Temperature regulation and microhabitat choice by free-ranging Galapagos fur seal pups (Arctocephalus galapagoensis)

Summary Behavioural activity, and core and surface temperatures of 4 unrestrained Galapagos fur seals were recorded in the natural habitat during their first weeks of life. Climatic variables were registered simultaneously. Pup behaviours were divided into bouts of resting (55% of total time), sucking (23%) and other activities (22%). Pups maintained a constant body temperature from their first day. Core temperature (T _e ) was 37.7° C±0.3° C (x ± SD) over 39 pup-days and 8 pup-nights. Skin temperature was correlated with T _c , but flipper temperature was not. No daily T _c rhythm was detected. Microclimate data were used to calculate operative temperature T _e . Environmental temperatures can be very high, with T _e above T _c 6–9 h a day for animals exposed to the sun, but below it in the shade. T _c is about 22° C at night. Pups avoid overheating mainly by withdrawing into the shade and reducing activity to a minimum during the hot hours of the day. Sun-exposed pups could be active at any time during the day if they had access to water, which was usually around high tide.     

Hemoglobin senses body temperature

When aspirating human red blood cells (RBCs) into 1.3 μm pipettes (ΔP = −2.3 kPa), a transition from blocking the pipette below a critical temperature T _c = 36.3 ± 0.3°C to passing it above the T _c occurred (micropipette passage transition). With a 1.1 μm pipette no passage was seen which enabled RBC volume measurements also above T _c. With increasing temperature RBCs lost volume significantly faster below than above a T _c = 36.4 ± 0.7 (volume transition). Colloid osmotic pressure (COP) measurements of RBCs in autologous plasma (25°C ≤ T ≤ 39.5°C) showed a T _c at 37.1 ± 0.2°C above which the COP rapidly decreased (COP transition). In NMR T₁-relaxation time measurements, the T₁ of RBCs in autologous plasma changed from a linear (r = 0.99) increment below T _c = 37 ± 1°C at a rate of 0.023 s/K into zero slope above T _c (RBC T₁ transition). In conclusion: An amorphous hemoglobin–water gel formed in the spherical trail, the residual partial sphere of the aspirated RBC. At T _c, a sudden fluidization of the gel occurs. All changes mentioned above happen at a distinct T _c close to body temperature. The T _c is moved +0.8°C to higher temperatures when a D₂O buffer is used. We suggest a mechanism similar to a “glass transition” or a “colloidal phase transition”. At T _c, the stabilizing Hb bound water molecules reach a threshold number enabling a partial Hb unfolding. Thus, Hb senses body temperature which must be inscribed in the primary structure of hemoglobin and possibly other proteins. This article is dedicated to Ludwig Artmann who died on July 21, 2001 on a beautiful summer day during which we performed experiments far away. Ludwig Artmann was a man who encouraged us to be strong and to study hard no matter what were the costs.     

Competition between cyanogenic and acyanogenic morphs of Trifolium repens

Summary To investigate the cost of the dimorphic cyanogenic system in Trifolium repens L., genotypes of the cyanogenic (T_c) and acyanogenic (T_a) morphs were grown in mixtures over a range of ratios and in pure stands at two levels of total density (low in a first experiment, high in a second experiment). The principles of the competition analysis employed were those related to the inverse linear model response. The morphs were compared using two interaction indices, the substitution rate and the relative resource total (RRT). The relative fitness of the two morphs, i.e. biomass and number of flowers per plant, suggests that the T_a morph has a competitive advantage over the T_c morph.     

Thermal buffering capacity of the germination phenotype across the environmental envelope of the Cactaceae

Recruitment from seeds is among the most vulnerable stage for plants as global temperatures change. While germination is the means by which the vast majority of the world's flora regenerate naturally, a framework for accurately predicting which species are at greatest risk of germination failure during environmental perturbation is lacking. Taking a physiological approach, we assess how one family, the Cactaceae, may respond to global temperature change based on the thermal buffering capacity of the germination phenotype. We selected 55 cactus species from the Americas, all geo‐referenced seed collections, reflecting the broad environmental envelope of the family across 70° of latitude and 3700 m of altitude. We then generated empirical data of the thermal germination response from which we estimated the minimum (T_b), optimum (T_o) and ceiling (T_c) temperature for germination and the thermal time (θ₅₀) for each species based on the linearity of germination rate with temperature. Species with the highest T_b and lowest T_c germinated fastest, and the interspecific sensitivity of the germination rate to temperature, as assessed through θ₅₀, varied tenfold. A left‐skewed asymmetry in the germination rate with temperature was relatively common but the unimodal pattern typical of crop species failed for nearly half of the species due to insensitivity to temperature change at T_o. For 32 fully characterized species, seed thermal parameters correlated strongly with the mean temperature of the wettest quarter of the seed collection sites. By projecting the mean temperature of the wettest quarter under two climate change scenarios, we predict under the least conservative scenario (+3.7°C) that 25% of cactus species will have reduced germination performance, whilst the remainder will have an efficiency gain, by the end of the 21st century.     

A hydrothermal time model explains the cardinal temperatures for seed germination

Temperature (T) and water potential (y) are two primary environmental regulators of seed germination. Seeds exhibit a base or minimum T for germination (T_b), an optimum T at which germination is most rapid (T_o), and a maximum or ceiling T at which germination is prevented (T_c). Germination at suboptimal T can be characterized on the basis of thermal time, or the T in excess of T_b multiplied by the time to a given germination percentage (t_g). Similarly, germination at reduced y can be characterized on a hydrotime basis, or t_g multiplied by the y in excess of a base or threshold y that just prevents germination (y_b). Within a seed population, the variation in thermal times to germination among different seed fractions (g) is based on a normal distribution of y_b values among seeds (y_b(g)). Germination responses across a range of suboptimal T and y can be described by a general hydrothermal time model that combines the T and y components, but this model does not account for the decrease in germination rates and percentages when T exceeds T_o. We report here that supra‐optimal temperatures shift the ψ_b(g) distribution of a potato (Solanum tuberosum L.) seed population to more positive values, explaining why both germination rates and percentages are reduced as T increases above T_o. A modified hydrothermal time model incorporating changes in ψ_b(g) at T > T_o describes germination timing and percentage across all T and ψ at which germination can occur and provides physiologically relevant indices of seed behaviour.     

The Genes Encoding the Somatic and Testis-Specific Isotypes of the Mouse Cytochrome c Genes Map to Paralogous Regions of Chromosomes 6 and 2

Using mouse probes specific to cytochrome c_S and to cytochrome c_T, the single-copy genes encoding these two proteins have been mapped to paralogous chromosomal regions by analysis of restriction fragment length variants in interspecific crosses. The gene for cytochrome c_S, Cycs, maps to a position between Tcrb and Cbl-1 on proximal mouse Chromosome 6, and the gene for cytochrome c_T, Cyct, maps between Gad-1 and Sfpi-1 on mouse Chromosome 2.     

NMR relaxation study of water protons in Syrian hamster fetal cells at 300 MHz

TheT ₁ andT ₂ relaxation times of water protons in two cell types in culture derived from Syrian hamster fetuses (normal primary or secondary fetal cells vs BP6T tumor cells derived from the normal cells transformed by carcinogens) were measured at 7.05 Tesla magnetic field (proton frequency =300 MHz). TheT ₁/T ₂ ratios and the correlation time, τ _c , calculated from theT ₁/T ₂ ratio of cellular water protons, are significantly different in these two fibroblastic cell types of the same biological origin and with similar morphologies and growth rates in culture.     

The effect of solvent viscosity and temperature on DNA viscoelastic behavior

The effect of solvent viscosity (η_s) and temperature (T) on the shape of the concentration dependence of the principal and total recoils in creep-recovery viscoelastometry experiments has been studied for T4 DNA solutions. The range of DNA concentration (c) was 2 – 40 μg/ml; glycerol, 70–80% v/v, sucrose, 60% v/v; NaCl, 5 mM – 1M; and T, 275 – 323 K. A linear proportionality between recoil and c was obtained at high η_s/T. At low η_s/T, the c-dependence was nonlinear, approaching saturation at higher c. At low c, the slope of both curves was the same. Transition between “linear” and “nonlinear” values occurred over a narrow range of η_s/T (a width of 1–5 K if η_s/T was changed by varying T). (η_s/T)_tr, the midpoint of the transition, was independent of solvent properties other than viscosity. Also, (η_s/T)_tr increased with c. For a given c, η_s/T values above this transitional value yield linear behavior; below this, nonlinear behavior. The ratio of linear to nonlinear recoil values is a linear function of c with K_c, the slope of this dependence, independent of η_s and T. A kinetic model for the observed nonlinearity of recoil with c is presented. It explains the independence of K_c on η_s and T. An attempt has been made to explain the linear–nonlinear transitions by comparison of τ₁ and T_R, the lifetime of the contact points of the polymer network in the de Gennes theory. The nonlinear values are consistent with a pseudogel that exists when τ₁ < T_R. At τ₁ > T_R, the DNA behavior is similar to that in dilute solutions (linear values). Thus, the condition for transition is τ₁ = T_R. However, some unsolved problems remain.     

Halothane-induced membrane reorganization monitored by DSC,freeze fracture electron microscopy and 31 P-NMR techniques

The effect of the volatile anaesthetic halothane on the structure and dynamics of lipid multilayers (dimyristoyl- and dipalmitoylphosphatidylcholine, DM-and DP-PC, aqueous dispersions) was studied using Differential Scanning Calorimetry (DSC), Freeze Fracture Electron Microscopy and solid state phosphorus-31 Nuclear Magnetic Resonance (³¹P-NMR). The action of the drug depends upon the halothane-to-lipid molar ratio, Ri, and temperature. With DPPC lipids, three main regions can be distinguished: i) 0 < Ri < 0.7, ii) 0.7 < Ri < 2 and iii) Ri > 2. As Ri increases in the first region, a linear decrease in the main gel-to-fluid phase transition temperature (T _c, a broadening in the DSC transition peak and a lowering in the enthalpy variation (H), are observed. A minimum in H is reached at Ri=0.7. In this region, ³¹P-NMR spectra indicate that the multibilayer structure is maintained. In the second region, T _c still decreases with the same slope, but H increases up to a plateau value for Ri=2. In the lipid fluid phase, an isotropic NMR line appears superimposed on the powder pattern that corresponds to a lamellar phase. For Ri > 2, T _c and H remain almost constant. At values of temperature that are greater than T _c a growing isotropic line occurs in ³¹P-NMR spectra. This means a new supramolecular structure made of lipids and halothane is stabilized. This structure has been characterized as small vesicles of about 400 Å to 600 Å diameter by Freeze Fracture electron microscopy observations. With DMPC and low ratios (Ri < 2), DSC and NMR results are similar to those obtained for DPPC. However, the minimum H is reached at Ri=0.2 and the decrease in T _c is faster than for DPPC when Ri increases from 0. For Ri > 2, while T _c and H remain constant as in the case of DPPC, ³¹P-NMR spectra of DMPC systems show a superimposition of an isotropic line and two powder patterns, which correspond to small tumbling vesicles, a possible hexagonal phase and a lamellar phase respectively. Halothane, thus acts on model membranes in two different steps: at low Ri the bilayer is disturbed but keeps its structure. Whereas for higher drug concentrations, a new organization of lipids seems to be stabilized for T > T _c.Abbreviations DPPC Dipalmitoylphosphatidylcholine - DMPC Dimyristoylphosphatidylcholine - DSC Differential scanning calorimetry - NMR Nuclear magnetic resonance - EDTA Ethylenediaminetetraacetic acid - DMSO Dimethyl sulfoxide - Ri Halothaneto-lipid molar ratio - T _c Main gel (L )-to-fluid (L ) phase transition temperature - T _m Maximum temperature of the transition - H Enthalpy variation - C _{p max} excess heat capacity at the maximum temperature of the transition T _m - n number of phospholipid molecules per cooperative unit Offprint requests to: J.-P. Renou     

Cell proliferation kinetics of six xenografted human cervix carcinomas: comparison of autoradiography and bromodeoxyuridine labelling methods

Abstract. Cell kinetic and histologic parameters of six xenografted tumours with volume doubling times ranging from 6 to 43 d were investigated in order to obtain kinetic information on a panel of tumours to be used in radiobiological studies. The six tumours covered a range of histologies and their DNA indices varied from 2–7 to 1–4. The length of the cell cycle (T_c), potential doubling time (T_pot) and labelling index (LI) were determined by continuous labelling with [³H]TdR and autoradiography in three tumours. T_c varied from 30 to 40 h. Determinations of the length of the S phase (T_s) were found to be less reliable by this method. Data on T_s and LI were also determined in all six tumours using bromodeoxyuridine (BrdU) labelling and the single sample method; values of T_pot were slightly longer than those obtained via the autoradiographic method. In addition, multiple samples were taken after BrdU labelling. T_c was determined by fitting the data obtained from mid-S, mid-G₂ and mid-G₁ windows to curves described by a damped oscillator. Data obtained via the mid-S window were found to be most reliable. Generally, cell cycle times obtained by the BrdU method were longer than those observed with the autoradiographic method. Differences between the two methods could be explained by inaccuracies in the determination of T_s, LI and T_c and differences in the experimental approach. We consider the BrdU labelling method to be a suitable alternative for the time-consuming autoradiography, if data on T_s or T_pot are sufficient. Due to difficulties in the reproducibility of the immunofluorescence staining and asynchronization of cells approximately 10 h after labelling, the method of windows analysis was affected by similar problems to those observed in interpretation of percentage labelled mitosis (PLM) curves. However, the method may serve as an alternative to determine cell cycle times in vitro and, if improved technically, in vivo. Careful comparison of the data obtained from mid-S, mid-G₁ and mid-G₂ windows may increase the reliability of the determination of cell kinetic parameters.     

Pigeon flight in a wind tunnel

Summary Core temperatureT _c, breast temperatureT _s–br and leg temperatureT _s–1 were measured simultaneously in pigeons during rest and flight in a wind tunnel, using thermistors.MeanT _c at rest is 39.8±0.7°C and is independent of ambient temperatureT _a (10–30°C). In the first minutes of flight,T _c increases to 1.5–3.0°C above resting level and remains at this higher level. This hyperthermia increases withT _a (v=const.). It is±constant in the lowT _a range (10.6–13.9°C) at flight speeds v ranging from 10–18 m s^–1 and normal body mass, but increases with v and elevated body mass in the highT _a range (23.7–28.8°C). T _s–1 is adapted toT _a at rest and increases in flight up to 3–4°C belowT _c. This increase inT _s–1 is linear toT _a. T _s–br is always lower thanT _c, in extreme cases reaching restingT _c in flight.Supported by the Deutsche Forschungsgemeinschaft     

The Optimum Recombination Rate That Realizes the Fastest Evolution of a Novel Functional Combination of Many Genes

The effect of genetic recombination (or crossover) by sexual reproduction on the time until a novel set of genes performing a combined function appears, spreads, and becomes fixed is studied. First, we study a haploid finite population with many binary loci, in which only one sequence (called a functional gene set) is significantly advantageous over the others. The time for evolution of the function (T_d) is defined as the mean number of generations until the advantageous sequence dominates in an initially random population. When the sequence diversity is initially stored sufficiently, the evolution timeT_dis roughly the product of the waiting time until the appearance of the advantageous sequence (creation timeT_c) and the average number of appearances of the advantageous sequence from its absence until its fixation (destruction numberN_d). Mutation and crossover reduce the former but enlarge the latter. If the mutation rate is low, there is an intermediate optimal rate of crossover that achieves the minimumT_d. In contrast, if the mutation rate is sufficiently high,T_dis smallest without crossover. Second, the breakdown of established functions by recurrent deleterious mutation in an infinite population is examined. The number of functional genes maintained decreases monotonically with the recurrent deleterious mutation rate. Thus in higher organisms having many functional sets of genes in the genome, the mutation rate must be kept very low to preserve them, and hence a high crossover rate made possible by sexual reproduction is important in accelerating the evolution of novel functional sets of genes. Implications of this long-term advantage of recombination in the maintenance of sexual reproduction in higher organisms are discussed.     

A Simple and Rapid PCR-based Procedure for Identifying Homozygous Transgenic Rice Plants

We present a simple and rapid method for screening second-generation transgenic rice plants (T₁) to identify homozygous plants. The plasmid (pfd11) used for rice transformation contains a partially deleted cytochrome c gene (cyc) for comparing with the endogenous cyc for copy number. After polymerase chain reaction (PCR) amplification of a segment of the cyc in transgenic rice DNA followed by agarose gel electrophoresis, two specific bands are obtained. The upper band represents the endogenous cyc, and the lower band represents the partially deleted cyc in the transgene. The first-generation plants (T₀) that harbor a single copy of the transgene are selected based on the fact that the density of the lower band is half as dense as the upper band. Next, only plants harboring a single copy of the transgene are advanced to the second generation (T₁). The same PCR procedure is used again, and homozygous T₁ plants are easily identified from samples in which the intensity of the two bands is the same.     

A Modified Gibbs Ensemble Method for Calculating Fluid Phase Equilibria

Abstract

A modification of the Gibbs ensemble Monte Carlo computer simulation method for fluid phase equilibrium is described. The modification, which is based on the assumption of a thermodynamic model for the vapor phase, reduces the computational time for the simulation as compared to the original Gibbs ensemble methods. Since the computational time is largely proportional to the number of particle-particle interactions, avoiding the direct simulation of the vapor phase typically leads to a thirty to forty percent reduction in computational time. For a pure Leonard-Jones-(12,6) fluid the results obtained at moderate reduced temperatures, T/T_c < 0.8, are in good agreement with the full Gibbs ensemble method.     

Adsorption of Carbon Dioxide to Polysaccharides in the Supercritical Region

The adsorption isotherms for C0₂ to several polysaccharides were measured in a pressure range between 0 and 29.4 MPa by the gravimetric method. The adsorption of C0₂ to two kinds of starches (potato and corn) and to dextrin increased linearly with increasing pressure to reach a maximum, and then decreased sharply to constant level at higher pressure. These adsorption characteristics are similar to those of proteins reported previously. On the other hand, the adsorption of C0₂ to cellulose showed a high level at the beginning of the increase in pressure, without any significant change in the sub-critical pressure region, and then fell to the minimum before reaching a constant level at higher pressures. These adsorption characteristics of cellulose could be related to its micropore structure. The pressure at which the maximum adsorption occurred (P_max) was located on the P-T line of the C0₂ phase diagram where (dpfdP)_T was a maximum, this result being different from the Menon correlation of P_max = P_c(T/T_c)² proposed for adsorption to macroporous adsorbents.     

THE EFFECT OF ESTRADIOL ON THE CELL KINETICS IN THE UTERINE AND CERVICAL EPITHELIUM OF NEONATAL MICE

The effect of estradiol-17β on the length of the various phases of the cell cycle was studied in the neonatal mouse uterine, and cervical epithelium. A double labelling method was used, and in addition labelled mitoses were counted. In the uterus proper, estradiol shortens the length of the total cell cycle, T_c, from 17-9 hr to 15-7 hr, and the duration of S phase, T_s, from 6–7 to 5-1 hr 6 hr after estradiol treatment. 12 hr after estradiol treatment, T_c is shortened to 7-4 hr and T_s to 4–5 hr. The shortening of T_c at 12 hr is mainly due to an effect on T_G1, which is shortened from 8–55 hr in untreated animals to 1–8 hr in estradiol treated animals. The T_c of cervix epithelium cells in untreated animals was found to be 21-8 hr. After treating the mice for 6 hr with estradiol the T_c was now increased to 47 hr and further to 61 -2 hr following 12 hr treatment with the hormone. T_s increases from 8-3 hr to 15-2 hr following 6 hr estradiol treatment, and to 15-4 hr after 12 hr treatment. The effect is most pronounced in T_G1, which is lengthened from 10–95 hr in untreated animals to 28-1 hr and 43 hr, respectively, in animals treated for either 6 or 12 hr with estradiol.     

Perfect temperature for protein structure prediction and folding

We have investigated the influence of the “noise” of inevitable errors in energetic parameters on-protein structure prediction. Because of this noise, only a part of all the interactions operating in a protein chain can be taken into account, and therefore a search for the energy minimum becomes inadequate for protein structure prediction. One can rather rely on statistical mechanics: a calculation carried out at a temperature T_* somewhat below that of protein melting gives the best possible, though always approximate prediction. The early stages of protein folding also “take into account” only a part of all the interactions; consequently, the same temperature T_* is favorable for the self-organization of native-like intermediates in protein folding. © 1995 Wiley-Liss, Inc.     

Synthesis of Polyoxamic Acid (2-Amino-2-deoxy-l-xylonic Acid

The rate of precipitation of the retrograded amylose product from a dil. amylose solution was determined by the centrifugal method. The results showed that the relation of the quantity of precipitate vs. time did not fit the typical second order reaction for the coalescence of colloidal particles but fitted the crystallization formula, in appearance.

The rate of precipitation was in proportion to (c-c_a)^1.5, where c is the amylose concentration and c_a the concentration of the dil. solution phase in the phase-separated solution. When the temperature dependence of the rate was treated according to the crystallization of polymers, it was found that the rate was in proportion to T_m²/T(ΔT)², where T_m is the melting point of the polymer in solution and ΔT is (T_m?T). The T_m thus obtained was 120°C for an amylose solution. These results suggested a certain correlation between the amylose retrogradation and the crystallization.     

Bioenergetics and thermal physiology of American water shrews (<Emphasis Type="Italic">Sorex palustris</Emphasis>)

Rates of O₂ consumption and CO₂ production, telemetered body temperature (T_b) and activity level were recorded from adult and subadult water shrews (Sorex palustris) over an air temperature (T_a) range of 3–32°C. Digesta passage rate trials were conducted before metabolic testing to estimate the minimum fasting time required for water shrews to achieve a postabsorptive state. Of the 228 metabolic trials conducted on 15 water shrews, 146 (64%) were discarded because the criteria for inactivity were not met. Abdominal T_b of S. palustris was independent of T_a and averaged 38.64±0.07°C. The thermoneutral zone extended from 21.2°C to at least 32°C. Our estimate of the basal metabolic rate for resting, postabsorptive water shrews (96.88±2.93 J g^–1 h^–1 or 4.84±0.14 ml O₂ g^–1 h^–1) was three times the mass-predicted value, while their minimum thermal conductance in air (0.282±0.013 ml O₂ g^–1 h^–1) concurred with allometric predictions. The mean digesta throughput time of water shrews fed mealworms (Tenebrio molitor) or ground meat was 50–55 min. The digestibility coefficients for metabolizable energy (ME) of water shrews fed stickleback minnows (Culaea inconstans) and dragonfly nymphs (Anax spp. and Libellula spp.) were 85.4±1.3% and 82.8±1.1%, respectively. The average metabolic rate (AMR) calculated from the gas exchange of six water shrews at 19–22°C (208.0±17.0 J g^–1 h^–1) was nearly identical to the estimate of energy intake (202.9±12.9 J g^–1 h^–1) measured for these same animals during digestibility trials (20°C). Based on 24-h activity trials and our derived ME coefficients, the minimum daily energy requirement of an adult (14.4 g) water shrew at T_a = 20°C is 54.0 kJ, or the energetic equivalent of 14.7 stickleback minnows.