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Int J Radiat Oncol Biol Phys. Author manuscript; available in PMC 2007 May 3.
Published in final edited form as:
PMCID: PMC1865112
NIHMSID: NIHMS19512

Correlation of Radiation Response with Tumor Oxygenation in the Dunning Prostate R3327-AT1 Tumor

Vincent A. Bourke, Ph.D.,a,# Dawen Zhao, MD, Ph.D.,a Joseph Gilio, Ph.D.,b Cheng-Hui Chang, Ph.D.,b Lan Jiang, Ph.D.,a Eric W. Hahn, Ph.D.,a and Ralph P. Mason, Ph.D.a

Abstract

Purpose

It is widely recognized that tumor oxygenation may modulate the efficacy of radiation therapy. Previously, a correlation was established between pre-treatment oxygenation and growth delay following radiation therapy in the slower growing HI subline of the R3327 Dunning prostate tumor. We have now investigated application to the more hypoxic, faster growing AT1 subline.

Methods and Materials

Dunning prostate R3327-AT1 tumors growing on Copenhagen rats were administered 30 Gy of X-ray radiation either with or without oxygen inhalation. Tumor oxygenation was sampled by 19F nuclear magnetic resonance echo planar imaging relaxometry (FREDOM) of the reporter molecule hexafluorobenzene, no more than 24 hours prior to irradiation.

Results

Large tumors (>3.0 cm3) exhibited significantly greater hypoxic fractions and lower mean pO2 than their smaller counterparts (<1.5 cm3). However unlike the R3327-HI subline, large AT1 tumors generally did not respond to oxygen inhalation in terms of altered hypoxic fraction or response to irradiation. While the tumors did not respond to oxygen inhalation, each tumor had a different pO2 and there was a clear trend between level of oxygenation at time of irradiation and tumor growth delay, with considerably better outcome when mean pO2 > 10 torr. The comparatively small baseline hypoxic fraction in the group of small tumors was virtually eliminated by breathing oxygen and the growth rate was significantly reduced for tumors on rats breathing oxygen during irradiation.

Conclusions

These results further validate the usefulness of NMR oximetry as a predictor of response to radiation therapy.

Keywords: prostate tumor, oxygen, hypoxia, radiation response, fluorine NMR

INTRODUCTION

For more than 50 years it has been recognized that tumor oxygenation may significantly modulate the efficacy of various therapeutic interventions, particularly radiation therapy 17. Hypoxic tumors are characteristically more resistant to radiotherapy, and the ability to sample pretreatment oxygenation may prove to be a useful predictor of therapeutic outcome. In principle, there are many techniques available for the manipulation of intratumoral oxygen tension for therapeutic advantage, such as inhalation of hyperoxic gases. However, few have shown significant improvement in clinical outcome and it is thought that this may be due to the inability, hitherto, to identify those patients, who would benefit most 8. Thus, the ability to dynamically sample the oxygenation status of tumors, and monitor the response to adjuvant intervention could be very valuable. As reviewed 912, various methods have been developed for probing tumor oxygenation including hypoxia reporter agents, polarographic electrodes, fiber optic probes, NIR spectroscopy, and various NMR techniques, but most are either highly invasive, lack spatial resolution or lack the ability to dynamically and quantitatively sample the response to intervention.

We have developed an approach to dynamically sample tumor oxygen tension at multiple locations simultaneously: FREDOM (Fluorocarbon Relaxometry using Echo planar imaging for Dynamic Oxygen Mapping) MRI, following direct intratumoral injection of the reporter molecule hexafluorobenzene (HFB) 9. We have applied this method to explore tumor pO2 in various rat prostate and breast tumors and human tumor xenografts with respect to interventions 9, 1317. We also showed that response to single high dose radiation therapy in the slower Dunning Prostate R3327-HI was related to pO2 18. Inhalation of oxygen during 30 Gy irradiation resulted in enhanced growth delay in larger HI tumors (>3.5 cm3), but had no effect on smaller tumors (<2 cm3). It was found that the larger HI tumors have a high baseline hypoxic fraction (HF10 >80%), but this could be effectively eliminated by breathing hyperoxic gas (HF10 ~20% with oxygen breathing). By contrast smaller tumors showed minimal baseline hypoxia (HF5 ~20%) and although this was diminished, it was relatively inconsequential. We have also assessed differential characteristic responses to hyperoxic gas breathing in other sublines of the Dunning prostate R3327 14, 15. Most notably, the faster growing AT1 tumors (VDT ~ 5 days) were significantly less well oxygenated than size matched HI tumors, and unlike the HI subline, the critical initially hypoxic regions responded little to oxygen inhalation 15. It thus appeared that the AT1 subline should provide an important extension to further validate the utility of oxygen tension measurements for predicting response to irradiation. In an initial test, we examined the growth delay in tumors on rats breathing oxygen or air during irradiation. We then expanded the investigation to include pO2 measurements based on the FREDOM technique. Since hypoxic fraction was previously observed to increase with the size of the tumor 15, we investigated cohorts of small and large AT1 tumors, while rats breathed air or oxygen.

METHODS AND MATERIALS

Investigations were conducted in accordance with accepted ethical and humane practices, and approved in advance by the UT Southwestern Medical Center Institutional Animal Care and Use Committee (IACUC).

Tumor Model

Syngeneic Dunning prostate R3327-AT1 carcinomas, a fast growing, poorly differentiated subline with a potential volume doubling time (Tpot) of 4.4 days, were originally obtained from Dr. J. T. Isaacs, of Johns Hopkins University and provided to us by Dr. Peter Peschke of the German Cancer Research Center (DKFZ), Heidelberg, Germany. For the preliminary study, tumors were implanted in surgically prepared foreback pedicles of 14 adult male Copenhagen rats (~250 g, Harlan, Indianapolis, IN) 19. In the preliminary study, when the tumors reached a suitable size (0.9 to 2.8 cm3), the rats were divided into three groups for therapy: Group 1: control sham irradiated tumors (no treatment, n=4; mean size 1.9 ± 1.0 (SD) cm3), Group 2-air: rats breathing air during tumor irradiation (n=5; mean tumor size 1.6 ± 0.7 cm3), and Group 2-O2: rats breathing oxygen during tumor irradiation (n=5, mean tumor size = 1.5 ± 0.3 cm3). For the more extensive second study 28 tumors were implanted as before. In this case, the rats were divided into five groups: Group 3: control rats (no treatment, n=6), Groups 4-air (n=5) and 4-O2 (n=5) rats with large tumors (>3.0 cm3, mean size at treatment = 4.3 ± 0.4 cm3), and Groups 5-air (n=6) and 5-O2 (n=6) rats with small tumors (<1.25 cm3, mean size at treatment = 0.8 ± 0.1 cm3). Groups breathed air or oxygen, respectively, as designated during irradiation. Tumor diameter was measured with calipers in three orthogonal axes beginning seven days after implantation, and continuing every 3-7 days until sacrifice. Tumor volume was calculated as V=(π/6)*abc, where a, b, and c are the three orthogonal diameters. In some cases, tumor volume was estimated for a given day by interpolating between actual measured sizes. For each group, mean tumor size on a given day was estimated using measurements acquired over three day intervals (e.g., day 2 = days 1–3, day 5= days 4–6).

Tumor Oximetry (Groups 4 and 5)

In approximately half of the animals which were irradiated (Large, n=6; Small, n=6), NMR oximetry measurements were obtained within 24 h prior to irradiation. Each rat was sedated with 200 μl ketamine hydrochloride (100 mg/kg, Aveco, Fort Dodge, IA) and maintained under general anesthesia [1.2 L/min, air+1.2% isoflurane (Baxter International Inc., Deerfield, IL)]. The animal was positioned on its side on a cradle, and body temperature was maintained with a warm water blanket. As previously described 9, hexafluorobenzene (50 μl; Lancaster, Gainesville, FL) was deoxygenated by bubbling with CO2 for 5 minutes prior to use, and then was injected using a Hamilton syringe (Reno, NV) and a fine sharp 32G needle. To ensure representative sampling of intratumoral oxygenation, the HFB was deposited along three diverging tracks encompassing both central and peripheral regions in a central plane coronal to the rat’s body. It is important to note that the AT1 subline tumors do not develop a central necrosis. Thus, the oxygenation data are obtained from viable tissues.

NMR imaging was performed on representative rats from Groups 4 and 5 using a 4.7 T horizontal bore NMR system (Varian Inc., Palo Alto, CA). A tunable (1H/19F) single turn solenoid volume coil (either 2 or 3.5 cm, size matched to tumor diameter) was placed around the tumor bearing pedicle, and conventional spin echo scout images were obtained for both 1H (200.1 MHz) and 19F (188.3 MHz) to reveal HFB distribution within the tumor.

19F pulse burst saturation recovery echo planar imaging (EPI) relaxometry of the HFB (FREDOM) was used to measure pO2, while rats breathed air or with respect to breathing air followed by oxygen. Fourteen delay times in the range 150 ms to 90 s were used to generate the relaxation data with in plane resolution 1.25 mm and 20 mm slice thickness as described in detail previously 9. Two rats from each Group were examined while breathing air only (four consecutive pO2 maps obtained over 24 mins). Four rats from each group were examined 4 times while breathing air followed by 4 consecutive measurements during the first 24 minutes following switching to breathing oxygen. Spin lattice relaxation rates (R1=1/T1) were estimated on a voxel by voxel basis and pO2 calculated using the relationship pO2 (torr)= [(R1- 0.0835)/0.001876] 9. Since even noise can give an R1 curve fit, voxels were rejected if T1 error >2.5 s, or ratio T1 error/T1 >50%. We also required that voxels give reliable pO2 measurements throughout the series of measurements: thus, each voxel provided four or eight consecutive pO2 measurements, which were deemed acceptable on the basis of the T1 error acceptance criteria.

Radiation Treatment (Groups 2, 4 and 5)

Within 24 hours of the NMR scans, the animals were sedated with 200 μl ketamine hydrochloride (100 mg/kg I.P.) and then irradiated with single dose of 30 Gy (2 Gy/min) using a 4MV Varian Clinac 4/100 linear accelerator under general gaseous anesthesia (1.2 L/min, gas +1.2% isoflurane) 20. Tissue equivalent bolus (1 cm thick) was placed over the tumor during irradiation to ensure dose uniformity. The rats in Group 2-air (n=5), 4-air (n=5) and 5-air (n=6) breathed air during irradiation, while those in Group 2-O2 (n=5), 4-O2 (n=5) and 5-O2 (n=6) breathed oxygen for 30 mins prior to irradiation and during irradiation. The rats examined by NMR on the previous day breathed the corresponding gas during irradiation. Tumor size was normalized to the initial size on the day of irradiation. Treatment response was evaluated based on reduction in the tumor growth rate and time to double in volume (T2) post irradiation. If a tumor failed to double in volume by the time of sacrifice, the day of sacrifice was taken as T2, though this may represent an underestimate for responsive tumors.

Statistical Analysis

The statistical significance of differences in mean tumor size, and changes in oxygenation, was assessed using an analysis of variance (ANOVA) based on Fisher’s protected least significant difference (PLSD). Hypoxic fractions (HF10 < 10 Torr) were calculated for each tumor by counting the number of hypoxic voxels versus total number of measured voxels in the respective pO2 map. Animals were excluded from hypoxic fraction analysis, if the associated pO2 map did not contain at least ten acceptable voxels. Kaplan-Meier hazard statistics were applied to test the significance of differences in T2, the time to double the initial treated tumor volume on day 0 (V0).

RESULTS

In our preliminary studies there was a significant growth delay by day 12 following irradiation (p<0.05) for rats breathing air or oxygen compared with controls and the relative mean tumor sizes were 3.7±0.9 cm3 (Group 1 (control)), 2.2±0.9 cm3 (Group 2-air) and 2.0± 0.6 cm3 (Group 2-O2). No differences were found between breathing air or oxygen (Fig. 1A). On Day 32 Group 2-air had a mean relative volume of 4.9 ±3.5 cm3 compared with a volume of 3.4 ±2.9 cm3 for Group 2-O2. The lack of difference may be attributed to the broad range of responses related to the range of initial tumor sizes and levels of oxygenation (Fig. 1B). Thus, we undertook a more detailed second investigation with tumors divided into Groups based on size (large and small) and with oxygen tension measurements in representative tumors.

Figure 1
Influence of radiation on Dunning prostate R3327-AT1 tumor growth

Overlay of the 19F and 1H NMR images shows distribution of the reporter molecule HFB (Fig. 2). Between 300 and 600 voxels indicated 19F signal in the echo planar images and provided relaxation curves in the FREDOM measurements. Applying the acceptance criteria caused rejection of 50 to 75% of these data voxels based on excessive T1 error (poor quality curve fits). Applying the further requirement that voxels give consistently acceptable T1 values throughout the series of measurements caused further voxels to be rejected. For both air and oxygen breathing groups one tumor for each size provided such poor quality data that fewer than 10 voxels remained. These tumors are included in the consideration of tumor growth delay in Table 2, but are omitted from consideration of pO2 measurement (Table 1). For the remaining tumors between 12 and 102 individual pO2 measurements were considered reliable in each AT1 tumor and representative maps are shown for a large AT1 tumor in Figure 2A, B, and C. Here, 51 voxels were acceptable indicating a mean (±SE) baseline pO2 = 0.1 ± 1.8 torr (mean baseline HF10 = 87.3 ± 1.8%) during the initial 6 minute air inhalation period, which was found to be stable over the next 18 mins. A modest, but significant (p<0.01) increase was observed by the last six minutes of oxygen inhalation (Fig. 2C), though mean HF10 remained unchanged. Large AT1 tumors were significantly more hypoxic than small ones, and hypoxic fractions generally did not respond significantly to oxygen inhalation (Figs. 2, ,3,3, and Table 1). The small tumors were initially better oxygenated, and showed much greater response to oxygen inhalation (Fig. 2D, E, F).

Figure 2
pO2 maps obtained using FREDOM in two representative AT1 tumors
Figure 3
Changes in oxygenation and hypoxic fraction in response to oxygen inhalation
Table 1
Oxygen tension in R3327-AT1 Dunning prostate tumors for rats breathing air or oxygen
Table 2
R3327-AT1 prostate tumor growth following irradiation for rats breathing air or oxygen during irradiation

The influence of oxygen breathing on response to radiation was evaluated as change in the tumor growth rate, based on mean tumor size at various times following irradiation, and T2, the time to double the initial tumor size on the day of treatment (Table 2). Each tumor was normalized to Vo, its initial size on the day of irradiation. Each tumor in the untreated control group was normalized to its size on post-implantation day 13, the day on which the control group reached a mean size of about 1 cm3. Untreated controls (Group 3) were allowed to grow until the tumor burden or condition required sacrifice and T2 was found to be 5.6 ±1.9 days over an 11 day period culminating on the 24th day following surgical implantation. Growth slowed for all tumors following irradiation, but at no point in the growth progression of large tumors was there a significant difference in size between the air and oxygen breathing groups (Fig. 4). Large tumors could only be monitored for about 20 days following irradiation, because the mean size was already 3.5 –4 cm3 on the day of irradiation. The T2 was found to be just over 12 days for both air and oxygen breathing rats.

Figure 4
Tumor growth with respect to irradiation

Small tumors also continued to grow with no significant difference between air and oxygen breathing until day 13 (Fig. 4B). From day 13 onwards until the animals were sacrificed (post-irradiation day 25), the mean size of the small tumors in rats breathing oxygen was significantly smaller than those breathing air (Table 2). The ratios of these volumes ranged from 1.3 to 1.5 and might be loosely interpreted as an oxygen enhancement ratio (OER). Oxygen tension was measured in 6 large and 6 small tumors, but in one tumor of each type the pO2 maps were of such poor quality (excessive errors in the estimates) that they were excluded from analysis involving pO2. In addition, one rat from each type was sacrificed early (as per IACUC guidelines) due to tumor ulceration leaving four small and four large tumors for correlative oxygen analysis. For the Group of large tumors, two were found to be relatively well oxygenated (mean pO2 > 10 torr) and two were poorly oxygenated (although in each case one breathed air and the other oxygen during irradiation). The response to irradiation was found to be very different depending on pO2, as shown for the post irradiation growth curves (Fig. 5A). Both small and large tumors showed correlations (R2 > 0.8) between the mean pretreatment pO2 and T2 (Fig. 5B).

Figure 5
Influence of oxygen on tumor growth following irradiation

DISCUSSION

This investigation provides further evidence for the value and importance of measuring tumor oxygenation as a basis for predicting response to irradiation. In the preliminary experiment, we found that merely having rats with a range of R3327-AT1 tumor sizes breathe oxygen, before and during irradiation, had no significant effect on tumor growth delay. In the subsequent investigation stratification by tumor size revealed a modest, but significant benefit for small tumors, when rats breathed oxygen during a single dose of radiation, but groups of large tumors showed no benefit. However, pO2 measurements indicated that regardless of tumor size better oxygenated tumors showed better response to irradiation. The results indicate correlations between pO2 at time of irradiation and subsequent time to double in volume for both small and large tumors, irrespective of inhaled gas (Fig. 5A, B).

In common with our previous observations, the larger AT1 tumors were significantly more hypoxic and had lower mean and median pO2 15, 21. Mean pO2 in large tumors responded to hyperoxic gas breathing, but the hypoxic fraction resisted modulation rendering the tumors resistant to radiotherapy. Both groups of large tumors (4-air and -O2) responded to irradiation with a significant reduction in growth rate: volume doubling time (VDT) reached 12 days post irradiation compared with a control VDT ~ 5 days. However, there was no benefit in terms of radiation response associated with oxygen breathing during irradiation for the groups of large AT1 tumors (Fig. 4, Table 2). However, the better oxygenated tumors showed better response to irradiation (Fig. 5A), and indeed, there was a correlation between time to double in volume (T2) and pretreatment pO2 in individual tumors (Fig. 5B). Thus, pO2 measurements appear to have prognostic value for this small cohort of tumors. A similar correlation was found previously in the slower growing and better differentiated Dunning prostate R3327-HI tumors 18.

For the smaller AT1 tumors, baseline pO2 was generally significantly higher with only a small hypoxic fraction (HF10 <20%), which responded to hyperoxic gas breathing, as also observed previously 15, 21. By day 4, the tumors in Group 5-O2 were significantly smaller than controls and by day 7 both Groups 5-air and -O2 showed significant growth delay compared with control tumors. After 13 days there was a significant effect of breathing oxygen and for all subsequent measurements tumors on oxygen breathing rats were significantly smaller than on air breathing rats (Fig. 4, Table 2). The continued increase in size following irradiation is in line with previous reports in similarly sized AT1 tumors with respect to single doses of X-rays 22. Assessment of T2 (the time to double in volume post irradiation) showed a linear relationship with pO2 (Fig. 5B). However, the slope of the regression was very different for small and large tumors respectively. Smaller AT1 tumors have been reported to grow much faster than large AT1 tumors (VDT = 2.5 vs. 5.6 days) 23, but it is intriguing to note that the regression lines for small and large tumors appear to coincide for low pO2. This may suggest an intrinsic growth rate and is similar to the growth expected for control non-irradiated tumors. Sauer et al. 24 previously examined the R3327-AT tumor and found a tendency towards greater hypoxia in larger tumors and greater DNA damage in the better oxygenated tumors as judged by the Comet assay.

The FREDOM approach provides measurements of pO2 and in some ways is analogous to the Eppendorf Histograph or ESR (electron spin resonance) approaches based on particulate reporters. Each requires insertion of a needle into the tumor, but since HFB is a mobile liquid, we are able to use a particularly fine (32 gauge) needle. As with the Histograph, mean and median pO2 and hypoxic fractions could be determined. Importantly, however, the hexafluorobenzene reporter molecules remain in the tumor for many hours allowing sequential measurements with respect to interventions 9. Thus, the relative stability of baseline pO2 could be observed (Fig. 3), as well as regional response to hyperoxic gas intervention (Figs. 2 and and3).3). By contrast, the Histograph requires new needle tracks for sequential measurements and very few studies have examined dynamic changes in pO2 distributions in animal models 25 or attempted such measurements the clinic 26, 27. Despite its invasiveness, the Histograph has been used in the clinic, particularly for accessible head and neck and cervical tumors and for limited studies in breast, brain and prostate 3, 2830. Measurements from multiple studies show strong predictive value for hypoxic fractions of cervical and head and neck tumors with respect to clinical outcome. Groups at both Dartmouth 31, 32 and Louvain 3335, have exploited ESR with particulate reporters to assess tumor pO2 dynamics. Although only a single location was interrogated within the tumor, O’Hara et al. 31 found a strong correlation between tumor growth rates and pre-therapy pO2 in CALU-3 tumors undergoing radio immunotherapy, closely similar to our observations in Figure 5. O’Hara et al. 32 also showed that pO2 measurements could be used to optimize timing of split dose radiotherapy..

The purpose of this study was to further evaluate the usefulness of NMR oximetry as a predictor of therapeutic outcome, so that tumor phenotypes (poorly) suited for oxygen manipulation may be identified in advance. A useful feature of the FREDOM technique is that it allows minimally invasive quantitative dynamic in vivo sampling of multiple regions within the tumor. Accordingly, tumors with a significant HF10 and more importantly those which resist therapeutic oxygen manipulation can be readily identified. In future clinical practice this could prompt application of hypoxia selective cytotoxins or radiation boost using IMRT 36, 37. Of course, we recognize that this study used a single high dose of radiation and may be less pertinent to traditional fractionated regimens. Nonetheless, as the trend towards high dose stereotactic treatment develops, pO2 measurements, as presented here, could become increasingly pertinent and valuable. To date, the FREDOM approach could not be translated to the clinic due to lack of access to clinical 19F MRI, but this is increasingly becoming available in major clinical centers. Moreover, extensive toxicological literature 3840 does suggest that HFB could be used in patients once GMP (good manufacturing practice) is applied.

FREDOM has identified intrinsic differences in intratumoral oxygenation between the various sublines of Dunning R3327, and more importantly, the association between persistent hypoxia, and outcome following radiation therapy. We believe the demonstration of relevance to this second tumor line strengthens the rationale for further development and application of FREDOM with a view to ultimate clinical application.

Acknowledgments

We are grateful to Drs. Vikram Kodibagkar and Anca Constantinescu for collegial support. The research was supported in part by NIH RO1 CA79515/EB2762, a Predoctoral Training supplement R01 CA79515-S and the Cancer Imaging Program pre-ICMIC P20 CA86354. NMR experiments were performed at the Mary Nell & Ralph B. Rogers NMR Center an NIH BTRP # P41-RR02584.

Footnotes

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