Eugene Mah, MSc
Department of Radiology, University of Alberta Hospitals
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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, eugenem@ix.netcom.com
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.
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A simple phantom (Figure 1) consisting of a number of polystyrene 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. |
| Figure 1: Phantom |
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.
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Fluoroscopic and cine image quality was tested using a low contrast 2% phantom (Figure 2) and high contrast resolution fluoroscopy phantom (Figure 3). The low contrast phantom 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). |
| Figure 2: Low contrast phantom | |
| 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. | |
| Figure 3: High contrast phantom |
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.
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.
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.
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| Figure 5: Fluoro skin entrance w/ Cu |
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.
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| Figure 6: Cine skin entrance w/ Cu |
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.
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