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CHAPTER 15 Management of Imaging Personnel Radiation Dose
307
A
B
Scattered
C
Collimator
X-ray
tube
Fig. 15.16 When the protective factors of distance and shield-
ing have been accounted for, the radiographer will receive the least amount of scattered radiation by standing at a right angle (90 degrees) to the scattering object (the patient) (in position A). The most scattered radiation would be received at point C because of backscatter coming from the patient. (Intensity, or quantity, of x-ray exposure at any given point is indicated in this picture by the number of scattered x-rays reaching that point.)
radiation
Primary (useful)
beam
Image
receptor
If possible, the radiographer should also attempt to stand at a right angle (90 degrees) to the x-ray beam– scattering object (the patient) line. This is the location at which the least amount of scattered radiation is re­ceived (Fig. 15.16). However, because distance and shielding have much more influence on the reduction of exposure to the technologist, those factors should be addressed first.

PROTECTION DURING C-ARM FLUOROSCOPY

Personnel Exposure Resulting From Scattered Radiation

Safety procedures are particularly important when mo­bile fluoroscopy (C-arm) systems are used. Because pat­terns of exposure direction are less predictable and the equipment is frequently operated by physicians whose training and experience in radiation safety may not match those of an experienced radiologist, the radiogra­pher should exercise special vigilance. For C-arm devices
LATERAL X-RAY TUBE ORIENTATION
IMAGE INTENSIFIER
LOW
SCATTERED
RADIATION
AREA
Fig. 15.17 Cross-table exposure during use of a C-arm fluoro-
scope. The exposure rate caused by scatter near the entrance surface of the patient (the x-ray tube side) exceeds the exposure rate caused by scatter near the exit surface of the patient (the image intensifier side). The location of lower potential scatter dose is on the side of the patient away from the x-ray tube (i.e., the image intensifier side). (From Mark Rzeszotarski.)
LOW
SCATTERED
RADIATION
AREA
HIGH
BACKSCATTER
REGION
HIGH
BACKSCATTER
REGION
X-RAY
TUBE
with similar fields of view, the dose rate for personnel located within a meter of the patient is comparable to that in routine fluoroscopy—approximately several mil­ligray in air (mGya) per hour. The exposure of personnel is primarily caused by radiation scattered from the pa­tient. During operating room procedures in which cross­table exposures are used (Fig. 15.17), an understanding of the patterns of x-ray scatter is particularly useful. The exposure rate caused by scatter near the entrance surface of the patient (the x-ray tube side) exceeds the exposure rate caused by scatter near the exit surface of the patient (the image intensifier side). The difference in the amount of scatter, typically a factor of 2 or 3, is caused by the higher radiation intensity at the entrance surface of the patient. Thus, the location of the lower potential scatter dose is on the side of the patient away from the x-ray tube (i.e., the image intensifier side). The radiographer should never encounter the actual useful beam.

Need for Protective Apparel for All Personnel and Monitoring of Imaging Personnel

The C-arm fluoroscope can be manipulated into almost any position and remain energized for lengthy periods to accommodate, for example, an orthopedic surgeon performing an open reduction of a fractured hip in the operating room or a vascular surgeon performing an interventional procedure. When radiographers and
308
CHAPTER 15 Management of Imaging Personnel Radiation Dose
other medical personnel participate in procedures that require this unit to be energized for significant dura­tions, they are subject to increased radiation exposure. Also, the physical configuration of a C-arm fluoroscopic unit limits the methods that can be used to achieve pro­tection from scattered radiation. For this reason, per­sonnel who routinely operate a C-arm fluoroscope or those who are in the immediate area of the unit when it is energized must wear a lead apron instead of crowding behind a portable lead–acrylic shield. This garment should be 0.5 mm lead equivalent to ensure adequate protection. A neck and thyroid shield of 0.5 mm lead equivalent should also be worn. Appropriate monitor­ing of imaging personnel who are typically involved in C-arm fluoroscopic procedures is mandatory.

Positioning of the C-Arm Fluoroscope

The positioning of a C-arm fluoroscope influences the radiation exposure to the patient and the radiographer. From the perspective of increased radiation safety, it is best to reverse the C-arm to place the x-ray tube under the table and the image intensifier over the table (see Fig. 11.23).

Exposure Reduction for Personnel

At the start of each procedure, the unit’s cumulative timer should be reset to zero so that it will be possible to be aware of the actual beam-on time.3 When an image storage device (e.g., last image hold) is used, beam-on time decreases, and therefore exposure reduction in­creases. If the image intensifier (II) is positioned as close to the patient as possible, the required fluoroscopic x-ray beam intensity is minimized. This equipment–patient arrangement also permits the image intensifier to func­tion more effectively as a scatter barrier between the patient and the person operating the C-arm fluoroscope. All these methods can lead to significant exposure re­duction to both personnel and patient.
During a C-arm procedure, it is imperative that the patient’s anatomic region of interest be oriented cor­rectly with minimal use of “positioning” the fluoro­scope.3 Furthermore, collimating the x-ray beam to the smallest anatomical area possible will decrease the amount of scattered radiation produced from the inter­action of the x-ray beam with the patient, the actual scattering object.
Because distance from the source of radiation is the simplest method of protection for occupationally exposed
personnel, C-arm operators should use it to their advan­tage whenever possible. Usually, this can be accomplished by using the foot pedal or the handheld exposure switch with the cables extended away from the machine as far as possible when making x-ray exposures.
For better visualization of small body parts, C-arm fluoroscopes can magnify the image. However, the use of magnification usually requires higher mA, which produces additional radiation exposure. Mag mode should be used only upon request by the physician per­forming the procedure.
3

PROTECTION DURING HIGH-LEVEL CONTROL INTERVENTIONAL PROCEDURES

Increased Importance of Radiation Safety Techniques

All of the previously mentioned standard precautions and procedures for the reduction of dose to personnel are applicable during interventional procedures. Here, these techniques take on increased importance because of the extended length of some of these procedures, the large number of digital images that may be taken, and, in particular studies, the frequent use of the high­level control (boost) mode of operation. In boost mode, the exposure rate may significantly exceed the rate used in routine fluoroscopy (e.g., maximum allowed entrance exposure rate dose to a patient in regular fluoroscopy is
8.8 cGY/minute [or 10 R/min exposure rate], whereas in high-level or boost mode this value can range upward to 20 to 40 cGy/minute).

Knowledge of Dose-Reduction Techniques Required by the Radiographer

Although the duration of the procedure and the number of the exposures taken are under the control of the radi­ologist or other interventional physician, the radiographer should verify that all dose-reducing features are available and in good working order. These include the presence of:
• High-quality, low-dose fluoroscopy mode
• Pulsed beam operation (e.g., using 7.5, 15, or 30 radia-
tion pulses/second in place of continuous fluoroscopy
radiation)
• Manual collimation
• Correct beam filtration
• Removable grids
CHAPTER 15 Management of Imaging Personnel Radiation Dose
309
• Road-mapping*
• Time interval differences
• Last image hold mode As previously discussed, using the last image hold
mode feature, the operator does not need to be exposed again to review the position of a catheter in relation to landmarks when no new information is required. Also, if possible, the patient beam entry side could be changed during the procedure to reduce the total dose to any one area of skin.
High-level control is to be used sparingly and only
when increased visualization is necessary during a criti­cal maneuver such as the deployment of stents4 (tubular support device that can be inserted into a blood vessel, canal, or duct to relieve obstruction). Many standard and C-arm interventional fluoroscopic systems now possess the technical capability for standardized dose
*Road-mapping is a method of digital image subtraction in which the frame that contains the greatest amount of contrast material in vessels is identified and is then subtracted from all subsequent images. Live fluoroscopic images of the catheter moving through the vasculature can then be seen even after the vessels contain less contrast. By using this equipment fea­ture, overlaying of two images can be accomplished (e.g., a stored image and a current image). Thus, there is a decrease of procedure time because fewer mask images (masking refers to a two-step imaging process that can be used to remove or obscure unwanted areas from the final or useful image by subtracting from a current image an initially or subsequently acquired reference image) are needed. This leads to some re­duction in radiation dose. Choosing the road-mapping fea­ture in place of cineradiography (a technique in which a cam­era is used to record continuous images, of nonstationary internal body structures, that are generated during selected intervals [e.g., 10 seconds] of nonstop radiation exposure) can also result in a lower radiation dose.
Time-interval difference (TID) is a method of digital image subtraction in which each TID image results from subtracting a previously acquired regular image from one that is a few frames in advance (e.g., if a time-interval difference of five images is chosen, the first TID image to appear will be that obtained when frame one is subtracted from frame six. The second image will contain the subtraction of frame two from frame seven, etc.). This technique progressively reveals vessels containing material and suppresses soft tissue in the images. It is less sensitive to patient motion than when the first image is selected as the “mask” or reference image and is then sub­tracted from all successive images.
structure reporting.5 These systems automatically fur­nish reports that yield an equivalent dose record for every examination.

How the Radiologist or Other Interventional Physician Can Reduce Radiation Exposure

The radiologist or other interventional physician can reduce radiation exposure by the following means:
• Decreasing the duration of the procedure, thereby shortening fluoroscopic beam-on time
• Obtaining fewer digital images
• Reducing the use of continuous fluoroscopic mode relative to the pulsed mode of operation
• Retaining the protective curtain, if available, on the image intensifier or leaving the scatter shield in place during a procedure
• Regularly using the last image hold feature to view the most recent fluoroscopic image These practices will substantially decrease exposure
not only to all participating personnel but to the patient as well.

Extremity Monitoring

Because the hands and forearms of physicians perform­ing interventional procedures can be subjected to sig­nificant radiation exposures if the safety protocol is not carefully followed—and sometimes this may not be possible—it is essential that extremities be monitored. Physicians need to be aware of the recommended dose limits that have been established for extremities. The NCRP currently recommends an annual EqD limit to localized areas of the skin and hands of 500 mSv (50 rem). To avoid remotely approaching this limit and conse­quently significantly increasing the possibility of future adverse effects, protective gloves should be worn when­ever feasible by any physician whose hands will, of neces­sity, often be close to the fluoroscopic beam.

DIAGNOSTIC X-RAY SUITE PROTECTION DESIGN

Requirement for Radiation-Absorbent Barriers

To reduce the EfD to radiographers, nonoccupationally exposed personnel, and the general public to levels deemed statistically safe by both federal and interna­tional bodies, every radiography room must be equipped
310
Leakage
CHAPTER 15 Management of Imaging Personnel Radiation Dose
BOX 15.3 Radiation-Absorbent Barrier
Design Considerations
The mean energy of the x-rays that will strike the barrier
Whether the barrier is of a primary or a secondary
nature
The distance from the x-ray source to a position of
occupancy 0.3 m from the barrier
The workload of the unit
The use factor of the unit
The occupancy factor behind the barrier
The intrinsic shielding (e.g., tube housing attenuation)
of the x-ray unit
Whether the area beyond the barrier is “controlled”
or “uncontrolled”
with radiation-absorbent barriers. The design of these barriers is based on considerations listed in Box 15.3.

Reason for Overshielding

The shielding design for radiographic rooms must in­clude all of the factors identified in Box 15.3 to meet necessary radiation protection standards. In addition, the designer should plan conservatively to satisfy future regulatory limits that may be more stringent. These considerations and the ALARA principle are why many diagnostic x-ray facilities are overshielded. Spending extra money up front for additional shielding is far easier and much less expensive than adding shielding after the suite has been completed.

Radiation Shielding Categories

As mentioned in previous sections, three categories of radiation sources are generated in an x-ray room. They are classified as follows:
1. Primary radiation
2. Scatter radiation
3. Leakage radiation The last two categories are collectively known as
secondary radiation.
Primary Radiation. Primary radiation emerges directly
from the x-ray tube collimator (Fig. 15.18) and moves without deflection toward a wall, door, viewing window, and so on. Because of this property, primary radiation, also is known as direct radiation, is energy that has not been degraded by scattering, and substantial portions of
Steel housing
Insulating oil
Fig. 15.18 Primary radiation emerges directly from the collimator
and spreads throughout the room.
Leakage
Fig. 15.19 Scatter radiation emerges from the patient and
spreads in all directions.
Primary
beam
Useful beam
radiation
Scatter
the initial beam may not have been attenuated. There­fore, a wall in the path of direct radiation requires the most protective shielding to ensure the safety of person­nel and the public. In a typical x-ray suite, the most crucial primary radiation barrier is that behind the wall Bucky unit.
Scatter Radiation. Recall that scatter radiation results
whenever a diagnostic x-ray beam passes through mat­ter. Compton interactions between the x-ray photons and the electrons of the atoms within the attenuating object deflect x-ray photons from their initial trajecto­ries. As a result, photons emerge from the object in all directions (Fig. 15.19). Scattered radiation is greatly re­duced in intensity relative to the incident beam. It also is substantially weakened in energy and consequently in penetrating power. The amount of shielding required to protect against scatter radiation is, therefore, usually much less than that for primary radiation. In general, the patient is the major source of scatter radiation.
CHAPTER 15 Management of Imaging Personnel Radiation Dose
311
Leakage Radiation. Leakage radiation is radiation gener-
ated in the x-ray tube that does not exit from the collimator opening but instead partially penetrates the protective tube housing and also, to some degree, the sides of the collima­tor (see Fig. 15.18 and 15.19). Leakage radiation is there- fore always present in some amount. When shielding is planned for a secondary barrier, the potential contribu­tions from leakage radiation must be added to those from the scatter radiation reaching that barrier.

Calculation Considerations

Workload. Because a diagnostic x-ray unit does not pro-
duce radiation 24 hours a day, 7 days a week, a parameter that reflects the unit’s radiation-on time has been used in the determination of barrier shielding requirements. The quantity, workload (W), is essentially the radiation output- weighted time that the unit is delivering radiation during the week. It has also been called the unit’s duty cycle. Work- loads are specified either in units of milliampere-seconds (mAs) per week or milliampere-minutes (mA-min) per week. The following example illustrates this concept.
Example: A radiographic x-ray suite is in operation 5 days per week. The average number of patients per day is 20, and the average number of images per patient is 3. The mean technical exposure factors are 90 kVp, 300 mA, and 0.1 sec. Find the weekly workload.
Solution:
( ) ( )
W 300 mA 0.1 sec 5 days/wk
( ) ( )
20 patients/d a y 3 images/patient
9000 mAs/wk
150 mA min/wk
Note that the kVp is not used in the workload calcu­lation. It is, however, an essential parameter in the cal­culation of barrier-shielding thickness. (This will be demonstrated later on in an example illustrating the calculation of shielding for a wall in an x-ray suite.)
Inverse Square Law. Just as the perceived brightness of
a light source decreases with distance from its origin, the intensity of an x-ray beam is lessened as the displace­ment from its source increases. The ISL, introduced earlier in this chapter, is the mathematical relation de­scribing this property and is a fundamental component of radiation protection. As such, the ISL plays a signifi­cant role in the design of radiation safety barriers. An example of its use is shown here.
Example
: At a distance of 1 m from an x-ray tube target, the dose rate measured by a radiation survey meter was 4.5 mGy per hour. What would that instru­ment read if it were moved back an extra 2 m?
Solution: ISL is mathematically given by the follow-
ing proportion:
5
(d )
2
2
1
II(d )
122
If the given data are substituted into the relation and
cross-multiplied, the following result is obtained:
2
3 I 4.5 1
 
2
9 I 4.5
2
I 0.5 mGy/hr
2
2
This result demonstrates a large reduction in radia­tion intensity. Its direct consequence is a greatly reduced barrier shielding thickness requirement.
The inverse square law is built into the combined mathematical and empiric (i.e., experimentally derived) formulas that determine primary barrier thickness values and secondary barrier thickness values. Because these relations are formulated to give answers for broad-beam
attenuation* rather than just for a very localized area, the
ISL effect is slightly less than it would be for an idealized situation. A short discussion with an example illustrating the usage of this for a primary barrier is presented in the following pages. Before this discussion proceeds, however, several other concepts of fundamental importance in the design of appropriate shielding have to be introduced.
Use Factor. If radiation, whether primary or secondary,
is never directed at a particular wall or structure, then conventional or existing construction is sufficient. Most structures in a diagnostic x-ray suite, however, are struck by radiation to some degree for some fraction of the weekly beam-on time. The use factor (U) was intro­duced to delineate this fractional contact time.
For primary radiation, the use factor represents the portion of beam-on time that the x-ray beam is directed at a primary barrier during the week. Consider a typical radiographic suite with a wall Bucky unit. If 50% of the
*As defined in NCRP Report 147 (see below), broad-beam attenuation refers to that effect occurring when the field area is large at the barrier and the point of measurement is near the barrier’s exit surface.
312
CHAPTER 15 Management of Imaging Personnel Radiation Dose
x-ray examinations involve this device, the wall behind the Bucky unit has a U (primary) 5 1/2.
Because scatter and leakage radiation emerge in all directions in the x-ray room, every wall, door, viewing window, and other surface will always be struck by some quantity of radiation. Therefore U (secondary) 5 1 for all radiation-accessible structures. Furthermore, if a particular wall is considered a primary barrier and its required shielding is designed on that basis, then in virtually all situations no supplementary shielding need be added for the secondary radiation that may also be striking this barrier.
Table 15.2 presents the most current recommended
use factor values. U also can be referred to as the beam
direction factor.
Occupancy Factor. Radiation barriers are installed to
protect personnel and the general public from radiation exposure. If no one will ever be present beyond an exist­ing wall in a particular area while the x-ray unit is being operated, the addition of extra shielding to that wall is unnecessary. For that location the shielding design
TABLE 15.2 Use Factors Recommended
by the International Commission on Radiological Protection
Use Factor Primary Barrier
Full use (U 5 1) Floors of radiation rooms except
dental installations, doors, walls, and ceilings of radiation rooms exposed routinely to the primary beam
Partial use
(U 5 ¼)
Occasional use
1
(U 5
)
16
From International Commission on Radiological Protection (ICRP): Report of Committee III on protection against x-rays
up to energies of 3 MeV and beta and gamma rays from sealed sources, ICRP Publication No. 3, New York, 1960,
Pergamon Press.
Doors and walls of radiation rooms
not exposed routinely to the primary beam; also floors of dental installations
Ceilings of radiation rooms not
exposed routinely to the primary beam; because of the low use factor, shielding requirements for a ceiling usually determined by secondary rather than primary beam considerations
statement would be that existing construction is suffi­cient. An example of this is an outside wall facing a
courtyard that “always” has no occupancies. The oppo­site extreme is an area in which someone is always pres­ent. When planning radiation protection shielding for a diagnostic x-ray suite, the designer must consider not only zero and full occupancy cases but also the more common partial occupancy situations. The occupancy
factor (T) is used to modify the shielding requirement
for a particular barrier by taking into account the frac­tion of the work-week during which the space beyond the barrier is occupied. Table 15.3 lists the latest recom- mended values for T.
Controlled and Uncontrolled Areas. If a region adjacent
to a wall of an x-ray room is to be used only by occupation­ally exposed personnel (e.g., radiographers), that location is designated a controlled area. Conversely, a nearby hall or corridor that is open to and frequented by the general public, is classified as an uncontrolled area. For the latter, the weekly maximum permitted equivalent dose (MPED) is equal to 20 microsieverts (20 µSv or 2 mrem); for controlled areas, it is a much more significant amount: 1000 µSv or 1 mSv (100 mrem). The main reason for allowing this huge disparity lies in the fact that the occupa­tionally exposed population makes up only a tiny fraction of the overall population. Therefore, the potential for det­rimental radiobiologic effects in the general public as a whole (i.e., its genetically significant dose [GSD] value) as a result of the higher MPED to occupationally exposed personnel is statistically negligible. Whether the area be­yond a structure is designated as controlled or uncon­trolled is clearly very significant in determining the amount of radiation shielding to be added to that structure. The following sections discuss the use of these concepts in the determination of radiation shielding requirements.

Calculating Barrier Shielding Requirements

For each wall, door, and other barrier in an x-ray room that is to provide protection from radiation, the product of W 3 U 3 T must be determined. The number of mA-minutes per week or workload is generally deter­mined by overall utilization of the x-ray unit. In con­trast, the use and occupancy factors are typically differ­ent among the various barriers. The shielding designer also must conclude whether the barrier is primary or secondary and whether the area beyond the barrier is controlled or uncontrolled.
CHAPTER 15 Management of Imaging Personnel Radiation Dose
313
TABLE 15.3 Suggested Occupancy
Factors*
Location
Administrative or clerical offices; laborato-
ries, pharmacies, and other work areas fully occupied by an individual; recep­tionist areas, attended waiting rooms, children’s indoor play areas, adjacent x-ray rooms, image reading areas, nurses’ stations, x-ray control rooms
Rooms used for patient examinations and
treatments
Corridors, patient rooms, employee
lounges, and staff rest rooms Corridor doors Public toilets, unattended vending areas,
storage rooms, outdoor areas with
seating, unattended waiting rooms,
patient holding areas Outdoor areas with only transient pedestri-
ans or vehicular traffic, unattended parking
lots, vehicular drop-off areas (unattended),
attics, stairways, unattended elevators,
janitors’ closets
*For use as a guide in planning shielding where other occupancy data are not available.
When using a low occupancy factor for a room immediately adjacent to an x-ray room, care should be taken to also consider the areas farther removed from the x-ray room. These areas may have significantly higher occupancy factors than the adjacent room and may therefore be more important in shielding design despite the larger distances involved.
The occupancy factor for the area just outside a corridor door can often be reasonably assumed to be lower than the occupancy factor for the corridor. Adapted from National Council on Radiation Protection and Mea­surements (NCRP): Structural shielding design for medical x-ray imaging facilities, Report No. 147, Bethesda, MD, 2004, NCRP.
Occupancy
Factor (T)
1
½
1
5
1
8
1
20
1
40
With the publication of NCRP Report No. 147,6 en­titled Structural Shielding Design for Medical Imaging Facilities, the objective of a shielding calculation is now described as determining the thickness of a barrier suf­ficient to reduce the air kerma* in a full or partially oc­cupied area to a value that is less than or at most equal
*Recall that air kerma (Ka) is essentially absorbed dose in air resulting from the passage of an x-ray beam through it. Its numeric value is specified in units of gray.
to the ratio P/T where the quantity P refers to the per­missible weekly radiation dose (note: for diagnostic x-rays, dose, and equivalent dose are numerically equal) to that location, and T is the area’s occupancy factor.
Primary Barrier Calculation. Using material from
NCRP Report No. 147, the combined mathematical and empiric relation that was briefly mentioned in the sec­tion on the ISL is introduced. For primary, or direct, radiation only, the mathematical expression is given by:
B P d / K NUT
5
2
(
(
)
p
)
r
where B is by definition the broad-beam x-ray trans-
mission factor and is the ratio of air kerma (Ka) behind
a barrier of material thickness “x” to the value of Ka at the same location with no intervening barrier; dp is the distance from the x-ray source to a representative loca­tion and distance behind the direct radiation barrier (e.g., one-third of a meter beyond the barrier is typical); Kr is the average unshielded air kerma per patient at a reference distance of 1 m from the source; N is the expected number of patients examined in the room per week; U and T are, as noted, previously, respectively, the use and occupancy factors; and P depends on whether the bar­rier is for a controlled or uncontrolled area. Once the value of B has been calculated for a particular situation, then plots (Fig. 15.20) of transmission factors (values of B) versus attenuating material thickness supplied in Appendix B of NCRP Report No. 147 may be used to obtain the required shielding thickness for the barrier.
6
The primary radiation intensity for a selected kVp at a barrier location for an x-ray suite may be determined by making air kerma measurements on the suite’s x-ray unit at a reference distance (e.g., 100 cm) from the x-ray tube target with the aid of a calibrated ionization chamber. This information can then be used to determine the amount of shielding necessary to attenuate the radiation to permissi­ble levels for that x-ray energy. The following example demonstrates determination of the primary barrier shield­ing requirement associated with a wall Bucky from an av­erage-usage radiographic room with an uncontrolled area existing behind the barrier (e.g., a public corridor).
Example:
Given the following specifications, determine the required shielding:
• The average kVp for the x-rays striking the barrier 5
100.
• P 5 0.02 mGy/wk because of the uncontrolled area.
314
CHAPTER 15 Management of Imaging Personnel Radiation Dose
1.0
8 6 4
2
−1
10
8 6 4
2
−2
10
8 6 4
2
−3
10
8 6 4
Transmission
2
−4
10
8 6 4
2
−5
10
8 6 4
2
−6
10
0.0 0.5 1.0 1.5
Primary Transmission Through Lead
Chest Room
Rad Room
(all barriers)
Lead thickness (mm)
(chest bucky)
Rad Room
(floor or other
barriers)
Rad Room
Rad Tube
(R&F Room)
2.0 2.5 3.0
Fig. 15.20 Assorted plots of primary broad-beam transmission
through lead. (From National Council on Radiation Protection and Measurements [NCRP]: Structural shielding design for medical x-ray imaging facilities, Report No. 147, Bethesda, MD, 2004.)
• dp 5 3 m
• 100 patients per week in this x-ray room.
• U 5 1/2
• T 5 1/4
• The measured value of Kr is 6 mGy per mA-min at 1 m at 100 kVp.
Solution:
Substituting the foregoing information into the expres­sion for the transmission factor “B” gives:
 B (0.02) (3) /[(6) (100) (0.5) (0.25)]
2
0.0024
From the graph in Fig. 15.20, using the curve for ra-
diographic room chest Bucky, a shielding requirement of
approximately 1.3 mm lead is obtained. Currently, in the United States shielding is specified in fractions of an inch of lead, most commonly, 1/32 and 1/16. The standard 1/32 inch is approximately 0.8 mm, and the standard 1/16 inch is equal to 1.58 mm. Because the calculation of shielding for the primary barrier required 1.3 mm lead, then in the United States the conservative choice would be to install 1/16-inch lead shielding for this barrier.
Secondary Barrier Calculation. Secondary barriers
intercept both scatter and leakage radiation. As has been
mentioned previously, no additional shielding against
secondary radiation is needed for areas already protected against primary radiation. Because scatter and leakage
radiation emerge in all directions, the use factor U for these is always 5 1.
Scatter radiation. The intensity and energy of the
scatter radiation at the location of a barrier are generally unknown because of all the potential variables involved. Therefore, the following properties, typically, are as­sumed for the determination of scatter radiation barrier shielding:
1. The energy of the scatter radiation is conservatively considered to be equal to that of the primary radiation.
2. The intensity of radiation scattered at 90 degrees at a distance of 1 m from its source is reduced by a factor of 1000 relative to the primary radiation for a field size of 400 cm2 (20 cm 3 20 cm). The larger the x-ray field dimension at the source of
the scatter radiation (usually the patient), the more sig­nificant will be the amount of generated scatter radia­tion. Also, notably of importance are the primary beam photon energy and the incident location of the x-ray beam on the patient. The ISL again plays a vital role in shielding requirements, but regarding scatter radiation, however, the distance is measured from the center of the irradiated portion of the patient (the prime source of scatter) rather than from the x-ray tube target.
Leakage radiation. Leakage radiation does not
emerge directly from the collimator opening but instead seeps out or leaks through the x-ray tube housing walls and also partially penetrates the sides of the collimator when the x-ray beam is on. Leakage radiation is there­fore an additional radiation output component that shielding designers must consider. Regulatory standards mandate that the maximum permissible leakage expo­sure rate at 1 m from the target of a diagnostic x-ray tube in all directions cannot exceed 100 millitoentgens
(mR) per hour or 0.88 milligray (mGy) air kerma per hour when the tube is being operated continuously at its
maximal permitted kVp and mA combination.
Because of the attenuation that occurs when leakage
radiation penetrates the tube housing walls, any emerging radiation is essentially monoenergetic; thus, the basic con­cept of half-value layer (HVL) may be applied at barriers to reduce leakage radiation levels to permissible values. Data tables incorporating this concept have been devel­oped to specify the amount of shielding needed to attenu­ate leakage radiation sufficiently at various distances from
CHAPTER 15 Management of Imaging Personnel Radiation Dose
315
the x-ray tube. This value should be compared with that necessary to attenuate scatter radiation satisfactorily. Tra­ditionally, if both shielding requirements do not differ substantially (i.e., are less than three HVLs of shielding material apart), then the conservative decision would be to install a composite that is the sum of the required shield- ing for each radiation source. However, if the needed bar­rier shielding for each of the two differs substantially (i.e., more than three HVLs), then, again conservatively, the larger value alone can be used for the shielding. The following example illustrates the method used in most existing diagnostic x-ray rooms for determining leakage radiation shielding requirements.
Example: If shielding must be added to a wall that is subject only to secondary radiation to protect a con­trolled area, then find the total thickness of lead needed, given the following information:
HVL for scatter and leakage radiation: 0.2 mm lead (Pb) for each. Shielding requirement for scatter radia­tion alone for a particular barrier: 0.75 mm Pb
Shielding requirement for leakage radiation alone for that barrier: 0.3 mm Pb
Solution: The difference in barrier shielding require­ments for scatter and leakage 5 0.45 mm lead, which is less than 3 HVL, which equals 3 3 0.2 mm lead, or 0.6 mm lead. Therefore, the conservative total shielding thickness amount for the barrier would be 0.75 1 0.3 5 1.05 mm Pb.

Current Approaches to Shielding

Among the most current approaches to shielding design detailed in NCRP Report No. 147, a more rigorous workload analysis incorporates the range of kVps actu­ally used. Also, the true role of leakage radiation in state-of-the-art equipment is now modeled explicitly, along with scatter. The traditional rule of adding an HVL if leakage and scatter barrier requirements are similar has now been abandoned in favor of exact calcu­lations. Use factors at present reflect an actual percent­age of the time that the beam is directed at various barriers. Some existing shielding that was generally ig­nored in older design calculations, such as the patient table, Bucky, and image receptor, is included in the new designs. Finally, the suggested occupancy factors have been reevaluated to approximate more closely the per­centage of the time that workers are expected to be pres­ent (see Table 15.3). In NCRP Report No. 49,7 a minimal occupancy factor of at least 1/16 was assumed. Under the revised guidelines, occupancy factors for areas such
TABLE 15.4 Brief Summary of National
Council on Radiation Protection and Measurements Report No. 147 New Shielding Guidelines
Item New Approach
Workload More realistic use of contemporary
survey data
Leakage and
scatter
Use factor Adjusted for beam direction data
Occupancy
factor
Adapted from National Council on Radiation Protection and Measurements (NCRP): Structural shielding design for medical imaging facilities, Report No. 147, Bethesda, MD, 2004, NCRP.
Explicit barrier calculations
reflecting actual usage patterns
Realistic assumptions of occupancy of
low-occupancy areas (e.g., stairwells)
as closets and stairways may be placed as low as 1/40. Some of the changes in the revision of NCRP Report No. 49 are listed in Table 15.4.

RADIATION CAUTION SIGNS

The appropriate deployment of radiation signs or elec­tronic notices is an essential component of safety in a ra­diology department. Specific rules and regulations vary somewhat according to the jurisdiction of the facility (i.e., state, federal, military, etc.). However, the main points concerning the type of signs and the circumstances under which posting is required are essentially the same. Each radiographer should check with the radiation safety offi­cer in the institution where employed, concerning specific regulations that govern the facility where they work.

Beam-On Indicator Sign

Some states require specific imaging equipment installa­tions, primarily computed tomography (CT) scanners, to include warning lights that are conspicuous near the door to the examination room from any corridor. The sign should read “x-ray beam on” or the equivalent and be self-illuminating whenever the x-ray equipment is energized. Some states require an interlock such that exposure is terminated if the door is opened.

General Posting

Radiation warning signs are posted within controlled areas of the hospital or facility. They are typically found
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CHAPTER 15 Management of Imaging Personnel Radiation Dose
BA
Fig. 15.21 Radiation warning signs typically found in a diagnostic radiologic facility. (A) A self-illuminated sign
used outside the door to a computed tomography (CT) scanner. (B) A general radiation warning sign used to indicate the potential for exposure that may exceed 0.05 mSv at 30 cm from a source of radiation. (A, From Brian Struble/DigitalMomentStudios.com, © 2017.)
on the door to CT and interventional x-ray rooms, lin­ear accelerator treatment rooms, and storage areas for radioactive materials. An example of the latter is shown on the right in Fig. 15.21. Such signs are required to be magenta or purple or black on a yellow background. Further specifications may be found in Recommended State Regulations of the Conference of Radiation Con­trol Program Directors.8 A sign reading “Caution Radia­tion Area” is usually adequate for rooms containing

S U M M A R Y

• An annual occupational effective dose of 50 mSv for whole-body exposure during routine operations and an annual effective dose of 1 mSv for individuals in the general population have been established.
• A CumEfd limits a radiation worker’s whole-body cumulative occupational effective dose to his or her age in years times 10 mSv.
• Radiation workers can receive a higher equivalent dose than the general public without altering the ge­netically significant dose (GSD).
• Occupational exposure must be kept ALARA.
• The following methods of reducing scatter radiation also reduce the occupational hazard for the radiographer:
• Use of beam-limitation devices, higher kVp and
lower mA techniques, appropriate beam filtra­tion, and adequate protective shielding
fixed diagnostic equipment. A radiation area is gener­ally an area in which radiation exposures may exceed
0.05 mSv (5 mrem) in 1 hour at 30 cm from a source. Other categories of caution signage exist for areas in which radiation exposures may exceed those encoun­tered in diagnostic radiology. These signs are required in radiation oncology or nuclear medicine departments and include the labels: High Radiation, Very High Radia­tion, Airborne Radioactivity, and Radioactive Materials.
• Proper utilization of protective apparel (lead aprons, gloves, thyroid shields)
• Reduction of repeat images
• The basic principles of time, distance, and shielding are to be employed to minimize occupational radia­tion exposure.
• Pregnant radiographers can wear an additional monitoring device at waist level to ensure that their monthly equivalent dose does not exceed
0.5 mSv.
• Primary and secondary protective barriers must be designed so that annual effective dose limits are not exceeded.
• A lead-lined, metal, diagnostic-type protective tube housing protects the radiographer and the patient from leakage radiation.