Lipid-Induced Modulation of the Protein Packing in Two-Dimensional Crystals of Bacteriorhodopsin

The mechanism by which bacteriorhodopsin (BR), the light-driven proton pump from the purple membrane (PM) of Halobacterium halobium, arranges in a 2D hexagonal array has been studied by reconstitution of BR in complexes of two types of bilayer made either with PM-derived lipids or with PM lipids and 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC). The unit cell dimensions of the 2D protein crystals, determined by correlation averaging analysis of freeze-fracture electron micrographs, were compared with the lattice constant of the PM. In complexes made with delipidated BR and with the polar lipids extracted from H. halobium cells (HHPL), BR trimers are arranged in a hexagonal lattice with the same lattice constant of 5.9 ± 0.2 nm as found in the PM. In BR-containing complexes made with PM-derived lipids and DMPC at several protein:lipid mole ratios, BR trimers are also arranged in a hexagonal lattice, but with a unit cell dimension of 9.2 ± 0.2 nm, which is about one-third larger compared to that measured in PM (Michel et al. , 1980). In a subclass of this type of complexes, orthogonal BR arrays were observed with a lattice constant of 5.9 × 9.9 ± 0.2 nm. It appears that insertion of DMPC into the BP/PM-derived lipid complexes increases the center-to-center distances in both array types by a discrete amount.     

The Kinetics of Hydrolysis of Animal Fat by Pancreatic Lipase

Hydrolysis of lipids from beef fat by pancreatic lipase was studied. The maximum release of free fatty acids was shown to occur at 40°C for the first 3 h of the experiment. After this, transetherification was predominant. The main kinetic parameters were the following: maximum hydrolysis rate, V = 1.25 ± 0.1 mg fat/ml min; Michaelis constant, K _M ^H = 100 ± 12 mg fat/ml; constant of substrate inhibition, K _S = 10.0 ± 0.8 mg fat/ml; equilibrium constant, K _P = 277 ± 170 mg fat/ml; and activation energy of beef fat hydrolysis by pancreatic lipase, E _a = 19.1 ± 1.1 kJ/mole. The kinetic method used could be applied to development of the method for biotransformation of poorly assimilated fats into more valuable products.     

The formation and development of cellulose-synthesizing linear terminal complexes (TCs) in the plasma membrane of the marine red algaErythrocladia subintegra Rosenv.

Summary The formation and development of linear terminal complexes (TCs), the putative cellulose synthesizing units of the red algaErythrocladia subintegra Rosenv., were investigated by a freeze etching technique using both rotary and unidirectional shadowing. The ribbon-like cellulose fibrils ofE. subintegra are 27.6 ± 0.8 nm wide and only 1–1.5 nm thick. They are synthesized by TCs which are composed of repeating transverse rows formed of four particles, the TC subunits. About 50.4 ± 1.7 subunits constitute a TC. They are apparently more strongly interconnected in transverse than in longitudinal directions. Some TC subunits can be resolved as doublets by Fourier analysis. Large globular particles (globules) seem to function as precursor units in the assembly and maturation of the TCs. They are composed of a central hole (the core) with small subunits forming a peripheral ridge and seem to represent zymogenic precursors. TC assembly is initiated after two or three gobules come into close contact with each other, swell and unfold to a nucleation unit resembling the first 2–3 transverse rows of a TC. Longitudinal elongation of the TC occurs by the unfolding of globules attached to both ends of the TC nucleation unit until the TC is completed. The typical intramembranous particles observed inErythrocladia (unidirectional shadowing) are 9.15 ± 0.13 nm in diameter, whereas those of a TC have an average diameter of 8.77 ± 0.11 nm. During cell wall synthesis membranes of vesicles originating from the Golgi apparatus and which seem to fuse with the plasma membrane contain large globules, 15–22 nm in diameter, as well as tetrads with a particle diameter of about 8 nm. The latter are assumed to be involved in the synthesis of the amorphous extracellular matrix cell wall polysaccharides. The following working model for cellulose fibril assembly inE. subintegra is suggested: (1) the ribbon-like cellulose fibril is synthesized by a single linear TC; (2) the number of glucan chains per microfibril correlates with the number of TC subunits; (3) a single subunit synthesizes 3 glucan chains which appear to stack along the 0.6 nm lattice plane; (4) lateral aggregation of the 3-mer stacks leads to the crystalline microfibril.Dedicated to Prof. Dr. Dr. h.c. Eberhard Schnepf on the occasion of his retirement     

Heterogeneity of tight junctions along the collecting duct in the renal medulla

Summary The tight junctions along the medullary collecting duct in the kidneys of the rat and the rabbit were studied with freeze-fracture electron microscopy and quantitated according to the number of strands and the apico-basal depth (nm) of the junctions.The most elaborate tight junctions were found in the inner stripe of the outer medulla; rat: 10.6±0.8 strands and 205±24nm; rabbit: 11.6±2.4 strands and 291±55 nm.The elaboration of the tight junctions decreased continuously towards the papillary tip. Inner zone I; rat: 9.3±2.6 strands and 186±38nm, rabbit: 9.5±2.3 strands and 247±59nm. Inner zone II; rat: 7.1±2.2 strands and 129±32nm, rabbit: 8.5±1.4 strands and 199±26nm. Inner zone III; rat: 6.0±1.6 strands and 111 + 19 nm, rabbit: 7.0±1.5 strands and 183±43 nm. In the inner zone III comprising the papillary tip tight junctions with only 1–3 strands were not infrequently seen. Preliminary findings in the kidney of the golden hamster indicate a similar decline of junctional tightness along the collecting duct.These morphological observations suggest that the permeability of the paracellular pathway of the medullary collecting duct increases towards the tip of the papilla, especially in the rat. The functional implications for the medullary recycling of urea and electrolytes, and for the urinary concentrating mechanism are discussed.In addition, the tight junctions of the papillary epithelium are described.     

50 Hz弱磁场诱导离体表皮生长因子受体聚集

利用原子力显微镜(atomic force microscope,AFM)观测到浓度为5滋g/mL离体表皮因子受体(epidermal growth factor receptor,EGFR)蛋白在50Hz磁场作用下发生聚集,其颗粒呈现倍数变大和变高趋势;利用透射电镜(transmission electronic microscope,TEM)也得到类似的蛋白变大趋势。结果表明,在AFM和TEM下观察到,磁场作用后蛋白聚集颗粒的平均半高宽(平均直径)由(21.7±2.2)nm(12.5nm)增大到(33.0±4.0)nm(23nm),最可几高度由(1.42±0.18)nm增加到(3.08±0.17)nm。这种由磁场引起的聚集效应呈时间依赖性。利用Alexa-488-EGF标记EGFR观察了磁场暴露对细胞上EGF受体表达的影响,提示EGF受体的表达可能稍有上调。上述结果提示50Hz磁场信号可能通过影响EGFR的膜上聚集状态来影响下游信号通路。这种对信号通路的影响可能是电磁场生物性效应的一种机制。     

High-performance liquid chromatographic assay for the measurement of azathioprine in human serum samples

A quantitative, highly sensitive HPLC-based method for the direct measurement of azathioprine is described, introducing a newly synthesized 9-methyl derivative of this immunosuppressant as internal standard in combination with isocartic HPLC and UV-absorbance measurement at 285 nm. Analysis was performed on a RP18 select B column with acetonitrile-0.01 M potassium phosphate buffer (12:88, v/v) at pH 2.3 as mobile phase. Results of precision analysis from serum samples spiked with 3.125, 12.5, and 25 ng azathioprine, respectively, were (mean±S.D.): 3.148±0.259 ng (8.22%), 12.594±0.571 ng (4.53%), and 25.016±0.658 ng (2.63%) with C.V. values in parentheses for n=5. The accuracy of the assay ranged from −7.6 to 0.7% (expressed as % bias) tested on five consecutive days. The limit of quantification was at 2.5±0.256 ng (C.V. 10.25%), thus allowing drug monitoring in long-term patients. The method can also be used to evaluate individual pharmacokinetic parameters of a single patient, as well as for drug monitoring of a cohort of patients who suffer from azathioprine-induced symptoms of toxicity. An example of the pharmacokinetic behaviour in an individual is given in this paper.     

Isolation and Characterization of Carotenosomes from a Bacteriochlorophyll c-less Mutant ofChlorobium tepidum

Chlorosomes are the light-harvesting organelles in photosynthetic green bacteria and typically contain large amounts of bacteriochlorophyll (BChl) c in addition to smaller amounts of BChl a, carotenoids, and several protein species. We have isolated vestigial chlorosomes, denoted carotenosomes, from a BChl c-less, bchK mutant of the green sulfur bacterium Chlorobium tepidum. The physical shape of the carotenosomes (86 ± 17 nm × 66 ± 13 nm × 4.3 ± 0.8 nm on average) was reminiscent of a flattened chlorosome. The carotenosomes contained carotenoids, BChl a, and the proteins CsmA and CsmD in ratios to each other comparable to their ratios in wild-type chlorosomes, but all other chlorosome proteins normally found in wild-type chlorosomes were found only in trace amounts or were not detected. Similar to wild-type chlorosomes, the CsmA protein in the carotenosomes formed oligomers at least up to homo-octamers as shown by chemical cross-linking and immunoblotting. The absorption spectrum of BChl a in the carotenosomes was also indistinguishable from that in wild-type chlorosomes. Energy transfer from the bulk carotenoids to BChl a in carotenosomes was poor. The results indicate that the carotenosomes have an intact baseplate made of remarkably stable oligomeric CsmA–BChl a complexes but are flattened in structure due to the absence of BChl c. Carotenosomes thus provide a valuable material for studying the biogenesis, structure, and function of the photosynthetic antennae in green bacteria.     

Superhelical DNA studied by solution scattering and computer models

We present here recent results on the structure of superhelical DNA and its changes with salt concentration between 0.01 and 1.5 M NaCl. Scattering curves of two different superhelical DNAs were determined by static light scattering. The measured radii of gyration do not change significantly with salt concentration. Small-angle neutron scattering, together with calculations from a Monte Carlo model, allows to determine the superhelix diameter. Measured and simulated scattering curves agreed almost quantitatively. Experimentally we find that the diameter decreases from 16.0±0.9 nm at 10 mM to 9.0±0.7 nm at 100 mM NaCl. The superhelix diameter from the simulated conformations decreased from 18.0±1.5 nm at 10 mM to 9.4±1.5 nm at 100 mM NaCl. At higher salt concentrations up to 1.5 M NaCl, the diameter stays constant at 9 nm.This revised version was published online in October 2005 with corrections to the Cover Date.     

Sister chromatid exchange in lymphocytes from patients with malignant lymphoma

Summary Sister chromatid exchange (SCE) frequencies were studied in differentially stained lymphocytes from 47 patients with malignant lymphoma. Thirteen patients were untreated when studied. The mean SCE frequency [±standard error (SE)] for these patients was 12.7±0.9 per mitosis. The mean score for 40 controls was 6.1±0.3. SCE mean scores were significantly higher in the untreated patients than in the controls (P<0.001). Seven patients were treated with radiotherapy alone. They demonstrated a mean SCE frequency (8.8±0.8) significantly lower (P<0.01) than that found in untreated patients. Eleven patients received cyclophosphamide within 4 weeks prior to study. They demonstrated a mean SCE frequency (14.3±1.3) significantly higher (P<0.05) than that found in patients who had received regimens that did not contain cyclophosphamide in the prior 4 weeks (11.1±1.3) or who had been off drugs for at least 8 weeks (10.1±0.8). Our data suggest that untreated patients with malignant lymphoma have elevated SCE frequencies, which may be further increased by certain chemotherapeutic agents.     

Gap junction ultrastructure in three states of conductance

Summary Junctional conductance between the epidermal cells of the beetle Tenebrio molitor is raised after exposure to the hormone 20-hydroxyecdysone and lowered reversibly by exposure to chlorpromazine. Gap Junctional particle size, density and arrangement associated with these conductance changes were studied. We found no significant difference in particle density in gap junctions of control (2456±471 particles/m², mean ±S.D.) and hormone-treated epidermis (2490±315); however, a significant increase in packing density occurred in chlorpromazine-uncoupled epidermis (3133±665). The particles are randomly arranged in all three states of conductance. Particle size measurements show that the E-face gap junctional particles are heterogeneous with a mean diameter ±S.D. of 15.2±2.0 nm. No significant difference in particle size between controls and experimentals was detected. Although glutaraldehyde irreversibly uncoupled these cells, the absence of glutaraldehyde fixation but presence of glycerol induced marked alterations in the appearance of the gap junctions such that quantification was no longer possible. From this particle-packing data and our previous thin-section data, we estimate that there are 90000 gap junctional particles per cell (within junctional plaques). The conductance of a single gap junctional channel (assuming one population) changes from 94 pS to 213 pS after hormone treatment.     

Quantitative gap junction alterations in mammalian heart cells quickly frozen or chemically fixed after electrical uncoupling

Summary The gap junction morphology was quantified in freeze-fracture replicas prepared from rat auricles that had been either quickly frozen at 6 K or chemically fixed by glutaraldehyde, in a state of normal cell-to-cell conduction or in a state of electrical uncoupling. The general appearance of the gap junctions was similar after both preparative procedures. A quantitative analysis of three gap junctional dimensions provided the following measurements in the quickly frozen conducting auricles (mean±sd): (a) P-face particles' diameter 8.27±0.74 nm (n =5709), (b) P-face particles' center-to-center distance 10.78±2.12 nm (n=4800), and (c) E-face pits' distance 9.99±2.19 nm (n=1600). Corresponding values obtained from chemically fixed tissues were decreased by about 3% for the particle's diameter and about 5% for the particles' and pits' distances. Electrical uncoupling by the action of either 1 mM 2–4-dinitrophenol (DNP), or 3.5 mMn-Heptan-1-ol (heptanol), induced a decrease of the particle's diameter, which amounted to –0.69±0.01 nm (mean ±se) in the quickly frozen preparations and –0.71±0.01 nm in the chemically fixed ones. The particles' distance was decreased by –0.96±0.04 nm in the quickly frozen samples and by –0.90 ±0.03 nm in the chemically fixed ones and the E-face pits' distance was similarly reduced. All differences were statistically significant (P<0.001 for all dimensions). Electrical recoupling after the heptanol effect promoted a return of these gap junctional dimensions towards normal values, which was about 50% complete within 20 min. It is concluded that very similar morphological alterations of the gap junctional structure are induced in the mammalian heart by different treatments promoting electrical uncoupling and that these conformational changes appear independently of the preparative procedure. The suggestion that the observed decrease of the particles' diameter is genuinely related to the closing mechanism of the unit cell-to-cell channel set in thei centers is thus confirmed.     

Keratocyte lamellipodial protrusion is characterized by a concave force-velocity relation

We report on the characterization of actin driven lamellipodial protrusion forces and velocities in keratocytes. A vertically mounted glass fiber acted as a flexible barrier positioned in front of migrating keratocytes with parallel phase contrast microscopy. A laser beam was coupled into the fiber and allowed detecting the position of the fiber by a segmented photodiode. Calibration of the fiber was carried out with the thermal oscillation method. Deflection and force signals were measured during lamellipodial protrusion. Velocity was constant during initial contact whereas loading force increased until finally the cell was stalled at higher forces. Stall forces were on the order of 2.9 ± 0.6 nN, which corresponds to a stall pressure of 2.7 ± 1.6 nN/μm². Assuming a density of actin filaments of 240 filaments per μm, we can estimate a stall force per actin filament of 1.7 ± 0.8 pN. To check for adaption of the cell against an external force, we let the cell push toward the glass fiber several times. On the timescale of the experiment (∼1 min), however, the cell did not adapt to previous loading events.     

Comparison of the structure of ribosomal 5S RNA from E. coli and from rat liver using X-ray scattering and dynamic light scattering

The structures of eukaryotic ribosomal 5S RNA from rat liver and of prokaryotic 5S RNA from E. coli (A-conformer) have been investigated by scattering methods. For both molecules, a molar mass of 44,500±4,000 was determined from small angle X-ray scattering as well as from dynamic light scattering. The shape parameters of the two rRNAs, volume V _c, surface O _c, radius of gyration R _s, maximum dimension of the molecule L, thickness D, and cross section radius of gyration R _sq, agree within the experimental error limits. The mean values are V _c=57±3 nm³, O _c=165±10 nm², R _s=3.37±0.05 nm, L=10.8±0.7 nm, D=1.57±0.07 nm, R _sa=0.92±0.01 nm.Identical structures for the E. coli 5S rRNA and the rat liver 5S rRNA at a resolution of 1 nm can be deduced from this agreement and from the comparison of experimental X-ray scattering curves and of experimental electron distance distribution function. The flat shape model derived for prokaryotic and eukaryotic 5S rRNA shows a compact region and two protruding arms. Double helical stems are eleven-fold helices with a mean base pair distance of 0.28 nm. Combining the shape information obtained from X-ray scattering with the information about the frictional behaviour of the molecules, deduced from the diffusion coefficients D _20,w ⁰ =(5.9±0.2)·10^-7 cm²s^-1 and (6.2±0.2)·10^-7 cm²s^-1 for rat liver 5S rRNA and E. coli 5S rRNA, respectively, a solvation shell of about 0.3 nm thickness around both molecules is determined. This structural similarity and the consensus secondary structure pattern derived from comparative sequence analyses suggest that all 5S rRNAs may indeed have conserved essentially the same type of folding of their polynucleotide strands during evolution, despite having very different sequences.     

Electron transfer in reaction centers of Rhodobacter sphaeroides and Rhodobacter capsulatus monitored by fluorescence of the bacteriochlorophyll dimer

Spectral and kinetic characteristics of fluorescence from isolated reaction centers of photosynthetic purple bacteria Rhodobacter sphaeroides and Rhodobacter capsulatus were measured at room temperature under rectangular shape of excitation at 810 nm. The kinetics of fluorescence at 915 nm reflected redox changes due to light and dark reactions in the donor and acceptor quinone complex of the reaction center as identified by absorption changes at 865 nm (bacteriochlorophyll dimer) and 450 nm (quinones) measured simultaneously with the fluorescence. Based on redox titration and gradual bleaching of the dimer, the yield of fluorescence from reaction centers could be separated into a time-dependent (originating from the dimer) and a constant part (coming from contaminating pigment (detached bacteriochlorin)). The origin was also confirmed by the corresponding excitation spectra of the 915 nm fluorescence. The ratio of yields of constant fluorescence over variable fluorescence was much smaller in Rhodobacter sphaeroides (0.15±0.1) than in Rhodobacter capsulatus (1.2±0.3). It was shown that the changes in fluorescence yield reflected the disappearance of the dimer and the quenching by the oxidized primary quinone. The redox changes of the secondary quinone did not have any influence on the yield but excess quinone in the solution quenched the (constant part of) fluorescence. The relative yields of fluorescence in different redox states of the reaction center were tabulated. The fluorescence of the dimer can be used as an effective tool in studies of redox reactions in reaction centers, an alternative to the measurements of absorption kinetics.Abbreviations Bchl bacteriochlorophyll - Bpheo bacteriopheophytin - D electron donor to P⁺ - P bacteriochlorophyll dimer - Q quinone acceptor - Q_A primary quinone acceptor - Q_B secondary quinone acceptor - RC reaction center protein - UQ₆ ubiquinone-30     

Cardiolipin modulates allosterically peroxynitrite detoxification by horse heart cytochrome c

Upon interaction with bovine heart cardiolipin (CL), horse heart cytochrome c (cytc) changes its tertiary structure disrupting the heme-Fe-Met80 distal bond, reduces drastically the midpoint potential out of the range required for its physiological role, binds CO and NO with high affinity, and displays peroxidase activity. Here, the effect of CL on peroxynitrite isomerization by ferric cytc (cytc-Fe(III)) is reported. In the absence of CL, hexa-coordinated cytc does not catalyze peroxynitrite isomerization. In contrast, CL facilitates cytc-Fe(III)-mediated isomerization of peroxynitrite in a dose-dependent fashion inducing the penta-coordination of the heme-Fe(III)-atom. The value of the second order rate constant for CL-cytc-Fe(III)-mediated isomerization of peroxynitrite (k_on) is (3.2 ± 0.4) × 10⁵ M⁻¹ s⁻¹. The apparent dissociation equilibrium constant for CL binding to cytc-Fe(III) is (5.1 ± 0.8) × 10⁻⁵ M. These results suggest that CL-cytc could play either pro-apoptotic or anti-apoptotic effects facilitating lipid peroxidation and scavenging of reactive nitrogen species, such as peroxynitrite, respectively.     

Further evidence from sectioned material in support of the existence of a linear terminal complex in cellulose synthesis

Summary Transmembrane linear terminal complexes considered to be involved in the synthesis of cellulose microfibrils have been described in the plasma membrane ofBoergesenia forbesii. Evidence for the existence of these structures has been obtained almost exlusively using the freeze etching technique. In the present study an attempt has been made to complete these studies using conventional fixation, staining, and sectioning procedures. In developing cells ofBoergesenia forbesii, strongly stained structures traversing the plasma membrane and averaging 598.9 nm ± 171.3 nm in length, 28.7 nm ± 4.2 nm in width, and 35.2 nm ± 6.6 nm in depth have been demonstrated. These structures are considered to be linear terminal complexes. At their distal (cell wall) surface, they appear to be closely associated with cellulose microfibrils. At the proximal (cytoplasmic) surface, they are associated with microtubules and polysomes. A model of the possible interrelation of the terminal complexes and microtubules leading to the generation of cell wall microfibrils is proposed.     

Seasonal and daily rhythms of body temperature in the European hamster (Cricetus cricetus) under semi-natural conditions

Body temperature of five European hamsters exposed to semi-natural environmental conditions at 47° N in Southern Germany was recorded over a 1.5-year period using intraperitoneal temperature-sensitive radio transmitters. The animals showed pronounced seasonal changes in body weight and reproductive status. Euthermic body temperature changed significantly throughout the year reaching its maximum of 37.9±0.2°C in April and its minimum of 36.1±0.4°C in December. Between November and March the hamsters showed regular bouts of hibernation and a few bouts of shallow torpor. During hibernation body temperature correlated with ambient temperature. Monthly means of body temperature during hibernation were highest in November (7.9±0.8°C) and March (8.2±0.5°C) and lowest in January (4.4±0.7°C). Using periodogram analysis methods, a clear diurnal rhythm of euthermic body temperature could be detected between March and August, whereas no such rhythm could be found during fall and winter. During hibernation bouts, no circadian rhythmicity was evident for body temperature apart from body temperature following ambient temperature with a time lag of 3–5 h. On average, hibernation bouts lasted 104.2±23.8 h with body temperature falling to 6.0±1.7°C. When entering hibernation the animals cooled at a rate of -0.8±0.2°C·h^-1; when arousing from hibernation they warmed at a rate of 9.9±2.4°C·h^-1. Warming rates were significantly lower in November and December than in January and February, and correlated with ambient temperature (r=-0.46, P<0.01) and hibernating body temperature (r=-0.47, P<0.01). Entry into hibrnation occured mostly in the middle of the night (mean time of day 0148 hours ±3.4 h), while spontaneous arousals were widely scattered across day and night. For all animals regression analysis revealed free-running circadian rhythms for the timing of arousal. These results suggest that entry into hibernation is either induced by environmental effects or by a circadian clock with a period of 24 h, whereas arousal from hibernation is controlled by an endogenous rhythm with a period different from 24 h.Abbreviations bw body weight - CET central European time - T _a ambient temperature - T _b body temperature - TTL transistor-transistor logic     

Investigations on the arrangement and fine structure ofPorphyridium cruentum phycobilisomes

Summary Phycobilisomes ofPorphyridium cruentum were investigated in ultrathin sectionsin situ and after isolation and positive or negative staining. The phycobilisomes have the approximate shape of one half of a compressed rotation ellipsoid with the following dimensions: length 2 a=40±4 nm, width 2 b=19±2 nm, height c=28±3 nm. The phycobilisomes form rows and pillars on the thylakoid membranes. A plug-like structure (foot) which apparently fixes the phycobilisomes to the thylakoid membrane is described.     

K+ and Ca++ in the receptor lymph of arthropod cuticular mechanoreceptors

Summary Two types of cuticular strain detectors, the campaniform sensilla on the haltere of the blowfly,Calliphora vicina, and the slit sensilla on the tibia of the spider,Cupiennius salei, were investigated. In campaniform sensilla a transepithelial voltage (43.6±10.7 mV), which depends on an intact metabolism, occurs. In spider slit sensilla no transepithelial voltage exists. The occurrence and the lack of a transepithelial voltage is paralleled with differences in the ionic composition of the receptor lymph in the two arthropod sensilla. We used double-barrelled ion-selective microelectrodes to measure potassium and calcium content in the receptor lymph with respect to the hemolymph. The potassium concentration in campaniform sensilla (121±15 mM) is five times larger than that of the wing hemolymph (25±7 mM) and nine times larger than that of the haltere hemolymph (13±3 mM). These differences are statistically significant. The calcium concentration in campaniform sensilla (0.8±0.5 mM) does not differ significantly from that of the hemolymph (1.2±0.7 mM). In spider slit sensilla no significant difference occurs between the potassium concentration of the receptor lymph (9.5 mM±5.5 mM) and that of the hemolymph (8±3 mM). The calcium concentration of the hemolymph (1.6±0.9mM) is 3 times higher than that of the receptor lymph (0.6±0.3 mM). This difference is significant.Abbreviation TEV transepithelial voltage     

Zur Kenntnis des Feinbaues der Proteinkristalle in den Zellkernen vonRivina humilis

Zusammenfassung In den Zellkernen vonRivina humilis treten bis zu zehn±stabförmige Eiweißkörper auf, die als Kristalle vorliegen. Der einzelne Körper ist entweder kompakt gebaut oder innen hohl. Das Lumen ist als ein einziger Hohlraum ausgebildet oder durch septenförmige Bildungen gegliedert.Die Kristalle sind aus ungefähr 60 Å großen,±globular erscheinenden Elementareinheiten aufgebaut, die in Gittern angeordnet sind.Die Abstände der Netzebenen liegen um 150 Å. Die Winkel sich schneidender Netzebenen variieren zwischen 60 und 70°. Demnach gehören die Kristalle offenbar dem trigonalen oder hexagonalen System an.

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Summary In the nuclei ofRivina humilis there occur up to 10±rod-like protein bodies which are present as crystals. The single body is built up compactly or its interior is hollow. The interior may be an only hollow or subdivided by septa formation.The crystals are composed of globular elements with a diameter of approximately 60 Å. They are arranged in a lattice.The distance from one lattice plane to the next amounts to 150 Å. The angles formed by two lattice planes vary from 60 to 70°. The crystals belong probably to the trigonal or hexagonal system.