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Technical Innovation |
1 Department of Radiology, Duke University Medical Center, Box 3808, Durham, NC
27710.
2 Radiation Safety Division, Duke University Health System, Durham, NC
27710.
Received May 30, 2001;
accepted after revision October 23, 2001.
Presented at the annual meeting of the American Roentgen Ray Society,
Seattle, AprilMay 2001.
Introduction
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All scans were obtained during the same session. Individual organ doses and the effective dose equivalent were estimated at a different session using thermoluminescent dosimeters (Harshaw TLD-100; Saint-Gobain Cystals & Detectors, Solon, OH) and an anthropomorphic phantom (RANDO phantom; The Phantom Laboratory, Salem, NY). Thermoluminescent dosimeter calibration was performed using a simulated CT beam with a half-value layer of 8 mm of aluminum at 120 kVp. Two thermoluminescent dosimeter chips were placed in various organs of the phantom. CT scans were obtained using the clinical renal-stone protocols at our institution for the CT/i scanner (peak kilovoltage, 140 kVp; varied amperage; pitch, 1; slice thickness, 5 mm) and the QX/i scanner (peak kilovoltage, 140 kVp; varied amperage; pitch, 3; slice thickness, 5 mm).
Two investigators, working by consensus, recorded the total number of calculi identified in each kidney at each dose. The reviewers were aware of the technical parameters of the scan, and one of the reviewers had participated in the stone implantation in the porcine kidneys. Three calculi in the left kidney shifted position during suturing of the kidney, and they became inseparable from other calculi on the CT scans. As a result, only 17 discrete stones were identified in the left kidney on the initial scans obtained using the standard diagnostic technique. This finding then served as a reference for subsequent scans obtained at lower exposures. The stones did not shift their position during transfer of the phantom from the QX/i to the CT/i scanner.
Six indicator calculi were identified on the initial scan. The size of each indicator calculi was evaluated at each varied exposure to assess for size distortion with differing techniques. A single investigator measured the size of the six indicator calculi at a workstation using electronic calipers. Kendall tau b correlation coefficients were computed for pairs of variables.
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The calculated dose to the phantom decreased in a linear fashion with the decreasing amperage on both the single-detector and multidetector scanners (Fig. 5). Specifically, on the CT/i, a decrease from 220 to 80 mA reduced the CT dose index from 11.1 to 3.8 mGy. The corresponding thermoluminescent dosimeter measurement for kidneys decreased from 28.5 to 10.3 mGy and the estimated effective dose equivalent decreased by 64% from 16.3 to 5.9 mSv (Fig. 6). On the QX/i, a decrease from 170 to 60 mA reduced the CT dose index from 14.9 to 5.2 mGy. The corresponding thermoluminescent dosimeter measurement for kidneys decreased from 34.6 to 12.2 mGy, and the estimated effective dose equivalent decreased by 65%from 22 to 7.8 mSv (Fig. 7).
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The main disadvantage of CT is that it exposes patients to a relatively high radiation dose. This high dose is of particular concern in those young patients who are repeated stone formers and thus may require multiple CT examinations in their lifetime.
In our phantom study, we found excellent detectability of all renal calculi, which ranged in size from 2-8 mm, when we used a much lower amperage and measured radiation dose than those of the standard protocols. At an exposure of 80 mA for single-detector CT and 60 mA for multidetector CT, all renal calculi were visualized in the porcine kidneys. These findings correspond to a 2.9-fold decrease in estimated radiation dose (11.1-3.8 mGy) on the single-detector CT scanner and a 2.9-fold decrease (14.9-5.2 mGy) on the multidetector CT scanner. In addition, the findings correspond to a 2.8-fold decrease in the estimated effective dose equivalent (16.3-5.9 mSv) on the single-detector CT scanner and a 2.8-fold decrease (22-7.8 mSv) on the multidetector CT. We measured a significantly greater dose on the QX/i (multidetector) scanner as compared with the CT/i (single-detector) scanner. We believe that this finding is primarily associated with the inherent design of multidetector CT scanners; that is, the QX/i produces a broadened beam profile beyond the umbra (the main beam over the detectors) and generates a very large penumbra radiation contribution.
Denton et al. [7] have raised the concern of an increased radiation dose with helical CT compared with conventional excretory urography. Their study found that the average effective dose of unenhanced helical CT was more than three times that of three-film excretory urography. They commented that the radiation risk is somewhat offset by the risks of contrast media reaction and contrast mediainduced nephrotoxicity. They concluded that the increased radiation risk may be justifiable if information that alters subsequent patient treatment is gained from CT that would not have been obtained from excretory urography. Liu et al. [8] described a low-dose CT protocol for evaluation of renal colic compared with exposure on excretory urography. The effective dose equivalent of their protocol was 2.8 mSv, which is double that of excretory urography. However, they used parameters of 120 kVp and 280 mAs on a single-detector CT, producing a greater dose than the standard renal-stone protocol at our institution. A study by Diel et al. [9] explored increasing the pitch as a means of reducing radiation dose in CT of patients with suspected renal colic. The average entrance exposures were estimated as 461 mR (1.19 x 10-4 C/kg), 553 mR (1.43 x 10-4 C/kg), and 913 mR (2.36 x 10-4 C/kg) at pitches of 3.0, 2.5, and 1.5, respectively. Although accuracy did not significantly change when they used the higher pitch of 3.0 versus 2.5, the image quality did decrease.
A limitation of our study is that the investigators were aware of the technical parameters of the scan during the evaluation of stone size and conspicuity; as the noise progressively increased with decreasing amperage, it was obvious to the reviewers which were the reduced-dose scans. A further limitation of our study is that we were unable to evaluate for ureteric stones in this phantom model; we were only able to evaluate stone size and detectability in the kidney. Visualization of a calculus in the lumen of a dilated ureter is direct evidence of acute urinary obstruction resulting from renal stone disease. Occasionally, the patient is scanned after passage of a stone, or the ureteric stone remains undetected because of volume averaging, lack of retroperitoneal fat, respiratory motion, or an abundance of phleboliths [10]. It is not known whether the ureter and the secondary signs of ureteral obstruction would be adequately evaluated with a reduced-dose technique. Furthermore, it is unclear how well this technique would visualize the remainder of the abdomen and pelvis to evaluate for other causes of acute flank or abdominal pain. A low-dose renal-stone protocol may prove most valuable in patients requiring follow-up scanning in the setting of known nephrolithiasis when other diagnoses are less likely. Clearly, a low-dose technique would not be possible for obese patients, who routinely require a higher exposure for diagnostic images.
In conclusion, this phantom study shows that renal stone detectability and size remain constant on both the single- and multidetector helical CT scanners at much lower radiation doses than those called for in the standard renal-stone protocol. Evaluation of the clinical performance of a low-dose renal-stone technique is warranted in this frequently ordered examination.
Acknowledgments
We thank G. Allan Johnson for his contribution in the formulation of the
study design and David DeLong for his help with statistical analysis.
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