A long, long time ago during my undergrad days, one of the requirements for my 4th year physics lab course (way back in 1990 or so) was to do some kind of research project. The project my lab partner and I settled on was to investigate the use of copper filters in the x-ray beam to reduce skin entrance exposure to pediatric cardiac cath patients. For the past few years it’s something that’s been pretty standard in fluoroscopic equipment now (although not something I can claim any credit for, I don’t think). I thought for posterity, I’d post our original write-up here.
Disclaimer: This work is from a project I did for one of my undergraduate labs a few years ago. The only review process this project has undergone was being scrutinized by my supervisor for this project and by the TA who marked it. Check my bibliography for other published papers on the subject.
If you’d like to comment on or criticize this, email me at eugenemah@gmail.com (or just leave a comment)
Abstract
Pediatric patients undergoing cardiac catheterization procedures can be subjected to large skin entrance exposures from both fluoroscopy and cine modes. To reduce the radiation exposure to the patient while minimizing loss in image quality, a small amount of copper filtration is added. In conjunction with standard radiation protection procedures (shielding and minimizing procedure time) the reduction in patient exposure can be reduced quite significantly. Preliminary phantom investigations demonstrate a decrease in exposure of up to 70% with the addition of 0.2 cm of copper filtration and little image quality degradation.
Introduction
Cardiac catheterization procedures involving pediatric patients can subject both the patient and operators to high radiation exposures. Because of the small size of the patients involved, children receive higher gonadal and thyroid exposures from scattered radiation. Children are also more sensitive to the effects of radiation than adults.
Several methods of reducing patient dose have been suggested such as minimizing procedure time, reducing the x-ray field size or placing lead shielding underneath the patient. Newer pulsed fluoroscopy systems where the x-ray beam is pulsed at the same rate as the video refresh rate of the monitor (30-60 pulses/second) has also shown to result in a significant saving in patient dose as well as improving image quality [7, 8, 13].
In keeping with the principle of ALARA, a method of reducing patient exposure by introducing additional beam filtration is proposed and investigated in this work. The additional filtration reduces radiation exposure by hardening the beam and removing the low energy x-rays which do not contribute to the formation of the x-ray image. Since the average kVp for pediatric patients is between 50-60 kVp, this should result in a large reduction in patient exposure without significant degradation in image quality. Aluminum filtration was also examined to compare the reduction in exposure between copper and aluminum. A similar method employed by den Boer et al [8] demonstrated a 55% reduction in patient exposure and 69% reduction in operator exposure with the combination of a high-output pulsed fluoroscopy and 0.4 mm of copper filtration.
Materials and Methods
Skin entrance exposures in typical cardiac catheterization procedures were examined for a Siemens cardiac catheterization laboratory equipped with a Siemens Polydoros 100 high frequency generator, Bicor biplane C-arms with variable FOV image intensifiers, Cinematic AEC 35 mm cine camera and Hicor digital imaging system.
A simple phantom consisting of a number of Lucite sheets was assembled to mimic a small patient approximately 6 cm thick. A small length of catheter was placed in the center of the phantom to serve as a reference marker and a rough indication of the image quality as the filters were added.
Skin entrance exposures for both fluoroscopy and cine were measured with a Keithly electrometer and a small ion chamber placed underneath the phantom. For fluoroscopy and cine, the skin entrance exposures for various amounts of aluminum and copper filtration were measured and graphed. Aluminum thicknesses ranging from 0-4.5 cm and copper thicknesses from 0-2.0 mm were used.
The low contrast phantom (Figure 2) was made up of a 0.4 cm thick plate of aluminum with 8 holes of 4 different sizes, 1.6, 3.2, 4.8 and 6.4 mm in diameter. This plate was sandwiched between two 0.8 cm blocks of aluminum so that the holes in the aluminum sheet were 2% of the total thickness (2.0 cm).
The high contrast resolution phantom is a 0.5 cm thick block of plastic with 8 metal grids of varying line pair densities embedded in it. Line pair densities range from 20 lpi (lines/inch) to 60 lpi.
Both phantoms were placed on the table top 30 cm away from the image intensifier and 40 cm above the x-ray tube and examined using fluoroscopy and cine. Image quality was evaluated using each phantom for a variety of filter thicknesses using the fluoroscopy display monitors and cine film.
Results
Image Quality
For the low contrast phantom and up to 0.2 mm of copper filtration added, all 4 holes were still easily visible. With 0.4 mm of copper filtration, the smallest hole (1.6 mm) became barely visible and was no longer visible with 0.5 mm of copper filtration.
High contrast resolution (HCR) was measured at about 28 lpi (lines/inch) with up to 0.2 mm of copper filtration. At 0.4 mm and 0.5 mm of copper filtration, HCR dropped to 24 lpi.
Exposure Rates
With the phantom placed on the table and the ion chamber underneath the phantom, fluoroscopic skin entrance exposure rates in mR/min were measured first with no aluminum filtration, and then with increasing amounts of aluminum added to the x-ray tube. X-ray techniques (kVp and mAs) were also recorded. Table 1 shows the results with the results illustrated graphically in Figure 4.
Table 1: Fluoroscopic skin entrance exposure rates for Al filter
Amt of Al (cm) | kVp | mAs | Exposure rate (mR/min) |
0 | 46 | 1.6 | 225 |
0.6 | 50 | 2.7 | 89 |
0.9 | 52 | 3.1 | 69.2 |
1.2 | 55 | 3.6 | 57 |
1.5 | 56 | 4 | 51.3 |
2.25 | 59 | 4.6 | 43 |
2.7 | 62 | 5.2 | 38.6 |
3 | 64 | 5.6 | 36.2 |
3.75 | 68 | 6.3 | 32.8 |
4.2 | 71 | 6.3 | 31.5 |
4.5 | 74 | 6.3 | 30.8 |
Figure 4 illustrates the dramatic decrease in skin entrance exposure with the addition of just 0.6 cm of additional aluminum filtration. The additional filtration results in a 60% reduction in patient exposure and only a slight increase in x-ray technique (from 46 kVp to 50 kVp and 1.6 mAs to 2.7 mAs).
The same measurements were performed using copper filtration, with the results tabulated in Table 2 and illustrated in Figure 5.
Table 2: Fluoroscopic skin entrance exposure rates for Cu filter
Amt of Cu (mm) | kVp | mAs | Exposure rate (mR/min) |
0 | 46 | 1.8 | 267 |
0.1 | 48 | 2.3 | 141 |
0.2 | 52 | 3 | 88 |
0.3 | 54 | 3.4 | 70 |
0.4 | 56 | 3.9 | 57 |
0.5 | 58 | 4.3 | 53 |
1.5 | 58 | 6.3 | 38.4 |
1.7 | 71 | 6.4 | 35.3 |
2 | 75 | 6.4 | 34.7 |
The reduction in patient exposure is nearly 50% with 0.1 mm of copper and 67% with 0.2 mm with very little change in x-ray technique (Figure 5). For larger filter thicknesses, the reduction in patient exposure is small relative to the increase in x-ray technique and the expected degradation in image quality resulting from the higher techniques.
Table 3 shows the cine skin entrance exposure with copper filtration, illustrated in Figure 6.
Table 3: Cine skin entrance exposure rates for Cu filter
Amt of Cu (mm) | kVp | mAs | Exposure rate (R/min) |
0 | 50.5 | 28 | 3.32 |
0.2 | 54 | 29 | 0.64 |
0.4 | 60.5 | 31 | 0.4 |
For cine procedures where exposure rates can be in the R/min range, 0.2 mm of copper filtration resulted in an 80% decrease in patient exposure with little change in technique. Unfortunately, due to time limitations and the arrival of a patient, fluoroscopy exposure rates were not obtained for copper filter thicknesses between 0.5 mm and 1.5 mm and only 3 measurements could be made in cine mode.
Conclusion
Inserting a small amount of additional filtration is a simple and effective way of obtaining significant exposure savings for pediatric patients undergoing cardiac catheterization procedures where they may be subjected to high radiation doses. From a practical viewpoint, copper would appear to be the most ideal filter, since copper provides much greater reduction in patient exposure and is much thinner than the equivalent amount of aluminum. An additional 0.2 mm of copper filtration appears to provide an optimum amount of filtration which maximizes the radiation exposure reduction and minimizes the degradation in image quality.
Bibliography
- Rueter FG, “Physician and patient exposure during cardiac catheterization”, Circulation, 58:134-139 1978
- Martin EC, Olson A, “Radiation exposure to the paediatric patient from cardiac catheterization and angiocardiography”, Br J Radiol, 53:100-106 1979
- Wu JR, Huang TY, Wu DK, Hsu PC, Weng PS, “Radiation exposure of pediatric patients and physicians during cardiac catheterization and balloon pulmonary valvuloplasty”, Am J Cardiol, 68:221-225 1991
- Leibovic SJ, Fellows KE, “Patient radiation exposure during pediatric cardiac catheterization”, Cardiovasc Intervent Radiol, 6:150-153 1983
- Martin EC, Olson AP, Seeg CN, Casarella WJ, “Radiation exposure to the pediatric patient during cardiac catheterization and angiocardiography”, Circulation, 64:153-157 1981
- Waldman JD, Rummerfield PS, Gilpin EA, Kirkpatrick SE, “Radiation exposure to the child during cardiac catheterization”, Circulation, 64:158-163 1981
- Schueler BA, Julsrud PR, Gray JE, Stears JG, Wu KY, “Radiation exposure and efficacy of exposure reduction techniques during cardiac catheterization in children”, Am J Roentgenol, 162:173-177 1994
- den Boer A, de Feyter PJ, Hummel WA, Keane D, Roelandt JRTC, “Reduction of radiation exposure while maintaiing high quality fluoroscopic images during interventional cardiology using novel x-ray tube technology with extra beam filtering”, Circulation, 89:2710-2714 1994
- Li LB, Kai M, Takano K, Ikeda S, Matsuura M, Kusama T, “Occupational exposure in pediatric cardiac catheterization”, Health Phys, 69:261-264 1995
- Johnson LW, Moore RJ, Balter S, “Review of radiation safety in the cardiac catheterization laboratory”, Cathet Cardiovasc Diagn, 25:186-194 1992
- Miller SW, Castronovo Jr FP, “Radiation exposure and protection in cardiac catheterization laboratories”, Am J Cardiol, 55:171-176 1985
- Faulkner K, Love HG, Sweeney JK, Bardsley RA, “Radiation doses and somatic risk to patients during cardiac radiological procedures”, Br J Radiol, 59:359-363 1986
- Holmes DR, Wondrow MA, Gray JE, Vetter RJ, Fellows JL, Julsrud PR, “Effect of pulsed progressive fluoroscopy on reduction of radiation dose in the cardiac catheterization laboratory”, J Am Coll Cardiol, 15:159-162 1990
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I have been doing similar work…just out of curiosity, what are you doing now? I guess you never published…to bad eh?! 🙂
Now I work as a clinical medical physicist in diagnostic radiology. This particular project was never published (did it back in 1991 I think), but I suppose with a little more work and time, it could have been.
A year or two after I worked on this little project, I saw companies starting to come out with fluoro units that used varying amounts of copper filtration in the beam for dose reduction.
One thing I’ve always wanted to investigate was just how much absorbed dose reduction the added filtration produces. There’s definitely a significant reduction in exposure, but does it correlate with a reduction in absorbed dose, and how much? I’m sure a little bit of literature searching will turn up whether this has been answered or not.