Radiobiological evaluation of the suitability of negative pions in tumor therapy; facts and theories

Summary A successful cancer radiotherapy consists mainly in sparing normal tissues and killing malignant cells. Negative pions seem to have several and unique gain factors, as Fowler and Perkins 1961 proposed. With the biomedical pion channel of the 590 MeV proton-accelerator of the Swiss Institute for Nuclear Research (SIN) we had since several years the opportunity to test some theoretical conceptions in comparison to several preliminary experiments performed with pions of low dose rate (Berkeley, CERN, Nimrod). The dosimetric measurements showed for the momentum of 180 MeV/c and a ratio e^–/ ^– of 0.1 an excellent depth curve with p. ex: a peak/plateau ratio of 2.5. Besides this important gain factor for radiotherapy, negative pions have the unique particularity to act on the tissues in the same treatment with two different types of radiations, in the peak (treatment volume) with high LET radiation (presumably high RBE) and low LET radiation in the plateau. Following systems have been used: Inactivation of single mammalian cells, induction of chromatid aberrations in Chinese hamster cells; small intestine of mouse (early and late effects); early and late effects in mouse foot; induction of anomalies in mouse embryos; induction of cerebral microvascular damages in neonatal rats; proliferation of Ehrlichascites carcinoma cells; induction of different types of mutation in different stages of male germ cells and somatic cells (Drosophila). The RBE-values in the peak region vary between 0.7–3.3, and are different even in the same system with the same end point but at different cell stages and conditions. For the plateau region the RBE-values lie mostly under 1 (compared with 140 kV-photons) and can be identical with 29 MeV-photons. The clinically important peak/plateau relation lies in every experiment over 1 and reaches even the value of 4.2. The unexpected RBE-values in peak under 1 lead to a new conception of RBE, the two system theory. In intrinsic radiosensitive euoxic systems (healthy tissue) the RBE of peak (star) pions can be under 1, in intrinsic radioresistant hypoxic systems (tumor cells) in contrary over 1. The two systems can also have different vulnerability of repair svstem.Invited paper, presented at the 14th Annual Meeting of European Society of Radiation Biology, Jülich, Germany, October 8–14, 1978Supported by the Swiss National Science Foundation (grant no. 3.682-0.75)Prof. Dr. A. Prader dedicated on the occasion of his 60th birthday     

Preclinical Radiobiology with Pions: RBE — Values for Mouse Skin Damage as a Function of Single Doses of Pions

Summary The macroscopic reaction of the mouse skin was used to derive RBE values for negative-Mesons. Hind limbs of mice were irradiated with pions or X-rays. The pions were produced by the 590 MeV accelerator of the Schweizerisches Institut für Nuklearforschung (SIN). Early skin reaction was assessed over a period of 6–30 days after irradiation with single doses (20–45 Gy). The radiation damage was scored using an arbitrary scale of effect. The time pattern of development of the skin reaction and the subsequent healing after exposure both to pions and X-rays were similar, indicating that depletion and repopulation of the basal cells of the skin were comparable, both after pions and X-rays. RBE values as a function of pion doses at the peak (dose maximum), plateau and at the postpeak (12 mm downstream of the dose maximum) were computed with nonparametric statistical methods. The RBE at the peak and at the plateau relative to X-rays of the same dose rate was 1.15–1.25 and 0.85, respectively. The RBE of peak pions manifested a marked dependence on dose, when plateau pions were chosen as reference radiation. In this experiment there was no significant difference in RBE between peak and postpeak. The importance of some experimental condition (dose rate, irradiation volume) is discussed.Supported by the Swiss National Science Foundation (grant no. 3.682-0.75)     

Chromatid breaks induced in Chinese hamster cells by low doses (12–100 rad) ofπ −-mesons

Summary Monolayer cultures of the fibroblast-like Chinese hamster cell-line 19/1 were irradiated in the G₂-phase of the cell cycle by ^–-mesons (6 rad/min peak-pion dose rate). Frequencies of induced single- and isochromatid breaks, acentric fragments and interchanges were compared with data obtained from 140 kV X-rays.The RBE-values were for the pion dose peak between 0.8–1.2 and for the pion dose plateau 0.5–0.9. Whereas for single chromatid breaks there was no significant difference between X-rays and peak pions for identical physical doses, the isochromatid breaks alone showed a significantly higher frequency for 100 rad peak pions.     

Pre-clinical studies of the negative pi-meson beam at TRIUMF

Summary The ^– flux from the biomedical channel at TRIUMF increases with increasing channel momentum, while the contaminating electron flux decreases. Since the electrons appear to result from conversion of the high energy-rays produced by ⁰ decay in the production target, the electron contamination can be reduced further by target configurations which minimize gamma conversion.The attenuation of ^– beams by in-flight interactions was found to decrease from an initial value of 1.67 ± 0.02 % per g/cm² at zero depth to 1.48 ± 0.02 % per g/cm² near the stopping peak.The inactivation of cultured CHO cells by an extended-peak ^– dose distribution has been measured using the gel technique. The survival data have been fitted by a model which characterizes the physical quality of the dose profile by means of measured star densities. This model provides a convenient method of analysis for large sets of survival data and may be useful for prediction of the biological effect of new ^– dose distributions.The RBE value for 50% survival measured at the centre of a 7 cm extended peak was found to be approximately 1.4, in reasonable agreement with recent values obtained at LAMPF and SIN.     

Piotron pion irradiation of cerebral capillaries in neonatal rats

Summary The microvasculature of the neonatal rat brain and its radiation-induced petechial hemorrhages were used as an in vivo model for studying the effect of negative pions on healthy normal tissue. By means of dose response curves (range: 2–6 gray) the RBE of peak pions with respect to 220 kVp X-rays was calculated. Whereas earlier studies involved irradiations with single beam pions (E3) of low dose rate (0.06–0.11 Gy per min) the present work was performed using pions of a multiport applicator (Piotron) of higher dose rate (1 Gy per min). The results obtained by Piotron pions agreed well with those obtained byE3 pions resulting in a RBE of 1.1. The difference between pion and X-rays, however, was statistically not significant. 0-(beta-hydroxyethyl)-rutosides known for their protective effect on radiation damage induced by either X-rays or electrons were used for evaluating any radioprotective effect on pion-induced damage of the microvasculature. They were applied subcutaneously in doses of 450 mg/kg body weight 30 min prior to irradiation. It could be demonstrated that the rutosides decreased the pion-induced radiation response significantly by a factor of 1.3.     

The suitability of negative pions for radiotherapy: 4 years preclinical research with the biomedicalΠE3-beam at SIN

Summary The radiobiological experiences over 4 years research with the biomedical pion channel of the 590 MeV proton-accelerator of the Swiss Institute for Nuclear Research (SIN) have been summarized. Mainly sensitive biological systems have been chosen (limiting factor: dose-rate not more than 10 rad/min, exceptionally till 30 rad/min). The RBE values in the peak region vary between 0.7–3.3 and in the plateau region between 0.4–1. The gain factors for pion radiotherapy of cancer are, beside the excellent physical dose distribution, irradiation in the same treatment with two types of radiation: sparsely ionizing (low LET) radiation in plateau (healthy tissue) region and densely ionizing (high LET) radiation in peak (tumor) region. The biological effectiveness ratio in peak and plateau as the clinically most important relation vary between 1.4–4.2. This is valid also for clinically limiting factors such as reaction of skin, of small intestine, vascular damage, dominant lethals in hypoxic cells, tumor induction. For peak pions the RBE in hypoxic cells (tumor cells) can be much higher than in euoxic cells (healthy tissue). This preclinical work supports the hope in a highly effective cancer therapy with negative pions.Supported by the Swiss National Science Foundation (grant no. 3.682-0.75) and the Swiss Mobilar Insurance Company     

Fluorescence of 3-keto-steroids in aqueous solution

The physiologically important 3-keto-steroids are non-fluorescent or only weakly fluorescent in protic as well as in aprotic solvents. In contrast, the 4,6,8(14)-triene-3-one steroids are highly fluorescent in aqueous solution but they do not appreciably fluoresce in other solvents. Evidence is presented that the introduction of double bonds into the skeleton of the 3-keto-steroids leads to a decrease of the energy of the lowest – ^* state, bringing this level into the neighbourhood of the non-fluorescent n – ^* state. As a consequence, for two states of approximately the same energy, relatively small perturbations such as those due to solvent interactions, protein binding and micelle formation, will then determine whether a system will fluoresce ( – ^* state lowest) or not (n – ^* state lowest). When the fluorescent 3-keto-steroids, having three conjugated double bonds, bind to proteins, the fluorescence intensity becomes almost zero, making these compounds useful as probes for steroid-protein interactions. This quenching of the fluorescence is explained by a decrease in energy of the n – ^* state relative to the – ^* state of the steroids due to hydrophobic interactions with the proteins.Abbreviations 6,8-BDT 6,8-bisdehydrotestosterone; DMSO, dimethylsulfoxide - HPLC high pressure liquid chromatography This work was presented in part at the Annual Meeting of the Gesellschaft für Biologische Chemie, September 26–29, 1983, in Göttingen. For an abstract see: Hoppe-Seyler's Z. Physiol. Chem. (1983) 364: 1151–1152Dedicated to Prof. Dr. F.-W. Zilliken on the occasion of his 65th birthday     

Detection of heavy-ion-induced DNA double-strand breaks using static-field gel electrophoresis

Radiation-induced DNA double-strand breaks (DSBs) were measured in Chinese hamster ovary cells (CHO-K1) using an experimental protocol involving static-field gel electrophoresis following exposure to various accelerated ions. Dose-effect curves were set up, and relative biological efficiencies (RBEs) for DSB induction were determined for different radiation qualities. RBEs around 1 were obtained for low energy deuterons (6–7 keV/µm), while for high energy oxygen ions (20keV/µm) an RBE value slightly greater than 1 was determined. Low energetic oxygen ions (LET=250 keV/µm) were found to show RBEs substantially below unity, and for higher LET particles (31 y-250 keVµm) RBEs for DSB induction were generally found to be smaller than 1. The data presented here are in line with the generally accepted view that not induced DSBs, but rather misrepaired or unrepaired DNA lesions are related to cellular inactivation.     

Mode of uptake of sterol by Arthrobacter simplex

The mechanism of uptake of water-insoluble -sitosterol by a newly isolated strain of Arthrobacter simplex SS-7 was studied. The production of an extracellular sterol-pseudosolubilizing protein during growth of A. simplex on -sitosterol was demonstrated by isolating the factor from the cell-free supernatant and its subsequent purification by Sephadex G-150 column chromatography. The M _r of the purified sterol-pseudosolubilizing protein determined by SDS–PAGE was 19kDa. The rate of sterol pseudosolubilization (5.2×10^–3g l^–1h^–1) could not adequately account for the rate of sterol uptake (72×10^–3g l^–1h^–1) and the specific growth rate (56×10^–3 h^–1). However in the unfavourable growth condition, when the cells were treated with sodium azide at the level of 30–60% of MIC, the sterol pseudosolubilization accounted for nearly 74% of the total growth containing 96% free cells. Cellular adherence to substrate particles was found to play an active role in the normal growth of the strain on -sitosterol. Unlike sodium acetate-grown cells, whose surface activity was negligible (60mNm^–1), the sterol-grown cells had strong surface activity (40mNm^–1). The high lipid content and long chain fatty acids in the cell-wall of -sitosterol-grown cells probably contribute to the high sterol adherence activity of the cells.     

Induction of HPRT- mutants in Chinese hamster V79 cells after heavy ion exposure

The induction of resistance to 6-thioguanine by heavy ion exposure was investigated with various accelerated ions (oxygen-uranium) up to linear energy transfer (LET) values of about 15000 keV/µm.31 y Survival curves are exponential with fluence; mutation induction shows a linear dependence. Cross-sections (_i: inactivation, _m: mutation) were derived from the respective slopes. Generally, _i rises over the whole LET range, but separateas into different declining curves for single ions with LET values above 200 keV/µm. Similar behaviour is seen for _m. The new SIS facility at GSI, Darmstadt, makes it possible to study the effects of ions with the same LET but very different energies and track structures. Experiments using nickel and oxygen ions (up to 400 MeV/u) showed that inactivation cross-sections do not depend very much on track structure, i.e. similar values are found with different ions at the same LET. This is not the case for mutation induction, where very energetic ions display considerably smaller induction cross-sections compared with low-energy ions of identical LET. Preliminary analyses using the polymerase chain reaction (PCR) demonstrate that even heavy ions cause small alterations (small deletions or base changes). The proportion of the total deletions seems to increase with LET.Submitted paper presented at the International Symposium on Heavy Ion Research: Space, Radiation Protection and Therapy, Sophia-Antipolis, France, 21–24 March 1994     

Identification of a glutathione-S-transferase effector domain for inhibition of jun kinase, by molecular dynamics

We have recently found that the glutathione-S-transferase -isozyme (GST-), a cellular detoxification enzyme, potently and selectively inhibits activation of jun protein by its upstream kinase, jun kinase (JNK). This newly identified regulatory activity of GST- is strongly inhibited by a group of agents that inhibit its enzymatic activity. Since loss of enzymatic activity in general does not correlate with loss of regulatory activity, it is likely that inhibitor binding induces changes in the structure of one or more domains of GST that block its interaction with JNK. To identify regions of GST that change conformation on the binding of inhibitors, we have performed molecular dynamics calculations on GST- to compute its average structure in the presence and absence of the inhibitor, glutathione sulfonate. Superposition of the two average structures reveals that several regions change local structure depending upon whether the inhibitor is bound or not bound. Two of these regions, residues 36–50 and 194–201, are highly exposed. We have synthesized peptides corresponding to these two segments and find that the 194–201 sequence strongly inhibits the ability of GST- to block the in vitro phosphorylation of jun by JNK. These results suggest that this region of GST- is critical to its functioning as a newly discovered regulator of signal transduction.     

Diversity,metabolic types and δ13C carbon isotope ratios in the grass flora of Namibia in relation to growth form,precipitation and habitat conditions

The grass flora of Namibia (374 species in 110 genera) shows surprisingly little variation in ¹³C values along a rainfall gradient (50–600 mm) and in different habitat conditions. However, there are significant differences in the ¹³C values between the metabolic types of the C4 photosynthetic pathway. NADP-ME-type C4 species exhibit the highest ¹³C values (–11.7 ) and occur mainly in regions with high rainfall. NAD-ME-type C4 species have significantly lower ¹³C values (–13.4 ) and dominate in the most arid part of the precipitation regime. PCK-type C4 species play an intermediate role (–12.5 ) and reach a maximum abundance in areas of intermediate precipitation. This pattern is also evident in genera containing species of different metabolic types. Within the same genus NAD species reach more negative ¹³C values than PCK species and ¹³C values decreased with rainfall. Also in Aristida, with NADP-ME-type photosynthesis, ¹³C values decreased from –11 in the inland region (600 mm precipitation) to –15 near the coast (150 mm precipitation), which is a change in discrimination which is otherwise associated by a change in metabolism. The exceptional C3 species Eragrostis walteri and Panicum heterostachyum are coastal species experiencing 50 mm precipitation only. Many of the rare species and monotypic genera grow in moist habitats rather than in the desert, and they are not different in their carbon isotope ratios from the more common flora. The role of species diversity with respect to habitat occupation and carbon metabolism is discussed.     

Stable isotope and radiocarbon compositions of methane emitted from tropical rice paddies and swamps in Southern Thailand

Stable isotopes (¹³C, D) and radiocarbon weremeasured in methane bubbles emitted from rice paddies and swamps in southernThailand. Methane emitted from the Thai rice paddies was enriched in¹³C (mean ¹³C; –51.5 ±7.1 and–56.5 ± 4.6 for mineral soil and peat soil paddies,respectively)relative to the reported mean value of methane from temperate rice paddies(– 63 ± 5). Large seasonal variation was observed in¹³C(32) in the rice paddies, whereas variationinD was much more smaller (20), indicating that variation in¹³C is due mainly to changes in methane production pathways.Values of ¹³C were lower in swamps (–66.1 ±5.1)than in rice paddies. The calculated contribution of acetate fermentation from¹³C value was greater in rice paddies (mineral soils:62–81%, peat soils: 57–73%) than in swamps (27–42%). Din methane from Thai rice paddies (–324± 7 (n=46)) isrelativelyhigher than those from 14 stations in Japanese rice paddies ranging from–362 ± 5 (Mito: n=2) to –322 ± 8(Okinawa: n=3), due tohigher D in floodwaters. ¹⁴C content in methane produced fromThai rice paddies (127±1 pMC) show higher ¹⁴Cactivity compared with previous work in paddy fields and those from Thai swamps(110±2 pMC).     

Growth and physiology of potassium-limited chemostat cultures of Paracoccus denitrificans

In potassium-limited chemostat cultures of Paracoccus denitrificans the maximum specific growth rate (µ_max) was found to depend on the input potassium concentration: At 0.21mM µ_max was 0.10–0.11 h^-1; at 0.44 mM 0.15–0.16 h^-1 and at 0.66 mM 0.20–0.21 h^-1. The plots of the specific rates of oxygen-, succinate-and potassium consumption against gave straight lines. The intracellular potassium concentration was a linear function of and varied from 1% (0.13 M) at a value of 0.034 h^-1 to 2.2% (0.29 M) at =0.26 h^-1; the potassium concentration gradient and the potassium concentration in the culture fluid in the steady state were dependent on the input potassium concentration. The potassium concentration gradient varied from 8,900-1,200. At all values 20–25% of the total energy production was used for potassium transport. 350,100 and 30 ATP molecules were calculated to be required to maintain one potassium ion intracellular during 1 h at values of 0.034, 0.197 and 0.257 h^-1 respectively. It is concluded that the amount of circulation of potassium is dependent on the potassium concentration gradient or on the potassium concentration in the culture in the steady state. The dependency of µ_max on the input potassium concentration was explained by the assumption that at low input potassium concentrations the net uptake of potassium (influx-efflux) is not rapidly enough to maintain the high potassium gradient in the existing cells and to establish it in the newly formed cells. At high values and at high input potassium concentrations µ_max is limited by the specific rate of oxygen consumption, which was found to be 11–12 mmol O₂ g dry weight^-1 h^-1 at µ_max for potassium-, succinate-and sulphate-limited chemostat cultures.     

Effects of <Emphasis Type="Italic">in vitro</Emphasis>rooting environments and irradiance on growth and photosynthesis of strawberry plantlets during acclimatization

Strawberry (Fragaria ananassaDuch. cv. Fengxiang) plantlets were cultured under two in vitroenvironments for rooting, and then acclimatized under two ex vitroirradiance conditions. At the end of rooting stage plant height, fresh weight and specific leaf area of T1-plants grown under high sucrose concentration (3 sucrose), low photosynthetic photon flux density (30 mol m^–2 s^–1) and normal CO₂ concentration (350–400 l l^–1) were significantly higher than those of T2-plantlets grown under low sucrose concentration (0.5), high photosynthetic photon flux density (90 mol m^–2 s^–1) and elevated CO₂ concentration (700–800 l l^–1). But T2-plantlets had higher net photosynthetic rate (Pn), effective photochemical quantum yield of PSII (_PSII), effective photosynthetic electron transport rate (ETR), photochemical quenching (q_P) and ratio of chlorophyll fluorescence yield decrease (Rfd). After transfer, higher irradiance obviously promoted the growth of plantlets and was beneficial for the development of photosynthetic functions during acclimatization. T2-plantlets had higher fresh weight, leaf area, _PSII and ETR under higher ex vitroirradiance condition.     

Rectification characteristics ofNitella membranes in respect to water permeability

Summary One of the membrane characteristics of plant cells, rectification, or the direction dependence of water permeability, was investigated inCharaceae internodes using the procedures we developed (Tazawa andKiyosawa 1973) for determining the endosmotic (k _pen) and exosmotic (k _pex) water permeabilities of the membranes (plasmalemma and tonoplast) in the transcellular osmosis system. Bothk _pen andk _pex were dependent on the osmotic pressure ( _o ) of the mannitol solution, which is the driving force for the transcellular osmosis. Thus, k_pen increased andk _pex decreased with _o . The rectification parameter, or the polarity (_p), defined ask _pen/k _pex tended to unity when _o approached zero.InNitella flexilis the specific resistances of the membranes to endosmosis and exosmosis,k _pen ^–1 andk _pex ^–1 , were linearly dependent on ₀. When the cell was partitioned into two equal halves,k _pen ^–1 =4.2×10⁴–1.1×10³₀,k _pex ^–1 =4.2×10⁴+2.9×10³₀, where the specific resistances are represented in cm^–1 sec atm. When _o is 0.1, 0.2, 0.3, 0.4, and 0.5 M mannitol eq., the rectification parameter is calculated as 1.3, 1.6, 1.9, 2.4, and 2.9, respectively. Essentially the same results were also obtained withChara australis.Results were discussed on the basis of changes in the hydration of the cytoplasm. Assuming that the driving force across the protoplasmic layer can be divided into two forces; one driving water across the plasmalemma and the other driving water across the tonoplast, we deduced that the cytoplasm on the endosmosis side is hydrated, while the cytoplasm on the exosmosis side is dehydrated. Analysis showed that changes in hydration depend on the rate of flow.This work was supported partly by a Research Grant from the Ministry of Education of Japan.     

The Use of the [13C]/[12C] Ratio for the Assay of the Microbial Oxidation of Hydrocarbons

The study deals with a comparative analysis of the relative abundances of the carbon isotopes ¹²C and ¹³C in the metabolites and biomass of the Burkholderia sp. BS3702 and Pseudomonas putida BS202-p strains capable of utilizing aliphatic (n-hexadecane) and aromatic (naphthalene) hydrocarbons as sources of carbon and energy. The isotope compositions of the carbon dioxide, biomass, and exometabolites produced during the growth of Burkholderia sp. BS3702 on n-hexadecane (¹³C = –44.6 ± 0.2) were characterized by the values of ¹³C_{CO 2} = –50.2 ± 0.4, ¹³C_biom = –46.6 ± 0.4, and ¹³C_exo = –41.5 ± 0.4, respectively. The isotope compositions of the carbon dioxide, biomass, and exometabolites produced during the growth of the same bacterial strain on naphthalene (¹³C = –21 ± 0.4) were characterized by the isotope effects ¹³C_{CO 2} = –24.1 ± 0.4, ¹³C_biom = –19.2 ± 0.4, and ¹³C_exo = –19.1 ± 0.4, respectively. The possibility of using the isotope composition of metabolic carbon dioxide for the rapid monitoring of the microbial degradation of petroleum hydrocarbons in the environment is discussed.     

The quantitative analysis of chromosome pairing and chiasma formation based on the relative frequencies of M I configurations

Whilst reliable estimates of chiasma frequencies can usually not be obtained, the probability (b) of a chromosome arm to be bound by at least one chiasma can often be determined. In the absence of interference this probability equals (1–e ^–2), where 2 is the average chiasma frequency of the chromosome arm and the average crossover frequency or map length. In the presence of interference is shown to retain its genetic meaning as an additive metric that may describe the chromosome arm or other distinctive chromosome segment in terms of genetic recombination. It is a form of potential map length, comparable to, but numerically different from the regular map length. It is termed provisionally crossing-over potential.A chromosome with armsm andn with crossing-over potentials and will form ring bivalents with a frequency (1–e ^–2).(1–e ^–2); open bivalents with a frequency (1–e ^–2).e ^–2+(1–e ^–2).e ^–2; univalent pairs with a frequencye ^–2.e ^–2. Estimates of these frequencies yield equations from which and may be solved. In rye (Secale cereale) their ratio (q) is approximately two and differs from the mitotic arm length ratio of 1.4, indicating localization of chiasmata in the long arms.Graphs are given to show how, with constantq, the relation between the probabilitiesb _m andb _n of the two arms being bound changes with changing averageb.Data are presented on chiasma frequencies in M I, and compared with the frequencies expected in the absence of interference to give an impression of the degree of interference. Apparent fusion of chiasmata simulates interference.     

Measurement of apoplasmic and cell-to-cell components of root hydraulic conductance by a pressure-clamp technique

A pressure-clamp technique was devised for the direct measurement of cell-to-cell and apoplasmic components of root hydraulic conductance; the experimental results were analyzed in terms of a theoretical model of water and solute flow, based on a composite membrane model of the root. When water is forced under a constant pressure into a cut root system, an exponential decay of flow is observed, until a constant value is attained; when pressure is released, a reverse water flow out of the root system is observed which shows a similar exponential behavour. The model assumes that the transient flow occurs through a cell-to-cell pathway and the observed decrease is the result of accumulation of solutes in front of the root semi-permeable membrane, whilst the steady-state component results from the movement of water through the parallel apoplasmic pathway. Root conductance components are estimated by fitting the model to experimental data. The technique was applied to the root systems of potted cherry (Prunus avium L.) seedlings; average apoplasmic conductance was 15.5 × 10^–9m³· s^–1· MPa^–1, with values ranging from 12.0 × 10^–9 to 18.5 × 10^–9m³· s^–1· MPa^–1; average cell-to-cell conductance was 11.7 × 10⁹ m³· s^–1· MPa^–1, with values ranging from 8.5 × 10^–9 to 15.3 × 10^–9 m³ · s^–1·MPa^–1. Cell-to-cell conductance amounted on average to 43% of total root conductance, with values between 41 and 45%. Leaf specific conductance (conductance per unit of leaf area supported) of the root systems ranged from 2.7 × 10^–8 to 5.6 × 10^–8 m· s^–1·MPa^–1, with an average of 3.7 × 10^–8 m · s^–1·MPa^–1. The newly developed technique allows the interaction of mass flow of water and of solutes to be explored in the roots of soil-grown plants.Abbreviations and Symbols A L_p root hydraulic conductance - A^aL _p ^a root apoplasmic conductance - A^ccL _p ^cc root cell-to-cell conductance - C_s(t) concentration of solutes in apical root compartment at time t - J_v flow of water through the root - J _v ^a apoplasmic flow of water - J_v/cc cell-to-cell flow of water - LSC leaf specific conductance of the root system - P root hydrostatic pressure - P_appl applied pressure - _s(t) root osmotic pressure at time t - _m osmotic pressure of rooting medium - reflection coefficient of root membrane - time constant of cell-to-cell flow decay This research was funded within the EC Project Long-term effects of CO₂-increase and climate change on European forests (LTEEF) (EV5V-CT94-0468); F.M. was supported by a Ministero dell' Universitá e della Ricerca Scientifica e Tecnologica — British Council agreement (Project The ecological significance of cavitation in woody plants); M.C. was supported by a Consiglio Nazionale delle Ricerche — British Council agreement. We gratefully thank Prof. P.G. Jarvis (University of Edinburgh, UK) for revising an earlier version of this paper and Prof. E. Steudle (University of Bayreuth, Germany) for helpful comments.     

1H, 15N, 13C and 13CO assignments and secondary structure determination of basic fibroblast growth factor using 3D heteronuclear NMR spectroscopy

Summary The assignments of the ¹H, ¹⁵N, ¹³CO and ¹³C resonances of recombinant human basic fibroblast growth factor (FGF-2), a protein comprising 154 residues and with a molecular mass of 17.2 kDa, is presented based on a series of three-dimensional triple-resonance heteronuclear NMR experiments. These studies employ uniformly labeled ¹⁵N- and ¹⁵N-/¹³C-labeled FGF-2 with an isotope incorporation >95% for the protein expressed in E. coli. The sequence-specific backbone assignments were based primarily on the interresidue correlation of C, C and H to the backbone amide ¹H and ¹⁵N of the next residue in the CBCA(CO)NH and HBHA(CO)NH experiments and the intraresidue correlation of C, C and H to the backbone amide ¹H and ¹⁵N in the CBCANH and HNHA experiments. In addition, C and C chemical shift assignments were used to determine amino acid types. Sequential assignments were verified from carbonyl correlations observed in the HNCO and HCACO experiments and C correlations from the carbonyl correlations observed in the HNCO and HCACO experiments and C correlations from the HNCA experiment. Aliphatic side-chain spin systems were assigned primarily from H(CCO)NH and C(CO)NH experiments that correlate all the aliphatic ¹H and ¹³C resonances of a given residue with the amide resonance of the next residue. Additional side-chain assignments were made from HCCH-COSY and HCCH-TOCSY experiments. The secondary structure of FGF-2 is based on NOE data involving the NH, H and H protons as well as ³J_H n _H coupling constants, amide exchange and ¹³C and ¹³C secondary chemical shifts. It is shown that FGF-2 consists of 11 well-defined antiparallel -sheets (residues 30–34, 39–44, 48–53, 62–67, 71–76, 81–85, 91–94, 103–108, 113–118, 123–125 and 148–152) and a helix-like structure (residues 131–136), which are connected primarily by tight turns. This structure differs from the refined X-ray crystal structures of FGF-2, where residues 131–136 were defined as -strand XI. The discovery of the helix-like region in the primary heparin-binding site (residues 128–138) instead of the -strand conformation described in the X-ray structures may have important implications in understanding the nature of heparin-FGF-2 interactions. In addition, two distinct conformations exist in solution for the N-terminal residues 9–28. This is consistent with the X-ray structures of FGF-2, where the first 17–19 residues were ill defined.