[Handling of material, including paraffin-embedded specimens, for diagnosis by electron microscopy].
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Biomedical subjects
Publications and source records attributed to V Torre.
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Molecular dynamics simulations of the K+ channel from Streptomyces lividans (KcsA channel) were performed in a membrane-mimetic environment with Na+ and K+ in different initial locations. The structure of the channel remained stable and well preserved for simulations lasting up to 1.5 ns. Salt bridges between Asp80 and Arg89 of neighboring subunits, not detected in the X-ray structure, enhanced the stability of the tetrameric structure. Na+ or K+ ions located in the channel vestibule lost part of their hydration shell and diffused into the channel inner pore in less than a few hundred picoseconds. This powerful catalytic action was caused by strong electrostatic interactions with Asp80 and Glu71. The hydration state of the metal ions turned out to depend significantly on the conformational flexibility of the channel. Furthermore, Na+ entered the channel inner pore bound to more water molecules than K+. The different hydration state of the two ions may be a determinant factor in the ion selectivity of the channel.
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This paper shows that the selectivity properties of monovalent cation channels found in biological membranes can originate simply from geometrical properties of the inner core of the channel without any critical contribution from electrostatic interactions between the permeating ions and charged or polar groups. By using well-known techniques of statistical mechanics, such as the Langevin equations and Kramer theory of reaction rates, a theoretical equation is provided relating the permeability ratio PB/PA between ions A and B to simple physical properties, such as channel geometry, thermodynamics of ion hydration, and electrostatic interactions between the ion and charged (or polar) groups. Diffusive corrections and recrossing rates are also considered and evaluated. It is shown that the selectivity found in usual K+, gramicidin, Na+, cyclic nucleotide gated, and end plate channels can be explained also in the absence of any charged or polar group. If these groups are present, they significantly change the permeability ratio only if the ion at the selectivity filter is in van der Waals contact with them, otherwise these groups simply affect the channel conductance, lowering the free energy barrier of the same amount for the two ions, thus explaining why single channel conductance, as it is experimentally observed, can be very different in channels sharing the same selectivity sequence. The proposed theory also provides an estimate of channel minimum radius for K+, gramicidin, Na+, and cyclic nucleotide gated channels.
In voltage- and cyclic nucleotide-gated ion channels, the amino-acid loop that connects the S5 and S6 transmembrane domains, is a major component of the channel pore. It determines ion selectivity and participates in gating. In the alpha subunit of cyclic nucleotide-gated channels from bovine rod, the pore loop is formed by the residues R345-S371, here called R1-S27. These 24 residues were mutated one by one into a cysteine. Mutant channels were expressed in Xenopus laevis oocytes and currents were recorded from excised membrane patches. The accessibility of the substituted cysteines from both sides of the plasma membrane was tested with the thiol-specific reagents 2-aminoethyl methanethiosulfonate (MTSEA) and [2-(trimethylammonium)ethyl]methanethiosulfonate (MTSET). Residues V4C, T20C, and P22C were accessible to MTSET only from the external side of the plasma membrane, and to MTSEA from both sides of the plasma membrane. The effect of MTSEA applied to the inner side of T20C and P22C was prevented by adding 10 mM cysteine to the external side of the plasma membrane. W9C was accessible to MTSET from the internal side only. L7C residue was accessible to internal MTSET, but the inhibition was partial, approximately 50% when the MTS compound was applied in the absence of cGMP and 25% when it was applied in the presence of cGMP, suggesting that this residue is not located inside the pore lumen and that it changes its position during gating. Currents from T15C and T16C mutants were rapidly potentiated by intracellular MTSET. In T16C, a slower partial inhibition took place after the initial potentiation. Current from I17C progressively decayed in inside-out patches. The rundown was accelerated by inwardly applied MTSET. The accessibility results of MTSET indicate a well-defined topology of the channel pore in which residues between L7 and I17 are inwardly accessible, residue G18 and E19 form the narrowest section of the pore, and T20, P21, P22 and V4 are outwardly accessible.
Properties of neural computation were studied in two types of neuronal networks: isolated leech ganglia and neuronal cultures of dissociated cortical neurons from neonatal rats. With appropriate experimental set-ups it was possible to obtain a precise description of the spread of excitation induced by specific inputs. The evoked spatio-temporal electrical activity was characterized by large variability and the electrical activity of neurons activated by the same stimulation was found to be statistically independent to a high degree. The variability presumably originates from basic properties of synaptic transmission, which is stochastic in nature. As a consequence, the large variability of the evoked spatio-temporal electrical activity appears to be a general property of neural computation and a typical feature of neuronal assemblies. It is shown, however, that the observed statistical independence of co-activated neurons may be used to reduce the effects of variability by appropriately averaging or pooling the electrical activity.
Schwannoma is a rare neoplasm in the E.N.T. areas although it is characteristic of this discipline. Indeed, examination of the most recent data in the literature shows that approximately 45% of all neoplasms of the peripheral nerve linings occur in the head and neck district, the most common neurogenic tumors are schwannomas and these constitute 35% of all head and neck tumors. In reviewing the literature attention was focused on schwannomas originating in unusual sites, neglecting the most common sites originating in the eighth and seventh pair of cranial nerves. It was seen that the site of origin and clinical manifestation of these lesions varies widely and the four cases presented here are no exception. These are four schwannomas which came under observation between 1994 and 1997. The sites of origin were, respectively: the floor of the mouth, the submandibular region (corresponding to the Warthon duct), the anterior wall of the external auditory canal and the hypopharynx (corresponding to the pyriform sinus). All of these cases proved quite rare in the literature. All the cases underwent accurate anatomopathological examination and the paper discusses the particular histological and immunohistochemical features encountered. Reference is also made to the problems of differential diagnosis vs. other types of soft tissue tumors. Emphasis is placed on the demonstrated difficulty in recognizing schwannomas from the macroscopic and surgical points of view. The absence of mitoses, necroses, invasiveness and specific features--i.e. hyperchromia and pleomorphism of the nuclei or the presence of large atypical cells--are all parameters confirming that the lesions observed in the present study were benign. No anatompathological features were observed that could justify any particular expression of the schwannoma in the specific sites involved. Nevertheless, the authors present these case because a review of the literature indicated that they are extremely rare and because differential diagnosis of these unusual manifestations is so complex.
This paper presents an extensive analysis of single-channel properties of cyclic nucleotide gated (CNG) channels, obtained by injecting into Xenopus laevis oocytes the mRNA encoding for the alpha and beta subunits from bovine rods. When the alpha and beta subunits of the CNG channel are coexpressed, at least three types of channels with different properties are observed. One type of channel has well-resolved, multiple conductive levels at negative voltages, but not at positive voltages. The other two types of channel are characterized by flickering openings, but are distinguished because they have a low and a high conductance. The alpha subunit of CNG channels has a well-defined conductance of about 28 pS, but multiple conductive levels are observed in mutant channels E363D and T364M. The conductance of these open states is modulated by protons and the membrane voltage, and has an activation energy around 44 kJ/mol. The relative probability of occupying any of these open states is independent of the cGMP concentration, but depends on extracellular protons. The open probability in the presence of saturating cGMP was 0.78, 0.47, 0.5, and 0.007 in the w.t. and mutants E363D, T364M, and E363G, and its dependence on temperature indicates that the thermodynamics of the transition between the closed and open state is also affected by mutations in the pore region. These results suggest that CNG channels have different conductive levels, leading to the existence of multiple open states in homomeric channels and to the flickering behavior in heteromeric channels, and that the pore is an essential part of the gating of CNG channels.
1. Amino acids with a charged or a polar residue in the putative pore region, between lysine 346 and glutamate 372 of the alpha-subunit of the cGMP-gated channel from bovine rods were mutated to a different amino acid. The mRNA encoding for the wild-type, i.e. the alpha-subunit, or mutant channels was injected in Xenopus laevis oocytes. 2. When glutamate 363 was mutated to asparagine, serine or alanine, the current activated by a steady cGMP concentration declined in mutant channels. No current decline was observed when glutamate 363 was mutated to aspartate, glutamine or glycine, when theronine 359, 360 and 364 were mutated to alanine or when other charged residues in the pore region were neutralized. 3. The amount of current decline and its time course were significantly voltage dependent. In mutant E363A the current decline developed within about 1.5 s at -100 mV, but in about 6 s at +100 mV. In the same mutant, the current declined to about 55% of its initial level at +100 mV and to about 10% at -100 mV. 4. The current decline in mutants E363A, E363S and E363N was only moderately dependent on the cGMP concentration (from 10 to 1000 microM) and was not caused by a reduced affinity of the mutant channels for cGMP. Analysis of current fluctuations at a single-channel level indicated that current decline was primarily caused by a decrease of the open probability. 5. The wild-type channel was not permeable to dimethylammonium. When glutamate 363 was replaced by a smaller residue such as serine, mutant channels became permeable to dimethylammonium. 6. The current decline observed in mutant channels is reminiscent of desensitization of ligand-gated channels and of inactivation of voltage-gated channels. These results suggest also that gating and permeation through the cGMP-gated channel from bovine rods are intrinsically coupled and that glutamate 363 is part of the molecular structure controlling both the gating and the narrowest region of the pore.
A single ganglion of the nervous system of the leech Hirudo medicinalis was isolated. One or both roots emerging from each side of the ganglion were sucked into suction pipettes used either for extracellular stimulation or for recording the gross electrical activity. The ganglion was stained with the fluorescence voltage sensitive dye Di-4-Anepps. The fluorescence was measured with a nitrogen cooled CCD camera. Our recording system allowed us to measure in real time slow optical signals corresponding to changes in light intensity of at least 5/1000. These signals were caused by the direct polarization of neuronal structures, the afterhyperpolarization or the afterdischarge induced by a prolonged stimulation. When images were acquired at fixed times, several of them could be averaged and optical signals of at least 2/1000 could be reliably measured. These optical signals originated from well identified neurons, such as T, P and N sensory neurons. By taking images at different times and at different focal planes, electrical events could be followed at a temporal resolution of 50 Hz. The three dimensional dynamics of electrical events, initiated by a specific stimulation, was imaged and the spread of excitation among leech neurons was followed. When two roots were selectively stimulated, their neuronal interactions could be imaged and the linear and non-linear terms of the interaction could be characterized.
Native cGMP-gated channels were studied in rod outer segments of the larval tiger salamander Ambystoma tigrinum. The alpha subunit of the cGMP-gated channel from bovine rods, here referred to as the wild type (w.t.), and mutant channels were heterologously expressed in Xenopus laevis oocytes. These channels were studied in excised membrane patches in the inside-out configuration and were activated by the addition of 100 or 500 microM cGMP. The effect of temperature on the ionic permeation was studied. The macroscopic current flowing through the native channel at +100 mV had an activation energy of 35.8, 30, 31.8, 34.5, 41.3, and 22.4 kJ mol-1 in the presence of Li+, Na+, K+, Rb+, Cs+, and NH4+, respectively. The macroscopic current flowing through the w.t. channel at +100 mV had an activation energy of 45.2, 38.2, 37.5, 47.3, 49.4, and 38.9 kJ mol-1 in the presence of Li+, Na+, K+, Rb+, Cs+, and NH4+, respectively. The activation energy of the macroscopic current flowing through the native and w.t. channels did not vary significantly when the ionic concentration of the permeant ion was changed between 2.5 and 110 mM. The activation energy of the single-channel current of the w.t. channel at +100 mV was 40.4 and 33 kJ mol-1 for Na+ and NH4+, respectively. The reversal potential of biionic solutions changed significantly with temperature. These results can be used to obtain an estimate of the enthalpic and entropic contributions to the barrier of the Gibbs free energy experienced by an ion during its permeation through the open channel. These estimates indicate that the ionic permeation and selectivity of the cGMP-gated channel are controlled both by enthalpic and entropic factors and that the selectivity of the native channel for Li+ over Na+ is primarily caused by entropic effects.
1. Native cGMP-gated channels were studied in rod outer segments of the larval tiger salamander, Ambystoma tigrinum. The alpha-subunit of the cGMP-gated channel, here referred to as the wild type (WT), and mutant channels were heterologously expressed in Xenopus laevis oocytes. These channels were studied in excised membrane patches in the inside-out configuration and were activated by the addition of 100 or 500 microM cGMP. The current carried by monovalent cations was measured under voltage-clamp conditions. 2. In the presence of 110 mM Na+ in the extracellular medium and different amounts of Na+ in the intracellular medium, the I-V relations of the native channel could be described by a single-site model with a profile of Gibbs free energy with two barriers and a well. A similar result was obtained in the presence of 110 mM Li+ in the extracellular medium and different amounts of Li+ in the intracellular medium. The well depth was 1.4RT (where R is the gas constant and T is the absolute temperature) for both Li+ and Na+. 3. The I-V relations of the native channel in the presence of 110 mM Na+ on one side of the membrane and 110 mM Li+ on the other side could not be described by the same single-site model with identical values of barriers and well obtained in the presence of Li+ or Na+ alone: the well for Li+ had to be at least 4RT. 4. In the presence of mixtures of 110 mM Li+ and Cs+ on the cytoplasmic side of the membrane, an anomalous mole fraction effect was observed both in the native and the WT channel. No anomalous behaviour was seen in the presence of Li(+)-Na+ and Li(+)-NH4+ mixtures. 5. The anomalous mole fraction effect with mixtures of Li+ and Cs+ was not observed in the channel where glutamate 363 was mutated to a glutamine (E363Q) or an asparagine (E363N). When glutamate 363 was mutated to an aspartate (E363D), the anomalous mole fraction effect with mixtures of Li+ and Cs+ was still observed, although significantly reduced. 6. When lysine 346, arginine 369, aspartate 370 and glutamate 372 were neutralized by mutation to glutamine, the ion permeation through the mutant channels and the WT channel had largely similar properties.(ABSTRACT TRUNCATED AT 400 WORDS)
Many animals, especially insects, compute and use optic flow to control their motion direction and to avoid obstacles. Recent advances in computer vision have shown that an adequate optic flow can be computed from image sequences. Therefore studying whether artificial systems, such as robots, can use optic flow for similar purposes is of particular interest. Experiments are reviewed that suggest the possible use of optic flow for the navigation of a robot moving in indoor and outdoor environments. The optic flow is used to detect and localise obstacles in indoor scenes, such as corridors, offices, and laboratories. These routines are based on the computation of a reduced optic flow. The robot is usually able to avoid large obstacles such as a chair or a person. The avoidance performances of the proposed algorithm critically depend on the optomotor reaction of the robot. The optic flow can be used to understand the ego-motion in outdoor scenes, that is, to obtain information on the absolute velocity of the moving vehicle and to detect the presence of other moving objects. A critical step is the correction of the optic flow for shocks and vibrations present during image acquisition. The results obtained suggest that optic flow can be successfully used by biological and artificial systems to control their navigation. Moreover, both systems require fast and accurate optomotor reactions and need to compensate for the instability of the viewed world.
Sensory transduction shares common features in widely different sensory modalities. The purpose of this article is to examine the similarities and differences in the underlying mechanisms of transduction in the sensory receptor cells for vision, olfaction, and hearing. One of the major differences between the systems relates to the nature of the stimulus. In both the visual and olfactory systems a quantal mechanism of detection is possible, because the absorption of a photon or the binding of an odorant molecule provides an energy change significantly greater than the thermal noise in the receptor molecule. In hearing, on the other hand, the energy of a phonon is far lower, and detection occurs by a "classical" mechanism. For vertebrate photoreceptors and olfactory receptor cells, sensory transduction employs a G protein cascade that is remarkably similar in the two cases, and that is closely homologous to other G protein signaling cascades. For auditory and vestibular hair cells, transduction operates via a mechanism of direct coupling of the stimulus to ion channels, in a manner reminiscent of the direct gating of post-synaptic ion channels in various synaptic mechanisms. The three classes of sensory receptor cell share similarities in their mechanisms of adaptation, and it appears in each case that cytoplasmic calcium concentration plays a major role in adaptation.
1. Patches in the inside-out configuration were excised from the membrane of outer and inner segments of the larval tiger salamander, Ambystoma tigrinum. The current flowing through single channels opened by cyclic GMP was studied with the voltage clamp technique. 2. Amplitude histograms of current recordings from patches containing only one flickering channel, excised from the inner segment and in the presence of 100 microM cyclic GMP, could be fitted by a theoretical scheme in which the single channel conductance was at least 55 pS at +40 mV and at least 45 pS at -40 mV. The mean open time was no longer than the time constant of our recording system, about 35 microseconds. Similar results were obtained by analysis of the amplitude histograms of patches from the outer segment containing many channels, and in the presence of 1-5 microM cyclic GMP. 3. In membrane patches excised from the outer segment, reducing the temperature from 24 to 8 degrees C did not reduce the flickering, but changed the amplitude histograms of current fluctuations activated by 1 microM cyclic GMP in a way consistent with a decrease of 50% in the single channel conductance and a decrease of 50% in the open probability. 4. In the presence of 1 microM cyclic GMP at +60 mV, when Na+ was replaced by NH4+ or K+, brief outward current transients flowing through single channels were observed. When Na+ was replaced with Li+, Rb+ or Cs+, current transients were very small. 5. The shape of the power spectrum of current fluctuations induced by 1 microM cyclic GMP at +60 mV did not change when the permeating ion was Na+, K+ or NH4+. Analysis of the amplitude histogram did not show any effect of the tested monovalent cations on the open probability or on channel gating. At +60 mV, the estimated single channel currents were at least 4, 2.8 and 2 pA for NH4+, Na+ and K+ respectively. 6. The addition of 0.5 or 1 mM Ca2+ to the medium bathing the cytoplasmic side of the membrane greatly reduced the frequency of openings, but single channel activity could still be observed. The blocking effect of 1 mM Ca2+ on the channel activity induced by 2 microM cyclic GMP could be counterbalanced by increasing the cyclic GMP concentration. The addition of 0.5 or 1 mM Ca2+ did not change the shape of power spectra obtained at membrane voltages between -100 and +100 mV.(ABSTRACT TRUNCATED AT 400 WORDS)
Single-channel properties of a cloned channel activated by cyclic GMP have been analysed. The mRNA encoding for the channel was injected into oocytes of Xenopus laevis and the current flowing through a single ionic channel activated by cGMP was studied in excised patches under voltage-clamp conditions. The ionic channel activated by cGMP had a single-channel conductance of 32 +/- 2 pS at +120 mV and 25 +/- 4 pS at -120 mV, and its conductance was not significantly affected by increasing the cGMP concentration from 20 microM to 200 microM. The single-channel currents in the presence of NH+4, Na+, K+, Li+ and Rb+ in the medium bathing the cytoplasmic side of the membrane at +140 mV were 5.3, 4.7, 3.8, 1.3 and 0.8 pA, respectively. The single-channel current in the presence of Cs+ was less than 0.5 pA. Ca2+ and Mg2+ (both 0.5 mM) in the presence of 100 microM cGMP did not appreciably affect the channel activity at membrane potentials more negative than -80 mV, whereas at +100 mV they reduced the single-channel conductance by about threefold. The ionic selectivity and the blockage by divalent cations of the native channel found in amphibian rods and in the cloned channel from bovine rods are quite similar. However, the cloned channel has well-resolved openings, especially at positive membrane voltages, whereas the native channel is characterized by a continuous flickering between the open and closed state.