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. Author manuscript; available in PMC: 2013 Sep 25.
Published in final edited form as: Eur J Radiol. 2011 Jun 8;81(8):1702–1706. doi: 10.1016/j.ejrad.2011.04.067

Estimated effective dose of CT-guided percutaneous cryoablation of liver tumors

Byung Kwan Park a,*, Paul R Morrison b, Servet Tatli b, Usha Govindarajulu c, Kemal Tuncali b, Phil Judy b, Paul B Shyn b, Stuart G Silverman b
PMCID: PMC3782862  NIHMSID: NIHMS305130  PMID: 21645981

Abstract

Purpose

To estimate effective dose during CT-guided cryoablation of liver tumors, and to assess which procedural factors contribute most to dose.

Materials and methods

Our institutional review board approved this retrospective, HIPAA-compliant study. A total of 20 CT-guided percutaneous liver tumor cryoablation procedures were performed in 18 patients. Effective dose was determined by multiplying the dose length product for each CT scan obtained during the procedure by a conversion factor (0.015 mSv/mGy-cm), and calculating the sum for each phase of the procedure: planning, targeting, monitoring, and post-ablation survey. Effective dose of each phase was compared using a repeated measures analysis. Using Spearman correlation coefficients, effective doses were correlated with procedural factors including number of scans, ratio of targeting distance to tumor size, anesthesia type, number of applicators, performance of ancillary procedures (hydrodissection and biopsy), and use of CT fluoroscopy.

Results

Effective dose per procedure was 72 ± 18 mSv. The effective dose of targeting (37.5 ± 12.5 mSv) was the largest component compared to the effective dose of the planning phase (4.8 ± 2.2 mSv), the monitoring phase (25.5 ± 6.8 mSv), and the post-ablation survey (4.1 ± 1.9 mSv) phase (p < 0.05). Effective dose correlated positively only with the number of scans (p < 0.01).

Conclusions

The effective dose of CT-guided percutaneous cryoablation of liver tumors can be substantial. Reducing the number of scans during the procedure is likely to have the greatest effect on lowering dose.

Keywords: Interventional oncology, Radiation, Cryoablation, Liver, Cancer

1. Introduction

Percutaneous radiofrequency ablation (RFA) and cryoablation are minimally invasive treatment alternatives for managing liver tumors in patients who are unable to undergo surgical resection [18]. CT is used often as a guidance modality for ablation because of its favorable spatial and contrast resolution and, in part, because of radiologists’ familiarity with the use of CT for guiding percutaneous needle biopsies and drainages. During cryoablation, CT can provide excellent visualization of the iceball in the liver, whereas CT monitoring of heat during hepatic RFA is not feasible. Like other interventional procedures, several intermittent CT scans are required during an ablation procedure and thus, there is the potential for high radiation doses.

To our knowledge, there are few reports that have focused on radiation dose of CT-guided RF ablation; there are none on cryoablation [9,10]. We performed this study to estimate effective dose of CT-guided cryoablation of liver tumors, and to assess which procedural factors contribute most to dose.

2. Materials and methods

2.1. Patients

Our institutional review board approved this retrospective, HIPAA-compliant study; patient informed consent was waived. Between December 2006 and December 2007, 29 cryoablations on liver tumors were performed. Of the 29, nine were conducted to treat two or more tumors in the same procedure and therefore were excluded from this study so as to yield a homogeneous population of procedures in which a single tumor was treated during each procedure. As a result, the study population consisted of 20 CT-guided cryoablation procedures during which a solitary liver tumor was treated in 18 patients (12 men and six women; age range, 44–88 years; mean age, 61.2 years). Of these 18 patients, 16 had a single procedure and two had two procedures each. One patient had two hepatic masses and underwent two ablation procedures at different times. The other patient had one tumor ablated during the first procedure; the same tumor was retreated during the second procedure.

A diagnosis was obtained via a percutaneous biopsy in all patients, either in a separate CT-guided procedure several days prior to (n = 13) or during (n = 7) the cryoablation procedure. Diagnoses consisted of 14 metastases and four primary tumors. Hepatic metastases originated from cancers of the colon (n = 5), ovary (n = 3), breast (n = 2), and one each from the kidney, tonsil, Cowper’s gland, and lung. Primary hepatic tumors included three hepatocellular carcinomas and one cancer consisting of both hepatocellular carcinoma and cholangiocarcinoma. Hepatic tumors were located in segment 7 (n = 5), segment 6 (n = 4), segment 8 (n = 3), segment 4 (n = 2), segment 2/3 (n = 2), segment 2 (n = 1), segment 5 (n = 1), segment 4/8 (n = 1), or segment 7/8 (n = 1). Tumor size was determined by measuring the maximum diameter of the tumor on contrast-enhanced CT scan or MRI examination performed prior to the cryoablation procedure. The mean maximum diameter of hepatic tumors was 3.1 ± 1.5 cm (1.4–7.3 cm).

2.2. CT-guided cryoablation procedures

Imaging for all cryoablation procedures was obtained with a 40-channel multi-detector CT scanner (Sensation Open, Siemens Medical Solutions, Forchheim, Germany). Automatic tube current modulation (Care Dose4D, Siemens Medical Solutions) was routinely applied for all spiral scans. Procedures were performed under monitored anesthesia care (n = 15) or general anesthesia (n = 5), in either supine (n = 19) or right anterior oblique (n = 1) position by a team consisting of an attending abdominal interventional radiologist and an abdominal interventional radiology fellow.

Unenhanced CT scans (spiral CT acquisition or as CT fluoroscopy) were acquired intermittently to image the tumor and surrounding anatomy during each of the four phases of the procedure that included planning, targeting, monitoring, and a post-ablation survey.

2.2.1. Planning phase

One or more planning CT scans (mean, 1.3; range, 1–3 scans) were performed with a surface grid in place to image the tumor and surrounding anatomy and to plan applicator insertion with respect to an appropriate skin entry site, insertion angle, and depth. The technical factors of CT acquisitions in this phase were the following: 120 kVp, 115–192 mAs, 0.85 pitch, 0.5 s rotation, and 24 × 1.2 mm collimation. The mean Z-axis length of these scans was 16.0 cm (range, 12.5–26.5 cm).

2.2.2. Targeting phase

Unenhanced CT scans, with additional CT fluoroscopy during 18 of the 20 procedures, were obtained during targeting to guide the placement of one or more 22 gauge reference needles, and subsequent placement in tandem fashion of multiple 17 gauge cryoablation applicators (mean, 3.9; range, 3–7; Galil Medical, Yokneam, Israel) placed using tandem trocar technique. Multiple applicators were placed with the goal of achieving an iceball large enough to freeze the entire tumor with a 1 cm margin. The targeting phase also included placing additional 22G fine needles (Chiba Biopsy Needle, Cook Medical, Bloomington, IN) for biopsy in seven procedures. Hydrodissection was performed in two patients to displace bowel away from the ablation zone. Hydrodissection was accomplished with the injection of 200–350 cm3 (mean, 275 cm3) of normal saline via a 22 gauge needle. The technical factors of CT acquisitions for the conventional (non-fluoroscopy) CT scans included: 120 kVp, 102–197 mAs, and 24 × 1.2 mm collimation. The mean Z-axis coverage was 10.4 cm (range, 4–29 cm). The technical factors for CT fluoroscopy scans included: 80–120 kVp, 30–50 mAs, 0.85 pitch, 0.5 s rotation, and 1.2 mm collimation.

2.2.3. Monitoring phase

After the cryoablation applicators were placed, two freeze–thaw cycles (15-min freeze and 10-min thaw each) were performed. A CT scan to include the iceball was performed approximately every 3 min during the freeze to monitor iceball growth. Monitoring was used to be sure the tumor was completely frozen and/or to protect adjacent critical structures. The technical factors of these CT acquisitions included: 120 kVp, 98–197 mAs, 0.85 pitch, 0.5 s rotation, and 24 × 1.2 mm collimation. The mean Z-axis coverage was 13.1 cm (range, 5–29 cm).

2.2.4. Post-ablation survey phase

After the treatment was completed, all cryoablation applicators were removed, and one or more unenhanced CT scans were obtained to survey the treated tumor and surrounding structures to determine whether the ablation was complete and to identify complications. The technical factors of CT acquisitions were the following: 120 kVp, 117–190 mAs, 0.85 pitch, 0.5 s rotation, and 24 × 5 mm collimation. The mean Z-axis coverage was 29.5 cm (range, 5.0–71 cm).

2.3. Effective dose

The effective dose (mSv) for each scan was determined by multiplying the dose length product (DLP, in mGy-cm) for each scan by a normalized-conversion factor for the abdomen (0.015 mSv/mGy-cm) [1113]. The effective dose for each phase (planning, targeting, monitoring, and post-ablation survey) was calculated by summing the effective dose for each CT scan performed during each phase. Total effective dose was calculated by summing the effective doses for each phase.

Effective doses for each phase were compared to determine which phase contributed most. To assess which factors contributed most for each procedure, we recorded the following variables: total number of scans for each cryoablation procedure, ratio of targeting distance to tumor size, anesthesia type (general anesthesia or monitored anesthesia care), number of cryoablation applicators, whether hydrodissection or biopsy was performed, and whether CT fluoroscopy was used. We correlated these variables with effective dose for each ablation procedure. The ratio of targeting distance to tumor size was a general measure of technical difficulty: the larger the ratio, the more difficult the tumor was to target [14]. Cryoablation applicators were placed deeply enough to encompass the most distant margin of the tumor. The targeting distance was measured from the skin entry site to the most distant margin of the tumor on the planning CT scan; tumor size was determined using the preprocedural diagnostic MRI exam.

2.4. Statistical analysis

Boxplots of the effective dose for each phase of the cryoablation procedure were created. Spearman correlation analysis was used to estimate the correlation between effective dose and the number of scans, the ratio of targeting distance to tumor size, the number of applicators, hydrodissection, biopsy, anesthesia type, and use of CT fluoroscopy.

In a separate analysis, both effective dose and number of scans were modeled separately in a mixed model in which measurements of effective dose and number of scans were repeated for each phase and for each patient. From each mixed model, we obtained least square adjusted mean values of effective dose and number of scans, and made comparisons among them to assess whether or not they were significantly different between phases. All statistical analyses were conducted at the 0.05 level of significance. Data analyses were performed with commercially available software (SAS V9.1, Cary, NC and SPSS for Microsoft Windows, version 11.0, Chicago, IL).

3. Results

Total effective dose (mean ± standard deviation) and effective dose range per procedure were calculated as 72 ± 18 mSv (46–117 mSv) (Table 1) (Fig. 1). The mean effective doses of planning, targeting, monitoring, and post-ablation survey phases were 4.8 ± 2.2 mSv (2–10 mSv), 37.5 ± 12.5 mSv (25–67 mSv), 25.5 ± 6.8 mSv (14–42 mSv), and 4.1 ± 1.9 mSv (2–8 mSv), respectively (Fig. 2). From the repeated measures model for effective doses, least square mean comparisons showed that effective dose for each phase were significantly different from each other (p < 0.0001) except for the planning and post-ablation survey phases (Table 2). The mean effective dose incurred during targeting accounted for 51.3% of the total dose incurred during the entire ablation procedure.

Table 1.

Mean dose length product and effective dose during CT-guided percutaneous cryoablation of liver tumors (n = 20).

Procedural phases Dose length product (mGy*cm)
Effective dose (mSv)
Mean±SD Range Mean±SD Range
Planning 322 ± 150 138–681 4.8 ± 2.2 2–10
Targeting 2496 ± 843 1662–4492 37.5 ± 12.5 25–67
Monitoring 1706 ± 454 937–2825 25.5 ± 6.8 14–42
Post-ablation survey 273 ± 123 135–548 4.1 ± 1.9 2–8
Entire procedure 4796 ± 1214 3059–7784 72 ± 18 46–117

Note: SD, standard deviation. Dose length product and effective dose for each phase were significantly different from each other (p < 0.0001) except for the planning and post-ablation survey phases (p > 0.05).

Fig. 1.

Fig. 1

Effective doses of CT-guided liver cryoablation procedures (n = 20). The graph illustrates the distribution of effective dose during CT-guided cryoablation procedures. Each square represents an effective dose for a procedure. The black dotted line indicates the mean effective dose.

Fig. 2.

Fig. 2

Box plot compares effective dose during each phase of CT-guided liver cryoablation procedures. The mean effective dose was highest during targeting followed by monitoring (p < 0.05). However, there was no significant difference between planning and post-ablation survey phases (p > 0.05). Horizontal line within the box indicates median value. The median values are 4 mSv for planning phase, 35 mSv for targeting phase, 26 mSv for monitoring phase, and 4 mSv for post-ablation survey phase.

Table 2.

Contribution (percent) to effective dose and to total number of scans from each phase during CT-guided cryoablation of liver tumors.

Procedural phases Effective dose
Number of scans
Mean±SD (%) Range (%) Mean±SD (%) Range (%)
Planning 6.7 ± 3.1 3–15 4.2 ± 2.3 2.3–11.1
Targeting 51.3 ± 7.5 38–70 53.8 ± 6.5 36.8–65.9
Monitoring 35.9 ± 7.2 24–48 37.9 ± 6.7 26.0–52.6
Post-ablation survey 6.0 ± 2.8 2–14 4.1 ± 3.2 2.3–17.4

Note: SD, standard deviation. The mean percent contribution of effective dose and the mean number of scans for each phase were significantly different from each other (p < 0.0001) except for the planning and post-ablation survey phases (p > 0.05).

Effective dose for each ablation procedure correlated significantly only with the number of scans (coefficient, 0.66; p < 0.0015). The mean number of scans was 30.1 ± 5.5 scans (19–44 scans). Using the repeated measures model for the number of scans, least square mean comparisons showed that the mean number of scans obtained during each phase was significantly different from each other (p < 0.0001) except for the planning and post-ablation survey phases. The greatest number of scans were obtained during the targeting phase (mean, 16.3 scans; range, 7–29 scans), followed by the number obtained during monitoring (mean, 11.5 scans; range, 7–15 scans), planning (mean, 1.3 scans; range, 1–3 scans), and the post-ablation survey (mean, 1.1 scans; range, 1–2 scans) (Table 2).

No significant correlation was found between effective dose and the ratio of targeting distance to tumor size, anesthesia type, the number of applicators, hydrodissection, biopsy, and use of CT fluoroscopy (coefficient, −0.08 to 0.45; p > 0.05). The mean targeting distance was 11.8 ± 3.0 cm (6.8–17.6 cm) and therefore, the mean ratio of targeting distance to tumor size was 4.6 ± 2.2 (1.4–8.6). The mean effective dose during CT fluoroscopy was 10.1 ± 8.6 mSv and the mean number of CT fluoroscopy scans 3.1 ± 2.6 (0–11 scans; n = 18 procedures).

4. Discussion

CT can be used successfully to guide percutaneous cryoablation of lung, kidney, liver, and bone tumors [4,5,1519]. It can be used to depict the tumor and surrounding critical structures so that ablation applicators can be placed safely and effectively. Unlike heat-based technologies, the iceball produced during cryoablation produces a well-demarcated region of hypoattenuation. Thus the growth of the iceball can be monitored with CT. While monitoring with serial CT scans allows the interventional radiologist to maximize the chance of freezing the entire tumor, while minimizing the risk of injury to adjacent structures, these CT scans contribute to radiation dose.

Although patient exposures from diagnostic CT scans has received much attention [20], radiation dose to patients undergoing CT interventional procedures has received little attention [9,10]. We estimated the mean effective dose of a CT-guided percutaneous liver cryoablation procedure to be 72 ± 18 mSv. For comparison, we estimated the effective dose of a typical diagnostic abdominal-pelvic CT scan (120 kVp, 200 effective mAs, 24 × 1.2 mm collimation) on the same scanner used in this study to be 8.9 mSv. Therefore, the mean effective dose to patients undergoing CT-guided cryoablation procedures (72 mSv) was comparable to approximately eight diagnostic abdominal CT scans. Thus, percutaneous CT-guided cryoablation can potentially lead to relatively high radiation doses.

Our result of 72 mSv is high when compared to effective doses for several vascular interventional procedures including abdominal angiograms (mean 12 mSv; range: 4–48) and coronary angioplasty (mean 7 mSv; range: 2–15.8) [21]. Also, our result is more than double the effective dose of CT-guided RF ablation of liver tumors (35.3 mSv) reported by Tsalafoutas et al. [9]. One possible explanation for this difference may be that the targeting phase of our cryoablation procedures included more applicator placements than what is needed during RF ablation procedures. For example, we typically placed three separate 17 gauge applicators to cryoablate a 2 cm tumor. Tsalafoutas et al. did not report the mean number of RF applicators, nor did they report tumor size or applicator type used in their ablation procedures [9]. However, in general, only one 17 gauge applicator is needed to RF ablate a 2 cm tumor [22]. Some RF devices are designed as a single applicator with a deployable array of tines or as a cluster of three applicators placed simultaneously. These RF applicators each alone may produce ablation zones of 4 cm or greater in diameter. Similar ablation volumes with cryoablation may require sequential placement of four or more applicators. A second reason why effective doses of CT-guided cryoablation were higher than the doses reported of CT-guided RF ablation is the use of CT to monitor iceball growth during cryoablation. Whereas CT is less useful in monitoring the RF ablation zone, CT is effective in monitoring the cryoablation zone, and therefore more scans would be expected to be used during cryoablation relative to RF ablation [14,1618,23]. We used CT to image the iceball every 3 min; one way to reduce dose would be to scan less frequently during monitoring when there are no nearby critical structures. Although scanning to monitor the ablation did contribute to the effective dose, most of the dose was incurred during targeting.

More than 50% of the CT scans were acquired during targeting, and the number of CT scans was the only significant procedural factor contributing to radiation dose. Thus, minimizing the number of scans during targeting would have the greatest impact on radiation dose reduction. This can be accomplished by improving the radiologists’ ability to target. Real-time navigation devices are being developed for abdominal intervention, including the liver, and are beginning to be used clinically [24,25]. These devices allow interventional radiologists to navigate using pre-procedural volumetric CT data that approximates the patient’s anatomy. Such devices may reduce the number of targeting attempts and therefore the number of scans acquired during the intervention [24,25].

Although other factors had less impact on dose, they too could be used to reduce dose. For example, since our CT fluoroscopy scans were obtained with low dose techniques, greater utilization of short CT fluoroscopy scans instead of conventional CT scans during targeting would reduce dose [26,27]. However, the reduction in radiation dose can be offset if the CT fluoroscopy scans are long, frequent, or performed with higher tube current or voltage. Use of CT-fluoroscopy did not reduce radiation dose in our study, most likely because it was not used enough to affect the mean effective dose for the study population. Nevertheless, if several scans are needed to target a lesion during ablation, use of short, intermittent low dose CT fluoroscopy scans in lieu of short, conventional CT scans will help reduce radiation exposure to patients. Also, radiation dose to patients may be reduced by scanning less frequently during the monitoring phase if adjacent critical structures are at safe distances from the ablation volume.

Since the effective dose of CT-guided cryoablation was substantial, MRI or ultrasonography (US) can be considered as alternative image-guidance modalities to reduce effective dose since they avoid ionizing radiation exposure entirely [2,3]. When performing cryoablation, MRI has been reported to be effective in delineating the iceball, separate from the tumor in near real time, and in multiple planes [1,23]. US has some utility for targeting or monitoring cryoablation but is less effective in depicting the entire tumor and iceball in part due to acoustic shadowing by the iceball, that prevents visualizing the entire iceball and structures behind it [23]. Nevertheless, US could be used in the CT suite initially to guide the placement of cryoablation applicators; CT could subsequently be used to monitor the iceball formation.

The study population was small but sufficient to study the effective dose incurred during the CT-guided cryoablation of a solitary liver tumor. By limiting the study to single liver mass ablation procedures, we were able to study the effect of other procedure-related factors on dose. All cryoablation procedures reported in this study were performed in a teaching hospital. The involvement of trainees during portions of these procedures may have had an impact to increase radiation dose.

Effective dose was used to estimate the radiation dose. Effective dose is limited in that it does not provide a measure of dose to an individual patient, to individual internal organs nor to the skin. It does not account for age, gender, or specific organ-weighted radiosensitivities. Also, while the DLP-to-effective dose conversion factor of 0.015 mSv/mGy-cm used in this report is consistent with Bongartz, other more recent values have been reported in the range of 0.016–0.018 [12]. However, in a retrospective study such as ours, effective dose does provide a reference value for this procedure and its phases; and could be used to compare with future ablation studies that use different protocols.

5. Conclusion

The effective radiation dose of CT-guided cryoablation of liver tumors can be substantial. Awareness of the potential radiation dose to patients undergoing CT-guided cryoablation warrants consideration of dose reduction strategies. Reducing the number of procedural scans as proposed in this report is likely to have the greatest impact on dose reduction.

Acknowledgement

The authors acknowledge the assistance of Richard Nawfel, MS in this work.

Footnotes

This publication was made possible by Grant Number RR019703 from NIH.

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