Dewey W C, Albright N
Radiation Oncology Research Laboratory, University of California San Francisco, 94103, USA.
Radiat Res. 1997 Nov;148(5):421-34.
A Monte Carlo computer program was written to introduce double-strand breaks (DSBs) randomly into cellular DNA that is configured according to different models of DNA replication. Then, from a review of the literature using DNA fiber autoradiography and other studies relating to rates of replication of DNA that is organized in approximately 3-Mbp regions or bands, a particular model for DNA replication was developed. Using this model, Monte Carlo calculations were made to predict the types and sizes of molecules that would result from introducing DSBs into DNA when synchronous cells are irradiated in the middle of S phase. Then results of the Monte Carlo calculations were compared with migration profiles obtained by pulsed-field gel electrophoresis (PFGE) for molecular size distributions of linear DNA molecules. For these comparisons, CHO cells irradiated in S phase also were pulse-labeled at the time of irradiation with [3H]dThd for 15 min to compare the migration patterns of 3H-labeled replicating DNA with those of the mass of S-phase DNA, measured by imaging with a CCD camera. For the Monte Carlo calculations, we assumed from the reports in the literature that molecules containing replication bubbles with and without forks would be trapped in the PFGE plug. We also assumed that those molecules that are < or = 8 Mbp, both linear and with replication forks, would be released into the lane. However, approximately 75% of the 3H-labeled DNA that is released from the plug migrated much more slowly than linear molecules, which we attributed to the slow migration of 3H-labeled molecules having replication forks not attached to bubbles. The percentages of both mass of S-phase DNA and 3H-labeled replicating DNA released from the plug, as determined by PFGE, were compared with comparable values determined from Monte Carlo calculations. A DNA replication model that provides good agreement between the PFGE results and Monte Carlo calculations is described. Furthermore, Monte Carlo methodology is presented that can be used for comparing data obtained with PFGE with results of Monte Carlo calculations that are based on different models of DNA replication and different assumptions for the migration of various types of replicating molecules.
编写了一个蒙特卡罗计算机程序,用于将双链断裂(DSB)随机引入根据不同DNA复制模型配置的细胞DNA中。然后,通过回顾使用DNA纤维放射自显影术的文献以及其他与约3兆碱基区域或条带中组织的DNA复制速率相关的研究,开发了一种特定的DNA复制模型。使用该模型进行蒙特卡罗计算,以预测当同步细胞在S期中期受到照射时,将DSB引入DNA后产生的分子类型和大小。然后将蒙特卡罗计算结果与通过脉冲场凝胶电泳(PFGE)获得的线性DNA分子大小分布的迁移图谱进行比较。对于这些比较,在S期受到照射的CHO细胞在照射时也用[3H]dThd脉冲标记15分钟,以比较3H标记的复制DNA与通过电荷耦合器件(CCD)相机成像测量的S期DNA质量的迁移模式。对于蒙特卡罗计算,我们从文献报道中假设,含有有叉和无叉复制泡的分子将被困在PFGE凝胶块中。我们还假设,那些小于或等于8兆碱基的线性且有复制叉的分子将释放到泳道中。然而,从凝胶块中释放的3H标记DNA中约75%的迁移速度比线性分子慢得多,我们将其归因于具有未连接到泡的复制叉的3H标记分子的缓慢迁移。通过PFGE确定的从凝胶块中释放的S期DNA质量和3H标记的复制DNA的百分比与从蒙特卡罗计算确定的可比数值进行了比较。描述了一种在PFGE结果与蒙特卡罗计算之间提供良好一致性的DNA复制模型。此外,还介绍了蒙特卡罗方法,该方法可用于将PFGE获得的数据与基于不同DNA复制模型和不同类型复制分子迁移假设的蒙特卡罗计算结果进行比较。