In the past cellular fast-mixing techniques have been used to investigate the time resolution of radiation processes that lead to modification of radiation response in bacterial and mammalian cellular systems. So far, published studies have been confined to effects with low-LET electron beams. The brief for this paper was to discuss where, and under what conditions, such a technique could be used to advantage with high-LET particle beams. Criteria for the experimental design, including conditions of flow rate, dose rate, and mixing times, are discussed. Radiobiological problems appropriate for applications of fast-particle beams are also discussed. These include studies to reveal possible multicomponents in cellular sensitization by oxygen and electron-affinic radiation sensitizers, studies designed to assist in the resolution of direct and indirect effects, and resolution of intracellular DNA damage.
{"title":"Cellular fast-mixing techniques: possible applications with particle beams.","authors":"G E Adams","doi":"","DOIUrl":"","url":null,"abstract":"<p><p>In the past cellular fast-mixing techniques have been used to investigate the time resolution of radiation processes that lead to modification of radiation response in bacterial and mammalian cellular systems. So far, published studies have been confined to effects with low-LET electron beams. The brief for this paper was to discuss where, and under what conditions, such a technique could be used to advantage with high-LET particle beams. Criteria for the experimental design, including conditions of flow rate, dose rate, and mixing times, are discussed. Radiobiological problems appropriate for applications of fast-particle beams are also discussed. These include studies to reveal possible multicomponents in cellular sensitization by oxygen and electron-affinic radiation sensitizers, studies designed to assist in the resolution of direct and indirect effects, and resolution of intracellular DNA damage.</p>","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"8 ","pages":"S40-6"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"15029190","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
H Tsunemoto, S Morita, T Ishikawa, S Furukawa, K Kawachi, T Kanai, H Ohara, T Kitagawa, T Inada
There are two facilities for clinical trials with protons in Japan: the National Institute of Radiological Sciences (NIRS), Chiba, and the Particle Radiation Medical Science Center (PARMS), University of Tsukuba. At the National Institute of Radiological Sciences, patient treatment with the 70 MeV proton beam began in November 1979, and 29 patients were treated through December 1984. Of 11 patients who received protons only, 9 have had local control of the tumor. Two of the 9 patients, suffering from recurrent tumor after radical photon beam irradiation, developed complications after proton treatment. In the patients treated with photons or neutrons followed by proton boost, tumors were controlled in 12 of 18 patients (66.6%), and no complications were observed in this series. Malignant melanoma could not be controlled with the proton beam. A spot-beam-scanning system for protons has been effectively used in the clinical trials to minimize the dose to the normal tissues and to concentrate the dose in the target volume. At the Particle Radiation Medical Science Center, University of Tsukuba, treatment with a vertical 250 MeV proton beam was begun in April 1983, and 22 patients were treated through February 1984. Local control of the tumor was observed in 14 of 22 patients (63.6%), whereas there was no local control in the treatment of glioblastoma multiforme. There have been no severe complications in patients treated at PARMS. The results suggest that local control of tumors will be better with proton beams than with photon beams, whereas additional modalities are required to manage radioresistant tumors.
{"title":"Proton therapy in Japan.","authors":"H Tsunemoto, S Morita, T Ishikawa, S Furukawa, K Kawachi, T Kanai, H Ohara, T Kitagawa, T Inada","doi":"","DOIUrl":"","url":null,"abstract":"<p><p>There are two facilities for clinical trials with protons in Japan: the National Institute of Radiological Sciences (NIRS), Chiba, and the Particle Radiation Medical Science Center (PARMS), University of Tsukuba. At the National Institute of Radiological Sciences, patient treatment with the 70 MeV proton beam began in November 1979, and 29 patients were treated through December 1984. Of 11 patients who received protons only, 9 have had local control of the tumor. Two of the 9 patients, suffering from recurrent tumor after radical photon beam irradiation, developed complications after proton treatment. In the patients treated with photons or neutrons followed by proton boost, tumors were controlled in 12 of 18 patients (66.6%), and no complications were observed in this series. Malignant melanoma could not be controlled with the proton beam. A spot-beam-scanning system for protons has been effectively used in the clinical trials to minimize the dose to the normal tissues and to concentrate the dose in the target volume. At the Particle Radiation Medical Science Center, University of Tsukuba, treatment with a vertical 250 MeV proton beam was begun in April 1983, and 22 patients were treated through February 1984. Local control of the tumor was observed in 14 of 22 patients (63.6%), whereas there was no local control in the treatment of glioblastoma multiforme. There have been no severe complications in patients treated at PARMS. The results suggest that local control of tumors will be better with proton beams than with photon beams, whereas additional modalities are required to manage radioresistant tumors.</p>","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"8 ","pages":"S235-43"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"14137025","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Between 1956 and 1977, the former synchrocyclotron in Uppsala was used for biological experiments and clinical tests with 185-MeV protons. Therapeutic irradiations have been performed since 1957 by cross-firing with pencil beams through small intracranial structures for the treatment of Parkinsonism and intractable pain and with the spread-out Bragg peak for the treatment of large malignant tumors. Radiological and radiophysical aspects of the use of charged-particle beams were studied in detail. The former accelerator is now being converted to a sector-focusing, frequency-modulated cyclotron, SFSC-200, to permit acceleration of protons up to 200 MeV and other light ions to corresponding energies. Production of spallation neutrons and radionuclides for biomedical uses is expected to start this year. Experiments with charged-particle beams will begin in 1986. This paper presents a discussion of accelerator developments for planned experimental and clinical programs.
{"title":"Biomedical program for the converted 200-MeV synchrocyclotron at the Gustaf Werner Institute.","authors":"B. Larsson","doi":"10.2307/3576662","DOIUrl":"https://doi.org/10.2307/3576662","url":null,"abstract":"Between 1956 and 1977, the former synchrocyclotron in Uppsala was used for biological experiments and clinical tests with 185-MeV protons. Therapeutic irradiations have been performed since 1957 by cross-firing with pencil beams through small intracranial structures for the treatment of Parkinsonism and intractable pain and with the spread-out Bragg peak for the treatment of large malignant tumors. Radiological and radiophysical aspects of the use of charged-particle beams were studied in detail. The former accelerator is now being converted to a sector-focusing, frequency-modulated cyclotron, SFSC-200, to permit acceleration of protons up to 200 MeV and other light ions to corresponding energies. Production of spallation neutrons and radionuclides for biomedical uses is expected to start this year. Experiments with charged-particle beams will begin in 1986. This paper presents a discussion of accelerator developments for planned experimental and clinical programs.","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"284 4 1","pages":"S310-8"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79643142","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Negative pi mesons (pions) were used to treat 227 patients at the Los Alamos Meson Production Facility (LAMPF) between 1974 and 1981. Persisting local control values for 129 patients treated with pions alone in the following tumor sites were recorded at a minimum post-treatment observation interval of 2.5 years in the following tumor sites: cerebral gliomas 3/29; head and neck, 8/31; lung, 1/7; pancreas, 0/17; large bowel, 3/13; cervix, 2/45; bladder, 3/4; prostate, 18/20; miscellaneous sites, 0/4. Late severe sequelae ranged from none to 30% for major sites. A dose-response relationship was seen for late severe sequelae with a high probability following dose levels of 4750 cGy (max) in approximately 38 fractions. RBE values for pions appeared to lie in the range of 1.4-1.6 for both acute normal tissue reactions and late sequelae. At the Swiss Institute for Nuclear Research (SIN), 126 patients were treated in Phase I-II protocol studies between 1982 and 1984 with a new technique of scanning with a focused spot of pions. With minimum observation intervals of only 6 months, the local complete response values in 67 evaluable patients treated with pions alone to selected sites are gliomas 1/15 (9 months); pancreas, 3/11; cervix, 4/8; bladder, 18/26 (at 1 year, 9/22); sarcomas, 4/5; biliary tract, 3/4. Late severe sequelae ranged from none to 50% for major sites. A steep dose-response relationship is seen for late severe sequelae with high probability following doses exceeding 3800 cGy (max) in 20 fractions and very low probability with doses below 3500 cGy (max).
{"title":"Review of the SIN and Los Alamos Pion Trials.","authors":"G. Schmitt, C. Essen, R. Greiner, H. Blattmann","doi":"10.2307/3583537","DOIUrl":"https://doi.org/10.2307/3583537","url":null,"abstract":"Negative pi mesons (pions) were used to treat 227 patients at the Los Alamos Meson Production Facility (LAMPF) between 1974 and 1981. Persisting local control values for 129 patients treated with pions alone in the following tumor sites were recorded at a minimum post-treatment observation interval of 2.5 years in the following tumor sites: cerebral gliomas 3/29; head and neck, 8/31; lung, 1/7; pancreas, 0/17; large bowel, 3/13; cervix, 2/45; bladder, 3/4; prostate, 18/20; miscellaneous sites, 0/4. Late severe sequelae ranged from none to 30% for major sites. A dose-response relationship was seen for late severe sequelae with a high probability following dose levels of 4750 cGy (max) in approximately 38 fractions. RBE values for pions appeared to lie in the range of 1.4-1.6 for both acute normal tissue reactions and late sequelae. At the Swiss Institute for Nuclear Research (SIN), 126 patients were treated in Phase I-II protocol studies between 1982 and 1984 with a new technique of scanning with a focused spot of pions. With minimum observation intervals of only 6 months, the local complete response values in 67 evaluable patients treated with pions alone to selected sites are gliomas 1/15 (9 months); pancreas, 3/11; cervix, 4/8; bladder, 18/26 (at 1 year, 9/22); sarcomas, 4/5; biliary tract, 3/4. Late severe sequelae ranged from none to 50% for major sites. A steep dose-response relationship is seen for late severe sequelae with high probability following doses exceeding 3800 cGy (max) in 20 fractions and very low probability with doses below 3500 cGy (max).","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"1 1","pages":"S272-8"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"89811260","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
L D Skarsgard, B G Douglas, J Denekamp, D J Chaplin, G K Lam, R W Harrison, R O Kornelsen, B Palcic
Patient treatments at TRIUMF (Tri-University Meson Facility, Vancouver, B. C.) use a moving spot raster scan technique where the pion range is modulated in depth for each position of the moving spot. The spot scans in a stepwise fashion and can produce any desired field shape. This approach provides very good dose uniformity across the treatment field and allows maximum flexibility in shaping the treatment volume. Survival of cultured cells has been used as a biological dosimeter to test the isoeffectiveness of the pion dose distributions, which must be shaped in depth to compensate for the depth-dependent LET distribution. Isoeffectiveness across the treatment field has also been verified using this system, which involves irradiating cells supported in a gelatin matrix. The response of pig skin to pion irradiation at TRIUMF has provided a check on the in vivo RBE for acute effects derived from our earlier studies with mouse foot. In addition, the pig skin reactions have been followed for several months to assess the later dermal response. The RBE of our pion beam relative to 270 kVp X rays is approximately 1.5 for both the acute epidermal and the later dermal responses.
{"title":"In vitro and in vivo studies of the TRIUMF pion therapy beam.","authors":"L D Skarsgard, B G Douglas, J Denekamp, D J Chaplin, G K Lam, R W Harrison, R O Kornelsen, B Palcic","doi":"","DOIUrl":"","url":null,"abstract":"<p><p>Patient treatments at TRIUMF (Tri-University Meson Facility, Vancouver, B. C.) use a moving spot raster scan technique where the pion range is modulated in depth for each position of the moving spot. The spot scans in a stepwise fashion and can produce any desired field shape. This approach provides very good dose uniformity across the treatment field and allows maximum flexibility in shaping the treatment volume. Survival of cultured cells has been used as a biological dosimeter to test the isoeffectiveness of the pion dose distributions, which must be shaped in depth to compensate for the depth-dependent LET distribution. Isoeffectiveness across the treatment field has also been verified using this system, which involves irradiating cells supported in a gelatin matrix. The response of pig skin to pion irradiation at TRIUMF has provided a check on the in vivo RBE for acute effects derived from our earlier studies with mouse foot. In addition, the pig skin reactions have been followed for several months to assess the later dermal response. The RBE of our pion beam relative to 270 kVp X rays is approximately 1.5 for both the acute epidermal and the later dermal responses.</p>","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"8 ","pages":"S135-44"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"15051966","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Most quantitative models of radiation action in mammalian cells make the implicit assumption that all relevant repair processes proceed in a dose-independent manner. Thus it is implicitly assumed that the repair processes (1) follow totally unsaturated kinetics, (2) are not themselves inactivated by the radiation, and (3) are not enhanced by the presence of radiation damage. Contradiction of any of these three assumptions could have important theoretical and practical implications. The possible relevance of (1) and (2) in mammalian cells is discussed by considering a selection of saturable repair (and related) models. Repair inactivation is improbable, but repair saturation provides a ready explanation of common radiobiological phenomena without the need for the existence of "sublethal" damage. Furthermore, such models can "explain" additional phenomena which appear as contradictions to some sublethal damage models. Recent experiments by Wheeler and Wierowski have demonstrated the existence of dose-dependent repair of DNA damage in mammalian cells.
{"title":"Saturable repair models of radiation action in mammalian cells.","authors":"D T Goodhead","doi":"","DOIUrl":"","url":null,"abstract":"<p><p>Most quantitative models of radiation action in mammalian cells make the implicit assumption that all relevant repair processes proceed in a dose-independent manner. Thus it is implicitly assumed that the repair processes (1) follow totally unsaturated kinetics, (2) are not themselves inactivated by the radiation, and (3) are not enhanced by the presence of radiation damage. Contradiction of any of these three assumptions could have important theoretical and practical implications. The possible relevance of (1) and (2) in mammalian cells is discussed by considering a selection of saturable repair (and related) models. Repair inactivation is improbable, but repair saturation provides a ready explanation of common radiobiological phenomena without the need for the existence of \"sublethal\" damage. Furthermore, such models can \"explain\" additional phenomena which appear as contradictions to some sublethal damage models. Recent experiments by Wheeler and Wierowski have demonstrated the existence of dose-dependent repair of DNA damage in mammalian cells.</p>","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"8 ","pages":"S58-67"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"14985209","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The concepts and tools of the Theory of Dual Radiation Action (e.g., proximity functions and gamma distributions) are outlined, and their connection to single-event cell inactivation is exemplified by an analysis and interpretation of the cross-section data obtained by Todd. It is shown that the biological effect of individual charged particles is dominated by the combined action of a few delta rays.
{"title":"Dual radiation action and the initial slope of survival curves.","authors":"M. Zaider, H. Rossi","doi":"10.2307/3576634","DOIUrl":"https://doi.org/10.2307/3576634","url":null,"abstract":"The concepts and tools of the Theory of Dual Radiation Action (e.g., proximity functions and gamma distributions) are outlined, and their connection to single-event cell inactivation is exemplified by an analysis and interpretation of the cross-section data obtained by Todd. It is shown that the biological effect of individual charged particles is dominated by the combined action of a few delta rays.","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"8 1","pages":"S68-76"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82465381","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
With confluent cultures of the C3H10T1/2 mammalian cell line, we have investigated the effects of heavy-ion radiation on neoplastic cell transformation. Our quantitative data obtained with high-energy carbon, neon, silicon, argon, iron, and uranium particles show that RBE is both dose- and LET-dependent for malignant cell transformation. RBE is higher at lower doses. There is an increase of RBE with LET, up to about 100-200 keV/micron, and a decrease of RBE with beams of higher LET values. Transformation lesions induced by heavy particles with LET values greater than 100 keV/micron may not be repairable in nonproliferating cells. RBE for slow and nonproliferating cells may be much higher than for actively growing cells.
{"title":"Neoplastic cell transformation by heavy charged particles.","authors":"T. Yang, L. Craise, M. Mei, C. Tobias","doi":"10.2307/3576645","DOIUrl":"https://doi.org/10.2307/3576645","url":null,"abstract":"With confluent cultures of the C3H10T1/2 mammalian cell line, we have investigated the effects of heavy-ion radiation on neoplastic cell transformation. Our quantitative data obtained with high-energy carbon, neon, silicon, argon, iron, and uranium particles show that RBE is both dose- and LET-dependent for malignant cell transformation. RBE is higher at lower doses. There is an increase of RBE with LET, up to about 100-200 keV/micron, and a decrease of RBE with beams of higher LET values. Transformation lesions induced by heavy particles with LET values greater than 100 keV/micron may not be repairable in nonproliferating cells. RBE for slow and nonproliferating cells may be much higher than for actively growing cells.","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"10 1","pages":"S177-87"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79471918","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The microdosimetric distribution of event sizes, especially for small exposures and high-LET radiation, represents both a fractional involvement of the exposed cell population and variable amounts of energy transferred to the "hit" cells. To determine the fraction of cells that will respond quantally (be transformed) after receiving a hit of a given size, a hit size effectiveness function (HSEF) which appears to have a threshold has been derived from experimental data for pink mutations in Tradescantia. The value of the HSEF at each event size, multiplied by the fractional number of cells hit at that event size, and summed over all event sizes, yields a single value representing the fractional number of quantally responding cells and thus the population impairment for a given exposure. The HSEF can be obtained by unfolding (deconvoluting) several sets of biological and microdosimetric data obtained with radiation of overlapping event size distributions.
{"title":"An alternative to absorbed dose, quality, and RBE at low exposures.","authors":"V. Bond, M. Varma, C. Sondhaus, L. Feinendegen","doi":"10.2307/3576632","DOIUrl":"https://doi.org/10.2307/3576632","url":null,"abstract":"The microdosimetric distribution of event sizes, especially for small exposures and high-LET radiation, represents both a fractional involvement of the exposed cell population and variable amounts of energy transferred to the \"hit\" cells. To determine the fraction of cells that will respond quantally (be transformed) after receiving a hit of a given size, a hit size effectiveness function (HSEF) which appears to have a threshold has been derived from experimental data for pink mutations in Tradescantia. The value of the HSEF at each event size, multiplied by the fractional number of cells hit at that event size, and summed over all event sizes, yields a single value representing the fractional number of quantally responding cells and thus the population impairment for a given exposure. The HSEF can be obtained by unfolding (deconvoluting) several sets of biological and microdosimetric data obtained with radiation of overlapping event size distributions.","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"7 1","pages":"S52-7"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75058007","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Ionizing radiation produces a range of damage types in cellular DNA. All damage types do not have the same biological significance. Here arguments are presented supporting the view that lesions in which damage is present on both strands in a local region of the DNA (locally multiply damaged sites--LMDS) will present problems for cellular repair processes. We have previously shown that lesions produced in DNA by individual OH radicals, i.e., single OH species acting alone, are ineffective in mammalian cell killing [J.F. Ward, W.F. Blakely, and E.I. Joner, Radiat. Res. 103, 383-392 (1985)]. We have similar evidence in mutagenesis studies (Ward and Calabro-Jones, unpublished data). Thus the formation of such damage by individual OH radicals formed by ionizing radiation would be similarly ineffectual. Earlier [J.F. Ward, Radiat. Res. 86, 185-195 (1981)] we suggested that OH-radical scavenging studies were consistent with the scavenging of OH radicals in volumes of high radical density, spurs, etc., i.e., in volumes which, when they overlap the DNA, will cause the production of LMDS. The individual constituent lesions of LMDS will be formed as a result of direct ionization or as a result of an OH-radical attack. Both mechanisms can lead to base damage or strand breakage. It is clear that damage in both bases of a deoxyribonucleotide pair leads to loss of base sequence information and can be repaired correctly only by accident or in a recombinational process.(ABSTRACT TRUNCATED AT 250 WORDS)
{"title":"Biochemistry of DNA lesions.","authors":"J F Ward","doi":"","DOIUrl":"","url":null,"abstract":"<p><p>Ionizing radiation produces a range of damage types in cellular DNA. All damage types do not have the same biological significance. Here arguments are presented supporting the view that lesions in which damage is present on both strands in a local region of the DNA (locally multiply damaged sites--LMDS) will present problems for cellular repair processes. We have previously shown that lesions produced in DNA by individual OH radicals, i.e., single OH species acting alone, are ineffective in mammalian cell killing [J.F. Ward, W.F. Blakely, and E.I. Joner, Radiat. Res. 103, 383-392 (1985)]. We have similar evidence in mutagenesis studies (Ward and Calabro-Jones, unpublished data). Thus the formation of such damage by individual OH radicals formed by ionizing radiation would be similarly ineffectual. Earlier [J.F. Ward, Radiat. Res. 86, 185-195 (1981)] we suggested that OH-radical scavenging studies were consistent with the scavenging of OH radicals in volumes of high radical density, spurs, etc., i.e., in volumes which, when they overlap the DNA, will cause the production of LMDS. The individual constituent lesions of LMDS will be formed as a result of direct ionization or as a result of an OH-radical attack. Both mechanisms can lead to base damage or strand breakage. It is clear that damage in both bases of a deoxyribonucleotide pair leads to loss of base sequence information and can be repaired correctly only by accident or in a recombinational process.(ABSTRACT TRUNCATED AT 250 WORDS)</p>","PeriodicalId":77888,"journal":{"name":"Radiation research. Supplement","volume":"8 ","pages":"S103-11"},"PeriodicalIF":0.0,"publicationDate":"1985-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"14981601","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}