AAPM T utorial Patient
Dose
Lawrence Patient
dose
gram
assessment different
is the
fect
.
for
Ofthe dose
best and
indicator discusses
PhD
PhD
in mammography especially
and
ment.
Balter,
in Mammography1
N. Rotbenberg,
al reasons,
dose
Stephen
for
is important evaluation and
types
and
of risk
comparison
must
of imaging
ofdosc
that
can
be
of patient
risk.
The
author
measurement
he
to a patient
measured
for
sever-
in a screening techniques
measured,
pro-
and mean
reviews
equip-
glandular
factors
that
af-
of dose.
INTRODUCTION
Patient dose is an important consideration in mammography. Patient dose is measumed for several reasons: (a) to evaluate the risk to the patient, a very important consideration when screening programs are set up in which large numbers of asymptomatic women will be imaged and for which a benefit-risk analysis should be performed; (b) to compare competing imaging techniques, such as screen-film mammography, xeromammography, or new image receptors; (c) to assess the perfonmance of mammographic equipment, both as part of the initial acceptance testing and during periodic quality control testing; (d) to answer questions from the patient and various physicians involved concerning dose; and (e) to comply with various regulations and guidelines related to mammography dose (one from the American College of Radiology [ACR] in its accreditation process, others from vanous states with regulations and guidelines for mammography) This article reviews different dose parameters, factors that affect dose, and measurement of dose. .
U DOSE PARAMETERS Which dose should be measured
and
which
dose
should
be reported?
It may
be
easier to measure certain quantities, yet more appropriate to report a different quantity that can be calculated from those measured quantities. Various dose parametens that might be considered are the in-air exposure at the position of the entrance surface of the breast (X,) the dose to the entrance surface of the breast ,
Abbreviations: = National S’steme Index
From 10021.
to the RSNA.
of Radiology. Cl)RH and Measurements,
= Center br l)evices NEXT Nationwide
and Radiological Evaluation of X-ray
Health. ‘Frends.
NCRI’ SI
Internationale terms:
RadioGraphics I
ACR American College on Radiation Protection
Council
Breast 1990;
the Department From the 1988
radiography.
radiation
dose
l)osimctry
#{149}
Physics
#{149}
l0:’39-6 of Medical Physics. Memorial Sloan-Kettering Cancer (;entcr. I 2’S \ork RSNA scientific assembly. Received and accepted April 10. 1990. Address
Ave. New reprint
York. NY requests
author. 1990
739
(D5) dular
the dose to the midline of the breast (Dmid) and the mean dose to the glantissue of the breast (Dg . av). The in-air surface exposure is easy to measure with an ionization chamber. This measure is useful for quick comparisons of different techniques that employ constant beam quality. However, if the beams are of different quality, surface exposure may not be representative of either the absolute or relative risk. In addition, this measure does not indicate the accumulated dose incurred when multiple ,
,
views
are obtained.
The surface dose is similarly easy to determine from the in-aim surface exposure, and it can also be measured directly on the patient on in phantoms. Measurements of surface dose result in overestimations of the absolute risk and are not repmesentative of relative risk at different beam qualities. Also, if two on more views of the breast are taken, the surface doses for the two views cannot be simply added to get an estimate of the total risk. Midline dose is difficult to measure directly. It is somewhat representative of
the risk
to the glandular
but it represents an underestimation for screen-film mammography. the best indicator of the risk to the patient from a mammographic examination, because it is commonly assumed that the cancem risk is linearly related to the dose and that breast cancers anise in the glandular tissue. Mean glandular dose cannot be measured directly but must be calculated of risk The
with
the
made breast sue,
tissue
for the low-energy mean glandular
results
of simple
in calculations will be firmly not
containing
measurements
to determine compressed glandular
per and lower) surfaces breast tissue composed analyses,
the
tissue,
is made
tissue
and
in that
tabulated
values.
The
assumptions
the mean glandular dose (1 ,2) are that (a) (Fig 1); (b) there is an outer layer of adipose that
of the breast of a uniform
assumption
50% glandular
of the breast,
beams used dose provides
(Fig 2) ; and mix of adipose
that
central
is roughly
there
0.5 (C)
cm
thick
on the
the
tis-
outer
(up-
there is a central portion of and glandular tissue. For most
is a mixture
of 50%
adipose
tissue
and
region.
Exposure measurements are normally made and then converted to dose values by multiplying by the f-factor (the exposure to dose conversion factor) The f-factons for glandular and adipose tissue, which are relatively constant over the range of beam energies used in mammography, are shown in Figure 3 Some calculations assume a single average value of about 0.79 rad/R. The unit used to express exposure in the international system of units (SI) is coulomb per kilogram (C/kg); however, it may be more convenient for our purposes to work in roentgens (R). The dose should be reported in SI units of gray (Gy) on milligray (mGy) and previously has been reported in rad or millirad. .
.
Figure
4 shows
qualities
screen-film dose
due
depth, dular ferent
the exposure
mammography, to the
which
lower-energy
is the midline
and
there beam
dose,
tissue dose for xemomammography. entrance exposures are shown
receptors, layers
how
at xemomammognaphy
and of the
the attenuation
beams
employed
with
and
absorbed
dose
screen-film
is more
rapid
employed.
due
(1 .2 mm
for different
Also,
the
below
is also
absorbed
dose
the average
different
a grid.
of the exposure
For these particular examples, to the different sensitivities of aluminum
beam
without
attenuation
is significantly
depth
vary
mammography
due
at 2 cm
value
of glan-
two difof the image
to the half-value
for xeromammography The mean glandular
0 .3 mm of aluminum for screen-film mammography) for these two exposures is 0.60 mGy (60 mrad) for screen-film 2 1 5 mGy (2 1 5 mrad) for xeromammography.
For
and
and dose
.
mammography
and
.
740
#{149}RadioGrapbics
#{149}Rothenberg
Volume
10
Number
4
x rays
x rays
ICDR
R
1. Drawing demonstrates the effect of firm compression on breast contour. The compressed breast (right) is essentially spread out laterally and made more uniform in thickness, so that x rays traverse less thickness (r) Consequently, a shorter cxposunc time is required, with corresponding reduction in dose. Scattered radiation reaching the image receptor (R) is also reduced, which significantly improves image contrast. The resulting improvement is indispensible in screen-film mammography. (Reprinted, with permission, from reference 3.) Figure
TT7//
T
Uniform
Mix:
[POS:-Gland
Uniform
1’
(i-i)
:LL
Phantom
.
Adipose
Adipose-Gland
Mix
Figure 2. Drawings of the compressed breast and two simple models to estimate dose. Transverse (a) and sagittal (b) diagrams of the firmly compressed breast show how compression makes the outline of the central, gland-bearing portion of the breast more nearly rectangular. (C) Computational model for determining average glandular dose (with a uniform mix of adipose and glandular tissue) r thickness measured in centimeters. (d) Computational model for average whole breast dose. Outer, hatched area in a, b, and C represents skin and outer adipose layer of thickness of 0.5 cm. (Reprinted, with permission, from refer-
Adipose
0
.
.5
‘;.
to
0 0
.0 0 U)
.0
ence
3.)
0
0 U)
Exposure-to-dose conversion factors for monochromatic x-ray beams
0 0.
w
1.(
0
1
2
-
-#{149} water
...
3
0.E
4
Depth (cm) Schematic shows x-ray exposure and absorbed dose versus depth for screenfilm mammography and xemomammography. The upper set of curves is representative of beams used for xeromammography (half-value layer of I .2 1 mm of aluminum) and the lower set of curves is typical of beams used for screen-film mammography (half-value layer of 0.3 1 mm of aluminum). Solid lines Figure
4.
refer to x-ray exposure; sorbed
dose
the entrance
to glandular
surface,
dashed tissue.
lines to ab-
1990
-
o
-
ar
-
mammary gland
-#{149}--------
V
0 0
,
adipose
U 0
,‘
tissue
-I,
0_i
-
0.4
-
On the left is
with exposure
nepnc-
sentcd by the solid line. The exposure decreases from the surface layer into the mix of adipose-glandular tissue and then into the exit surface layer. The rectangular frame of the graph represents a breast approximately 4 cm thick when compressed. The outer sunface layers (0.5-cm-thick regions on the left and right) do not contain glandular tissue. Computed average glandular doses per view are 0.60 mGy and 2. 1 5 mGy, respectively, for screen-film mammography and xeromammography. (Reprinted, with permission, from reference 3.)
July
o.
10
20 Photon
30
40 Energy
60 (key)
Figure 3. Graph depicts variation tors with photon energy for water, my gland, and adipose tissue.
Rothenberg
of f-facmamma-
U
Ra4ioGrapbics
U
741
FACTORS AFFECTING DOSE
Several following
factors affect discussion,
dose for a properly exposed mammogram. (Throughout a concurrent change in milliampeme seconds may often
the also
be assumed to maintain a properly exposed mammogmam or xeromammogram.) If a longer exposure time is necessary to fulfill increased exposure requirements, an extra increase in the overall exposure may be required because of mcciprocity law failure. In other words, the required film exposure and its accompanying patient dose will not be determined by a single tube current-exposure time
product (mAs); for some greater for a long time-low product. At higher kilovoltages,
screen-film current with
mammography product than
an appropriate
to maintain the same image density, theme penetrating x-ray beam produced but also Three-phase and constant-potential x-ray trating beam than single-phase generators, from a high ripple to a constant-potential
systems, for a short
reduction
the requirement time-high current
in milliampere
is
seconds
will be a reduced dose due to the more some loss of subject contrast. generators will provide a more peneso that as the voltage waveform changes shape, the dose will be somewhat me-
duced. Again, some slight loss in contrast may result from a constant potential waveform, compared with that from more varying waveforms. The effect of changing the x-ray tube target from a tungsten to a molybdenum is that there will be more low-energy trum. In a shift from tungsten to molybdenum, will be improved. There may be a choice offilter type, such target
photons the
in the molybdenum dose will increase,
as molybdenum
and
speccontrast
or aluminum
filters,
with different tube targets. Filters of special metal such as rhodium or of different thicknesses may be used. In general, as the filters are varied to make a beam of higher half-value layer, the dose will be somewhat reduced and so will the contrast. A change of the x-ray tubefocal spot should produce no effect on dose. The compression device, which is used for essentially all mammographic exposures, forms part of the overall filtration of the machine, and its thickness and matenial will affect the half-value layer of the beam. In addition, increased compression on the breast will spread the tissue out further and make the compressed breast less attenuating, a characteristic that results in a reduced dose. Patients with greater breast thickness (of the same composition) will require a higher dose. As thefraction ofadipose tissue to glandular tissue changes toward more adipose tissue as it does in older women, there will be reduced absorption,
which will lead More scattered
to lower
required
dose.
radiation will be removed as the grid ratio goes up; thus, milliampere seconds must be greatly increased to get a properly exposed image. The transmission factor of the grid will be important in determining how much additional exposure is required when a grid is used. In general, compared with nongrid techniques, the doses are raised by a Bucky factor of 2-3 when a typical lowratio grid (5 : 1) is used for mammography. As scattered radiation is reduced by the grid, the dose to the patient must be increased to maintain proper film density. Theme are a variety of screen-film image receptors, including different speed screens, different speed films, single screens, double screens, single-emulsion films, and double-emulsion films. Whatever changes are made to increase the me-
cepton
742
5
Ra4ioGrapbks
speed
#{149} Rothenberg
will
lead
to a reduction
in dose.
Volume
10
Number
4
1.3
i
1 .2 I
Mammography General Diagnostic
-U-
t,
.
0..
Figure
a,
:
,
5.
variation
lI
_n%D
1 .0
..
measurements
#{149}#{149}a
.
I
-
0.1
10.0
(mm Al)
There are various development tunes of the development chemicals
chemicals, forfllm
(solid
times of development, processing. As these
are
and temperaadjusted to
to have
mately
and
source-image
distance.
techniques,
the overall
As the
changed. An increase in the magnification tient, since the breast will be relatively However, in magnification radiography,
tened
radiation
is already
In that
geometry.
case,
reduced theme
due
may
choose
used in the and filters
an ionization
is moved
factor
and
up
the
source-
approxi-
down
for the image
will
to the aim gap built
be only
a small
increase,
into
designed
be
any magnification
no change,
compared with with a grid.
that
on even
resulting
measurement of dose include the ionization chamber, for the half-value layer measurements. It is desirable
chamber
for
will lead to increased dose to the pacloser to the target for the same technique. the grid may not be needed because scat-
duction in dose for magnification radiography conventional screen-film radiography performed
Instruments electrometer,
breast
magnification
and
(dotted ranges. layer.
increase the speed of development, dose will be reduced. Adjustments of distance can be made on many of the machines, image distance varies from one unit to another. Newer units tend a 65-cm
mam-
line)
general diagnostic line) x-ray energy HVL halfvalue
I
#{149}
1.0 HVL
magnification
factor
in the
mography 0.9
shows
with beam quality for ionization chambers designed for
Ia.,. (
Graph in correction
specifically
for the low-energy
a re-
from
to
MEASUREMENT OF DOSE
beams
used for mammography, particularly screen-film mammography. The ionization chamber should have an appropriate collection volume to give a reasonable size signal for the exposure being measured, and it must have a well-known, preferably almost constant, energy response in the mammography energy mange. This may me-
quime that the materials of the chamber walls be different from those used in chambers employed for routine diagnostic x-ray measurements in the 60- 1 50 kVp range. Figure 5 shows correction factors for a chamber designed specifically for mammography measurements
July
1990
dosimetry versus those at higher half-value
for a chamber layers.
designed
for
general
diagnostic
Rothenberg
#{149}RadioGrapbics
#{149} 743
TLD
Relative sensitivity
1.0
-
C C 1.01 c’J
0.9
_f
0.9c
Figure 6. Graph shows variation in sensitivity of a thermoluminescent dosimetcr (in this case, lithium fluoride
TLD-
1 00
shaw/Filtrol,
with
0.8
.
0.8C C,)
ci
[Har-
0.7
7
Clevelandi)
beam
half-value
quality.
HVL
=
0.25
0.50
Table 1 Average
.00
1.25
FirstHVL
Glandular
Breast
Dose
(D5N)
Molybdenum
Thickness (cm)
per
Unit
Target
and Beam (mmAl)ofo.3P
Exposure
Tungsten
in Air
Target
and
1.50
1.75
2.00
225
ImmAl)
(rad/R) Beam
HVLs
(mm
Al)
of
HVL 0.30
0.80
1.00
1.20
1.40
1.60 0.710 0.665 0.630 0.595 0.565
3.0 3.5 4.0 4.5 5.0
0.220 0.195 0.175 0.155 0.140
0.220 0.200 0.185 0.170 0.150
0.470 0.430 0.396 0.365 0.335
0.535 0.490
0.595 0.550
0.455
0.515
0.425 0.395
0.480 0.450
0.645 0.605 0.570 0.540 0.510
5.5
0.125
0.140
0.315
0.375
0.425
0.485
0.540
6.0 6.5
0.115 0.105 0.095
0.125 0.110 0.100
0.295 0.275 0.260
0.350 0.330 0.310 0.290 0.275
0.400 0.380 0.360 0.340 0.325
0.460 0.435 0.415 0.395 0.375
0.515 0.490 0.470 0.445 0.425
7.0 7.5
0.245
8.0
0.230
Note.-HVL - Only one
beam
half-value quality
lybdenum
spectra
does
layer. Reprinted, with permission, is given, since the half-value layer not
Thermoluminescent in the
change
dosimeters
measurements served
0.75
layer.
on the actual use
the dosimeter
measurements,
made, which
particularly are used
much
may
also
patient
of thermoluminescent
chips
raphy
very
and
their
reference
3.
molybdenum-mo-
kilovoltage.
be used
for
Several
mammographic
precautions
exposure
have
to be ob-
materials. In particular, the selection of and annealing are important. In mammogenergy correction, shown in Figure 6, must be
handling
a significant
for beams for screen-film
surfaces.
with
from of the
with half-value mammography.
layers of 0.3-0.4 mm of aluminum, Fading corrections are also me-
quimed if the dosimeters are exposed and not read out for a significant length of time. Aluminum filters used in mammography measurements should be thin, about 0. 1 mm. The aluminum filters that may come in a standard quality assurance pack for routine diagnostic measurements may be as thick as 0.5 on 1 .0 mm, which is inappropriate for measuring half-value layers in mammography, particularly for the beams for screen-film imaging. The filters should have uniform thickness and also be of high purity: 99% purity (type 1 100 aluminum) on better. Impurities of
high-atomic-number ment
744
#{149}RadioGrapbics
of beam
#{149}Rothenberg
materials quality
for x-ray
can significantly beams
used
change
the results
of the measure-
in mammography.
Volume
10
Number
4
Table 2 Typical Values
of Mean
Glandular
Dose
Mammographic Technique Screen-film’ All examinations Examinations
Mean
Average Glandular
0.93 with
Examinations
grids
without
1.28
0.55
grids
Xenomammographyt All examinations Positive Negative
3.94
mode mode
examinations examinations
4.08 3.40
Note-Adapted from reference 8. #{149} Doses for a 4.7-cm-thick compressed tissue. t
Doses
Value of Dose (mGy)
for a 5.0-cm-thick
compressed
breast
of 50% adipose
tissue
and
50% glandular
breast
of 50% adipose
tissue
and
50% glandular
tissue.
Although cases,
the average
it is convenient
glandular
dose
to tabulate which is the
glandular dose DgN, face of the breast. Measurements exposure
the
in air.
tables
to the
to arrive
Tables
(4)
.
are then
measured
made
values
at reasonably
to be reported
in most
are
sun-
machine
of
at the mammography
multiplied
accurate
average entrance
by the
estimates
values
of DgN from
of the average
glandular
dose
patients.
sources,
ments
These
is the quantity
on to obtain tables of the normalized dose pen unit exposure in air at the
of values
of
including
the
(NCRP) With these
breast,
which The types
posune
match
it with
the
target
and
provided
,
half-value
the measured in-air used either to generate
of testing,
such
control,
can
as the
by a number
Protection
and
be made
used
of the
of a variety
used,
and
obtain
If only
of acrylic and into the beam.
related
should be of materials whose composition with a range of thicknesses from about
a factor
dose. cx-
reproducibility
look
for
is be-
a consistent
to the adipose-glandular
mimics 2 to 8 cm.
with
glandular
on for other of the automatic
reproducibility
of materials.
block is put
in measurements
layer
of
Measure-
Health (CDRH) of the compressed
exposure to obtain average new tables of DgN values
evaluation
one could use a simple each time the block
Phantoms
1 have been on Radiation
as Table Council
(3) and the Center for Devices and Radiological tables, one can locate the appropriate thickness
to multiply phantoms
ing tested, sure reading
such National
DgN,
expo-
tissue
the actual Among the
mix
tissue composition, phantom materials
commercially available for this purpose are BR- 1 2 (5) which closely simulates a 50% adipose tissue-50% glandular tissue mix, and RF-1 and RM-1 (6), which simulate fat and muscle, respectively, such that an appropriate combination of the two can simulate different compositions of the breast. The acrylic phantom used ,
as part
thick
of the
ACR
compressed
In summary,
accreditation
process
(7)
represents
an approximately
4.5-cm-
breast.
to calculate
mean
glandular
dose,
one
should
(a)
measure
the
expo-
sure in air at the breast entrance surface, (b) measure the half-value layer of the beam, (c) determine the average thickness of the compressed breast for the range of patients being examined, and (d) estimate the composition of the breast tissue (the fraction of adipose and glandular tissue) With these values determined, the
SUMMARY AND RECOM-
MENDATIONS
.
mean glandular Typical values
dose can be calculated and of dose have been reported
reported. from a survey
the Nationwide
Evaluation
(NEXT)
CDRH
July
1990
and
the
Food
and
of X-ray Drug
Trends
Administration.
These
program values
performed
(8) are
as part
carried given
out in Table
Rothenberg
of
by the 2.
#{149} RadioGrapbics
#{149} 745
Some changes will be seen in these values in the future: We may expect the mean glandular dose for screen-film mammography to decrease somewhat because faster screen-film combinations have been introduced. Of the single-screen, single-emulsion film combinations, several have been introduced in recent years that are on the order of 25%-50% faster. Double-screen, double-emulsion systems now in use reduce the exposure by a factor of two or more, compared with some of the older systems used when the NEXT data in Table 2 were calculated. Table 2 shows that xemomammogmaphy requires significantly higher mean glandular dose than that needed for screen-film mammography.
The
NCRP
has recommended
that
for an examination
of a 4.5-cm-thick
com-
pressed breast, the average glandular dose should be less than 1 mGy (1 00 mnad) for one view for screen-film mammography without a grid, less than 4 mGy (400 mrad) for screen-film mammography with a grid, and less than 4 mGy (400 mnad) for xemomammognaphy (3) New York State has decided in its regulations that the .
average than
glandular 3 mGy
(300
dose mrad)
Acknowledgments: Sloan-Kettering eral helpful
REFERENCES
1
.
2.
3.
.
rather
mammography
than
the
4 mGy
The author
Cancer discussions
Center on this
is grateful to Mary and Leonard Stanton, topic and for providing
Hammerstein GR, Miller DW, Masterson ME, Woodard HQ, JS. Absorbed radiation dose mography. Radiology 1979;
White DR, Laughlin in mam130:485-
be less (9).
MS, of Memorial
1977;
Hermann Lietz
50:814-82
K-P, Geworski
R, Harden
D.
1.
L, Hatzky
Muscle-
and
T, fat-
Stanton L, Villafana T, DayJL, Lightfoot DA. Dosage evaluation in mammogra-
tube voltages below 1 00 kV. Biol 1986; 31:1041-1046.
phy. Radiology
1984;
Mammography:
a user’s
no.
85.
Bethesda,
7.
150:577-584.
guide. Md:
NCRP National
Council on Radiation Protection and Measurements, 1986. Rosenstein M, Andersen LW, Warner GG. Handbook of glandular tissue in mammography.
DHHS
8.
publica-
FDA 85-8239. Rockville, Md: U.S. Department of Health and Human 5cr-
vices, 1985.
#{149} RadioGrapbics
Masterson,
should NCRP
MS, of Hahnemann University for sevmost of the original drawings.
Radiol
6.
White DR, Martin RJ, Darlison R. oxy resin-based tissue substitutes.
#{149} Rothenberg
EpBrJ
Phys
Med
Mammography accreditation program. Reston, Va: American College of Radiology, 1987. Conway BJ, ed. Nationwide evaluation of x-ray trends (NEXT) , tabulation, and graphical summary of surveys, 1984 through 1987. CRCPD publication 893 Frankfort, Ky: Conference of Radiation Control Program Directors, 1989. Quality assurance programs for providens of mammography services. Publicaiion no. PH-7. Albany, NY: New York State Department of Health, 1987. .
iion
746
Ellen
a grid by the
equivalent polyethylene-based phantom materials for x-ray dosimetry at
doses
5.
with
suggested
491.
report
4
for screen-film
9.
Volume
10
Number
4