Charles A. Waldren

Radiation risk to low fluences of particles may be greater than we thought

Based principally on the cancer incidence found in survivors of the atomic bombs dropped in Hiroshima and Nagasaki, the International Commission on Radiation Protection (ICRP) and the United States National Council on Radiation Protection and Measurements (NCRP) have recommended that estimates of cancer risk for low dose exposure be extrapolated from higher doses by using a linear, no-threshold model. This recommendation is based on the dogma that the DNA of the nucleus is the main target for radiation-induced genotoxicity and, as fewer cells are directly damaged, the deleterious effects of radiation proportionally decline. In this paper, we used a precision microbeam to target an exact fraction (either 100% or ≤20%) of the cells in a confluent population and irradiated their nuclei with exactly one α particle each. We found that the frequencies of induced mutations and chromosomal changes in populations where some known fractions of nuclei were hit are consistent with non-hit cells contributing significantly to the response. In fact, irradiation of 10% of a confluent mammalian cell population with a single α particle per cell results in a mutant yield similar to that observed when all of the cells in the population are irradiated. This effect was significantly eliminated in cells pretreated with a 1 mM dose of octanol, which inhibits gap junction-mediated intercellular communication, or in cells carrying a dominant negative connexin 43 vector. The data imply that the relevant target for radiation mutagenesis is larger than an individual cell and suggest a need to reconsider the validity of the linear extrapolation in making risk estimates for low dose, high linear-energy-transfer (LET) radiation exposure.

A low, adaptive dose of gamma-rays reduced the number and altered the spectrum of S1− mutants in human-hamster hybrid AL cells

We examined the effects of a low, adaptive dose of 137Cs-gamma-irradiation (0.04 Gy) on the number and kinds of mutants induced in AL human-hamster hybrid cells by a later challenge dose of 4 Gy. The yield of S1- mutants was significantly less (by 53%) after exposure to both the adaptive and challenge doses compared to the challenge dose alone. The yield of hprt- mutants was similarly decreased. Incubation with cycloheximide (CX) or 3-aminobenzamide largely negated the decrease in mutant yield. The adaptive dose did not perturb the cell cycle, was not cytotoxic, and did not of itself increase the mutant yield above background. The adaptive dose did, however, alter the spectrum of S1- mutants from populations exposed only to the adaptive dose, as well as affecting the spectrum of S1- mutants generated by the challenge dose. The major change in both cases was a significant increase in the proportion of complex mutations compared to small mutations and simple deletions.

Cellular and molecular analysis of mutagenesis induced by charged particles of defined linear energy transfer

Mutation induction by charged particles of defined linear energy transfer (LET) and gamma rays was scored using human-hamster hybrid AL cells. The LET values for charged particles accelerated at the Radiological Research Accelerator Facility ranged from 10 keV/microm protons to 150 keV/microm 4He ions. The induced mutant fractions at both the S1 and HGPRT loci were dependent on the dose and LET. In addition, for each dose examined, the mutant yield at the S1 locus was 30-60 fold higher than at the corresponding HGPRT locus. To determine whether the mutation spectrum was comparably dependent on dose and LET, independent S1- and HGPRT- mutants induced by 150 keV/microm 4He ions and gamma rays were isolated, and their DNA was analyzed by both Southern blotting and multiplex PCR methods. While the majority of radiation-induced mutants showed deletions of varying sizes, the relative percentage of large deletions was found to be related to both the dose and LET of the radiation examined. Using a mutation system that can detect multilocus changes, results of the present study show that radiation-induced chromosomal loss can be in the millions of base pairs.

Heavy ion mutagenesis: linear energy transfer effects and genetic linkage.

We have characterized a series of 69 independent mutants at the endogenoushprt locus of human TK6 lymphoblasts and over 200 independent S 1-deficient mutants of the humanxhamster hybrid cell line AL arising spontaneously or following low-fluence exposures to densely ionizing Fe ions (600 MeV/amu, linear energy transfer = 190 keV/µm). We find that large deletions are common. The entirehprt gene (>44 kb) was missing in 19/39 Fe-induced mutants, while only 2/30 spontaneous mutants lost the entirehprt coding sequence. When the gene of interest (S1 locus = M1C1 gene) is located on a nonessential human chromosome 11, multilocus deletions of several million base pairs are observed frequently. The S1 mutation frequency is more than 50-fold greater than the frequency ofhprt mutants in the same cells. Taken together, these results suggest that low-fluence exposures to Fe ions are often cytotoxic due to their ability to create multilocus deletions that may often include the loss of essential genes. In addition, the tumorigenic potential of these HZE heavy ions may be due to the high potential for loss of tumor suppressor genes. The relative insensitivity of thehprt locus to mutation is likely due to tight linkage to a gene that is required for viability.

Mutation Induction and Relative Biological Effectiveness of Neutrons in Mammalian Cells: Experimental Observations

The induction of mutation by graded doses of monoenergetic neutrons was examined using the human-hamster hybrid cell system. The AL cells, formed by fusion of human fibroblasts with the gly- A mutant of the Chinese hamster ovary cells, contain the standard set of hamster chromosomes plus a single human chromosome, number 11. These cells contain specific human cell surface antigens that render them sensitive to killing by specific antisera in the presence of complement. Mutant AL cells that have lost the surface markers, however, would survive and give rise to scorable colonies. The cells were irradiated with neutrons produced at the Radiological Research Accelerator Facility of Columbia University. Doses corresponding to low, moderate, and high cytotoxicities and in energies ranging from 0.33 to 14 MeV were used. Neutrons induced a dose-dependent cytotoxicity and mutation frequency in the AL cells. Over the range of doses examined, it was found that the mutagenesis induced by neutrons was energy-dependent and the frequencies were a curvilinear function of dose for both the a1 and a2 antigenic loci examined. In comparison to gamma rays, the relative biological effectiveness (RBE) for cell lethality at the 10% survival level ranged from 5.2 for 0.33 MeV to 1.8 for 14 MeV neutrons. The RBE for mutation induction at the a1 locus, however, ranged from 30 for 0.33 MeV to 4.2 for 14 MeV neutrons at or around the lowest levels of effect examined. Results of the present study demonstrated that neutrons, when measured under conditions which permit detection of a spectrum of gene and chromosomal mutations, in fact, are more efficient mutagens than previously thought.

Comparison of repair of DNA double-strand breaks in identical sequences in primary human fibroblast and immortal hamster-human hybrid cells harboring a single copy of human chromosome 11.

Abstract Fouladi, B., Waldren, C. A., Rydberg, B. and Cooper, P. K. Comparison of Repair of DNA Double-Strand Breaks in Identical Sequences in Primary Human Fibroblast and Immortal Hamster–Human Hybrid Cells Harboring a Single Copy of Human Chromosome 11. We have optimized a pulsed-field gel electrophoresis assay that measures induction and repair of double-strand breaks (DSBs) in specific regions of the genome (Löbrich et al., Proc. Natl. Acad. Sci. USA 92, 12050–12054, 1995). The increased sensitivity resulting from these improvements makes it possible to analyze the size distribution of broken DNA molecules immediately after the introduction of DSBs and after repair incubation. This analysis shows that the distribution of broken DNA pieces after exposure to sparsely ionizing radiation is consistent with the distribution expected from randomly induced DSBs. It is apparent from the distribution of rejoined DNA pieces after repair incubation that DNA ends continue to rejoin between 3 and 24 h postirradiation and that some of these rejoining events are in fact misrejoining events, since novel restriction fragments both larger and smaller than the original fragment are generated after repair. This improved assay was also used to study the kinetics of DSB rejoining and the extent of misrejoining in identical DNA sequences in human GM38 cells and human–hamster hybrid AL cells containing a single human chromosome 11. Despite the numerous differences between these cells, which include species and tissue of origin, levels of TP53, expression of telomerase, and the presence or absence of a homologous chromosome for the restriction fragments examined, the kinetics of rejoining of radiation-induced DSBs and the extent of misrejoining were similar in the two cell lines when studied in the G1 phase of the cell cycle. Furthermore, DSBs were removed from the single-copy human chromosome in the hamster AL cells with similar kinetics and misrejoining frequency as at a locus on this hybrids CHO chromosomes.

A versatile image analysis approach for simultaneous chromosome identification and localization of FISH probes

Modern cytogenetic techniques, such as comparative genomic hybridization (CGH) and the multi-color fluorescence in situ hybridization (FISH) techniques of multiplex fluorescence in situ hybridization (M-FISH) and spectral karyotyping (SKY), require a coordinated banding analysis to maximize their usefulness. All of the methods currently used, including Giemsa (G-) banding, Alu banding, and 4′,6-diamidino-2-phenyl-indole (DAPI) banding, have serious drawbacks. A simple and effective method to band chromosomes concurrently with FISH is needed. To address this problem, we stained chromosomes with DAPI and chromomycin A3, and then used an image analysis program to generate banding by dividing the image taken with a DAPI excitation filter by the image taken with a chromomycin A3 excitation filter. The result was a metaphase spread in which the chromosomes possessed a banding pattern characteristic of R-banding. The image analysis program was then used to generate linescans of pixel intensity versus relative position along the length of chromosomes that were banded using this technique, which we have called D/C R-banding. Each chromosome in a genome was represented by a characteristic scan profile, which was unaffected by FISH signals. Reference linescans were prepared by karyotyping D/C R-banded chromosomes for a given species, and then drawing lines along the length of the known chromosomes. The linescans were combined into a spreadsheet database, which was linked by dynamic data exchange to the image analysis program and normalized for length and intensity. The linescan of an unknown chromosome was then transferred to the spreadsheet, where it was normalized for length and intensity and overlaid on the linescans of each chromosome in the genome. Unknown chromosomes were identified by comparison of their graphs with graphs in the standardized reference genome. We have used this approach to create reference linescan karyotypes of several species, and to identify chromosomes on which FISH was performed.

Analysis of mutant quantity and quality in human-hamster hybrid AL and AL-179 cells exposed to 137Cs-gamma or HZE-Fe ions.

We measured the number of mutants and the kinds of mutations induced by 137Cs-gamma and by HZE-Fe (56Fe [600 MeV/amu, LET = 190 KeV/micrometer) in standard AL human hamster hybrid cells and in a new variant hybrid, AL-179. We found that HZE-Fe was more mutagenic than 137Cs-gamma per unit dose (about 1.6 fold), but was slightly less mutagenic per mean lethal dose, DO, at both the S1 and hprt- loci of AL cells. On the other hand, HZE-Fe induced about nine fold more complex S1- mutants than 137Cs-gamma rays, 28% vs 3%. 137Cs-gamma rays induced about twice as many S1- mutants and hprt-mutants in AL-179 as in AL cells, and about nine times more of the former were complex, and potentially unstable kinds of mutations.

Chromosomal mutations and chromosome loss measured in a new human-hamster hybrid cell line, ALC: studies with colcemid, ultraviolet irradiation, and 137Cs gamma-rays

Small mutations, megabase deletions, and aneuploidy are involved in carcinogenesis and genetic defects, so it is important to be able to quantify these mutations and understand mechanisms of their creation. We have previously quantified a spectrum of mutations, including megabase deletions, in human chromosome 11, the sole human chromosome in a hamster-human hybrid cell line AL. S1- mutants have lost expression of a human cell surface antigen, S1, which is encoded by the M1C1 gene at 11p13 so that mutants can be detected via a complement-mediated cytotoxicity assay in which S1+ cells are killed and S1- cells survive. But loss of genes located on the tip of the short arm of 11 (11p15.5) is lethal to the AL hybrid, so that mutants that have lost the entire chromosome 11 die and escape detection. To circumvent this, we fused AL with Chinese hamster ovary (CHO) cells to produce a new hybrid, ALC, in which the requirement for maintaining 11p15.5 is relieved, allowing us to detect mutations events involving loss of 11p15.5. We evaluated the usefulness of this hybrid by conducting mutagenesis studies with colcemid, 137Cs gamma-radiation and UV 254 nm light. Colcemid induced 1000 more S1- mutants per unit dose in ALC than in AL; the increase for UV 254 nm light was only two-fold; and the increase for 137Cs gamma-rays was 12-fold. The increase in S1- mutant fraction in ALC cells treated with colcemid and 137Cs gamma-rays were largely due to chromosome loss and 11p deletions often containing a breakpoint within the centromeric region.

Measuring the Spectrum of Mutation Induced by Nitrogen Ions and Protons in the Human–Hamster Hybrid Cell Line ALC

Abstract Kraemer, S. M., Kronenberg, A., Ueno, A. and Waldren, C. A. Measuring the Spectrum of Mutation Induced by Nitrogen Ions and Protons in the Human–Hamster Hybrid Cell Line ALC. Astronauts can be exposed to charged particles, including protons, α particles and heavier ions, during space flights. Therefore, studying the biological effectiveness of these sparsely and densely ionizing radiations is important to understanding the potential health effects for astronauts. We evaluated the mutagenic effectiveness of sparsely ionizing 55 MeV protons and densely ionizing 32 MeV/nucleon nitrogen ions using cells of two human–hamster cell lines, AL and ALC. We have previously characterized a spectrum of mutations, including megabase deletions, in human chromosome 11, the sole human chromosome in the human–hamster hybrid cell lines ALC and AL. CD59– mutants have lost expression of a human cell surface antigen encoded by the CD59 gene located at 11p13. Deletion of genes located on the tip of the short arm of 11 (11p15.5) is lethal to the AL hybrid, so that CD59 mutants that lose the entire chromosome 11 die and escape detection. In contrast, deletion of the 11p15.5 region is not lethal in the hybrid ALC, allowing for the detection of chromosome loss or other chromosomal mutations involving 11p15.5. The 55 MeV protons and 32 MeV/nucleon nitrogen ions were each about 10 times more mutagenic per unit dose at the CD59 locus in ALC cells than in AL cells. In the case of nitrogen ions, the mutations observed in ALC cells were predominantly due to chromosome loss events or 11p deletions, often containing a breakpoint in the pericentromeric region. The increase in the CD59– mutant fraction for ALC cells exposed to protons was associated with either translocation of portions of 11q onto a hamster chromosome, or discontinuous or “skipping” mutations. We demonstrate here that ALC cells are a powerful tool that will aid in the understanding of the mutagenic effects of different types of ionizing radiation.