam quality, exposure time), and irradiation geometry, size of irradiated volume, and material and thickness of protective apron. In nuclear medicine, the (staff) foetal dose due to internal and external contamination of the mother depends on the energy of the radionuclide, activity (Bq), decay modes (γ, β, α), if is inhaled or ingested, acute or prolonged intake, and the foetal stage and foetus size. Data on these parameters can be input to physio-biological models in order to estimate foetal dose (ICRP Publication 88 (2001)). It can be concluded that for radionuclides that do not cross the placenta, the foetal dose is derived from the radioactivity in maternal tissues. With radionuclide that potentially can cross the placenta and concentrate in a specific organ, such as 131I in the thyroid gland, foetal irradiation can cause conditions like permanent hypothyroidism (ICRP Publication 84 (2000)). According to ICRP 84, 99m Tc does not cross the maternal placenta. However, it has been shown that 99mTc (NaTCO4) (sodium pertechnenate) has the potential to cross the placental barrier (Isopharma AS (IFETEC code: MO.3S)).
In order to evaluate how these factors impact on foetal dose, a survey of published data on foetal dose to staff from a variety of diagnostic X-ray and nuclear medicine examinations was carried out. As data on staff foetal dose from positron emission tomography (PET) examinations were limited, PET studies were excluded from this survey. However, it should be noted that the contribution to staff foetal dose from PET examinations is not negligible considering that the PET nuclides (18F, 11C, 15O) yield annihilation photons of high energy. The contribution from PET nuclides to the staff dose is expected to increase due to that the amount of PET examinations is rapidly increasing. The survey was complemented by additional measurements on X-ray and
nuclear medicine staff working at the Karolinska University Hospital/Site Solna, in Stockholm.
Based on the results of this study, the recommended threshold dose of 2 mSv (entrance dose) measured on the abdomen of a female worker, and suggested by the ICRP in Publication 84 (2000), was assessed.
2 MATERIAL AND METHODS
Initially, procedures in X-ray and nuclear medicine applications that can deliver high doses to staff were defined. These include angiographic and computed tomography (CT;
especially with trauma-patients) procedures in X-ray. In nuclear medicine, staff exposure relates to the handling of radionuclides with high activity and/or high energies, and from patients whom have had nuclides injected or orally administered for examinations or therapy. Direct handling of nuclides (extraction, injection and oral administration) can result in external and/or internal contamination of nuclear medicine staff. Such exposure can be augmented due to possible contamination also of laboratories/examination rooms.
2.1 X-RAY
2.1.1 Angiographic procedures
Publications on foetal dose in X-ray focus on different kinds of angiographic procedures. This work summarizes the techniques used and the major results reported by four groups: Kicken et al (1999), Mcparland et al (1990), Osei and Kotre (2001), and Faulkner and Marshal (1993). In order to compare the results from the different groups, special attention was given to the type of examination, beam quality, irradiation geometry, and to the technique used for dose estimation.
Irradiation geometry
Most angiographic procedures are performed using undercoach X-ray tube and overcoach image intensifier (II). This geometry is illustrated in figure 1. All groups report results using this geometry. Osei and Kotre (2001) and Faulkner and Marshall (1993) additionally report results using overcoach tube/undercoach II.
Figure 1. Schematic presentation of the most common irradiation geometry used in angiographic X-ray procedures; reproduced from [6].
Foetal equivalent dose versus entrance dose
In the article by Osei and Kotre (2001), Monte Carlo simulations of foetal dose to staff in angiographic procedures were performed assuming a mean foetal depth of 8 cm (i.e.
distance from a block-shaped phantom surface to the mid-plane of an inner phantom representing the uterus (see figure 2)). To validate the Monte Carlo results, TLD measurements were made using an Alderson female anthropomorphic phantom.
Experimental verification was performed both in scattered (geometry as in figure 1) and in primary radiation beam.
Figure 2. Schematic presentation of the irradiation geometry used to estimate staff dose using the Monte Carlo simulation method. The outer block represents the trunk of an adult staff member, and the inner block represents the uterus. Reproduced from [6].
Results presented by other groups Kicken et al (1999), Mcparland et al (1990) and Faulkner and Marshall (1993) are based on similar irradiation geometry (see table 2).
Consequently, a mean foetal depth of 8 cm was assumed to be representative for the results of foetal equivalent dose versus entrance dose also in these studies.
2.1.2 Computed tomography
Under normal conditions, computed tomography (CT) examinations are performed such that staff leaves the examination room during acquisition of image data. In this way, radiographers and other medical staff stay in radiation protected areas during the CT examination, and there is no need for additional protective barriers, such as lead aprons, to reduce staff doses.
However, in some situations staff needs to stay close to the patient during CT-scanning.
A typical example is patients suffering from some kind of trauma that requires a close-
to-patient assistance from medical staff during the CT-examination. In order to evaluate staff doses from such procedures, measurements using a diode dosimeter (EDD-30;
Unfors Instruments) were performed on a total of eight trauma patients undergoing CT- examinations of the trunk at the emergency ward at the Karolinska University Hospital/Site Solna. In CT, the patient dose can be estimated from the dose-length- product (DLP; [mGycm]). The DLP-value for each patient was then used together with the measured staff dose to calculate a staff dose burden coefficient [μSv/mGycm]. All measurements on staff were performed with the dosimeter positioned on the waist level below a protective apron (0.25-0.35 mm Pb equivalence).
2.2 NUCLEAR MEDICINE
Publications on foetal dose (staff) from nuclear medicine procedures focus on the one hand on external irradiation originating in the patient and from contamination of clothes and the body surface, and on the other hand on internal irradiation due to ingestion or inhalation of radionuclides. This work summarizes the results in publications focused on estimating foetal dose to nuclear medicine staff (Stather et al (2003), Barber et al (2003), Mountford and Steele (1995), Alvem (2002) [private communication]). In order to compare the results from the different groups, special attention was given to the irradiation source, work task, and to the techniques and/or models used for dose estimation.
2.2.1 External irradiation
Mountford and Steele (1995) used 99mTc and 131I to irradiate an Alderson anthropomorphic phantom equipped with TL-dosimeters at different depths, thus simulating different foetal stages. The foetal dose was estimated at a reference depth of 7,1 cm, corresponding to the mean midline foetal abdominal depth along an anteroposterior (AP) projection, averaged over the full period of pregnancy (range 6.0- 8.5 cm). Based on measured attenuation factors together with published data on exposure time and dose rate, they report maximum effective dose for the mother (staff) and foetus from one examination.
Based on their results, the corresponding ratio (foetal/maternal effective dose) was then calculated in this work.
Alvem (2002) reports on the dependence of the dosimeter reading on its position on the trunk. Double dosimeter measurements (one at breast level plus one at abdominal level) were performed on 11 non-pregnant staff members during a period of 4 weeks. All types of work tasks (preparation and measurements of activity of radionuclides, injection, cleaning and patient handling) typical of a nuclear medicine department were being monitored during this period. The results were used to calculate a conversion coefficient between the measured doses at breast level (normal dosimeter position) to the dose at abdominal level (CFbreast/abdomen).
Using data from Mountford and Steele (1995) the ratio of effective dose foetus/staff doseabdomen (see table 3), together with data of CFbreast/abdomen from Alvem (2002), the ratio of effective dose foetus/staff dosebreast was estimated by:
breast foetus abdomen
breast
abdomen foetus
tivedose Staffeffec
ose Effectived CF
tivedose Staffeffec
ose Effectived
=
/
/ (1)
2.2.2 Internal irradiation
Stather et al (2003) report different intake scenarios in order to estimate foetal doses due to inhalation and ingestion of radionuclides. They applied the biokinetic and dosimetric models suggested in ICRP Publication 88 (2001) in order to calculate foetal dose following radionuclide intake by the mother both before and during pregnancy.
Barber et al (2003) performed whole-body counter measurements on staff in charge of cleaning following 131I-treatment of patients. Measurements were performed before the on-set of cleaning (pre-cleaning internal+external contamination), directly after the cleaning was completed (post-cleaning internal+external contamination), and after changing into clean clothes (post-cleaning internal contamination). They did not report any results from purely external contamination in their series of measurements on cleaning staff, and assumed that the contribution from external contamination could be
disregarded. They calculated the cumulative effective dose to the foetus from data on the dose coefficients for the foetus at different foetal stages following acute maternal intake by ingestion of 131I. They used dose coefficients reported by the National Radiological Protection Board (NRPB) (2001), which are based on the model for iodine by Berkovski (1999).
In order to estimate the ratio of effective dose to the foetus and to the mother in this work, data on the effective dose to a non-pregnant woman following injection of 131I (non-saturated thyroid gland) was taken from ICRP Publications 53 (1998) and ICRP Publications 80 (1998) and was combined with the results by Barber et al (2003).
According to the ICRP data, an administered activity of 1 kBq 131I to an adult female yields an effective dose of 24 µSv/kBq. The ratio of the foetal dose coefficients by NRPB (2001) and the ICRP estimated adult female effective dose, was calculated according to equation 2, and used as an estimate of the foetal/maternal effective dose ratio:
Mother Foetus kBq
Sv ose
Effectived
kBq Sv oefficient
Do
adult
foetus =
) / (
) / ( sec
μ
μ (2)
Alvem (2002) reports staff total body internal contamination detected by whole-body counter measurements on eight nuclear medicine staff members at the Karolinska University Hospital/Site Solna, following administration of 99mTc with a mean administrated activity of 2.5 GBq.
The cumulative effective dose to the foetus from daily internal contamination of 99mTc (nuclear medicine nurses) and 131I (cleaning staff) was then estimated in this work by using data from Alvem (2002) and Barber et al (2003) on administered versus detected activities together with foetal dose coefficients ICRP 88, according to equation 3.
Cumulative effective dose
∑
= − − + −
= n
i
i i
i
i x f x f x
x
1 ( 1)( ( ) ( 1))
2
1 (3)
xi = week index no; i=[0,5]; i = 0 (week no 0), i = 1 (week no 5), i = 2 (week no 10), i = 3 (week no 15), i = 4 (week no 25), i = 5 (week no 35) f(xi) = dose coefficient data (ICRP 88)
3 RESULTS AND DISCUSSION
3.1 X-ray
3.1.1 Angiographic procedures
The results reported by four groups on staff foetal dose from X-ray angiographic procedures are summarized in table 2.
Table2
Staff foetal dose from X-ray procedures. Summary of methods and results reported by four groups.
Reference Method Staff/phantom Irradiation
geometry Procedure Mean staff entrance dose per procedure (µGy)
Foetal equivalent dose per procedure (µSv)
Ratio equivalent dose to the uterus and entrance dose Kicken et
al (1999)
TLD at abdominal level, outer surface of a 0.5 mm lead apron
Operator Undercouch tube and overcouch image intensifier
Cerebral arteriography
Abdominal arteriography
Peripheral arteriography Percutaneous translumina angioplasty
22 58 51 75
240 (m.d.p.p)
0.4 1.2 1.0 1.5
4.8 (m.d.p.p)
0.018 0.021 0.019 0.02
0.02 (m.d.p.p) McParland
et al (1990)
TLD at waist level under the 0.25 mm lead apron
Cardiologist
Nurse
Undercouch tube and overcouch image intensifier
Cardiac
catherization 78 (max) 21 (min)
31 (max) 14 (min)
29 (max) 7.8 (min)
11 (max) 5.2 (min)
0.37 (max) 0.37 (min)
0.35 (max) 0.37 (min) Osei and
Kotre (2001)
1) Monte Carlo (EGS4)
Block- shaped phantom
Both of overcouch and undercouch tube
Fluoroscopy 0.038
(a, oc,o.l.a, 0.25mm Pb,MC) 0.37 ( a, oc, u.l.a, 0.25mm Pb,MC) 0.047 (a, uc,o.l.a,
2a) TLD at waist;
secondary radiation
2b) TLD at waist both over and under 0.25mm lead apron;
primary radiation
Alderson female Rando anthropo- morphic phan-tom
Both of overcouch and undercouch tube
0.25mm Pb,MC) 0.37 ( a, uc, u.l.a, 0.25mm Pb,MC)
0.24-0.40 (u.l.a, 0.05- 0.35mmPb)
0.5 (u.l.a,0.25m mPb)
Faulkner and
Marshall (1993)
Film at chest and waist level under a lead apron;
secondary radiation
Alderson Rando phantom
Both of overcouch and undercouch tube
Fluoroscopy 0.09 (oc,at
90kVp, u.l.a, c.l ) 0.14 (oc,at 90kVp,u.l.a w.l ) 0.35 (uc,at 90kVp, u.l.a, c.l ) 0.29 (uc,at 90kVp,u.l.a w.l ) m.d.p.p (the maximum dose per procedure), [4]
a, oc, o.l.a,0.25mm Pb; MC (average at tube potentials 61,90 and 112kVp, overcouch tube , over lead apron, 0.25 mm equivalent lead, Monte Carlo simulation), [6]
a, oc, u.l.a,0.25mm Pb; MC (average at tube potentials 61,90 and 112kVp, overcouch tube , under lead apron, 0.25 mm equivalent lead, Monte Carlo simulation), [6]
a, uc, o.l.a,0.25mm Pb; MC (average at tube potentials 61,90 and 112kVp, undercouch tube , over lead apron, 0.25 mm equivalent lead, Monte Carlo simulation), [6]
a, uc, u.l.a,0.25mm Pb; MC (average at tube potentials 61,90 and 112kVp, undercouch tube , under lead apron, 0.25 mm equivalent lead, Monte Carlo simulation), [6]
oc.at 90 kVp, u.l.a, c.l ; (overcouch tube, at 90 kVp tube potential, under lead apron and independent of lead apron thickness, at chest level), [7]
oc.at 90 kVp, u.l.a, c.l ; (overcouch tube, at 90 kVp tube potential, under lead apron and independent of lead apron thickness, at waist level), [7]
oc.at 90 kVp, u.l.a, c.l ; (undercouch tube, at 90 kVp tube potential, under lead apron and independent of lead apron thickness, at chest level), [7]
oc.at 90 kVp, u.l.a, c.l ; (undercouch tube, at 90 kVp tube potential, under lead apron and independent of lead apron thickness, at waist level), [7]
Influence of irradiation geometry on foetal dose
The effect of irradiation geometry on foetal dose has been studied by Osei and Kotre (2001), and by Faulkner and Marshall (1993). Their results are illustrated in figures 3 a- b and 4, respectively.
a) Entrance dose measured in front of lead apron
0,00 0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,00
0,05 0,10 0,15 0,20 0,25 0,30
Overcoach X-ray tube
Equivalent dose to uterus / entrance dose
Lead thickness [mm]
61 [kVp]
90 [kVp]
112 [kVp]
0,00 0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,00
0,05 0,10 0,15 0,20 0,25 0,30
Undercoach X-ray tube
Equvalent dose to uterus / entrance dose
Lead thickness [mm]
61 [kVp]
90 [kVp]
112 [kVp]
b) Entrance dose measured behind lead apron
0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,20
0,25 0,30 0,35 0,40
Overcoach X-ray tube
Equvalent dose to uterus / entrance dose
Lead thickness [mm]
61 [kVp]
90 [kVp]
112 [kVp]
0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,20
0,25 0,30 0,35 0,40
Undercoach X-ray tube
Lead thickness [mm]
61 [kVp]
90 [kVp]
112 [kVp]
Equvalent dose to uterus / entrance dose
Figure 3. Ratio between the equivalent dose to the uterus and entrance dose at waist level of a staff member standing beside the patient during a fluoroscopy procedure. Data were generated using Monte Carlo simulations [6]. Results using a 0.25 mm lead apron at 90 kVp (representative of the clinical situation) are indicated by the dotted lines.
70 80 90 100 110 0,00
0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,40
Equivalent dose to uterus / entrance dose
Tube potential [kVp]
c.l,u.l.a,oc w.l,u.l.a,oc c.l,u.l.a,uc w.l,u.l.a,uc
c.l,u.l.a,oc - chest level; under lead apron; overcouch x-ray tube w.l,u.l.a,oc - waist level; under lead apron; overcouch x-ray tube c.l,u.l.a,uc - chest level; under lead apron; undercouch x-ray tube w.l,u.l.a,uc - waist level; under lead apron; undercouch x-ray tube
Figure 4. Ratio between the equivalent dose to the uterus and entrance dose estimated from film badge readings at chest and waist level under a lead apron of a staff member standing beside the patient during a fluoroscopy procedure [7]. Results at 90 kVp are indicated by dotted lines.
The measurements by Osei and Kotre (2001) on an Alderson female Rando Phantom using TL-dosimeters yielded similar results to the Monte Carlo simulations. With the set-up depicted in figure 1 and including both over- and undercoach tube geometry, the ratio between equivalent dose to the uterus and entrance dose measured under a lead apron (0.05-0.35 mm Pb) was in the range 0.24-0.40.
From table 2 it can be concluded that all four groups report similar conversion factors between uterus dose and entrance dose with undercoach X-ray tube geometry. In case of entrance dose measurements performed with a detector positioned in front of a lead apron, the uterus dose is below 10% of the detector dose for typical beam qualities and with an apron thickness >0.25 mm Pb equivalence. With a detector positioned behind the protective lead apron, the uterus dose is always below 40% of the detector dose for apron thickness up to 0.35 mm Pb equivalence.
3.1.2 Computed tomography procedures
In this series of measurements on trauma patients, the mean DLP value was 2705 ± 934 (1 STD) mGycm, and the staff dose burden coefficient was 1.6 ± 5.6*10-4 (1 STD) nSv/mGycm. Assuming a DLP of 5000 mGycm per examination, and that the uterus dose amounts to 40% of the staff abdominal dose, such an examination would imply a foetal dose of approximately 3.2 µGy.
3.2 NUCLEAR MEDICINE
The results reported by four groups (including one private communication) on staff foetal dose from in nuclear medicine procedures are summarized in table 3.
Table 3.
Staff foetal dose from nuclear medicine procedures. Summary of methods and results reported by four groups (including one private communication).
Reference Method Staff/Phantom Irradiation source
Procedure Maximum effective doseto the mother from one patient (µSv)
Maximum effective dose to the foetus from one patient (µSv)
Ratio of effective dose to the foetus versus maternal dose1 Mounford
and Steele (1995)
TLD - at abdominal level for different source to phantom distances, and at different depths.
Imaging technologist
Nurse (clinical ward)
99mTc
131I
131I
99mTc
Bone Lever Dynamic renal
Thyroid ablation (w-b.c) Thyroid therapy (w-b.s)
1.53 0.23 0.35
8.9 11.8
155 63 29 4.7 2.3
1.12 0.17 0.26
6.7 9.0
86 37 18 3.3 1.6
0.73 0.74 0.74
0.75 0.76
0.55(pc.t.h) 0.58(pc.p.h) 0.62(pc.cf/bf) 0.70 (pc.s.a) 0.69 (pc.t.a) Barber et
al(2003)
Whole-body counter.
The iodine model of Berkovski
Cleaning staff Intake by ingestion
131I 0.003(f.s.0w)
0.003(f.s.5w)
(1999) and NRPB(2001) used to calculate the foetal effective dose.
0.008(f.s.10w) 0.5 (f,s.15w) 1.42(f.s.25w) 2.30(f.s.35w)
Stather et al(2003)
Biokinetic and dosimetric models given in ICRP Publication 88 (2001) used to calculate the foetal dose coefficient.
Intake by inhalation
90Sr
131I
99m Tc
Intake by ingestion
90Sr
131I
99mTc
0.04 (b.c.-26) 0.10 (f.s.0 w) 0.31(f.s.25w) 0.26(f.s.35w)
0.01 (b.c.-26) 0.01 (f.s.0 w) 0.01(f.s10.w) 1.62(f.s.25w) 2.84(f.s.35w) 0.01 (b.c.-26) 0.01 (f.s.0 w) 0.02(f.s10.w) 0.02(f.s.25w) 0.02(f.s.35w)
0.03 (b.c.-26) 0.09 (c.0 w) 2.25(f.s.25w) 2.50(f.s.35w)
0.01 (b.c.-26) 0.01 (f.s.0 w) 0.01(f.s.10w) 1.55(f.s.25w) 2.73(f.s.35w)
0.01 (b.c.-26) 0.11 (f.s.0 w) 0.70(f.s.10w) 0.91(f.s.25w) 0.81(f.s.35w) Alvem
(2002) TLD- at the breast and abdominal level
Nuclear medicine nurse
99mTc Ratio breast
to
abdominal dose:
1.15±0.46 ( 1 STD)
1 For external irradiation, the maternal dose corresponds to the abdominal surface dose; for internal irradiation it is given by the dose inhalated or ingested by the mother.
Data related to references [9],[10] and [11] were calculated from their corresponding published results.
w-b.s – ( whole- body scan) [ref]
pc.t.h – (patient category totally helpless) [9]
pc.p.h – (patient category partially helpless) [9]
pc.cf/bf – (patient category chair/bedfast) [9]
pc.s.a – (patient category semi -ambulant) [9]
ps.t.a – (patient category totally ambulant) [9]
intake at indicated time; negative times are prior to pregnancy [10]
b.c.-26 –acute intake 6 months before conception [10]
f.s.0 w – acute intake at time of conception [10]
f.s.25w - intake of 25 weeks of foetal stage [10],[11]
f.s.35w - intake of 35 weeks of foetal stage [10, [11]
STE – standart deviation of mean (standard error) [15]
3.2.1 External irradiation
Based on the results presented by Mountford and Steele (1995), the ratio of the effective dose to the foetus and the dose registered on the abdominal surface of the pregnant staff was calculated. The results for an imaging technologist performing patient studies were almost identical for both 99mTc and 131I, with a foetal/maternal dose ratio close to 0.73- 0.75. For a nurse at a clinical ward, the corresponding ratio was in the range 0.55-0.70 depending on the caring needs of the patient (data only for 99mTc). These results indicate that the foetal dose from external irradiation of the mother is almost independent on the type of nuclide and type of work task, and yield a mean ratio foetal/maternal effective dose close to 0.7 (0.69 ± 0.08 (1STD)) for a dosimeter positioned at waist level.
As regards the dependence of the dosimeter reading on its position on the trunk for nuclear medicine staff, Alvem (2002) reports a dose reading breast/abdomen ratio of 1.15± 0.46 (1 STD). This results in a mean ratio foetal/maternal effective dose for a dosimeter positioned at breast level (external irradiation) of about 0.6 (0.59 ± 0.12 (1STD)).
3.2.2 Internal irradiation
Dependence of gestational age on foetal dose
The dependence of gestational age on the foetal versus maternal dose from inhalation and ingestion for different nuclides as reported by Stather et al (2003), (2002) is presented in figure 5a and 5b. The dose ratio for both 131I and 90Sr display a significant dependence of gestational age. The sharp increase in the relative dose to the foetus for
131I and 125I after the first trimester is related to the increased uptake once the thyroid gland is fully developed (Stather et al (2003), Stather et al (2002)). 90Sr is chemically similar to calcium, and can cause a significant uptake in the skeleton towards the end of the gestational period. This is pronounced in case of ingestion of 90Sr, in which case the placenta easily transmits this nuclide (Stather et al (2003), Stather et al (2002), Phipps et al (2003)). 99mTc is a short lived radionuclide that does not cause large fetal doses, especially in case of inhalation, as the nuclide does not cross the placenta (ICRP publication (2000)). The foetal dose for 99mTc is then derived from the radioactivity in maternal tissue. Comparing the two most commonly used radionuclides, 131I and 99mTc, it can be seen that for an acute maternal inhalation after the first trimester, 131I results in a higher effective dose ratio than 99mTc. This reflects the different type of decay and half-life of these nuclides, with 99mTc being a short-lived nuclide (half-life=6.02 h) and has a γ- dacay, while 131I has a beta minus (β-) decay and a significantly longer half-life (8 days).
-30 -20 -10 0 10 20 30 40 0,0
0,5 1,0 1,5 2,0 2,5 3,0
Ratio of effectiv dose foetus/mother
Foetal stages [Week]
90Sr
99mTc
125I
131I
137Cs
Inhalation
Figure 5a. Ratio of the effective dose to the foetus and to a female staff member following an acute maternal inhalation of different nuclides [10], [19]. Foetal stage “0” indicates the moment of conception.
-30 -20 -10 0 10 20 30 40
0,0 0,5 1,0 1,5 2,0 2,5 3,0
Ratio of effective dose foetus/mother
Foetal stages [Week]
90Sr
99mTc
125I
131I
137Cs Ingestion
Figure 5b. Ratio of the effective dose to the foetus and to a female staff memberfollowingto an acute maternal ingestion of different nuclides [10], [19]. Foetal stage “0” indicates the moment of conception.
Dependence of intake scenario on foetal dose
The results of the calculation of the ratio of effective dose foetus/mother in case of ingestion of 131I, using the same dose coefficient data as in Barber et al (2003), are displayed in figure 6. Corresponding results reported by Stather et al (2003), using dose coefficient data from ICRP Publication 88, are included for comparison, together with their data on inhalation. As can be seen in figure 6, there is a discrepancy between the two data sets on ingestion. This is despite the fact that the dose coefficient data used by Barber et al (i.e., NRPB (2001)) are identical to the ICRP data (Publication 88). It is assumed that this reflects different techniques in maternal dose estimation. However, as Stather et al (2003) do not give details on how they estimate maternal dose, it was not possible to verify this assumption.
-30 -25 -20 -15 -10 -5 0 5 10 15 20 25 30 35 40
0,0 0,5 1,0 1,5 2,0 2,5 3,0
Ratio of effective dose foetus/mother
Foetal stages [Week]
Ingestion [Barber],[Calc by Narine G.]
Inhalation [Stather]
Ingestion [Stather]
Intake scenarios of 131I by inhalation and ingestion
Figure 6. Ratio between the effective dose to the foetus and to the mother at different gestational age due to internal contamination with 131I [10, 11]. Foetal stage “0” indicates the moment of conception.
Whole-body counter measurements of internal contamination as reported by Alvem (2002) for nuclear medicine nurses (99mTc), and by Barber et al (2003) for cleaning staff (131I ) are summarized in figure 7.
0 2 4 6 8 10 12 0,00
0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,40 0,45 0,50 0,55 0,60 0,65 0,70
Detected activity [kBq]
Administreted activity [GBq]
99mTc (Nuclear medicine nurses)
131I (Cleaning staff) Internal contamination
Figure 7. Whole body counter measurements of internal contamination of cleaning staff [11], and nuclear medicine nurses [15], respectively, after changing clothes.
In the case of 99mTc, the mean activity administered (2.5 GBq) was considered typical for nuclear medicine nurses during one day. The corresponding cumulative effective dose to the uterus during a pregnancy was estimated according to the method by Barber et al (2003), and using dose ingestion coefficients from ICRP Publication 88 (2001); [se table 4], together with maximum (0.32 kBq) and mean (0.11 kBq) internal contamination activity (Alvem (2002) [se table 5]).
Table 4
Dose ingestion coefficient in utero for 99mTc and 131I (ICRP 88 [13]).
Dose ingestion coefficient [µSv/kBq]
Foetal stage (Week no)
99mTc 131I
0 0.0097 0.078
5 0.0094 0.081
10 0.015 0.21
15 0.017 12.0
25 0.017 34.0
35 0.016 55.0
Table 5
The cumulative effective dose to the foetus from regular intake of 99mTc by nuclear medicine nurses, based on dose ingestion coefficients and maximum and mean contamination activities during one day.
Effective dose from regular intake [µSv]
Foetus at
Week max - 0.32 [kBq] mean - 0.11[kBq]
5 0.018 0.005
10 0.038 0.012
15 0.064 0.021
25 0.091 0.030
35 0.117 0.039
In the case of 131I, corresponding dose estimations were performed for the maximum detected activity, that is, 0.68 kBq Barber et al (2003). According to Barber et al, their results should be considered “worst case” as regards internal contamination of cleaning staff working close to patients undergoing 131I therapy due to very strict cleaning routines in the UK. The result is shown in table 6.
Table 6
The cumulative effective dose to the foetus from regular intake of 131I by cleaning staff, based on the dose ingestion coefficient (see table 4, ICRP 88) and maximum contamination activities during one day.
Effective dose from regular intake [µSv]
Foetus at Week
max-0.68 [kBq]
5 0.27
10 0.76
15 21.5
25 177
35 480
The results show that the foetal dose due to internal contamination from 99mTc for nuclear medicine staff is insignificant, and can be neglected at the time of estimating staff foetal doses. In case of internal contamination of 131I, the foetal dose can be considerably higher, and routines to estimate such dose burden to pregnant staff should be considered. A reasonable approach seems to be to exclude pregnant staff in the third trimester from working with 131I.
4 CONCLUSION
X-ray
Radiation doses to staff in X-ray diagnostic radiology are in general low. Procedures that, under normal work conditions, potentially could yield doses in excess of the current foetal dose limit of 1 mSv during the full length of the pregnancy, are angiographic examinations (including interventions), and CT procedures on patients in trauma conditions.
Based on the publications included in this study, and including a “safety margin”, a dose ratio factor of 2 between the dose registered by a dosimeter positioned below a lead apron (at least 0.25 mmPb) and the dose to a foetus is suggested. This means that an accumulated dose during pregnancy (i.e. sum of dosimeter readings) of 2 mSv, measured behind a lead apron at the surface of the trunk (breast or waist level), is the threshold dose to a pregnant staff member working in X-ray diagnostic radiology in order to maintain the foetal dose below 1 mSv.
Computed tomography examinations on trauma patients often involve the assistance by staff not wearing dosimeters. The dose measurements performed during CT-scanning of the thorax-abdomen region of adult trauma patients in this work indicate a staff dose burden coefficient of approximately 1.6 nSv/mGycm (measured below lead apron at waist level). Assuming a maximum DLP of 5000 mGycm during which staff is standing beside the trauma patient, and applying a dose ratio factor of 2 for the dose to the foetus, would restrict the number of such examinations for a pregnant staff member to 250 during the pregnancy. This maximum DLP is almost twice the DLP estimated for such examinations in this study, and therefore yields a very conservative estimate of the maximum number of patients for which a pregnant member of staff can assist.
This recommendation naturally implies that the dose limits applied for other body parts, such as hands, are not exceeded, and that the pregnant staff member is not exposed to ionizing radiation while performing other work tasks.
Nuclear medicine
In nuclear medicine, the foetal dose depends on if the irradiation of the mother is external or internal.
The foetal dose from external irradiation of the mother is almost independent on the type of nuclide (99mTc, 131I) and type of work task (nuclear medicine nurse, cleaning staff), with a mean ratio foetal/maternal effective dose close to 0.7 (0.69 ± 0.08 (1STD)) for a dosimeter positioned at waist level. Corresponding data for a dosimeter positioned at breast level was about 0.6 (0.59 ± 0.12 (1STD)).
Foetal doses from internal contamination of the mother depend on the type of intake (inhalation/ingestion), type of radionuclide, and gestational stage of foetus. For 131I there is a very steep increase in the effective dose ratio foetus/mother in the period 10- 35 weeks post conception, starting with a dose ratio of about 1%, increasing to almost a factor of 3 at the end of the pregnancy. The results are almost identical for both inhalation and ingestion. For 99mTc there is a marked difference between the foetal dose due to maternal inhalation compared to ingestion, with a very insignificant foetal dose from inhalation during the whole gestational period (about 1-2% of maternal dose), while ingestion yields substantial foetal dose starting from 10 weeks post conception (maximum about 90% of maternal dose). This difference is most likely related to that intake by ingestion of 99mTc has the potential to cross the placenta, and thereby contributing substantially to foetal dose.
In general, staff foetal dose from internal contamination of 99mTc can be neglected, and only external irradiation needs to be considered. In this case, an accumulated dose during pregnancy (i.e. sum of dosimeter readings) of 1.5 mSv, measured behind a lead apron at the surface of the trunk (breast or waist level), can be used as the threshold dose to a pregnant nurse in nuclear medicine, in order to maintain the foetal dose below 1 mSv. In case of 131I, internal contamination can no longer be neglected, especially during the third trimester of pregnancy. As it is difficult to properly monitor internal contamination, it is suggested that pregnant staff do not participate in work with 131I starting from the third trimester until the end of the pregnancy. This is especially important in case of cleaning staff caring for patients undergoing 131I therapy. Following such a recommendation, the reported threshold dose of 1.5 mSv), should ensure that the foetal dose is within the 1 mSv limit.
5 ACNOWLEDGEMENTS
I am very grateful to my main supervisor, Dr. Annette Fransson, for her guidance and encouragement, and to my co-supervisor Dr.Linda Persson for introducing and helping me in understanding work and measurements in nuclear medicine and for interesting conversations.
This diploma work would never have been accomplished without the help from these people. It has been interesting and enjoyable working with them.
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