The kinetics of repair in mouse lung after fractionated irradiation

The kinetics of repair of sublethal damage in mouse lung was studied after fractionated doses of 137Cs gamma-rays. A wide range of doses per fraction (1.7-12 Gy) was given with interfraction intervals ranging from 0.5 to 24 h. The data were analysed by a direct method of analysis using the incomplete repair model. The half-time of repair (T1/2) was 0.76 h for the pneumonitis phase of damage (up to 8 months) and 0.65 h for the later phase of damage up to 12 months. The rate of repair was dependent on fraction size for both phases of lung damage and was faster after large dose fractions than after small fractions. The T1/2 was 0.6 h (95 per cent c.1. 0.53, 0.69) for doses per fraction greater than 5 Gy and 0.83 h (95 per cent c.1 0.76, 0.92) for doses per fraction of 2 Gy. Repair was nearly complete by 6 h, at least for the pneumonitis phase of damage. To the extent that extrapolation of these data to humans may be valid, these results imply that treatments with multiple fractions per day that involve the lung will not be limited by the necessity for interfraction intervals much longer than 6 h.     

Repair capacity and kinetics in spheroids from a lung metastasis of a human soft tissue sarcoma: a growth delay study.

Spheroids grown from the human cell line EF8 of a lung metastasis of a human malignant fibrous histiocytoma were given fractionated irradiation with 60Co gamma rays at passages 31 and 32. The mean diameter of the spheroids at the time of treatment was 250 microns. Growth delay was used as the end point in these studies. Two experiments were carried out to determine the capacity and kinetics of repair of sublethal damage. In the first experiment, one, two, and five fractions were given at three or four dose levels with fixed intervals of 360 min. In the second experiment, schedules with two and four dose fractions and intervals of 0, 20, 60, 120, and 360 min were used, each at two dose levels. Data analysis was performed by a direct method based on the alpha/beta model and first-order repair kinetics of radiation damage. In both experiments, the alpha/beta value of EF8 spheroids was estimated to be about 8 (6-10) Gy. The rate constant of repair, mu, and its 95% confidence interval were estimated to be 0.62 (0.40-0.84) 10(-2) min-1, equivalent to a half-time of repair (T1/2) of 112 (83-172) min. A more detailed analysis of the data of the second experiment revealed a significant dependence of the rate constant of repair, mu, on the total radiation effect induced by the fractionated radiation treatments with short overall times. With increasing level of effect, mu decreased. These data indicate that the half-time of recovery of a human tumor can be longer than that of the surrounding normal tissue, in this case lung, at least for a limited range of doses and for some fractionation schedules.     

A test of equal effect per fraction in the kidney of the mouse.

Measurements of renal damage in the mouse were made to determine if there was an equal effect per fraction during a course of repeated 240-kVp X-ray doses. An X-ray dose of 2 Gy was given 2, 8, 14, or 20 times with interfraction intervals of 12 h. Some animals were also irradiated with twenty 2-Gy doses using a 5-h interfraction interval. The underlying effect per fraction (-logeSF of the notional target cell population) was determined from the additional top-up dose of d(4)-Be neutrons needed to produce measurable renal impairment assessed by decreased clearance from the plasma of [51Cr]EDTA and by a reduction in the hematocrit at 25, 29, 33, and 39 weeks after treatment. There was no significant influence of the time of assay on the values of underlying effect measured. A mean value of underlying effect was therefore calculated for the two different assays of each mouse, from the measurements at the four times. This gave approximately 40 estimates (one for each animal assessed) with each assay of the effectiveness of 2-Gy fractions in each of the four fractionation schedules, a total of 321 determinations in the study with 12-h intervals. Regression analysis showed that there was no significant trend in underlying effect per fraction with number of fractions, i.e., the damage per fraction was constant regardless of the number of fractions used. With underlying effect normalized to 1 unit of damage for a single 2-Gy dose, the slope of this plot was -0.0013 per fraction2 +/- 0.0097 (95% CL). The assumption of equal effect per fraction was therefore not invalidated in the kidney of the mouse. With a 5- instead of a 12-h interfraction interval, the 20-fraction schedule was 7% more effective as measured by the two assays analyzed together; this was significant at P = 0.0001. This shows that 5 h is not sufficient time between fractions for full repair to occur in the kidney, and underlines the need for intervals of at least 6 h between the doses in clinical radiotherapy using more than one fraction per day. The data are consistent with an alpha/beta ratio approximately 1.6 Gy, with a repair half-time approximately 1.3 h. However, these experiments were not designed to determine these parameters and their values should be regarded only as rough estimates.     

Radiation-induced renal damage: the effects of hyperfractionation

The response of mouse kidneys to multifraction irradiation was assessed using three nondestructive functional end points. A series of schedules was investigated giving 1, 2, 4, 8, 16, 32, or 64 equal X-ray doses, using doses per fraction in the range of 0.9 to 16 Gy. The overall treatment time was kept constant at 3 weeks. Kidney function was assessed from 19 to 48 weeks after irradiation by measuring changes in isotope clearance, urine output, and hematocrit. The degree of anemia (assessed from the hematocrit measurements) is a newly developed assay which is an early indicator of the extent of renal damage after irradiation. All three assays yielded steep dose-effect curves from which the repair capacity of kidney could be estimated by comparing the isoeffective doses in different schedules. There was a marked influence of fractionation, with increasing dose being required to achieve the same level of damage for increasing fraction number, even between 32 and 64 fractions. The data are well fitted by a linear quadratic dose-response equation, and analysis of the data in this way yields low values (approximately 3.0 Gy) for the ratio alpha/beta. This would suggest that hyperfractionation , using extremely small X-ray doses per fraction, would spare kidneys relative to tumors and acutely responding tissues.     

An 'incomplete-repair' model for survival after fractionated and continuous irradiations

An incomplete-repair (IR) model of survival after fractionated or continuous irradiation is derived from the concept of 'dose-equivalent' of incomplete repair. The model gives reasonably good predictions of the effect of interfraction interval, dose per fraction, and dose rate on cell survival in vivo and on tissue responses. This model is compared to the 'lethal, potentially lethal' (LPL) model after the latter has been generalized to an arbitrary number of fractions and to low dose-rate, continuous exposures. It is shown that the two models are equivalent, given certain constraints on the size of dose per fraction and dose rate. For example, in a particular cell line the equivalence of fractionation models breaks down if dose per fraction is well in excess of 4 Gy (the IR model employs the linear-quadratic survival model). The equivalence of low dose rate models breaks down for dose rates well in excess of 20 cGy/min. The assumptions on which the generalized LPL model is based are used to give a radiobiological interpretation to the incomplete-repair model. The larger beta/alpha ratio characteristic of late-responding normal tissues is interpreted in terms of the relatively faster fixation of potentially reparable lesions in the target cells of acutely responding tissues, on account of progression in the cell cycle. According to this interpretation the beta/alpha ratios estimated from isoeffective fractionation regimens are directly related to the parameters of clonogenic cell killing.     

Multifraction radiation response of mouse lung

The response of mouse lung to repeated doses of 60Co gamma-rays of as low as 115 cGy per fraction was measured using death from pneumonitis between 80 and 120 days after irradiation as the endpoint. A fractionation interval of 3 h was maintained for most regimens but in the longer experiments some 12 h intervals were introduced for logistic reasons. The longest overall duration (for a 43 fraction regimen) was 8 days. The total doses required to produce 50 per cent mortality increased continuously as dose/fraction was decreased, even from 160 to 115 cGy per fraction. Of clinical relevance, the steepness of the isoeffect curve over the dose range 115-500 cGy indicates that the lung shows greater sparing from dose fractionation than is characteristic of more rapidly-responding normal tissues, resembling, in this respect, other more slowly-responding tissues such as spinal cord. The plot of the reciprocal of the LD50 values as a function of dose per fraction was non-linear, suggesting that a linear quadratic dose response model may not be appropriate or that repair of cellular injury in lung is not complete in 3 h, or both.     

Calf thymus composition: a comparison of differential centrifugation and chemical fractionation procedures

The extraction behavior of thymus and the composition of fractions prepared from this organ has been studied. Sequential extraction methods using 0.15 M NaCl followed by water gave information with respect to the weight fraction of cytoplasmic and nuclear constituents. Lipide, nucleic acid, and electrophoretic analysis of the extracts provided additional information. A less complex electrophoretic pattern was obtained from subsequent extracts in the sequence. Sucrose and saline dispersates obtained from tissue fragmented with either the Potter-Elvehjem homogenizer or in a Waring blendor were fractionated, using standard differential sedimentation methods. The fractions obtained by means of four different dispersion procedures were compared in terms of yield, chemical analysis, and electrophoretic composition. The quantity of material in thymus having the sedimentation characteristics of liver mitochondrial and microsomal fractions was remarkably small. Both the suspension medium employed and the method used to bring about a disruption of the cells in the tissue affected the yield of "particulate" material. The components present in the later extracts in the sequence, E(4) to E(7), in the case of sequential extraction study resembled with respect to chemical composition and electrophoretic characteristics, the microsome fraction prepared by differential sedimentation methods. About 76 per cent of the PNA in the tissue appeared to be in the cytoplasm. The remaining 24 per cent PNA was found in the nucleus and accounted for 1.7 per cent of nucleus on a dry weight basis. From 75 to 88 per cent of cytoplasmic PNA was extracted from the tissue and 76 to 94 per cent of the PNA in the extract was found in the final supernatant solutions, depending upon the dispersion methods and suspension medium used in the extraction procedure. The composition of the final supernatant fractions using differential sedimentation methods were comparable in terms of electrophoretic properties, protein concentration, nucleic acid content, and fractionation behavior to saline extracts E(1) to E(3), of thymus used in earlier studies.     

Molecular modifications associated with Aging of globin messenger RNA in vitro.

Using polyacrylamide gel elution-electrophoresis in aqueous medium, highly purified rabbit globin mRNA can be fractionated into several populations of molecules differing by their mean poly(A) content. Both alpha and beta globin mRNA are heterogenous with respect to their electrophoretic mobilities. With the conditions used no separation of alpha and beta globin mRNA occurs during electrophoresis. From the specific radioactivity distribution in the different mRNA fractions one can conclude that the polyadenylate sequence at the 3' end of globin mRNA molecules becomes shorter with aging. This shortening occurs on alpha as well as beta, globin mRNAs and the extent of heterogeneity in poly(A) content is similar for both globin mRNAs. Furthermore, using two different methods of mRNA fractionation (polyacrylamide gel elution-electrophoresis and elution of poly (U)-Sepharose-bound mRNA at increasing temperatures) it is shown that old mRNA molecules differ from relatively young messages in their ability to direct cell-free globin synthesis. Modifications reducing template activity in vitro thus seem to take place during globin mRNA aging.     

The interaction between X-rays and 3 MeV neutrons in the skin of the mouse foot

Mouse feet were irradiated with mixtures of 3 MeV neutrons and 140 kVp X-rays given simultaneously or within 24 hours of each other. The effects of different treatments were contrasted by comparing the doses required to give equal skin reactions. Irradiation was given as 1, 2, 4 or 8 equal fractions, in order to assess r.b.e. and the shapes of the underlying dose-response curves for mixed beams over a wide range of dose per fraction. All dose-effect curves were well fitted by a linear-quadratic (alpha, beta) model. For X-rays and neutrons given simultaneously, the linear coefficient (alpha) decreased by a factor of 4.80 while the quadratic coefficient (beta) increased by a factor of only 1.44 when the proton contamination in the beam increased from 11 to 100 per cent, with alpha/beta changing from 95.0 to 13.8. The data from simultaneous X-ray and neutron irradiation were consistent with full interaction of those effects from the two radiations which give rise to the total quadratic component of effect. When the two radiations are separated by up to 24 h, this interaction decreases but does not entirely disappear.     

Bystander and delayed effects after fractionated radiation exposure

Human immortalized keratinocytes were exposed to a range of single or fractionated doses of gamma rays from (60)Co, to medium harvested from donor cells exposed to these protocols, or to a combination of radiation and irradiated cell conditioned medium (ICCM). The surviving fractions after direct irradiation or exposure to ICCM were determined using a clonogenic assay. The results show that medium harvested from cultures receiving fractionated irradiation gave lower "recovery factors" than direct fractionated irradiation, where normal split-dose recovery occurred. The recovery factor is defined here as the surviving fraction of the cells receiving two doses (direct or ICCM) separated by an interval of 2 h divided by the surviving fraction of cells receiving the same dose in one exposure. After treatment with ICCM, the recovery factors were less than 1 over a range of total doses from 5 mGy-5 Gy. Varying the time between doses from 10 min to 180 min did not alter the effect of ICCM, suggesting that two exposures to ICCM are more toxic than one irrespective of the dose used to generate the response. In certain protocols using mixtures of direct irradiation and ICCM, it was possible to eliminate the bystander effect. If bystander factors are produced in vivo, then they may reduce the sparing effect of the dose fractionation.     

The structures of the carbohydrate moieties of mouse kidney gamma-glutamyltranspeptidase: occurrence of X-antigenic determinants and bisecting N-acetylglucosamine residues

Paper electrophoresis and Bio-Gel P-4 column chromatography of the oligosaccharides released from mouse kidney gamma-glutamyltranspeptidase by hydrazinolysis gave fractionation patterns quite distinct from those of the bovine and rat kidney enzymes. Structural studies of the fractionated oligosaccharides by sequential exoglycosidase digestion in combination with methylation analysis showed that mouse kidney gamma-glutamyltranspeptidase contains a series of bisected complex-type asparagine-linked sugar chains with the following oligosaccharides as their outer chain moieties: GlcNAc beta 1----, Sia alpha 2----Gal beta 1----4GlcNAc beta 1----, Gal beta 1----4(Fuc alpha 1----3)GlcNAc beta 1----, and sialylated N-acetyllactosamine repeating sugar chains. Some of these sugar chains were found for the first time in glycoproteins.     

Bovine follitropin. Isolation and characterization of the native hormone and its alpha and beta subunits

1) A reproducible procedure was developed for the purification of bovine follitropin. 2) The method involved ammonium sulfate precipitation, ion exchange and adsorption chromatography, concanacaline-A-Sepharose chromatography and gel filtration. 3) A specific radioligand receptor assay was used to monitor each chromatographical step. 4) The potency of highly purified bovine follitropin as measured by Steelman and Pohley bioassay was 62 times the NIH-FSH-B1 standard preparation. 5) Contaminations of bovine follitropin by other glycoprotein hormones such as thyrotropin and lutropin amounted to 3 and 0.45 per cent by weight respectively as measured by specific radioimmunoassays and radioligand receptor assays. 6) The subunits alpha and beta of bovine follitropin were obtained by incubation in acidic urea, the chains being then separated by anion exchange chromatography. The subunits were subjitted to complete characterization. The amino-terminal residue of the alpha subunit is phenylalanine while a half cystine residue was found at the aminoterminal end of the beta chain. 8) Cross-contamination of the alpha and beta subunit preparations was measured by specific radioimmunoassays and amounted to 0.02 and 0.1 per cent by weight respectively.     

The relationship between o.e.r., r.b.e. and number of fractions for X-ray- or neutron-induced skin damage.

The skin reactions in aerated and hypoxic mouse tails after single or fractionated doses of 250 kV X-rays or fast neutrons (6 MeV deuterons on beryllium) have been measured. The o.e.r. for one to sixteen fractions of X-rays remains constant, while that for one to ten fractions of neutrons decreases with increasing neutron fractionation and decreasing neutron dose/fraction. The o.e.r. for X-rays was 1.7, for single-neutron doses 1.4, and for ten fractions of neutrons 1.25. It was anticipated that the o.e.r. for neutron-induced damage would decrease further as neutron fractionation is increased because the contribution to damage from the highest LET components of dose, the alpha and heavy recoil particles, would increase relative to the lowe LET components. The r.b.e. values obtained for skin damage were higher at all neutron doses/fraction examined in this study on tails than all those previously obtained in studies on skin at other sites on four species. This may be due to the influence of hypoxia on the r.b.e. measurements in the mouse tail.     

Early changes in mouse urinary bladder function following fractionated X irradiation.

Functional changes in the mouse urinary bladder following single-dose or fractionated irradiation were assessed by cystometry, i.e., by measuring the intravesical volume-pressure relationship during transurethral filling. The early response presented as a dose-dependent and transitory decrease in the reservoir function of the organ as defined by the intravesical volume at a filling pressure of 10 or 20 mm Hg, V10 or V20. The quantal dose response used in the present study was a reduction in the individual bladder volume (V10 and V20) by at least 50%. After single doses greater than or equal to 10 Gy, the reaction occurred between Days 7 and 25 with maximum prevalence between Days 7 and 14. The individual duration of the response was 3-9 days. Treatment with single doses and 2, 3, 5, and 10 fractions demonstrated a significant sparing effect with ED50 values of 18.3, 24.9, 26.8, 29.8, and 38.0 Gy, respectively. The linear-quadratic model fitted the data reasonably well when tested according to Tucker (Int. J. Radiat. Oncol. Biol. Phys. 10, 1933-1939, 1984). The alpha/beta ratios estimated with different two-step techniques ranged from 11.1 to 12.4 Gy. Analysis of the data as proposed by Thames et al. (Int. J. Radiat. Biol. 49, 999-1009, 1986) yielded an alpha/beta value of 13.9 Gy (95% confidence limits 8.4 and 24.6 Gy), illustrating a fractionation effect typical for acutely responding tissues, although no clear cell depletion occurred in the urothelium.     

Characteristics of asparagine-linked sugar chains of sphingolipid activator protein 1 purified from normal human liver and GM1 gangliosidosis (type 1) liver

Asparagine-linked sugar chains of sphingolipid activator protein 1 (SAP-1) purified from normal human liver and GM1 gangliosidosis (type 1) liver were comparatively investigated. Oligosaccharides released from the two SAP-1 samples by hydrazinolysis were fractionated by paper electrophoresis and by Aleuria aurantia lectin-Sepharose and Bio-Gel P-4 (under 400 mesh) column chromatography. Structures of oligosaccharides in each fraction were estimated from data on their effective molecular sizes, behavior on immobilized lectin columns with different carbohydrate-binding specificities, results of sequential digestion by exoglycosidases with different aglycon specificities, and methylation analysis. Sugar chains of SAP-1 purified from normal human liver and from GM1 gangliosidosis (type 1) liver were different from each other, although both of them were derived from complex-type sugar chains. The sugar chains of the former were the following eight degradation products from complex-type sugar chains by exoglycosidases in lysosomes: Man alpha 1----6(Man alpha 1----3)Man beta 1----4GlcNAc beta 1----4GlcNAcOT, Man alpha 1----6(Man alpha 1----3)Man beta 1----4GlcNAc beta 1----4(Fuc alpha 1----6)GlcNAcOT, Man alpha 1----6Man beta 1----4GlcNAc beta 1----4GlcNAcOT, Man alpha 1----6Man beta 1----4GlcNAc beta 1----4(Fuc alpha 1----6)GlcNAcOT, Man beta 1----4GlcNAc beta 1----4GlcNAcOT, Man beta 1----4GlcNAc beta 1----4(Fuc alpha 1----6)GlcNAcOT, GlcNAc beta 1----4GlcNAcOT, and GlcNAcOT. In contrast to these, the sugar chains of the latter were sialylated and nonsialylated mono- to tetraantennary complex-type sugar chains that were not fully degraded due to a metabolic defect in acid beta-galactosidase activity.     

Polyoma virus minichromosomes: associated enzyme activities.

Polyoma minichromosomes were isolated and fractionated on glycerol gradients as described by Gourlie et al. (J. Virol. 38:805-814, 1981). Specific assays for DNa polymerases alpha, beta, and gamma, DNA topoisomerase I, and RNase H were carried out on each fraction. The number of units of activity in each fraction was compared with the number of total polyoma and replicative intermediate DNA molecules in each fraction determined by quantitative electron microscopy (M. R. Krauss and R. M. Benbow, J. Virol. 38:815-825, 1981). DNA polymerase alpha cosedimented with polyoma replicative intermediate DNA molecules. DNA polymerase beta and DNA topoisomerase I activities sedimented with mature polyoma minichromosomes. Although the bulk of RNase H activity sedimented in the minichromosome region, the peak of activity was found one fraction behind the peak of mature minichromosomes. Virtually no DNA polymerase gamma activity cosedimented with polyoma minichromosomes.     

Renal damage in the mouse: the effect of d(4)-Be neutrons

A further study on the response of the mouse kidney to d(4)-Be neutrons (EN = 2.3 MeV) is described. The results confirm and augment the work published previously by Stewart et al. [Br. J. Radiol. 57, 1009-1021 (1984)]; the present paper includes the data from a "top-up" design of experiment which extends the measurements of neutron RBE (relative to 240 kVp X rays) down to X-ray doses of 0.75 Gy per fraction. The mean RBE for these neutrons increases from 5.8 to 7.3 as X-ray dose per fraction decreases from 3.0 to 1.5 Gy in the kidney. This agrees with the predictions from the linear quadratic (LQ) model, based on the renal response to X-ray doses above 4 Gy per fraction. The mean RBE estimate from a single dose group at 0.75 Gy per fraction of X rays is, however, 3.9. This is below the LQ prediction and may indicate increasing X-ray sensitivity at low doses. Data from this study and from those published previously have been used to determine more accurately the shape of the underlying response to d(4)-Be neutrons; an alpha/beta ratio of 20.5 +/- 3.7 Gy was found. The best value of alpha/beta for X rays determined from these experiments was 3.04 +/- 0.35 Gy, in agreement with previous values.     

'Fading times' required for apparently complete repair in irradiated tissues assuming the linear quadratic model of dose response

The time required between well-separated pairs of doses of X-rays (e.g. 2F/day) for repairable damage to be apparently completed increases with dose per fraction and with the alpha/beta ratio, even when the underlying half-life is invariant.     

Isolation of two forms of rat alpha-fetoprotein and comparison of their binding parameters with estradiol-17beta.

In polyacrylamide gels, highly purified rat alpha1-fetoprotein shows a molecular heterogeneity, i.e. a "slow" and a "fast" moving fraction. We have isolated by electrophoretic fractionation and subsequent elution these two forms of alpha1-fetoprotein, and we have studied comparatively the binding parameters for estradiol-17beta of whole alpha1-fetoprotein preparations and of the isolated forms. We have shown that the number of binding sites per molecule of whole alpha1-fetoprotein is always, in our experimental conditions, a fractional number, inferior to unity (0.3). Furthermore, the analysis of the binding parameters of the "two forms" of alpha1-fetoprotein allows discrimination between different classes of binding sites. For the "slow" fraction, the number of predominant binding sites per molecule of protein is close to unity (0.7-0.9), whereas for the "fast" fraction, a very low fractional value is found (0.1). The corresponding association constants are reproducibly different for the two fractions: Ka = 0.1.10(8) M-1 for the "slow" alpha1-fetoprotein, and Ka = 0.7.10(8) M-1 for the "fast" alpha1-fetoprotein. Traces of a very high affinity (10(9) M-1) minor class of binding sites are demonstrated in the "slow" fraction. These results point to the existence of a molecular population of alpha1-fetoprotein, some forms of which have a strong or very strong affinity, and some a negligible affinity, for estrogens.     

Divergent metabolism of human chorionic gonadotropin subunits within rat ovarian lysosomes

Pseudopregnant rats were injected with either native human chorionic gonadotropin or with (125I)-human chorionic gonadotropin and their ovarian homogenates fractionated on Percoll density gradients. The levels of alpha and beta subunits within subcellular fractions were measured using radioimmunoassays specific for each subunit. Radioactivity measurements of fractions obtained from rats injected with (125I)-human chorionic gonadotropin were used as a separate index of alpha subunit distribution. The alpha subunit was primarily restricted to a combined plasma membrane/prelysosomal vesicle fraction. Immunoreactive beta subunit was present at high concentrations within both this plasma membrane/prelysosomal vesicle fraction and within lysosomes. The striking difference in alpha and beta subcellular distribution may arise from differential sensitivities to lysosomal enzymes.