Response of mouse intestine to 14 MeV neutrons.

At the Hamburg-Eppendorf Hospital neutron facilities the relative biological effectiveness (r.b.e.) of d,T-neutrons was determined with respect to survival of mouse intestinal crypts. (CBA/Rij x C57BL/Rij)F1 mice were irradiated to the whole body at different depths inside a tissue-equivalent phantom. Irradiations were carried out with a collimated neutron beam at about 6 rad/min given in single doses ranging from 450 to 1000 rad. For reference, gamma-rays from a 60Co therapy unit were used. The number of surviving intestinal crypts per circumference of the jejunum was determined 3 1/2 days after irradiation according to the method of Withers and Elkind. The number of surviving stem cells was calculated on the basis of Poisson statistics. The doses necessary to reduce survival to ten crypt stem cells per circumference amounted to 689 +/- 19 rad for neutrons and 1449 +/- 29 rad for 60Co gamma-rays. From these figures an r.b.e. of 2 . 1 +/- 0 . 1 is obtained. Measurements at different depths in the phantom did not show any variation of r.b.e. with depth along the axis of the neutron beam.     

Study of dose-rate effects of neutron radiation in a wild-type and a repair-deficient yeasts saccharomyces

We report here a comparative analysis of RBE for lethality of a single pulse (duration 65 micros) of fast neutron with ultra high dose rates (up to 6 x 10(6) Gy/s) and continuous neutron radiation (3.6 x 10(3) s) of the pulse reactor BARS-6. Three diploid strains, one haploid strain and three diploid repair-deficient strains (rad52-1/rad52-1; rad54/rad54; rad2/rad2) were used. The RBE values (D(0gamma)/1D(0n)) of a single pulse and continuous neutron irradiation were equal (1.7-1.8) with maximum RBE (4.1-3.1) in region of low doses (shoulder region). Haploid cells were found to be more (3 times) sensitive to both gamma-rays and neutrons than the wild type. There was no obvious decrease in the RBE of 1.9 in highly sensitive haploid cells as compared with highly resistant diploid cells. The repair-deficient strains (rad52-1/rad52-1; rad54/rad54) were more (up to 10 fold) sensitive to both neutrons and gamma-rays as compared with their parent line. The RBE values of 1.5-1.7 of neutrons for these mutants (independent by of the mode of irradiation) were found. The repair-deficient mutant rad2/rad2 had similar sensitivity as a wild type and a RBE value was 2.0. We have concluded that biological effectiveness of the neutrons of pulse reactor BARS-6 was independent of the dose-rate, differing up to 10(8) fold. The RBE didn't vary significantly with the capacity of cells to repair DNA damages.     

The effect of graded doses of fission neutrons or X rays on the lymphoid compartment of the thymus in mice

Young adult CBA/H mice were exposed to graded doses of whole-body irradiation with either fast fission neutrons or 300 kVp X rays at center-line dose rates of 0.1 and 0.3 Gy/min, respectively. Dose-response curves were determined at Days 2 and 5 after irradiation for the total thymic cell survival and for the survival of thymocytes defined by monoclonal anti-Thy-1, -Lyt-1, -Lyt-2, and -T-200 antibodies as measured by flow cytofluorometric analysis. Cell dose-response curves of thymocytes show, 2 days after irradiation, a two-component curve with a radiosensitive part and a part refractory to irradiation. The radiosensitive part of the dose survival curve of the Lyt-2+ cells, i.e., mainly cortical cells, has a D0 value of about 0.26 and 0.60 Gy for neutrons and X rays, respectively, whereas that of the other cell types has corresponding D0 values of about 0.30 and 0.70 Gy. The radiorefractory part of the dose-response curves cannot be detected beyond 5 days after irradiation. At that time, the Lyt-2+ cells are again most radiosensitive with a D0 value of 0.37 and 0.99 Gy for neutrons and X rays, respectively. The other measured cell types have corresponding D0 values of about 0.47 Gy. The fission neutron RBE values for the reduction in the thymocyte populations defined by either monoclonal anti-Thy-1, -Lyt-1, -Lyt-2, or -T-200 antibodies to 1.0% vary from 2.6 to 2.8. Furthermore, the estimated D0 values of the Thy-1-, T-200- intrathymic precursor cells which repopulate the thymus during the bone marrow independent phase of the biphasic thymus regeneration after whole-body irradiation are 0.64-0.79 Gy for fission neutrons and 1.32-1.55 Gy for X rays.     

The relative biological effectiveness in V79 Chinese hamster cells of the neutron capture reactions in boron and nitrogen

V79 Chinese hamster cells were irradiated in the presence of different amounts of boric acid with thermal neutrons at the Medical Research Reactor at Brookhaven National Laboratory. From the linear dose-survival curves observed, a D0 value of 66 rad for the 10B(n, alpha) 7Li neutron capture reaction was obtained. No dependence of this value on the concentration of boric acid was found. Comparing this value to the D0 value of 150 rad obtained with 250 kVp X rays between 10 and 0.01% survival, an extrapolated RBE value of 2.3 was calculated. By irradiation of the same line of cells with cold neutrons at the Institut Laue - Langevin , a D0 value for the 14N(n,p)14C reaction of 77 rad was obtained, with a corresponding RBE value of 1.9. Comparison is made with previously published RBE values for the 10B(n, alpha) 7Li reaction.     

Repair of potentially lethal damage in yeast induced by fast neutrons

Survival curves of 3 diploid (D7) yeast strains: one wild-type, one deficient in excision of pyrimidine dimers (UV-sensitive) and one blocked in DNA double-strand-break repair (X-ray-sensitive), were compared after irradiation with cyclotron-produced fast neutrons. It was observed that both the UV-sensitive (rad3/rad3) and the X-ray-sensitive (rad52/rad52) mutants were more sensitive to neutrons than the wild-type. The role of DNA double-strand-breaks in neutron-induced cell death was further studied by comparing the relative sensitivity of the rad52/rad52 mutant to gamma-rays and fast neutrons. A comparison of the dose modification factors revealed that the deficiency in DNA double-strand-break repair did not make the yeast cells more sensitive to neutrons than to photons, which suggests that lesions of a different type may also be produced by neutrons. Survival curves obtained upon immediate plating and after delayed plating of neutron-irradiated cells showed that all 3 yeast strains were efficient in liquid holding recovery. The role of different repair pathways in cellular recovery from neutron-induced lethal damage is discussed.     

Neutron RBEs and the radiosensitive target for mouse immature oocyte killing

The highly radiosensitive immature oocytes of mice were irradiated in vivo with graded doses of 252Cf fission radiation, 0.43- or 15-MeV neutrons, or 60Co gamma rays. Comparisons of oocyte survival for neutrons and for gamma rays demonstrate that neutron RBEs for the killing of these important cells do not reach the high values (30-50 or more) at low doses observed for several other biological end points. Rather, neutrons differ little in effectiveness from gamma rays in killing these extremely sensitive murine oocytes. For 0.43-MeV neutrons, RBEs obtained from fitted survival curves reach only 1.7 at 0.1 rad. For 15-MeV neutrons, they are not significantly different from 1 at any dose tested (lowest, 4.5 rad). For 252Cf fission neutrons (E = 2.15 MeV), RBEs are intermediate between those for 0.43- and 15-MeV neutrons. For all neutron energies tested, the RBEs are particularly low in the juvenile period, a time when murine immature oocytes are especially radiosensitive. With exposure just prior to birth, however, when these cells are much less easily killed, higher, more usual RBEs are found. The minimum size of the lethality target in mouse immature oocytes, estimated from the inactivation constant for 0.43-MeV neutrons and microdosimetric values, is larger than the nucleus but not larger than the cell. This and related analytical considerations suggest that the hypersensitive target in these particular oocytes is the plasma membrane, a finding which is in excellent accord with results from other experiments using different, contrasting radiations and dose deliveries (accelerated Si14+ ions, gamma rays, and beta rays from 3HOH compared with those from [3H]thymidine).     

The effects of graded doses of 1 MeV fission neutrons or X rays on the murine hematopoietic stroma.

The acute radiosensitivity in vivo of the murine hematopoietic stroma for 1 MeV fission neutrons or 300 kVp X rays was determined. Two different assays were used: (1) an in vitro clonogenic assay for fibroblast precursor cells (CFU-F) and (2) subcutaneous grafting of femora or spleens. The number of stem cells (CFU-S) or precursor cells (CFU-C), which repopulated the subcutaneous implants, was used to measure the ability of the stroma to support hemopoiesis. The CFU-F were the most radiosensitive, and the survival curves after neutron and X irradiation were characterized by D0 values of 0.75 and 2.45 Gy, respectively. For regeneration of CFU-S and CFU-C in subcutaneously implanted femora, D0 values of 0.92 and 0.84 Gy after neutron irradiation and 2.78 and 2.61 Gy after X irradiation were found. The regeneration of CFU-S and CFU-C in subcutaneously implanted spleens was highly radioresistant as evidenced by D0 values of 2.29 and 1.49 Gy for survival curves obtained after neutron irradiation, and D0 values of 6.34 and 4.85 Gy after X irradiation. The fission-neutron RBE for all the cell populations was close to 3 and varied from 2.77 to 3.28. The higher RBE values observed for stromal cells, compared to the RBE of 2.1 reported previously for hemopoietic stem cells, indicate that stromal cells are relatively more sensitive than hemopoietic cells to neutron irradiation.     

Marked difference in sensitivity to gamma-ray-induced cataract between BALB/c and CBA-C3H strain mice]

Nineteen BALB/c, 14CBA/KI, 12C3H/HeJ and 15 (CBA/Kl x C3H/HeJ) F1 female mice were irradiated with 850 rad gamma-rays and transferred with 10(7) syngeneic bone marrow cells 24 hrs later. The occurrence of cataract was examined in these animals. All the BALB/c mice showed visible lens opacification in both eyes between 113 and 149 days after irradiation. All the animals were autopsied 6 months after irradiation and examined for opacification of their lenses. The proportion of opaque lenses was 100, 7.1, 16.7 and 0% in BALB/c, CBA/Kl, C3H/HeJ and (CBA/Kl x C3H/HeJ) F1 mice, respectively. The results indicate that BALB/c mice are much more sensitive to radiation-induced cataractogenesis than CBA and C3H mice.     

Evidence for similarities between radiation damage expressed by beta-araA and damage involved in the interaction effect observed after exposure of V79 cells to mixed neutrons and gamma radiation

Plateau-phase V79 cells were exposed sequentially to fast neutrons and gamma rays. A dose-dependent reduction in the shoulder width of the gamma-ray survival curve was observed after preexposure of cells to neutrons. A similar effect was demonstrated on the neutron survival curve when cells were preirradiated with gamma rays. Treatment of cells with 150 microM beta-araA after either gamma or neutron irradiation reduced primarily the shoulder of the survival curve. When beta-araA was given to the cells after exposure to mixed radiation modalities, survival curves similar to those observed after exposure to a single radiation modality and treatment with beta-araA were obtained. The kinetics of loss of the interaction observed after exposure of cells to gamma rays following neutron irradiation was similar to the kinetics of loss of sensitivity to beta-araA (T1/2 = 1 h) measured by delaying drug administration after exposure to gamma rays. The results suggest that the PLD expressed by beta-araA is at least partly involved in the interactive effect observed after combined exposure of plateau-phase V79 cells to neutrons and gamma rays.     

Life shortening in mice exposed to fission neutrons and gamma rays. V. Further studies with single low doses

Data are presented on the mean after survival of female B6CF1 mice exposed to single doses of neutrons (1 to 40 rad) or gamma rays (22.5, 45, and 90 rad). For gamma-ray exposures and for neutron exposures up to 10 rad, the dose-response curves are indistinguishable from linear; higher neutron doses produce significant departures and linearity. Consequently, in these data, an upper limit of the relative biological effectiveness (RBE) exists for life shortening from all causes of death after single neutron exposures; this value is 15.0 +/- 5.1. The RBE depends on the cause of death, ranging from 2 to 5 for lymphoreticular tumors to 23-24 for lung tumors.     

Neoplastic transformation is enhanced by multiple low doses of fission-spectrum neutrons

The neoplastic transformation of C3H mouse 10T1/2 cells was measured induced by fission-spectrum neutrons delivered at a high dose rate in five fractions over 4 days. The transformation frequency was significantly enhanced over that due to single equivalent total doses. These new data, in the low dose region, demonstrate an increased transformation frequency by fractionated versus single exposures of high-dose-rate fission-spectrum neutrons; an increase equal to that observed with low-dose-rate fission-spectrum neutrons (i.e., 0.086 rad/min). Estimates of the dose modifying factor (DMF), based upon the ratio of the initial linear portions of the induction curves for high and for low dose rates, suggest the same DMF (approximately 7.8) for both five daily fractions of high-dose-rate neutrons and for low-dose-rate neutrons. However, when these results are compared to those following high-dose-rate 60Co gamma rays (100 rad/min), the relative biological effectiveness (RBE) for low-dose-rate fission-spectrum neutrons based upon slope ratios is 19.6; similarly, the RBE relative to five daily fractions of 60Co gamma rays is 78.8.     

Relative biological effectiveness measurements using murine lethality and survival of intestinal and hematopoietic stem cells after fermilab neutrons compared to JANUS reactor neutrons and 60Co gamma rays

The relative biological effectiveness (RBE) of the 25-MeV (average energy) neutron beam at the Fermi National Accelerator Laboratory was measured using murine bone marrow (LD50/30) and gut (LD50/6) lethality and killing of hematopoietic colony forming units (CFU-S) or intestinal clonogenic cells (ICC). The reference radiation was 60Co gamma rays. The LD50/30 and LD50/6 for mice exposed to the Fermilab neutron beam were 6.6 and 8.7 Gy, respectively, intermediate between those of JANUS neutrons and 60Co gamma rays. The D0 values for CFU-S and ICC were 47 cGy and 1.05 Gy, respectively, also intermediate between the lowest values found for JANUS neutrons and the highest values found after 60Co gamma rays. The split-dose survival ratios for CFU-S at intervals of 1-6 hr between doses were essentially 1.0 for both neutron sources, while the corresponding split-dose survival ratio for 60Co gamma rays was consistantly above 1, reaching a maximum of 1.7 with a 1-hr interval between doses. The 3-hr split-dose survival ratios for ICC were 1.0 for JANUS neutrons, 1.85 for Fermilab neutrons, and 6.5 for 60Co gamma rays. The RBE estimates for LD50/30 were 1.5 and 2.3 for Fermilab and JANUS neutrons, respectively. Based on LD50/6, the RBEs were 1.9 (Fermilab) and 3.0 (JANUS). The RBEs for CFU-S D0 were 1.4 (Fermilab) and 1.9 (JANUS) and for jejunal microcolony D0 1.4 (Fermilab) and 2.8 (JANUS).     

Interpretation of cytogenetic damage induced in the germ line of male mice exposed for over 1 year to 239Pu alpha particles, fission neutrons, or 60Co gamma rays

The relative biological effectiveness (RBE) of 239Pu alpha particles, fission neutrons (0.85 MeV), and 60Co gamma rays has been evaluated for the induction of reciprocal chromosome translocations in spermatogonia and of chromosome/chromatid fragments and chromatid rearrangements in the primary spermatocyte of adult male B6CF1 mice. Age concurrency was maintained for both internal and external radiations which were delivered at about 1 rad/week for 239Pu (single intravenous dose of 10 microCi/kg), 0.67, 1.67, and 2.67 rad/week for neutrons, and 6.95, 17.4, and 32 rad/week for gamma rays for at least 60 weeks. In terms of frequency of translocations, the response to the alpha emitter was nonlinear (concave downward) with little dose-response predictability; to cumulative neutron exposures the response was linear, without evidence of a dose-rate effect; and to gamma radiation the responses were linear, and a significant dose-rate effect was seen. RBE estimates are variable. For translocations, the n/gamma ratio is between 10 and 24, depending upon weekly dose level, and the ratio is 1 or less for the alpha particle relative to the neutron. For fragments, the n/gamma ratio is 18 to 22, depending upon age factors, and alpha/n is 1.5. For chromatid rearrangements, n/gamma is 7 and alpha/n is essentially indeterminate, but much below one. The overall response to the alpha emitter is interpreted to be a complex function of (a) microdosimetric heterogeneity, (b) a nearly invariant deposition pattern in the gonad, (c) the high sensitivity of differentiating spermatogonia to cell killing, and (d) the capacity of stem cells in relatively radiation-free areas to progressively assume the major spermatogenic role.     

An analysis of the cytogenetic effects of gamma and neutron irradiation in a human lymphocyte culture at the G0 and G1 stages of the mitotic cycle (a structural-functional approach)

A study was made of the dose dependence of the chromosome aberration frequency in human lymphocytes exposed to 60Co-gamma radiation and neutrons (mean energy of 0.85 MeV) at the G0 stage and in different periods of the G1 and G1/S stages of the cycle. With gamma irradiation the dose dependence for cells at the G1 and G1/S stages was at a higher level than that for cells at the G0 stage, whereas the opposite picture was observed for cells exposed to neutron radiation. The difference was also noted in the time-response curves where gamma radiation increased and neutrons, on the contrary, decreased the aberration yield in the cells that passed from G0 to G1 stage. The experimental data obtained are attributed to activation of repair system at the G1 stage which is mainly conditioned by chromatin decondensation; the activating, that is, the functional factor influences the aberration induction with gamma irradiation, while the decondensation, that is, the structural factor, with neutron irradiation.     

Life-shortening and disease incidence in C57Bl mice after single and fractionated gamma and high-energy neutron exposure

C57Bl Cnb mice were exposed to single or fractionated d(50)+Be neutrons or 137Cs gamma-ray exposure at 12 weeks of age and were followed for life-shortening and disease incidence. The data were analyzed by the Kaplan-Meier procedure using as criteria cause of death and possible cause of death. Individual groups were compared by a modified Wilcoxon test according to Hoel and Walburg, and entire sets of different doses from one radiation schedule were evaluated by the procedure of Peto and by the Cox proportional hazard model. No significant difference was found in life-shortening of C57Bl mice between a single gamma and neutron exposure. Gamma fractionation was clearly less effective in reducing survival time than a single exposure. On the contrary, fractionation of neutrons was slightly although not significantly more effective in reducing life span than a single exposure. Life-shortening appeared to be a linear function of dose in all groups studied. The data on causes of death show that malignant tumors, particularly leukemias including thymic lymphoma, and noncancerous late degenerative changes in lung were the principal cause of life-shortening after a high single gamma exposure. Exposure delivered in 8 fractions 3 h apart was more effective in causing leukemias and all carcinomas and sarcomas than one delivered in 10 fractions 24 h apart or in a single session. Following a single neutron exposure, leukemias and all carcinomas and sarcomas appeared to increase somewhat more rapidly with dose than after gamma irradiation. No significant difference in the incidence of leukemias and all carcinomas and sarcomas was noted between a single and a fractionated neutron exposure.     

Effects of single and split doses of cobalt-60 gamma rays and 14 MeV neutrons on mouse stem cell spermatogonia

The long-term effects of ionizing radiation on male gonads may be the result of damage to spermatogonial stem cells. Doses of 10 cGy to 15 Gy (60)Co gamma rays or 10 cGy to 7 Gy 14 MeV neutrons were given to NMRI mice as single or split doses separated by a 24-h interval. The ratios of haploid spermatids/2c cells and the coefficients of variation of DNA histogram peaks as measures of both the cytocidal and the clastogenic actions of radiation were analyzed by DNA flow cytometry after DAPI staining. The coefficient of variation is not only a statistical examination of the data but is also used here as a measure of residual damage to DNA (i.e. a biological dosimeter). Testicular histology was examined in parallel. At 70 days after irradiation, the relative biological effectiveness for neutrons at 50% survival of spermatogonial stem cells was 3.6 for single doses and 2.8 for split doses. The average coefficient of variation of unirradiated controls of elongated spermatids was doubled when stem cells were irradiated with single doses of approximately 14 Gy (60)Co gamma rays or 3 Gy neutrons and observed 70 days later. Split doses of (60)Co gamma rays were more effective than single doses, doubling DNA dispersion at 7 Gy. No fractionation effect was found with neutrons with coefficients of variation.     

The response of ataxia-telangiectasia lymphoblastoid cells to neutron irradiation

The response of control and ataxia-telangiectasia (A-T) cells to increasing doses of high-linear-energy-transfer (LET) ionizing radiation (neutrons) was compared. Ataxia-telangiectasia cells were markedly more sensitive to neutron irradiation than were control cells. The D0 value for the two A-T cell lines was 0.4 Gy while the value for controls was approximately 1.4 Gy. Fast neutrons were considerably more effective than gamma rays in inducing cell death in both cell types, but the sensitivity factor remained approximately the same as with gamma rays. A minimal depression of DNA synthesis was observed in ataxia-telangiectasia cells after neutron irradiation, similar to that reported previously after gamma irradiation. The extent of inhibition was not significantly greater in control cells, contrary to that seen with gamma rays. In time-course experiments a significant difference in degree of inhibition of DNA synthesis was observed between the cell types. Low doses of fast neutrons induced a G2-phase delay in both cell types, but the degree and extent of this delay was greater in ataxia-telangiectasia cells as observed previously with low-LET radiation.     

Independent effect of a mixed-beam regimen of fast neutrons and gamma rays on a murine fibrosarcoma

Biological effectiveness of a mixed-beam regimen of fast neutrons and photons was studied in an animal tumor system. NFSa , a spontaneous fibrosarcoma in a C3H mouse, was transplanted in the right hind legs of syngeneic male mice and locally irradiated with a single dose or five daily doses. Tumor control experiments showed that five gamma-ray doses increased TCD50 values by 20 Gy and produced a shallower slope on the dose-response curve compared to that after a single fraction. Fractionated neutron doses also increased the TCD50 value by 9 Gy without changing the slope of the dose-response curve. A mixed-beam regimen of N-gamma-gamma-gamma-N resulted in an independent effect on the tumor. Second, tumor cell survival was examined by the lung colony assay. Nembutal anesthesia reduced the tumor oxic cell fraction, resulting in a single component dose-response curve after a single gamma ray. Five fractionated doses of gamma rays increased both D0 and extrapolation number while those of fast neutrons increased only extrapolation number. The D0 and extrapolation number of the mixed-beam regimen were again identical to those values assuming that the mixed-beam effect was independent. RBEs obtained from cell survival were fairly close to those from TCD50 assays except single-dose experiments.     

The dose-response relationships for myeloid leukemia and malignant lymphoma in BC3F1 mice

The present analysis of data on the induction of lymphoma and myeloid leukemia in BC3F1 mice has indicated some new and interesting aspects regarding the shapes of the dose-effect curves. The incidence data can be interpreted by radiobiological models of the induction process coupled with cell inactivation. In particular, for malignant lymphoma the dose-response curve after X rays can be described assuming a quadratic model corrected for cell inactivation, while the incidence data after fission neutrons are best fitted by a linear model which also allows for cell inactivation. Myeloid leukemia has also been induced in BC3F1 mice. The bell-shaped dose-response curves observed after irradiation with either X rays or neutrons are explained by assuming simultaneous initial transforming events and cell inactivation with the data for cell inactivation at higher doses being in agreement with data reported for other strains of mice. A value for relative biological effectiveness of 4 is obtained at the lowest neutron dose used. The value of the inactivation parameters can be compared with those of the cell inactivation probability per unit dose for the bone marrow hematopoietic stem cells, which are believed to be the target cells for these tumors.     

Radiation-induced pulmonary endothelial dysfunction and hydroxyproline accumulation in four strains of mice

C57BL mice exposed to 14 Gy of whole-thorax irradiation develop significant histologic lung fibrosis within 52 weeks, whereas CBA and C3H mice do not exhibit substantial fibrosis during this time. The purpose of the present study was to determine whether this strain-dependent difference in radiation histopathology is associated with genetic differences in pulmonary endothelial metabolic activity or in endothelial radioresponsiveness. C57BL/6J, C57BL/10J, CBA/J, and C3H/HeJ mice were sacrificed 12 weeks after exposure to 0 or 14 Gy of 300-kV X rays to the whole thorax. Lung angiotensin converting enzyme (ACE) activity and plasminogen activator (PLA) activity were measured as indices of pulmonary endothelial function; and lung hydroxyproline (HP) content served as an index of pulmonary fibrosis. Lung ACE and PLA activities in sham-irradiated C57BL/6J and CB57BL/10J mice were only half as high as those in sham-irradiated CBA/J and C3H/HeJ mice. Exposure to 14 Gy of X rays produced a slight but nonsignificant reduction in lung ACE and PLA activity in the C57BL strains, and a significant reduction in the CBA/J and C3H/HeJ mice. Even after 14 Gy, however, lung ACE and PLA activities in CBA/J and C3H/HeJ mice were higher than those in sham-irradiated C57BL/6J and C57BL/10J mice. Lung HP content in all four strains increased significantly after irradiation, but this increase was accompanied by an increase in lung wet weight. As a result, HP concentration (per milligram wet weight) remained constant or increased slightly in both C57BL strains and actually decreased in the CBA/J and C3H/HeJ mice. These data demonstrate significant genetic differences in both intrinsic pulmonary endothelial enzyme activity and endothelial radioresponsiveness among the four strains of mice. Specifically, strains prone to radiation-induced pulmonary fibrosis (C57BL/6J, C57BL/10J) exhibit only half as much lung ACE and PLA activity as do strains resistant to fibrosis (CBA and C3H).