Abstract

Synchronous CHO cells were X-irradiated in G1 or mid-S phase with 30-750 Gy, and then the size distribution of DNA molecules resulting from DNA double-strand breaks (DSBs) was studied by pulsed-field gel electrophoresis (PFGE). Cells irradiated in S phase also were pulse-labeled with [3H]dThd for 15 min to compare the migration patterns of replicating DNA with those of DNA mass, measured by imaging with a CCD camera. When cells were irradiated immediately after pulse labeling, a large amount of the 3H-labeled replicating DNA was trapped in the plug, i.e. > 90% for doses < 100 Gy. As the dose increased, the percentage trapped decreased, i.e. to approximately 50% for 750 Gy. The same results were observed for DNA mass when cells were irradiated in S phase, except that much less of the DNA was trapped, i.e. approximately 60% for 70-100 Gy, which produced approximately 2-Mbp molecules, compared to approximately 10% for 750 Gy, which produced approximately 0.3-Mbp molecules. These results and the migration patterns of DNA released into the lane indicated that large molecules are trapped more readily than small molecules because they contain more replicating regions (bands with bubbles) of DNA than small molecules. Our interpretation is that as the dose increases, a greater fraction of the breaks occur between the replicating bands, thus releasing linear molecules that are not replicating. The relatively small amount of 3H-labeled replicating DNA that is released from the PFGE plug migrates aberrantly, with a small amount migrating like linear G1-phase molecules and a large amount, depending on dose, migrating much more slowly than the DNA mass from cells irradiated in G1 or S phase. To explain these results, a Monte Carlo computer program was written to introduce DSBs randomly into DNA that is configured according to a model of DNA replication that is developed in a related study (Dewey and Albright, Radiat. Res. 148, 421-434, 1997). In relating the experimental observations to the results of the Monte Carlo calculations, we assumed that (a) molecules containing replication bubbles with and without forks are trapped in the PFGE plug, (b) linear molecules and molecules with replication forks only that are < or = 8 Mbp are released into the lane, and (c) molecules having replication forks migrate more slowly than linear molecules.

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