The kinetics of postirradiation chromatin restitution as revealed by chromosome aberrations detected by premature chromosome condensation and fluorescence in situ hybridization.

In a study of X-ray-induced chromosome aberrations in human G(0) lymphocytes irradiated with 4 Gy using premature chromosome condensation (PCC) and fluorescence in situ hybridization (FISH), the time-dependent pattern of chromosome fragments and interchromosomal exchanges involving chromosome 4 was recorded after postirradiation incubation times varying from 0.5 to 46.5 h. Unattached acentric fragments and incomplete interchromosomal exchanges have high initial yields, followed by an exponential decrease, while complete interchromosomal exchanges have almost zero initial yield with a subsequent increase in their number. Plateau values of all yields are reached after about 25 h. This temporal variation of aberration yields can consistently be explained by the competition of disruptive PCC stress with the progress of postirradiation structural restitution at the sites of radiation-induced chromatin instabilities. Details of the temporal pattern of incomplete exchanges reflect the different kinetics of the alpha and beta components of the yield of aberrations. The observed large difference between late-PCC and metaphase yields of unattached acentric fragments and the almost perfect conversion from incomplete prematurely condensed chromosomes into complete metaphase exchanges are explained by a difference in the magnitude of chromosome condensation stress between PCC and mitotic conditions. Chromatin sites prone to fragmentation and incompleteness under conditions of PCC can therefore persist as genetic instabilities hidden during mitosis.

Chromosome aberrations induced in human lymphocytes by 3.45 MeV alpha particles analyzed by premature chromosome condensation.

Premature chromosome condensation (PCC) experiments using human lymphocytes with centromere staining have shown that after exposure to 3.45 MeV alpha-particle radiation, the full number of dicentric chromosomes appears when the cell fusion protocol is applied immediately after irradiation. In this case, the time available for repair and misrepair of DNA damage is only about 30 min. The number of dicentrics does not change with a further increase in the time available for chromatin rearrangement. This fast response confirms the expectation based on our previous experiments using PCC with 150 kV X rays in which the alpha component of the yield of dicentrics was found to appear when the cell fusion protocol was applied immediately after irradiation, whereas the beta component was delayed by several hours. The time constant for rejoining of the excess acentric chromosome fragments is found to be donor-specific and not to differ for alpha particles and X rays, but alpha-particle radiation leaves a larger fraction of the excess acentric fragments unrejoined. The RBEs of the 3.45 MeV alpha-particle radiation compared to 150 kV X rays, evaluated for the alpha component for the yield of dicentrics and for the yield of unrepaired acentric fragments, have almost equal values of about 4. This is consistent with data in the literature on chromosome aberrations observed in metaphase that show the equality of the RBE values for production of dicentrics and acentric fragments. Our experimental results concerning the fast kinetics of the alpha component of the yield of exchange-type chromosome aberrations are not consistent with Lea's pairwise lesion interaction model, and they support the proposed alternative mechanism of lesion-nonlesion interaction between chromatin regions carrying clustered DNA damage and intact chromatin regions.

Kinetics of the formation of chromosome aberrations in X-irradiated human lymphocytes: analysis by premature chromosome condensation with delayed fusion.

Human lymphocytes irradiated with graded doses of up to 5 Gy of 150 kV X rays were fused with mitotic CHO cells after delay times ranging from 0 to 14 h after irradiation. The yields of dicentrics seen under PCC conditions, using C-banding for centromere detection, and of excess acentric fragments observed in the PCC experiment were determined by image analysis. At 4 Gy the time course of the yield of dicentrics shows an early plateau for delay times up to 2 h, then an S-shaped rise and a final plateau which is reached after a delay time of about 8 to 10 h. Whereas the dose-yield curve measured at zero delay time is strictly linear, the shape of the curve obtained for 8 h delay time is linear-quadratic. The linear yield component, alpha D, is formed entirely in the fast process manifested in the early plateau, while component beta D2 is developed slowly in the subsequent hours. Analysis of the kinetics of the rise of the S-shaped curve for yield as a function of time leads to the postulate of an "intermediate product" of pairwise DNA lesion interaction, still fragile when subjected to the stress of PCC, but gradually processed into a stable dicentric chromosome. It is concluded that the observed difference in the kinetics of the alpha and beta components explains a number of earlier results, especially the disappearance of the beta component at high LET, and opens possibilities for chemical and physical modification of the beta component during the extended formation process after irradiation observed here.

Characterization and mapping of a highly conserved processed pseudogene and an intron-carrying gene of the heat shock cognate protein 70 (Hsc70) gene family in the rat.

A processed pseudogene of the rat Hsc70 gene, Hsc70-ps1, is described, which still presents the open reading frame of the original gene. The pseudogene does not appear to be expressed. It maps to rat Chromosome (Chr) 2. The intron-carrying Hsc70 gene localizes to Chr 8. Hsc70-specific probes detect a large number of more than 20 cross-hybridizing fragments, which show only limited length polymorphism among various inbred rat strains.