Site-specific strand breaks in RNA produced by (125)I radiodecay

Decay of ¹²⁵I produces a shower of low energy electrons (Auger electrons) that cause strand breaks in DNA in a distance-dependent manner with 90% of the breaks located within 10 bp from the decay site. We studied strand breaks in RNA molecules produced by decay of ¹²⁵I incorporated into complementary DNA oligonucleotides forming RNA/DNA duplexes with the target RNA. The frequencies and distribution of the breaks were unaffected by the presence of the free radical scavenger dimethyl sulfoxide (DMSO) or by freezing of the samples. Therefore, as was the case with DNA, most of the breaks in RNA were direct rather than caused by diffusible free radicals produced in water. The distribution of break frequencies at individual bases in RNA molecules is narrower, with a maximum shifted to the 3′-end with respect to the distribution of breaks in DNA molecules of the same sequence. This correlates with the distances from the radioiodine to the sugars of the corresponding bases in A-form (RNA/DNA duplex) and B-form (DNA/DNA duplex) DNA. Interestingly, when ¹²⁵I was located close to the end of the antisense DNA oligonucleotide, we observed breaks in RNA beyond the RNA/DNA duplex region. This was not the case for a control DNA/DNA hybrid of the same sequence. We assume that for the RNA there is an interaction between the RNA/DNA duplex region and the single-stranded RNA tail, and we propose a model for such an interaction. This report demonstrates that ¹²⁵I radioprobing of RNA could be a powerful method to study both local conformation and global folding of RNA molecules.     

Strand breaks in whole plasmid dna produced by the decay of (125)I in a triplex-forming oligonucleotide.

DNA strand breaks produced by the decay of (125)I positioned against a specific site in plasmid DNA via a triplex-forming oligonucleotide were studied both in the immediate vicinity of the site of the decay with a single nucleotide resolution and in the whole plasmid by measuring the percentages of supercoiled, open-circular and linear forms. The localized breaks are distributed within 10 bp in each direction from the decay site with maxima in both strands just opposite the (125)I-dC residue in the triplex-forming oligonucleotide. The distributions of breaks in the two DNA strands are almost symmetrical, in agreement with the geometry of the pyrimidine motif triplex. We found that about 25% of the double-strand breaks were located outside the 90-bp fragment containing the triplex-forming oligonucleotide binding sequence. The ratio of single- to double-strand breaks in the whole plasmid was 11 for bound triplex-forming oligonucleotide compared to 26 when the triplex-forming oligonucleotide was free in solution. The number of double-strand breaks per decay of (125)I was 0.46 for bound triplex-forming oligonucleotide and 0.17 for free triplex-forming oligonucleotide. Comparing the data on the localized damage and those for the whole plasmid, we concluded that, in addition to DNA breaks that are confined to a helical turn around the (125)I atom, the decay can produce breaks hundreds of base pairs away in the plasmid molecule. This linear plasmid molecule containing radiation-induced damage at a specific DNA site should be useful in studies of the molecular mechanisms of DNA repair.     

Radioprobing of DNA: distribution of DNA breaks produced by decay of 125I incorporated into a triplex-forming oligonucleotide correlates with geometry of the triplex.

The distribution of breaks produced in both strands of a DNA duplex by the decay of 125I carried by a triplex-forming DNA oligonucleotide was studied at single nucleotide resolution. The 125I atom was located in the C5 position of a single cytosine residue of an oligonucleotide designed to form a triple helix with the target sequence duplex. The majority of the breaks (90%) are located within 10 bp around the decay site. The addition of the free radical scavenger DMSO produces an insignificant effect on the yield and distribution of the breaks. These results suggest that the majority of these breaks are produced by the direct action of radiation and are not mediated by diffusible free radicals. The frequency of breaks in the purine strand was two times higher that in the pyrimidine strand. This asymmetry in the yield of breaks correlates with the geometry of this type of triplex; the C5 of the cytosine in the third strand is closer to the sugar-phosphate backbone of the purine strand. Moreover, study of molecular models shows that the yield of breaks at individual bases correlates with distance from the 125I decay site. We suggest the possible use of 125I decay as a probe for the structure of nucleic acids and nucleoprotein complexes.     

Strand breaks in plasmid DNA after positional changes of Auger electron-emitting iodine-125: direct compared to indirect effects.

To elucidate the nature and kinetics of DNA strand breaks caused by low-energy Auger electron emitters, we compared the yields of DNA breaks in supercoiled pUC19 DNA in the presence of the (.)OH scavenger dimethyl sulfoxide (DMSO) after the decay of (125)I (1) in proximity to DNA after minor-groove binding ((125)I-iodoHoechst 33342, (125)IH) and (2) at a distance from DNA ((125)I-iodoantipyrine, (125)IAP). DMSO is efficient at protecting supercoiled plasmid DNA from the decay of (125)I free in solution (dose modification factor, DMF = 59 +/- 4) and less effective when the (125)I decays occur close to DNA (DMF = 3.8 +/- 0.3). This difference is due mainly to the inability of DMSO to protect DNA from the double-strand breaks produced by groove-bound (125)I (DMF = 1.0 +/- 0.2). Additionally, the fragmentation of plasmid DNA beyond the production of single-strand and double-strand breaks that is seen after the decay of (125)IH and not (125)IAP (Kassis et al., Radiat. Res. 151, 167-176, 1999) cannot be modified by DMSO. These results demonstrate that the mechanisms underlying double-strand breaks caused by the decay of (125)IH differ in nature from those caused by the decay of (125)IAP.     

125I-induced DNA double strand breaks: use in calibration of the neutral filter elution technique and comparison with X-ray induced breaks

The neutral filter elution assay, for measurement of DNA double strand breakage, has been calibrated using mouse L cells and Chinese hamster V79 cells labelled with [125I]dUrd and then held at liquid nitrogen temperature to accumulate decays. The basis of the calibration is the observation that each 125I decay, occurring in DNA, produces a DNA double strand break. Linear relationships between 125I decays per cell and lethal lesions per cell (minus natural logarithm survival) and the level of elution, were found. Using the calibration data, it was calculated that the yield of DNA double strand breaks after X-irradiation of both cell types was from 6 to 9 X 10(-12) DNA double strand breaks per Gy per dalton of DNA, for doses greater than 6 Gy. Neutral filter elution and survival data for X-irradiated and 125I-labelled cells suggested that the relationships between lethal lesions and DNA double strand breakage were significantly different for both cell types. An attempt was made to study the repair kinetics for 125I-induced DNA double strand breaks, but was frustrated by the rapid DNA degradation which occurs in cells that have been killed by the freezing-thawing process.     

Targeting the human mdr1 gene by 125I-labeled triplex-forming oligonucleotides

Antigene radiotherapy is our approach to targeting specific sites in the genome by combining the highly localized DNA damage produced by the decay of Auger electron emitters, such as 125I, with the sequence-specific action of triplex-forming oligonucleotides (TFO). As a model, we used the multidrug resistance gene (mdr1) overexpressed and amplified nearly 100 times in the human KB-V1 carcinoma cell line. Phosphodiester pyrrazolopyrimidine dG (PPG)-modified TFO complementary to the polypurine-polypyrimidine region of the mdr1 gene were synthesized and labeled with 125I-dCTP at the C5 position of two cytosines by the primer extension method. 125I-TFO were delivered into KB-V1 cells with several delivery systems. DNA from the 125I-TFO-treated cells was recovered and analyzed for sequence-specific cleavage in the mdr1 target by Southern hybridization. Experiments with plasmid DNA containing the mdr1 polypurine-polypyrimidine region and with purified genomic DNA confirmed the ability of the designed 125I-TFO to bind to and introduce double-strand breaks into the target sequence. We showed that 125I-TFO in nanomolar concentrations can recognize and cleave a target sequence in the mdr1 gene in situ, that is, within isolated nuclei and intact digitonin-permeabilized cells. Our results demonstrate the ability of 125I-TFO to target specific sequences in their natural environment, that is, within the eukaryotic nucleus. The nearly 100-fold amplification of the mdr1 gene in KB-V1 cells affords a very useful cell culture model for evaluation of methods to produce sequence-specific DNA double-strand breaks for gene-specific radiotherapy.     

Induction and repair of double- and single-strand DNA breaks in bacteriophage lambda superinfecting Escherichia coli

Induction and repair of double- and single-strand DNA breaks have been measured after decays of 125I and 3H incorporated into the DNA and after external irradiation with 4 MeV electrons. For the decay experiments, cells of wild type Escherichia coli K-12 were superinfected with bacteriophage lambda DNA labelled with 5'-(125I)iodo-2'-deoxyuridine or with (methyl-3H)thymidine and frozen in liquid nitrogen. Aliquots were thawed at intervals and lysed at neutral pH, and the phage DNA was assayed for double- and single-strand breakage by neutral sucrose gradient centrifugation. The gradients used allowed measurements of both kinds of breaks in the same gradient. Decays of 125I induced 0.39 single-strand breaks per double-strand break. No repair of either break type could be detected. Each 3H disintegration caused 0.20 single-strand breaks and very few double-strand breaks. The single-strand breaks were rapidly rejoined after the cells were thawed. For irradiation with 4 MeV electrons, cells of wild type E. coli K-12 were superinfected with phage lambda and suspended in growth medium. Irradiation induced 42 single-strand breaks per double-strand break. The rates of break induction were 6.75 x 10(-14) (double-strand breaks) and 2.82 x 10(-12) (single-strand breaks) per rad and per dalton. The single-strand breaks were rapidly repaired upon incubation whereas the double-strand breaks seemed to remain unrepaired. It is concluded that double-strand breaks in superinfecting bacteriophage lambda DNA are repaired to a very small extent, if at all.     

Iodine-125 decay in a synthetic oligodeoxynucleotide. II. The role of auger electron irradiation compared to charge neutralization in DNA breakage

Lobachevsky, P. N. and Martin, R. F. Iodine-125 Decay in a Synthetic Oligodeoxynucleotide. II. The Role of Auger Electron Irradiation Compared to Charge Neutralization in DNA Breakage. The dramatic chemical and biological effects of the decay of DNA-incorporated (125)I stem from two consequences of the Auger electron cascades associated with the decay of the isotope: high local deposition of radiation energy from short-range Auger electrons, and neutralization of the multiply charged tellurium atom. We have analyzed the extensive data reported in the companion paper (Radiat. Res. 153, 000-000, 2000), in which DNA breakage was measured after (125)I decay in a 41-bp oligoDNA. The experimental data collected under scavenging conditions (2 M dimethylsulfoxide) were deconvoluted into two components denoted as radiation and nonradiation, the former being attributed to energy deposition by Auger electrons. The contribution of the components was estimated by adopting various assumptions, the principal one being that DNA breakage due to the radiation mechanism is dependent on the distance between the decaying (125)I atom and the cleaved deoxyribosyl unit, while the nonradiation mechanism, associated with neutralization of the multiply charged tellurium atom, contributes equally at corresponding nucleotides starting from the (125)I-incorporating nucleotide. Comparison of the experimental data sets collected under scavenging and nonscavenging (without dimethylsulfoxide) conditions was used to estimate the radiation-scavengeable component. Our analysis showed that the nonradiation component plays the major role in causing breakage within 4-5 nucleotides from the site of (125)I incorporation and produces about 50% of all single-stranded breaks. This overall result is consistent with the relative amounts of energy associated with Auger electrons and the charged tellurium atom. However, the nonradiation component accounts for almost four times more breaks in the top strand, to which the (125)I is bound covalently, than in the bottom strand, thus suggesting an important role of covalent bonds in the energy transfer from the charged tellurium atom. The radiation component dominates at the distances beyond 8-9 nucleotides, and 36% of the radiation-induced breaks are scavengeable.     

Measurement of double-strand breaks in Chinese hamster cell DNA by neutral filter elution: calibration by 125I decay

We labeled the DNA of Chinese hamster lung V79 cells with 125I in the form of iododeoxyuridine and subsequently measured the elution of the DNA through polycarbonate filters at pH 9.6 and pH 7.2. Since decay of incorporated 125I produces predominantly double-strand breaks (DSB) in DNA at a rate close to one DSB per 125I decay, this measurement provides an absolute calibration for the assay of DSBs by neutral filter elution. Neutral elution profiles are not first order with respect to elution time; thus we have examined the relationships between accumulated 125I decays and several functions of retention of DNA on the filter at various times during the elution process. At both pH 9.6 and pH 7.2 there were linear relationships between accumulated decays and certain retention functions. The retention function most closely correlated to 125I decays for both pH values was the logarithm of the ratio of the retention of control DNA to that of 125I-labeled DNA, both evaluated at the 9th fraction (13.5 h of elution). The linear relationship between this ratio and 125I decays allows DSB induction to be determined directly from retention values. The calibration was used to measure DSBs induced by X rays.     

Quantitative detection of (125)IdU-induced DNA double-strand breaks with gamma-H2AX antibody

When mammalian cells are exposed to ionizing radiation and other agents that introduce DSBs into DNA, histone H2AX molecules in megabase chromatin regions adjacent to the breaks become phosphorylated within minutes on a specific serine residue. An antibody to this phosphoserine motif of human H2AX (gamma-H2AX) demonstrates that gamma-H2AX molecules appear in discrete nuclear foci. To establish the quantitative relationship between the number of these foci and the number of DSBs, we took advantage of the ability of (125)I, when incorporated into DNA, to generate one DNA DSB per radioactive disintegration. SF-268 and HT-1080 cell cultures were grown in the presence of (125)IdU and processed immunocytochemically to determine the number of gamma-H2AX foci. The numbers of (125)IdU disintegrations per cell were measured by exposing the same immunocytochemically processed samples to a radiation-sensitive screen with known standards. Under appropriate conditions, the data yielded a direct correlation between the number of (125)I decays and the number of foci per cell, consistent with the assumptions that each (125)I decay yields a DNA DSB and each DNA DSB yields a visible gamma-H2AX focus. Based on these findings, we conclude that gamma-H2AX antibody may form the basis of a sensitive quantitative method for the detection of DNA DSBs in eukaryotic cells.     

125Iodine decay in DNA: A discussion of its effectiveness for the breaking of DNA strands

Summary ¹²⁵I incorporated in DNA is known to be exceptionally toxic. Values of D₀ range from about 40 to about 90 decays for survival of mammalian cells. The effectiveness of¹²⁵I in DNA with respect to the induction of breaks of the DNA strands, however, appears to be comparatively low. The numbers of strand breaks per energy deposited in subnuclear cellular structures such as DNA is smaller for a disintegration of¹²⁵I than for-rays. The difference in effectiveness diminishes with increasing mass of the considered sensitive volume. The apparent inefficiency of¹²⁵I-decay may, on one hand, result from a waste of local energy deposition. On the other hand, it may be caused by a multitude of local strand breaks (clusters) induced by¹²⁵I-decay which are measured as one break only by the conventionally applied techniques of strand break measurement. The apparent inefficiency of¹²⁵I may be evidence furthermore for the importance of considering not only the DNA as the sensitive target but with equal pertinence the gross sensitive volume, i.e. the whole cell nucleus [12]. Further, for drawing meaningful comparisons, it may be necessary to take into consideration the microdosimetric event size distributions for the critical targets [1].Dedicated to Prof. L.E. Feinendegen on the occasion of his 60th birthday     

Sequence specificity of 125I-labelled Hoechst 33258 in intact human cells

Using polyacrylamide/urea DNA sequencing gels, the DNA sequence selectivity of 125I-labelled Hoechst 33258 damage has been determined in intact human cells to the exact base-pair. This was accomplished using a novel procedure with human alpha RI-DNA as the target DNA sequence. In this procedure, after size fractionation, the alpha RI-DNA is selectively purified by hybridization to a single-stranded M13 clone containing an alpha RI-DNA insert. The sequence specificity of [125I]Hoechst 33258 was indistinguishable in intact cells from purified high molecular weight DNA; and this is surprising considering the more complex environment of DNA in the nucleus where DNA is bound to nucleosomes and other DNA binding proteins. The ligand preferentially binds to DNA sequences which have four or more consecutive A.T base-pairs. The extent of damage was measured with a densitometer and, relative to the damage hotspot at base-pair 94, the extent of damage was similar in both purified high molecular weight DNA and intact cells. [125I]Hoechst 33258 causes only double-strand breaks, since single-strand breaks or base damage were not detected. These experiments represent the first occasion that the sequence specificity of a DNA damaging agent, which causes only double-strand breaks, has been determined to the exact base-pair in intact cells.     

Chemical and biological consequences of the radioactive decay of iodine-125 in plasmid DNA

Doubly labeled [U-14C, 5-125I]iododeoxycytidine (IdC) triphosphate was synthesized and incorporated enzymatically into defined positions of the plasmid pBR322. After storage under various conditions, the stable end products were analyzed using radio-GC, radio-HPLC, and electron microscopy. In addition, solutions of 14C-IdC-labeled DNA containing Na125I as an internal radiation source were studied to investigate the influence of internal radiolysis. Transmutation of the covalently bound 125I leads to complete destruction of the labeled nucleotide, giving rise to 14CO2 and 14CO as major products. Fragmentation of the pyrimidine base is independent of solvent and DNA configuration. Internal radiolysis caused by Na125I leads to only minor damage. Electron microscopy studies reveal that decay-induced double strand breaks (dsb) occur both at the site of decay and in areas as far as hundreds of base pairs apart from that site. Number and distribution of the breaks is strongly dependent on solvent and DNA configuration. A direct correlation exists between the extent of fragmentation of the nucleotide and the mean number of dsb.     

Determination and analysis of site-specific 125I decay-induced DNA double-strand break end-group structures

End groups contribute to the structural complexity of radiation-induced DNA double-strand breaks (DSBs). As such, end-group structures may affect a cell's ability to repair DSBs. The 3'-end groups of strand breaks caused by gamma radiation, or oxidative processes, under oxygenated aqueous conditions have been shown to be distributed primarily between 3'-phosphoglycolate and 3'-phosphate, with 5'-phosphate ends in both cases. In this study, end groups of the high-LET-like DSBs caused by 125I decay were investigated. Site-specific DNA double-strand breaks were produced in plasmid pTC27 in the presence or absence of 2 M DMSO by 125I-labeled triplex-forming oligonucleotide targeting. End-group structure was assessed enzymatically as a function of the DSB end to serve as a substrate for ligation and various forms of end labeling. Using this approach, we have demonstrated 3'-hydroxyl (3'-OH) and 3'-phosphate (3'-P) end groups and 5'-ends (> or = 42%) terminated by phosphate. A 32P postlabeling assay failed to detect 3'-phosphoglycolate in a restriction fragment terminated by the 125I-induced DNA double-strand break, and this is likely due to restricted oxygen diffusion during irradiation as a frozen aqueous solution. Even so, end-group structure and relative distribution varied as a function of the free radical scavenging capacity of the irradiation buffer.     

Gene targeted DNA double-strand break induction by (125)I-labeled triplex-forming oligonucleotides is highly mutagenic following repair in human cells.

A parallel binding motif 16mer triplex-forming oligonucleotide (TFO) complementary to a polypurine-polypyrimidine target region near the 3'-end of the SupF gene of plasmid pSP189 was labeled with [5-(125)I]dCMP at position 15. Following triplex formation and decay accumulation, radiation-induced site-specific double-strand breaks (DSBs) were produced in the pSP189 SupF gene. Bulk damaged DNA and the isolated site-specific DSB-containing DNA were separately transfected into human WI38VA13 cells and allowed to repair prior to recovery and analysis of mutants. Bulk damaged DNA had a relatively low mutation frequency of 2.7 x 10(-3). In contrast, the isolated linear DNA containing site-specific DSBs had an unusually high mutation frequency of 7.9 x 10(-1). This was nearly 300-fold greater than that observed for the bulk damaged DNA mixture, and >1.5 x 10(4)-fold greater than background. The mutation spectra displayed a high proportion of deletion mutants targeted to the(125)I binding position within the SupF gene for both bulk damaged DNA and isolated linear DNA. Both spectra were characterized by complex mutations with mixtures of changes. However, mutations recovered from the linear site-specific DSB-containing DNA presented a much higher proportion of complex deletion mutations.     

Gossypol Interferes with Both Type I and Type II Topoisomerase Activities Without Generating Strand Breaks

A considerable number of agents with chemotherapeutic potentials reported over the past years were shown to interfere with the reactions of DNA topoisomerases, the essential enzymes that regulate conformational changes in DNA topology. Gossypol, a naturally occurring bioactive phytochemical is a chemopreventive agent against various types of cancer cell growth with a reported activity on mammalian topoisomerase II. The compounds targeting topoisomerases vary in their mode of action; class I compounds act by stabilizing covalent topoisomerase-DNA complexes resulting in DNA strand breaks while class II compounds interfere with the catalytic function of topoisomerases without generating strand breaks. In this study, we report Gossypol as the interfering agent with type I topoisomerases as well. We also carried out an extensive set of assays to analyze the type of interference manifested by Gossypol on DNA topoisomerases. Our results strongly suggest that Gossypol is a potential class II inhibitor as it blocked DNA topoisomerase reactions with no consequently formed strand breaks.     

Simulation of <Superscript>125</Superscript>I decay in a synthetic oligodeoxynucleotide with normal and distorted geometry and the role of radiation and non-radiation actions

Within the track structure code PARTRAC, DNA strand break induction by direct and indirect radiation action was calculated for the E. coli catabolite gene activator protein (CAP) DNA complex with ¹²⁵I located at the position of the H₅ atom of the cytosine near the center. The shape of the resulting DNA fragment size distributions was found to be in reasonable agreement with corresponding experimental results. However, the calculated yield was considerably lower than the measured one. To study possible reasons for this, recently published experimental data on DNA strand breaks in a 41-mer synthetic oligodeoxynucleotide (oligoDNA) with incorporated ¹²⁵I were analyzed aiming at an evaluation of the non-radiation-related component due to the neutralization of the initially highly charged ^125mTe daughter ion. This was done by assuming that the differences between simulated radiation-induced distribution and the measured total fragment size distributions were due to the neutralization process. The neutralization effect defined in this way was found to dominate the strand breakage frequency within a range of 5–7 base pairs around the ¹²⁵I decay site on both strands. After implementing this neutralization effect derived from the oligoDNA analysis into the PARTRAC simulation for the CAP-DNA complex, the agreement of the calculated DNA fragment distributions with the corresponding experimental data was considerably improved. The results indicate that DNA conformation may be explored by incorporation of ¹²⁵I into the DNA, measurement of fragment size distributions, and comparison with simulation calculation for various hypothetical DNA models.     

Use of polyethylenimine-adenovirus complexes to examine triplex formation in intact cells

Triplex-forming oligonucleotides (TFOs) show potential for sequence-specific DNA binding and inhibition of gene expression. We have applied this antigene strategy using a TFO incorporating an Auger-emitting radionucleotide, 125I, to study the production of double-strand breaks (dsb) in the rat aquaporin 5 (rAQP5) cDNA. 125I-TFO bound to the pCMVrAQP5 plasmid in vitro in a dose-dependent manner and formed stable triplexes up to 65 degrees C and in the presence of 140 mM KCl. Further, 125I-TFO resulted in a predictable dsb when analyzed by Southern hybridization. To deliver TFOs to epithelial cells, we employed 125I-TFO-polyethyleneimine-adenovirus (125I-TFO-PEI-Ad) complexes. We hypothesized that these complexes would take advantage of adenoviral characteristics to transfer 125I-TFO to the cell nucleus. Adenovirus-containing complexes brought about greater uptake and nuclear localization of TFOs compared with delivery with 125I-TFO-PEI complexes alone. No significant degradation of 125I-TFO was found after delivery into cells using PEI-Ad complexes and freezing and thawing. We next used PEI-Ad complexes to deliver 125I-TFO and pCMVrAQP5 separately to epithelial cells to determine if triplexes can form de novo within cells, resulting in the specific dsb in the rAQP5 cDNA. After delivery, cell pellets were stored at -80 degrees C for more than 60 days. Thereafter, plasmid DNA was isolated from cells and analyzed for dsb by Southern hybridization. However, none were detected. We conclude that under the experimental conditions employed, effective triplexes, with 125I-TFO and pCMVrAQP5, do not form de novo inside cells.     

The Schrödinger''s Cat Quandary in Cell Biology: Integration of Live Cell Functional Assays with Measurements of Fixed Cells in Analysis of Apoptosis

The existing cytometric methodologies do not allow one to directly correlate, within the same cells, functional cell attributes that are revealed supravitally with features that require cell fixation to be detected or measured. Taking advantage of the "file merge" feature of the laser-scanning cytometer, we have been able to correlate the supravital changes that occur during apoptosis, namely the drop in mitochondrial transmembrane potential (Delta Psim) and generation of the reactive oxygen intermediates (ROIs), with features revealed by analysis of fixed cells: the cell cycle position and DNA fragmentation. The cell cycle position was established based on the cell's stainability with propidium iodide while DNA fragmentation was assessed by in situ DNA strand break labeling using exogenous terminal deoxynucleotidyltransferase. During apoptosis of HL-60 cells induced by the DNA topoisomerase I inhibitor camptothecin (CPT), the dissipation of Delta Psim occurred preferentially in S-phase cells and preceded the appearance of DNA strand breaks. Essentially all cells with DNA strand breaks had dissipated Delta Psim. Compared to the decrease of Delta Psim, the CPT-induced rise in ROIs during apoptosis was less restricted to S-phase cells. Furthermore, no elevation of ROIs was detected in a significant proportion of cells with DNA strand breaks. The data suggest that DNA fragmentation may occur in some cells prior to the increase in ROIs and thus, unlike the dissipation of Delta Psim, the oxidative stress may not be a prerequisite for activation of an endonuclease. Alternatively, the oxidative stress may be a transient event, occupying a narrow "time window" during the apoptotic process. The approach opens a possibility to study direct relationships, within the same cells, between cellular changes (e.g., occurring during apoptosis, mitogenesis, differentiation, etc.) detected by functional assays of live cells and changes that cannot be analyzed supravitally.     

Fragmentation of chromatin with 125I radioactive disintegrations.

The DNA in Chinese hamster cells was labeled first for 3 h with [3H]TdR and then for 3 h with [125I]UdR. Chromatin was extracted, frozen, and stored at -30 degrees C until 1.0 X 10(17) and 1.25 X 10(17) disintegrations/g of labeled DNA occurred for 125I and 3H respectively. Velocity sedimentation of chromatin (DNA with associated chromosomal proteins) in neutral sucrose gradients indicated that the localized energy from the 125I disintegrations, which gave about 1 double-strand break/disintegration plus an additional 1.3 single strand breaks, selectively fragmented the [125I] chromatin into pieces smaller than the [3H] chromatin. In other words, 125I disintegrations caused much more localized damage in the chromatin labeled with 125I than in the chromatin labeled with 3H, and fragments induced in DNA by 125I disintegrations were not held together by the associated chromosomal proteins. Use of this 125I technique for studying chromosomal proteins associated with different regions in the cellular DNA is discussed. For these studies, the number of disintegrations required for fragmenting DNA molecules of different sizes is illustrated.