Electrical responses of the marine ciliate Euplotes vannus (Hypotrichia) to mechanical stimulation at the posterior cell end

Electrical responses upon mechanostimulation at the posterior cell end were investigated in the marine hypotrichous ciliate Euplotes vannus. A new mechanostimulator was developed to mimic stimuli that are identical with those involved in cell-cell collisions. The receptor potential hyperpolarized by 18–35 mV within 12–25 msec, reached a peak value of -62 mV with a delay of 4–9 msec after membrane deformation, and was deactivated after 50–70 msec. Cirri were stimulated to beat accelerated backward. The corresponding receptor current exerted a similar time course with a peak of 2.4 nA. The shift of the reversal potential by 57.6 mV at a tenfold increase of [K⁺] ₀ identifies potassium ions as current carriers within the development of the receptor potential. An intracellular K concentration of 355 mmol/liter was calculated for cells in a medium that was composed similar to sea-water. The mechanically activated potassium current was totally inhibited by extracellular TEA and intracellular Cs⁺, and partially inhibited by extracellular 4-AP. The total inhibition of the current by injected EGTA points to a Ca dependence of the posterior mechanosensitivity. It was confirmed by the increase of the peak current amplitude with rising [Ca²⁺] ₀ . Sodium presumably repolarizes the receptor potential because the repolarization was delayed and after-depolarizations were eliminated in media without sodium. Since deciliation did not affect mechano-sensitivity, the corresponding ion channels reside within the soma membrane.The authors wish to thank Mr. Norbert Spreckelmeier from the electronics workshop and Mr. Herbert Lutter from the fine-mechanical workshop of the department for their excellent work, Mrs. G. Key and Mr. H. Mikoleit for skillful technical assistance and for preparing the figures. This work was supported by Deutsche Forschungsgemeinschaft, SFB 171, C7.     

Localization of the lampbrush loop pair Nooses on the Y chromosome of Drosophila hydei by fluorescence in situ hybridization

We have used fluorescence in situ hybridization to map the positions of the different repetitive DNA sequences from the region forming the lampbrush loop pair Nooses on the Y chromosome of Drosophila hydei. This region harbours a megabase cluster of tandemly organized repeats of the Y-specific ay1 family and a megabase cluster of tandem repeats of the related Y-specific YsI family. In addition, ay1 repeats also occur in short blocks that are interspersed by other repetitive DNA sequences that we call Y-associated, since they have additional copies on other chromosomes. Using specific probes for ay1, YsI and Y-associated DNA sequences, we show that there is one large proximal cluster of YsI repeats and one, more distally located, large cluster of ay1 repeats. The Y-chromosomal copies of the Y-associated sequences are located in the most distal part of the ay1 cluster. This is consistent with the juxtaposition of ay1 and Y-associated sequences in more than 300 kb of cloned genomic DNA. Since both ay1 and Y-associated sequences have been shown to be transcribed in the Nooses, the lampbrush loop is formed in a distal region of the short arm of the Y chromosome, adjacent to the terminally located nucleolus organizer region. The clusters of homogeneous ay1 and YsI repeats are of no functional significance for the formation of the lampbrush loop.     

Topography of the enteric nervous system in Peyer's patches of the porcine small intestine

The mechanisms of intercommunication between the immune and nervous systems are not fully understood. In the case of the intestine, the enteric nervous system is involved in the regulation of immune responses. It was therefore decided to employ immunohistochemical techniques to investigate the structural organization of the enteric nervous system in Peyer's patches of the porcine small intestine. Using antibodies against various nervous system-specific markers (protein gene product 9.5, neuron-specific enolase, neurofilament 200, S-100 protein and the glial fibrillary acidic protein), an intimate and specific structural association could be demonstrated between enteric nerves and the compartments of Peyer's patches: follicles, interfollicular regions and domes. Peyer's patches have a close topographical relationship to the two submucosal plexuses. Enteric nerves are located around the follicle in the interfollicular area — the so-called traffic area-and in the dome area, which plays an important role in the uptake and presentation of antigens.     

Pressurized gas transport in two Japanese alder species in relation to their natural habitats

Oxygen uptake measurements have shown that pressurized gas transport, resulting from the physical effect of thermo-osmosis of gases, improves oxygen supply to the roots of the seedlings in two alder speciesAlnus japonica (Thunb.) Steud. andAlnus hirsuta (Spach) Rupr., which are both native in Japan. When gas transport conditions were established by irradiation of the tree stems the internal aeration was increased to a level nearly equal to the oxygen demand of the root system in leafless seedlings ofA. hirsuta, but was higher inA. japonica so that excess oxygen was excreted into the environment. An increase of superoxide dismutase (SOD) activity, which protects plants from toxic oxygen radicals and post-anoxic injury, has been observed in root tissues ofA. japonica when the seedlings were flooded for 3 days. The increase of SOD activity, in concert with high gas transport rates, may enable this tree species to grow in wet sites characterized by low oxygen partial pressure in the soil and by varying water tables. A less effective gas transport, flood-induced reduction of SOD activity in root tissues, and reduced height growth in waterlogged soil may be responsible for the fact thatA. hirsuta is unable to inhabit wettland sites.     

Parameter des Sauerstoffverbrauches

Zusammenfassung Es wurde bei mehreren Kulturen von P. scaber die Abhängigkeit des Sauerstoffverbrauches von verschiedenen Kulturbedingungen untersucht.Ständige Haltung bei 5°C unterbindet das Einsetzen der Fortpflanzungsperiode im Frühling.In sämtlichen anderen Kulturen besteht im Herbst/Winter eine starke Proportionalität zwischen und relativem Darmgewicht, während im Frühling der der Tiere mit leerem Darm derart ansteigt, daß die Abhängigkeit des Sauerstoffverbrauches von der Darmfüllung sehr viel geringer wird. Diese Stoffwechseländerung wird höchstwahrscheinlich durch das Einsetzen von Speicher- und Aufbauprozessen vor der Gonadenreifung bewirkt.Darüber hinaus hängt das Niveau des Sauerstoffverbrauches sehr stark von äußeren Bedingungen ab. Je höher die Temperatur in der Kultur oder im Biotop vor der Messung, desto höher der durchschnittliche bei 20°C. Diese Beziehung erklärt einige der bisher als paradoxe Akklimatisation interpretierten Fälle von Temperaturabhängigkeit des Sauerstoffverbrauches in der Literatur.Unregelmäßige Beleuchtung reduziert den Sauerstoffverbrauch.Plötzliche Temperaturerhöhung (zumindest wenn sie Ende Februar geboten wird) kann die Umschaltung vom Winterstoffwechsel zum Frühlingsstoffwechsel bewirken.Abgesehen davon ist zum Einsetzen des Brutverhaltens stets das Überschreiten einer unteren Temperaturschwelle notwendig. Diese Schwelle liegt über 5°C und unter 15°C. Die erhöhte Temperatur muß jedoch mehrere Tage lang auf die Tiere einwirken, um wirksam zu sein.Ein künstlicher Langtag von 16 Stunden kann während des ganzen Jahres die Verwandlung des Winterstoffwechsels in den Frühlingsstoffwechsel herbeiführen. Ein Kurztag von 7 Stunden unterbindet diese physiologische Entwicklung. Hingegen summieren sich zwei hintereinander gebotene Kurztagperioden mit verschiedener Phase, so daß beide eine Lichtperiode von zusammen 12 Stunden ergeben, zu einer Langtagwirkung.Die Proportionalität zwischen und Darmgewicht kann in einigen Fällen gestört erscheinen, indem immer wieder Individuen auftreten (vor allem in den Kunstlichtkulturen), die bei mehr oder minder vollem Darm einen niederen aufweisen. Hieraus resultiert in gewissen Populationen eine eingipfelige Kurve, mit dem Maximum des Sauerstoffverbrauches bei Tieren mit halbgefülltem Darm, während sowohl Individuen mit leerem als auch solche mit vollem Darm einen geringeren Sauerstoffverbrauch aufweisen. Für letzteren Fall kann die Möglichkeit einer zentralen Regelung nicht ausgeschlossen werden.Die ökologische Bedeutung der Koppelung von Temperatur und Licht zur Steuerung des Stoffwechsels wird diskutiert.     

Complete subunit sequences, structure and evolution of the 6 x 6-mer hemocyanin from the common house centipede, Scutigera coleoptrata.

Hemocyanins are large oligomeric copper-containing proteins that serve for the transport of oxygen in many arthropod species. While studied in detail in the Chelicerata and Crustacea, hemocyanins had long been considered unnecessary in the Myriapoda. Here we report the complete molecular structure of the hemocyanin from the common house centipede Scutigera coleoptrata (Myriapoda: Chilopoda), as deduced from 2D-gel electrophoresis, MALDI-TOF mass spectrometry, protein and cDNA sequencing, and homology modeling. This is the first myriapod hemocyanin to be fully sequenced, and allows the investigation of hemocyanin structure-function relationship and evolution. S. coleoptrata hemocyanin is a 6 x 6-mer composed of four distinct subunit types that occur in an approximate 2 : 2 : 1 : 1 ratio and are 49.5-55.5% identical. The cDNA of a fifth, highly diverged, putative hemocyanin was identified that is not included in the native 6 x 6-mer hemocyanin. Phylogenetic analyses show that myriapod hemocyanins are monophyletic, but at least three distinct subunit types evolved before the separation of the Chilopoda and Diplopoda more than 420 million years ago. In contrast to the situation in the Crustacea and Chelicerata, the substitution rates among the myriapod hemocyanin subunits are highly variable. Phylogenetic analyses do not support a common clade of Myriapoda and Hexapoda, whereas there is evidence in favor of monophyletic Mandibulata.     

Labeling of insulin with non-radioactive I and application to incorporation of radioactive I for use in receptor-binding experiments by high-performance liquid chromatography

Conditions for the labeling of insulin with radioactive iodine isotopes were investigated by means of incorporation of non-radioactive ¹²⁷I into the peptide. Either the chloramine-T (CT) or lactoperoxidase-hydrogen peroxide (LPO) technique was applied and reversed-phase high-performance liquid chromatography (RP-HPLC) was used for analysis of the reaction products. The LPO method provided the ¹²⁷I-labeled peptide within 15–30 min, whereas the CT alternative yielded the labeled substrate even within 15 s. However, the latter reaction can only be controlled in a reproducible manner with difficulty and undesirad side-reactions became increasingly prominent when t a few seconds. In another experiment, the LPO technique was applied for radiolabeling insulin with ¹²⁵I. The product was first purified by size-exclusion chromatography (SEC) and then subjected to RP-HPLC. SEC yielded two peaks. The smaller one, which eluted at a slightly higher K_d value (accounting for about 14% of total radioactivity) predominantly consisted of material eluting at the column's void volume under the conditions of RP-HPLC, whereas the main SEC fraction (accounting for about 86% of total radioactivity) yielded a single peak, as shown by HPLC. The radioactive material attributable to the main SEC fraction revealed the expected receptor-binding properties, as evidenced by displacement experiments with non-radioactive insulin, as well as the action of tetradecanoyl phorbol acetate on the binding characteristics and thus indicating formation of a labeled hormone retaining biological activity.     

Davydov Soliton Dynamics in Proteins: II. The General Case

We performed long time simulations using the |D₁> approximation for the solution of the Davydov Hamiltonian. In addition we computed expectation values of the relevant operators with the state (_D/J)|D₁> and the deviation |> from the exact solution over long times, namely 10 ns. We found that in the very long time scale the |D₁> ansatz is very close to an exact solution, showing expectation values of the relevant physical observables in the state (_D/J)|D₁> being about 5-6 orders of magnitudes larger than in the deviation state |>. In the intermediate time scale of the ps range such errors, as known from our previous work, are somewhat larger, but still more or less negligibly. Thus we also report results from an investigation of the very short time (in the range 0-0.4 ps) behaviour of the |D₁> state compared with that of an expansion of the exact solution in powers of time t. This expansion is reliable for about 0.12 ps for special cases as shown in the previous paper. However, the accuracy of the exactly known value of the norm and the expectation value of the Hamiltonian finally indicates up to what time a given expansion is valid, as also shown in the preceding paper. The comparison of the expectation values of the operators representing the relevant physical observables, formed with the third order wave function and with the corresponding results of |D₁> simulations has shown, that our expansion is valid up to a time of roughly 0.10-0.15 ps. Within this time the second and third order corrections turned out to be not very important. This is due to the fact that our first order state contains already some terms of the expansion, summed up to inifinite order. Further we found good agreement of the results obtained with our expansion and those from the corresponding |D₁> simulations within the time of about 0.10 ps. At later times, the factors with explicit powers of t in second and third order become dominant, making the expansion meaningless. Possibilities for the use of such expansions for larger times are described. Alltogether we have shown (together with previous work on medium times), that the |D₁> state, although of approximative nature, is very close to an exact solution of the Davydov model on time scales from some femtoseconds up to nanoseconds. Especially the very small time region is of importance, because in this time a possible soliton formation from the initial excitation would start.