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PubMed1987

A microdosimetric model of astatine-211 labeled antibodies for radioimmunotherapy.

Astatine-211 is an alpha-emitter with a short half-life (7.2 hr). This paper discusses the potential of 211At targeted by antibodies for tumor therapy and the possible advantage of 211At over beta- and gamma-emitting radionuclides such as 131I currently employed in the field of radioimmunotherapy. Since the longest range alpha-particle from 211At is only 67 microns and the rate of energy loss is high (track averaged linear energy transfer LT approximately 120 keV/micron), a disintegration of 211At produces a large and extremely localized deposition of energy. A Monte-Carlo model has been developed for studying the stochastic fluctuation of alpha-particle hits and energy deposition in cell nuclei in an attempt to determine the efficacy of 211At-labeled antibodies for tumor cell inactivation. Calculations have been performed for 2 extreme conditions: (a) the case of 211At retained in the capillary, and (b) for a homogeneous distribution of 211At-labeled antibody in the tumor. The results of these two calculations represent the boundary conditions between which any real solution must lie. Finally, developments to the model to include antibody transport across the capillary membrane and through the tumor tissue are discussed.

Antibodies, Neoplasm↗

PubMed1995

Meta-[131I]iodobenzylguanidine uptake and meta-[211At]astatobenzylguanidine treatment in human medulloblastoma cell lines.

Uptake of radioiodinated meta-iodobenzylguanidine (MIBG) has been demonstrated in the neural crest tumors, including neuroblastoma, pheochromocytoma, and carcinoid tumors, and is presently in use diagnostically and therapeutically in these settings. Cells comprising medulloblastoma, the most common central nervous system malignancy in childhood, may be derived from a common germinal neuroepithelial cell as neural crest tissue, and as a result, also may have the capacity for accumulating MIBG. To investigate this hypothesis, we measured the in vitro binding of [131I]MIBG to 9 medulloblastoma-derived cell lines and the SK-N-SH neuroblastoma line known to accumulate MIBG. Seven of the medulloblastoma lines exhibited MIBG binding. The cell line with the greatest uptake, D384 Med, bound 11.2 +/- 0.9% of added [131I]MIBG activity compared with 47.1 +/- 2.3% for the SK-N-SH cell line. When 2 of the cell lines, D384 Med and D458 Med, were treated with the alpha-particle emitting analogue meta-[211At]astatobenzylguanidine ([211At]MABG), as much as a 3-log cell kill was observed in limiting dilution clonogenic assays. Exposure to considerably higher activity levels of [211At]astatide was required to achieve a similar degree of cell kill, suggesting that this cytotoxicity was not related to nonspecific effects of alpha-particle irradiation. We conclude that the uptake capacity of medulloblastoma cell lines for [131I]MIBG uptake in vitro, while lower than that seen in SK-N-SH neuroblastoma cells, is sufficient to permit [211At]MABG to be used with significant therapeutic effectiveness.

3-Iodobenzylguanidine↗

PubMed2002

Design and synthesis of 225Ac radioimmunopharmaceuticals.

The alpha-particle-emitting radionuclides 213Bi, 211At, 224Ra are under investigation for the treatment of leukemias, gliomas, and ankylosing spondylitis, respectively. 213Bi and 211At were attached to monoclonal antibodies and used as targeted immunotherapeutic agents while unconjugated 224Ra chloride selectively seeks bone. 225Ac possesses favorable physical properties for radioimmunotherapy (10d half-life and 4 net alpha particles), but has a history of unfavorable radiolabeling chemistry and poor metal-chelate stability. We selected functionalized derivatives of DOTA as the most promising to pursue from out of a group of potential 225Ac chelate compounds. A two-step synthetic process employing either MeO-DOTA-NCS or 2B-DOTA-NCS as the chelating moiety was developed to attach 225Ac to monoclonal antibodies. This method was tested using several different IgG systems. The chelation reaction yield in the first step was 93+/-8% radiochemically pure (n=26). The second step yielded 225Ac-DOTA-IgG constructs that were 95+/-5% radiochemically pure (n=27) and the mean percent immunoreactivity ranged from 25% to 81%, depending on the antibody used. This process has yielded several potential novel targeted 225Ac-labeled immunotherapeutic agents that may now be evaluated in appropriate model systems and ultimately in humans.

Actinium↗

PubMed2004

Plutonium microdistribution in the lungs of Mayak workers.

The degree of nonuniform distribution of plutonium in the human lung has not been determined; thus current dosimetric models do not account for nonuniform irradiation. A better scientific basis is needed for assessing the risk of developing radiation-induced disease from inhaled alpha-particle-emitting radionuclides. We measured the distribution of plutonium activity in the lung by autoradiography and related the activity to specific compartments of the lung. The study materials were lung specimens from deceased workers employed by the Mayak Production Association. The approach to analyzing these lung samples used contemporary stereological sampling and analysis techniques together with quantitative alpha-particle autoradiography. For the first time, plutonium distribution has been quantified in the human lung. The distribution of long-term retained plutonium is nonuniform, and a significant portion of plutonium was retained in pulmonary scars. In addition, a large fraction of plutonium was present in the parenchyma, where it was retained much longer than was estimated previously. The sequestration of plutonium particles in scars would greatly reduce the radiation exposure of the critical target cells and tissues for lung cancer. Thus the prolonged retention of plutonium in lung scars may not increase the dose or risk for lung cancer.

Adult↗

PubMed1996

Chromosomal abnormalities in neutron-induced acute myeloid leukemias in CBA/H mice.

Acute myeloid leukemias (AMLs) induced in CBA/H mice by 1 MeV fission neutrons have been examined for chromosomal abnormalities by G-band analysis. In common with X-ray- and alpha-particle-induced AMLs in CBA/H mice, more than 90% (16/17) of the myeloid leukemias had chromosome 2 abnormalities, in this case, all interstitial deletions. Chromosome 2 breakpoints were not wholly consistent, but clustering in three specific G-band regions was observed. Very distal (H-region) breakpoints were more common in the neutron AMLs than in X-ray- or alpha-particle-induced leukemias. These data indicate that neutron-induced AMLs in CBA/H mice are not characterized by a specific chromosome deletion but that a variety of chromosome 2 deletion types are associated with the disease. Trisomy of chromosome 1(12.5% AMLs) and aneusomy of chromosomes 6 (31% AMLs) and Y (37.5% AMLs) were noted. While chromatid breakage was observed occasionally in neutron-induced AML, no clear indications of persistent chromosomal instability or high levels of stable chromosomal change were apparent.

Acute Disease↗

PubMed1981

The influence of ionization density on the DNA synthetic phase and survival of irradiated mammalian cells.

Depression of the DNA synthetic rate of exponentially growing V79 cells was transient with a dose-dependent maximum at 1 hour after exposure to sparsely or densely ionizing radiation. The dose-effect curves were biphasic for 241Am alpha-particles as well as for 60Co gamma-rays, being partly congruent if inhibition of DNA synthesis was expressed per S-phase cell. The lesions responsible caused a prolongation of the DNA synthetic period (S-phase) after sparsely ionizing X- or 60Co gamma-rays. However, no such effect was observed during the first 4 hours after exposure to densely ionizing alpha particles, peak pions and high LET neon ions. The effect was dose-rate independent. The inhibition of the DNA synthetic rate seems to be only partly related to survival.

Americium↗

PubMed2005

Radiation effectiveness factors for use in calculating probability of causation of radiogenic cancers.

This paper presents so-called radiation effectiveness factors that are intended to represent the biological effectiveness of different radiation types, relative to high-energy Co gamma rays, for the purpose of estimating cancer risks and probability of causation of radiogenic cancers in identified individuals. Radiation effectiveness factors are expressed as subjective probability distributions to represent uncertainty that arises from uncertainties in estimates of relative biological effectiveness obtained from radiobiological studies of stochastic endpoints, limited data on biological effectiveness obtained from human epidemiological studies, and other judgments involved in evaluating the applicability of available information to induction of cancers in humans. Primarily on the basis of reviews and evaluations of available data by experts, probability distributions of radiation effectiveness factors are developed for the following radiation types: neutrons of energy less than 10 keV, 10-100 keV, 0.1-2 MeV (including fission neutrons), 2-20 MeV, and greater than 20 MeV; alpha particles of any energy emitted by radionuclides; photons of energy 30-250 keV and less than 30 keV; and electrons of energy less than 15 keV. Photons of energy greater than 250 keV and electrons of energy greater than 15 keV are assumed to have the same biological effectiveness as reference Co gamma rays and are assigned a radiation effectiveness factor of unity, without uncertainty. For neutrons and alpha particles, separate probability distributions of radiation effectiveness factors are developed for solid tumors and leukemias, and small corrections to represent an inverse dose-rate effect are applied to those distributions in cases of chronic exposure. A radiation effectiveness factor different from unity for 15-60 keV electrons is discussed but is not adopted due to a lack of relevant radiobiological data. Radiation effectiveness factors presented in this paper are incorporated in the Interactive RadioEpidemiological Program and were developed for use by The National Institute for Occupational Safety and Health and U.S. Department of Labor in evaluating claims for compensation for radiogenic cancers by workers at U.S. Department of Energy facilities.

Algorithms↗

PubMed2005

Revised rates for the stellar triple-alpha process from measurement of 12C nuclear resonances.

In the centres of stars where the temperature is high enough, three alpha-particles (helium nuclei) are able to combine to form 12C because of a resonant reaction leading to a nuclear excited state. (Stars with masses greater than approximately 0.5 times that of the Sun will at some point in their lives have a central temperature high enough for this reaction to proceed.) Although the reaction rate is of critical significance for determining elemental abundances in the Universe, and for determining the size of the iron core of a star just before it goes supernova, it has hitherto been insufficiently determined. Here we report a measurement of the inverse process, where a 12C nucleus decays to three alpha-particles. We find a dominant resonance at an energy of approximately 11 MeV, but do not confirm the presence of a resonance at 9.1 MeV (ref. 3). We show that interference between two resonances has important effects on our measured spectrum. Using these data, we calculate the triple-alpha rate for temperatures from 10(7) K to 10(10) K and find significant deviations from the standard rates. Our rate below approximately 5 x 10(7) K is higher than the previous standard, implying that the critical amounts of carbon that catalysed hydrogen burning in the first stars are produced twice as fast as previously believed. At temperatures above 10(9) K, our rate is much less, which modifies predicted nucleosynthesis in supernovae.

Journal Article↗

PubMed1991

Differential locus sensitivity to mutation induction by ionizing radiations of different LETs in Chinese hamster ovary K1 cells.

Mutation induction after exposures to 250 kVp X-rays, alpha-particles from the radon daughter 212Bi, and fission-spectrum neutrons from the JANUS reactor was studied in Chinese hamster ovary (CHO) K1 cells and in CHO-10T5, a K1 derivative containing the bacterial gene xanthine-guanine phosphoribosyl transferase (gpt). Mutation induction was analyzed at three genetic loci: the gpt locus, the hypoxanthine-guanine phosphoribosyl transferase (hprt) locus, and the thymidine kinase (tk) locus. After X-irradiation, mutants were induced at the tk loci at approximately 8-9 times the rate of mutant induction at the hprt locus, and the rate of mutant induction at the gpt locus was 8-10 times greater than that at the hprt locus. Neutron and alpha-radiation were more effective mutagenic agents. Mutant frequencies were approximately 4- to 6-fold higher than for X-rays at the hprt and gpt loci and greater than 12-fold greater than X-rays at the tk locus. The greater sensitivity of the tk locus to mutation induction by ionizing radiation (especially neutron and alpha-particle radiation) compared to the hprt locus is likely to be due to the recovery of an additional class of mutants, possibly ones containing larger-sized mutational events. Approximately half of the X-ray-induced tk-1- mutants were small-colony mutants, and 75% of the alpha- and neutron-induced tk-1- mutants were small-colony mutants. The increase in the proportion of small-colony mutants seen with increasing radiation linear energy transfer (LET) suggests that the radiation quality influenced the type of mutation recovered at this locus. There is probably a different reason for the hypersensitivity of the gpt locus because the frequency of gpt mutants, compared to the hprt locus, was independent of radiation quality. Therefore, the LET dependence of mutant induction is gene specific and not necessarily related to the size of deletion recoverable.

Animals↗

PubMed2005

Evidence for complexity at the nanometer scale of radiation-induced DNA DSBs as a determinant of rejoining kinetics.

The rejoining kinetics of double-stranded DNA fragments, along with measurements of residual damage after postirradiation incubation, are often used as indicators of the biological relevance of the damage induced by ionizing radiation of different qualities. Although it is widely accepted that high-LET radiation-induced double-strand breaks (DSBs) tend to rejoin with kinetics slower than low-LET radiation-induced DSBs, possibly due to the complexity of the DSB itself, the nature of a slowly rejoining DSB-containing DNA lesion remains unknown. Using an approach that combines pulsed-field gel electrophoresis (PFGE) of fragmented DNA from human skin fibroblasts and a recently developed Monte Carlo simulation of radiation-induced DNA breakage and rejoining kinetics, we have tested the role of DSB-containing DNA lesions in the 8-kbp-5.7-Mbp fragment size range in determining the DSB rejoining kinetics. It is found that with low-LET X rays or high-LET alpha particles, DSB rejoining kinetics data obtained with PFGE can be computer-simulated assuming that DSB rejoining kinetics does not depend on spacing of breaks along the chromosomes. After analysis of DNA fragmentation profiles, the rejoining kinetics of X-ray-induced DSBs could be fitted by two components: a fast component with a half-life of 0.9+/-0.5 h and a slow component with a half-life of 16+/-9 h. For alpha particles, a fast component with a half-life of 0.7+/-0.4 h and a slow component with a half-life of 12+/-5 h along with a residual fraction of unrepaired breaks accounting for 8% of the initial damage were observed. In summary, it is shown that genomic proximity of breaks along a chromosome does not determine the rejoining kinetics, so the slowly rejoining breaks induced with higher frequencies after exposure to high-LET radiation (0.37+/-0.12) relative to low-LET radiation (0.22+/-0.07) can be explained on the basis of lesion complexity at the nanometer scale, known as locally multiply damaged sites.

Cells, Cultured↗

PubMed1990

Steps towards cancer therapy with radionuclides--a review including radiation biophysical aspects.

Though great advantages will be connected with endoradiotherapy, a lot of problems has still to be overcome, the greatest of them being without doubt the problem of selectivity of the carrier compounds. Some few of them have proved to be able to accumulate in certain cancers by reason of their incorporation as metabolites, especially in melanomas. The other great hope are the monoclonal antibodies or their fragments, and in this field much endeavour has been spent in the last years. Especially the two-step method of loading the radioactive nuclide to the antibodies when their binding to the cancer cells is complete appears very promising. Some other, unspecific vehicles may also prove suitable for accumulation in certain tumor types. For the selection of the nuclides it has to be considered that radiation biophysical experiments demonstrated that the critical targets for radiation action are with high probability the DNA superstructure units, and that the distribution of ionizations within them is decisive for the inactivation of a cell. With sparsely ionizing radiation (e.g. beta-radiation) rather high doses are required for reaching an adequate concentration of ionizations in these DNA units. Densely ionizing radiation with an LET of about 150 keV/microns exhibits the maximum relative biological effectiveness (12-16 referred to X-radiation). Therefore emitters of alpha-particles the LET of which lies actually somewhat lower, near 100 keV/microns, seem to be very suitable for endoradiotherapy. Moreover the short ranges of these particles (about 60 microns in tissue) render an extensive sparing of the surrounding normal tissue possible. The second group of effective nuclides is that of Auger electron emitters. The low-energy proportion of Auger electrons leads to a high ionization density in small volumes. The very short ranges of these electrons (in the nanometer range), however, require an incorporation of the nuclide into the cell nucleus if an effective cell inactivation is to occur. 211At (alpha-emitter) and 125I (Auger electron emitter) already proved their high inactivating effectiveness in cell cultures and their curative action in animal experiments, and studies of binding 211At to monoclonal antibodies are encouraging. Some other approaches proposed for the transport of radionuclides into tumor cells or for generating them within tumor tissue are also aimed in essential at the release of densely ionizing alpha-particles or of Auger electrons.

Animals↗

PubMed1999

Radioimmunotherapy using vascular targeted 213Bi: the role of tumor necrosis factor alpha in the development of pulmonary fibrosis.

A monoclonal antibody (201B) specific to murine thrombomodulin, covalently linked to cyclohexyl diethylenetriaminepentaacetic acid, successfully delivers chelated 213Bi, an alpha-particle emitter, (213Bi-201B) rapidly to lung vascular endothelium. When injected at doses of 1 MBq/mouse, 213Bi-201B destroyed most of the 100 colonies of EMT-6 mammary carcinomas growing as lung tumors of up to 2000 cells/colony. Some mice were cured of lung tumors, and others had extended life spans compared to untreated control animals but eventually succumbed to tumor recurrence. At injected doses of 4-6 MBq/mouse, 100% of lung tumor colonies were eliminated; however, 3-4 months later, these mice developed pulmonary fibrosis and died. The mechanisms leading to the fibrotic response in other pulmonary irradiation models strongly implicate tumor necrosis factor alpha (TNF-alpha), released from damaged tissues, as the pivotal inflammatory cytokine in a cascade of events that culminate in fibrosis. Attempts to prevent the development of pulmonary fibrosis, by using antibodies or soluble receptor (rhuTNFR:Fc) as inhibitors of TNF-alpha, were unsuccessful. Additionally, mice genetically deficient for TNF-alpha production developed pulmonary fibrosis following 213Bi-201B treatment. Interestingly, non-tumor-bearing BALB/c mice receiving rhuTNFR:Fc or mice genetically deficient in TNF-alpha production and treated with 213Bi-201B, had significantly reduced life spans compared to mice receiving no treatment or 213Bi-201B alone. We speculate that in normal mice, although TNF-alpha may induce an inflammatory response following alpha-particle radiation mediated tumor clearance and pulmonary damage, its effects in the post-tumor clearance time period may actually retard the development of fibrosis.

Animals↗

PubMed2005

Biodistribution of 225Ra citrate in mice: retention of daughter radioisotopes in bone.

Alpha-particle-emitting radionuclides have potential for therapy of localized disease due to their high linear energy transformation and short pathlengths. Radiometals that home naturally to bone can be exploited for this purpose, and 223Ra (t(1/2)=11.4 days) recently has been studied for therapy of bone tumors in mice and rats. Actinium-225 (t(1/2)=10 days) is also an attractive radioisotope for endoradiotherapy. In a single decay of a 225Ac nucleus and its subsequent decay daughters, over 27 MeV ( approximately 90% of total energy) is released by sequential emission of four alpha particles, ranging in energy from 5.7 to 8.4 MeV. Although Ac3+ does not home naturally to bone, its parent radioisotope 225Ra (beta(-), t(1/2)=15 days) can be used as an in vivo source for 225Ac. Thus, injection of 225Ra takes advantage of the bone-homing properties of radium coupled with the significant amount of energy released from the 225Ac decay chain. Our data confirm that a large fraction of radium citrate injected intravenously into mice localizes rapidly in bone. Injected doses per gram (ID/g) for 225Ra range from 25% in skull to about 10% in sternum. Once deposited, the 225Ra remains in the bone with a biological half life of >40 days. Furthermore, >95% of the daughter radioisotope, 225Ac, is retained in the bone. However, a significant fraction of one of the daughter radioisotopes, 213Bi, is found in kidney. The biodistribution data indicate that 225Ra injection should be a powerful agent for killing cells associated with bone; however, the toxicity of this radioisotope which is similar to that of other alpha emitters limits the dose that can be tolerated.

Animals↗

PubMed1993

Systemic deposits of thorium in thorotrast patients with particular reference to sites of minor storage.

It is well established that injected Thorotrast is deposited in the liver, spleen, bone marrow, and lymph nodes, but accumulations in organs with lower macrophage activity have previously been given little attention. In this work, neutron activation analysis has been used to investigate concentrations of thorium in autopsy samples taken at sites of major and minor deposition in 24 Thorotrast patients. In the latter category, the highest values were found in the testis [40 x 10(-6) g/g(wet)], followed by those in the adrenal gland, gallbladder, lung, and pancreas. The resulting alpha-particle dose rates (mGy/year) are tentatively estimated to be 8.5 to the testis, 5.5 to the gallbladder, and 5.3 to the lung. These results may be relevant to the residual excess mortality among Thorotrast patients after diseases of the principal organs of deposition have been excluded; they also support previous indications that thorium deposited in pulmonary tissues is responsible for an important component of the total dose to the lung. In another context, our data may bear on the connection, postulated elsewhere, between exposure to alpha-particle emitters and elevated incidence of leukemia in the children of workers engaged in the reprocessing of nuclear fuel.

Adult↗

PubMed1990

Prediction of cell survival curves from DNA double-strand break repair data for low- and high-LET radiation.

A model developed previously (Ostashevsky 1989), was applied to calculate survival curves from the DNA double-strand break (dsb) repair data for Ehrlich ascites tumour (EAT) cells irradiated with X-rays or 3.4 MeV alpha-particles (Blöcher 1988). It is shown that the calculated curves are in agreement with experiments. The relationship between the low-dose-rate survival curve slopes for low- and high-LET radiations was obtained. Data for relatively radioresistant cells (EAT, normal fibroblasts, V-79 and CHO-K1) seem to be in agreement with the predicted numbers, while those for radiosensitive cells (AT fibroblasts and xrs-6) do not. Possible reasons for this discrepancy are discussed. In the framework of the model, three factors are important for the high RBE of alpha-particles: (1) an increased radiation yield of induced dsb; (2) a reduced dsb repair rate and (3) an increased probability of losing fragments from the DNA.

Animals↗

PubMed1992

Radon-induced deletions in human cells: role of nonhomologous strand rejoining.

Radon is a ubiquitous inhaled human carcinogen that is thought to be the largest single natural source of human exposure to radiation. We report that a freely replicating episome in human cells exposed to radon gas underwent mutagenic changes, a high proportion of which were large deletions involving many thousands of base pairs. These deletions were not randomly distributed but started and ended in defined regions as if caused by the passage of a single alpha-particle track through a coiled chromatin structure. The sizes appeared to be defined by structural features of chromatin: the minimum size was 2435 base pairs, and the maximum size was 8051 base pairs, close to the upper limit that would leave intact the plasmid sequences required for selection in bacteria. Ends were rejoined by nonhomologous recombination involving up to 6 base pairs of homology. This process may not be confined to the repair of exogenously induced double-strand breaks but may be used for rejoining free DNA ends generated by a variety of cellular processes. The mechanism of alpha-particle deletion mutagenesis may account for the high relative biological effectiveness of radon irradiation for many end points and its consequences for lung carcinogenesis.

Base Sequence↗

PubMed2005

Increased sensitivity to sparsely ionizing radiation due to excessive base excision in clustered DNA damage sites in Escherichia coli.

PURPOSE: In order to clarify the cellular processing and repair mechanisms for radiation-induced clustered DNA damage, we examined the correlation between the levels of DNA glycosylases and the sensitivity to ionizing radiation in Escherichia coli. MATERIALS AND METHODS: The lethal effects of gamma-rays, X-rays, alpha-particles and H2O2 were determined in E. coli with different levels of DNA glycosylases. The formation of double-strand breaks by post-irradiation treatment with DNA glycosylase was assayed with gamma-irradiated plasmid DNA in vitro. RESULTS: An E. coli mutM nth nei triple mutant was less sensitive to the lethal effect of sparsely ionizing radiation (gamma-rays and X-rays) than the wild-type strain. Overproduction of MutM (8-oxoguanine-DNA glycosylase), Nth (endonuclease III) and Nei (endonulease VIII) increased the sensitivity to gamma-rays, whereas it did not affect the sensitivity to alpha-particles. Increased sensitivity to gamma-rays also occurred in E. coli overproducing human 8-oxoguanine-DNA glycosylase (hOgg1). Treatment of gamma-irradiated plasmid DNA with purified MutM converted the covalently closed circular to the linear form of the DNA. On the other hand, overproduction of MutM conferred resistance to H2O2 on the E. coli mutM nth nei mutant. CONCLUSIONS: The levels of DNA glycosylases affect the sensitivity of E. coli to gamma-rays and X-rays. Excessive excision by DNA glycosylases converts nearly opposite base damage in clustered DNA damage to double-strand breaks, which are potentially lethal.

DNA Damage↗

PubMed1992

Stability and permeability of amphiphile bilayers.

In this review the rupture and permeability of bilayers are considered on the basis of a mechanism of the formation of microscopic holes as fluctuations in the bilayers. The hole formation is treated as a nucleation process of a new phase in a two-dimensional system with short-range intermolecular forces. Free rupture and deliberate rupture (by alpha-particles) of foam bilayers (Newtonian black films) are discussed. A comparison is made between the rupture of foam and emulsion bilayers. Experimental methods for obtaining foam and emulsion bilayers from thin liquid films are considered. Methods for investigating the stability and permeability of foam bilayers, which are based on a microscopic model allowing the use of amphiphile solutions with very low concentrations, are described. Experimental dependences of the lifetime of bilayers, the probability of observing the foam bilayer in a foam film, the gas permeability of bilayers, etc. on the concentration of amphiphile molecules in the solution are reported. The influence of temperature and external impact (e.g. alpha-particle irradiation) have also been experimentally studied. A good agreement between theory and experiment is established, allowing determination of several characteristics of foam and emulsion bilayers obtained from ionics or non-ionics: the specific edge energy of bilayer holes, equilibrium surfactant concentration below which the bilayer is thermodynamically metastable, work for the formation of a nucleus hole, number of vacancies in the nucleus hole, coefficient of gas diffusion through the bilayer, etc. On the basis of the effect of temperature on the rupture of foam bilayers the binding energy of a surfactant molecule in the bilayer is determined. The adsorption isotherm of surfactant vacancies in the foam bilayer is obtained which shows a first-order phase transition. Some applications to scientific, technological and medical problems are considered. The foam bilayer is used as a model for investigating short-range forces in biological structures, the interaction between membranes and cell fusion. It is also shown that the foam bilayer is a suitable model for studying the alveolar surface and stability. On that basis a clinical diagnostic method is developed for assessment of the human foetal lung maturity.

Animals↗