Effect of geometrical irregularities on propagation delay in axonal trees.

Multiple successive geometrical inhomogeneities, such as extensive arborization and terminal varicosities, are usual characteristics of axons. Near such regions the velocity of the action potential (AP) changes. This study uses AXONTREE, a modeling tool developed in the companion paper for two purposes: (a) to gain insights into the consequence of these irregularities for the propagation delay along axons, and (b) to simulate the propagation of APs along a reconstructed axon from a cortical cell, taking into account information concerning the distribution of boutons (release sites) along such axons to estimate the distribution of arrival times of APs to the axons release sites. We used Hodgkin and Huxley (1952) like membrane properties at 20 degrees C. Focusing on the propagation delay which results from geometrical changes along the axon (and not from the actual diameters or length of the axon), the main results are: (a) the propagation delay at a region of a single geometrical change (a step change in axon diameter or a branch point) is in the order of a few tenths of a millisecond. This delay critically depends on the kinetics and the density of the excitable channels; (b) as a general rule, the lag imposed on the AP propagation at a region with a geometrical ratio GR greater than 1 is larger than the lead obtained at a region with a reciprocal of that GR value; (c) when the electronic distance between two successive geometrical changes (Xdis) is small, the delay is not the sum of the individual delays at each geometrical change, when isolated. When both geometrical changes are with GR greater than 1 or both with GR less than 1, this delay is supralinear (larger than the sum of individual delays). The two other combinations yield a sublinear delay; and (d) in a varicose axon, where the diameter changes frequently from thin to thick and back to thin, the propagation velocity may be slower than the velocity along a uniform axon with the thin diameter. Finally, we computed propagation delays along a morphologically characterized axon from layer V of the somatosensory cortex of the cat. This axon projects mainly to area 4 but also sends collaterals to areas 3b and 3a. The model predicts that, for this axon, areas 3a, 3b, and the proximal part of area 4 are activated approximately 2 ms before the activation of the distal part of area 4.     

THE DISTRIBUTION OF SYNAPSES ON A PHYSIOLOGICALLY IDENTIFIED MOTOR NEURON IN THE CENTRAL NERVOUS SYSTEM OF THE LEECH : An Electron Microscope Study after the Injection of the Fluorescent Dye Procion Yellow

The fine structure of a physiologically identified motor neuron in the segmental ganglion of the leech central nervous system and the morphology of synapses on it were studied after injection of the fluorescent dye Procion yellow as a marker. The injected cell and its processes within the neuropil were located in thick or thin sections with fluorescence optics after initial fixation with glutaraldehyde and brief treatment with osmium tetroxide. The same or adjacent thin sections could then be examined in the electron microscope. Comparison with uninjected cells showed that the general features of the injected cell are retained although some organelles are distorted. The main features of the geometry of this neuron are the same from animal to animal: a single large process runs from the soma through the neuropil to bifurcate and enter the contralateral roots. Within the neuropil the main process gives off long branches (up to 150 µ), but these are greatly outnumbered by short branches and spines, one or a few microns in length, which were not appreciated in previous light microscope studies after injection of Procion yellow. Serial thin sections of selected areas along the main process within the neuropil showed that there are synapses on most of the shorter branches and spines; occasional synaptic contacts were also made on the main process itself and on longer branches. At least two morphologically distinct types of synapse could be recognized. A minimum estimate of the total number of synapses on the motor cell is 300, based on their occurrence in reconstructed segments.     

Laser microbeam axotomy and conduction block show that electrical transmission at a central synapse is distributed at multiple contacts

Touch (T) sensory neurons in the leech innervate defined regions of skin and synapse on other neurons, including other T cells, within the ganglionic neuropil. The cells' receptive fields in the periphery are comprised of a central region, innervated by thick axons, and adjoining regions (minor fields) innervated by thinner axons. Secondary branches, known to be sites of synapses, emerge from the thinner and thicker axons. Pairs of T cells appear to make up to 200 separate contacts distributed within the neuropil. When the T cell is hyperpolarized, as occurs during natural stimulation of the cell, action potentials generated in the minor field and travelling into the ganglion along the thin axons may fail to conduct at central branch points. Evidence is presented, using axon conduction block and laser axotomy of cells filled with 6-carboxy-fluorescein, that synapses between separate groups of branches can function independently. Thus, selective activation of branches of the thin anterior axon produced a synaptic potential 36 +/- 6% of control amplitude, which was consistent with counts of 39 +/- 6% of contacts made by these branches. Laser axotomy of postsynaptic neurons showed that the anterior contacts indeed made the principal or only contacts activated during anterior conduction block. The results show that conduction block can modulate transmission within the ganglion, and it operates by silencing particular contacts between cells.     

Structure of multinucleated smooth muscle cells of the ascidian Halocynthia roretzi

Summary Cells isolated from ascidian smooth muscle were about 1.5–2 mm in length. Each contained 20–40 nucle in proportion to cell length. The cytoplasm was characterized by the presence of an enormous quantity of glycogen particles, tubular elements of sarcoplasmic reticulum coupled to the cell membrane, and conspicuous contractile elements. Thick and thin filaments had diameters of about 14–16 nm and 6–7 nm, respectively. The population density of the thick filaments was much higher (mean 270/m² filament area) than in vertebrate smooth muscles. The ratio of thick to thin filaments was about 16. All the thick filaments were surrounded by a single row of 5–9 thin filaments forming a rosette, and cross-bridges with periodicities of 14.5 and 29 nm were found between them. The contractile apparatus consisted of numerous myofibrils which were arranged nearly along the cell axis and were separated from each other by a network of 10-nm filaments. The myofibrils further consisted of many irregularly arranged sarcomerelike structures, each of which was comprised of a small group of thick and thin filaments with attached dense bodies.     

Changes in scleractinian coral <Emphasis Type="Italic">Seriatopora hystrix</Emphasis> morphology and its endocellular <Emphasis Type="Italic">Symbiodinium</Emphasis> characteristics along a bathymetric gradient from shallow to mesophotic reef

The algae living endosymbiotically within coral are thought to increase algal pigmentation with increasing depth to capture the diminishing light. Here, we follow distribution of the hermatypic coral Seriatopora hystrix along a 60-m bathymetric gradient in the Gulf of Eilat, Red Sea, to study coral ecophysiology and response to light regimes. Combining work on coral morphology, pigment content and genotyping of the photosymbiont, we found that total chlorophyll concentration per zooxanthellae cell and the dark- and light-acclimated quantum yield of photosystem II did not vary significantly along the 60-m gradient. However, the chlorophyll a/c ratio increased with depth. This suggests that the symbiotic algae in S. hystrix possess a mechanism for acclimatization or adaptation that differs from previously described pathways. The accepted photoacclimatory process involves an increase in chlorophyll content per alga as light intensity decreases. Based on corallite and branch morphology, this research suggests that S. hystrix has two depth-dependent ecophenotypes. Above 10 m depth, S. hystrix exhibits sturdier colony configurations with thick branches, while below 30 m depth, colonies are characterized by thin branches and the presence of a larger polyp area. Between 10 and 30 m depth, both ecophenotypes are present, suggesting that corallite morphology may act as another axis of photoacclimation with depth.     

SARCOPLASMIC RETICULUM OF AN UNUSUALLY FAST-ACTING CRUSTACEAN MUSCLE

The fast-acting, synchronous "remotor" muscle of the lobster second antenna was examined by light and electron microscopy and was found to have a more profuse sarcoplasmic reticulum (SR) than any other muscle known. Myofibrils are widely separated from one another and occupy only about one-fourth of the volume of the muscle; most of the remaining volume is taken up by the SR, which resembles the smooth-surfaced reticulum of steroid-secreting cells. Dense granules (0.03–0.1 µ in diameter) are scattered through the reticulum. T-tubules penetrate into the fibers and form dyads along the A bands of myofibrils; however, ferritin-labeling experiments show that the volume of the T-system is very small compared with that of the SR. Myofibrils are ~0.5 µ x 1.0 µ in cross section and consist of thick filaments, which appear tubular except at the M region, and thin filaments, which are situated midway between neighboring thick filaments. The ratio of thin to thick filaments is 3:1. The extreme development of the SR in this muscle is discussed in relation to the exceedingly short duration of the contraction-relaxation cycle.     

Sarcomere lattice geometry influences cooperative myosin binding in muscle

In muscle, force emerges from myosin binding with actin (forming a cross-bridge). This actomyosin binding depends upon myofilament geometry, kinetics of thin-filament Ca²⁺ activation, and kinetics of cross-bridge cycling. Binding occurs within a compliant network of protein filaments where there is mechanical coupling between myosins along the thick-filament backbone and between actin monomers along the thin filament. Such mechanical coupling precludes using ordinary differential equation models when examining the effects of lattice geometry, kinetics, or compliance on force production. This study uses two stochastically driven, spatially explicit models to predict levels of cross-bridge binding, force, thin-filament Ca²⁺ activation, and ATP utilization. One model incorporates the 2-to-1 ratio of thin to thick filaments of vertebrate striated muscle (multi-filament model), while the other comprises only one thick and one thin filament (two-filament model). Simulations comparing these models show that the multi-filament predictions of force, fractional cross-bridge binding, and cross-bridge turnover are more consistent with published experimental values. Furthermore, the values predicted by the multi-filament model are greater than those values predicted by the two-filament model. These increases are larger than the relative increase of potential inter-filament interactions in the multi-filament model versus the two-filament model. This amplification of coordinated cross-bridge binding and cycling indicates a mechanism of cooperativity that depends on sarcomere lattice geometry, specifically the ratio and arrangement of myofilaments.     

Ultrastructural diversity in motor units of crustacean stomach muscles

The physiological and ultrastructural properties of muscle fiber.s comprising three motor units in the gastric mill of blue crabs are described. In their contractile properties muscle fibers in all motor units are similar and resemble the slow type fibers in crustacean limb muscles. The majority of fibers generate large excitatory post-synaptic potentials which do not facilitate strongly. Structurally two types of fibers are found. The one type has long sarcomeres (greater than 6 mum), thin to thick myofilament ratios of 5-6:1 and diads located near the ends of the A-band. The other type has shorter sarcomeres (less than 6 mum), thin to thick myofilament ratios of 3:1 and diads located at mid sarcomere level. Both types of fibers occur within a single motor unit and this differs from the vertebrate situation. Furthermore, the finding of fibers with a low thin to thick myofilament ratio of 3:1 demonstrates that they are not exclusive to fast type crustacean muscle but also occur in slow stomach muscles.     

Structure of the cross-striated adductor muscle of the scallop

The structure of the cross-striated adductor muscle of the scallop has been studied by electron microscopy and X-ray diffraction using living relaxed, glycerol-extracted (rigor), fixed and dried muscles. The thick filaments are arranged in a hexagonal lattice whose size varies with sarcomere length so as to maintain a constant lattice volume. In the overlap region there are approximately 12 thin filaments about each thick filament and these are arranged in a partially disordered lattice similar to that found in other invertebrate muscles, giving a thin-to-thick filament ratio in this region of 6:1.The thin filaments, which contain actin and tropomyosin, are about 1 μm long and the actin subunits are arranged on a helix of pitch 2 × 38.5 nm. The thick filaments, which contain myosin and paramyosin, are about 1.76 μm long and have a backbone diameter of about 21 nm. We propose that these filaments have a core of paramyosin about 6 nm in diameter, around which the myosin molecules pack. In living relaxed muscle, the projecting myosin heads are symmetrically arranged. The data are consistent with a six-stranded helix, each strand having a pitch of 290 nm. The projections along the strands each correspond to the heads of one or two myosin molecules and occur at alternating intervals of 13 and 16 nm. In rigor muscle these projections move away from the backbone and attach to the thin filaments.In both living and dried muscle, alternate planes of thick filaments are staggered longitudinally relative to each other by about 7.2 nm. This gives rise to a body-centred orthorhombic lattice with a unit cell twice the volume of the basic filament lattice.     

Rhythmical Variations Accompanying Gustatory Stimulation Observed by Means of Localization Phenomena

When two taste stimuli are presented, one to each side of the tongue, with a time delay of up to 1 msec., the taste sensation seems to move across the tongue. This phenomenon which is similar to directional hearing, can be used to show periodic fluctuations in sensation magnitude as well as other aspects of sensation. When the apparatus was refined to present taste stimuli, it was possible to observe rhythmic changes in the perception of taste. An analogy is demonstrated between hearing and taste sensation, even to some quantitative values.     

四种类型栓皮栎栲胶含量

为了阐明不同类型(薄皮深裂、薄皮浅裂、厚皮深裂、厚皮浅裂)栓皮栎各器官栲胶含量,系统采集了秦岭南坡商州区4种类型的栓皮栎不同径级植株根、主干木材、叶片、枝条和树皮样品,用紫外光分光光度法(UV Spectrophotometry)测定了4种类型栓皮栎不同器官栲胶含量,分析了林木生长与栲胶含量的关系。结果表明,(1)4种类型栓皮栎的根、主干木材、叶片、枝条和树皮单宁含量平均值分别为2.64%—3.02%、1.74%—2.02%、6.63%—7.21%、4.69%—5.10%、8.87%—9.46%,叶片、枝条和树皮均可以作为栲胶生产主要原材料。(2)不同类型各器官单宁含量存在极显著差异(P0.01),4种类型的树皮、叶片、枝条单宁含量均表现为:厚皮深裂型厚皮浅裂型薄皮深裂型薄皮浅裂型;根部和主干木材在4种类型间单宁含量表现为:薄皮深裂型薄皮浅裂型厚皮深裂型厚皮浅裂型;厚皮深裂类型的栓皮栎是提取栲胶的最佳类型。(3)4种类型栓皮栎各器官单宁含量与胸径呈显著正相关,各器官单宁含量随着栓皮栎胸径增大而增多,并最终趋于稳定,在第Ⅳ径级(胸径20.1—25cm)时,栲胶含量均值最大。因此,栲胶生产可以高效利用第Ⅳ径级及其以上径级的栓皮栎,并对第Ⅳ径级以下栓皮栎进行定向培育和重点保护。     

THE FINE STRUCTURE OF THE VENTRAL INTERSEGMENTAL ABDOMINAL MUSCLES OF THE INSECT RHODNIUS PROLIXUS DURING THE MOLTING CYCLE : I. Muscle Structure at Molting

Rhodnius prolixus, a South American insect, molts five times in its development to an adult after emerging from the egg. Each molting cycle is triggered with a blood-meal. The ventral intersegmental abdominal muscles of Rhodnius develop during each molting cycle and are functional at molting. The fine structure of these fully developed muscles from fourth stage larval insects is studied. They have the characteristic structure of slow muscles. They have multiple motor nerve endings, and the myofibrils are poorly defined in cross-section. Longitudinal sections show long sarcomeres (8–10 µ), irregular Z-lines, and no apparent H zones. No M line is seen. Transverse sections through the A-band region show that each hexagonally arranged thick filament is surrounded by 12 thin filaments. Two thin filaments are shared by two neighboring thick filaments. The ratio of thin to thick filaments is 6:1. This structure is related to that found in vertebrate skeletal muscle and insect flight muscle.     

‘Steady/equilibrium approximation’ in relaxation and fluctuation: I. Procedure to simplify first-order reaction

A general procedure to simplify a complex first-order reaction by two approximations, the principle of fast equilibration and the steady-state approximation, is presented. Rate constants are classified into two groups: those of the order of unity and those of the order of ?(? 1) or less, and are represented in the schemes by thick and thin arrows, respectively. The fast and the slow components are defined: from the fast component at least one thick arrow originates and from the slow component no thick arrow originates. Fast components are divided into several groups. In a group, the fast components are connected by thick arrows in both directions in each reaction step. When at least one thick arrow originates from the components in a group G and terminates on a component not belonging to group G (group G is open), then the steady-state approximation or principle of fast equilibration holds on each component in group G after an induction period T°. When no thick arrow originating from group G is directed to components not belonging to group G (group G is closed), the principle of fast equilibration holds on the fast components in group G after T°. The induction period T° is less than the order of I/?.     

ELECTROMECHANICAL COUPLING IN TUBULAR MUSCLE FIBERS : I. The Organization of Tubular Muscle Fibers in the Scorpion Leiurus quinquestriatus

The tubular fibers of the claw-closer muscle of the scorpion have a central core containing nuclei and mitochondria. The myofibrils have the shape of thin lamellae (1 µ) extending radially from the core to the surface membrane (20 µ). The thick myofilaments are organized in a hexagonal array with orbits of 10–13 thin myofilaments. The ratio of thick-to-thin filaments is 1:5. Transverse tubular system (TS) openings are located between lamellated myofibrils. In each sarcomere two TS's are found, one on each side of the H band. The TS is composed of a transverse tubule and tubular pockets (TP). The TP's form diadic contact with the terminal cisternae of the sarcoplasmic reticulum. The TS can be traced from the cell membrane down to the cell core. The surface area of the TS was calculated to be six times that of the outer surface membrane.     

Morphological and physiological properties of the giant interneuron of the hermit crab (Pagurus pollicaris)

The physiological and morphological properties of the giant interneurons in the hermit crab Pagurus pollicaris are described. The cell bodies are located anteriorly in the supraesophageal ganglion, close to the mid-line. Each cell sends a neurite posteriorly and then laterally, so that they cross over in the center of the ganglion. Each axon then branches: one branch runs laterally while the other travels posteriorly and leaves the ganglion in the circumesophageal connective on the side contralateral to the cell body. The giant axons travel in the circumesophageal connectives and through the thoracic and abdominal ganglia without branching. Each giant axon makes synaptic contact with its ipsilateral giant abdominal flexor motor neuron and with a second flexor motor neuron that has its axon in the contralateral third root. In the supraesophageal ganglion there is a bidirectional synapse between the two giant interneurons. Intracellular recordings from the giant axons show that there is a delay of 0.5 to 0.75 ms that cannot be accounted for by spike propagation along the axons, and may be accounted for by a chemical synapse between the giant interneurons.     

Countercurrent multiplication may not explain the axial osmolality gradient in the outer medulla of the rat kidney

It has become widely accepted that the osmolality gradient along the corticomedullary axis of the mammalian outer medulla is generated and sustained by a process of countercurrent multiplication: active NaCl absorption from thick ascending limbs is coupled with the counterflow configuration of the descending and ascending limbs of the loops of Henle to generate an axial osmolality gradient along the outer medulla. However, aspects of anatomic structure (e.g., the physical separation of the descending limbs of short loops of Henle from contiguous ascending limbs), recent physiologic experiments (e.g., those that suggest that the thin descending limbs of short loops of Henle have a low osmotic water permeability), and mathematical modeling studies (e.g., those that predict that water-permeable descending limbs of short loops are not required for the generation of an axial osmolality gradient) suggest that countercurrent multiplication may be an incomplete, or perhaps even erroneous, explanation. We propose an alternative explanation for the axial osmolality gradient: we regard the thick limbs as NaCl sources for the surrounding interstitium, and we hypothesize that the increasing axial osmolality gradient along the outer medulla is primarily sustained by an increasing ratio, as a function of increasing medullary depth, of NaCl absorption (from thick limbs) to water absorption (from thin descending limbs of long loops of Henle and, in antidiuresis, from collecting ducts). We further hypothesize that ascending vasa recta that are external to vascular bundles will carry, toward the cortex, an absorbate that at each medullary level is hyperosmotic relative to the adjacent interstitium.     

Flight muscle differentiation in nymphs of a dragonfly Anax imperator

Flight muscle fibers of Anax imperator nymphs, in different developmental stages are analyzed for several morphological features, such as the arragnement and numerical ratio of actin and myosin filaments, the pattern of the T system and sarcoplasmic reticulum, the number of microtubules and the fractional volume of mitochondria in each fiber. The T system is initially represented by longitudinal grooves on the cell surface, joined with vesicles of the sarcoplasmic reticulum; this pattern rapidly changes and the grooves start to break up into longitudinal segments. The thin to thick filament ratio is at first quite high (about 4-4.5:1) but rapidly falls to the final (3:1) when the myofibrils are well developed at the fiber periphery. Statistical analyses show that the measured values are significantly different in the various stages of development, also indicating a progressive reduction of the ratio variability. The reduction of thin to thick filament ratio and the variance decrease fit quite well with the hypothesis that the synthesis of actin and myosin depends on independently regulated messenger RNA molecules.     

Propagation of action potentials between parallel chains of cardiac muscle cells in PSpice simulation

Propagation of action potentials between parallel chains of cardiac muscle cells was simulated using the PSpice program. Excitation was transmitted from cell to cell along a strand of three or four cells not connected by low-resistance tunnels (gap-junction connexons) in parallel with one or two similar strands. Thus, two models were used: a 2 x 3 model (two parallel chains of three cells each) and a 3 x 4 model (three parallel chains of four cells each). The entire surface membrane of each cell fired nearly simultaneously, and nearly all the propagation time was spent at the cell junctions, thus giving a staircase-shaped propagation profile. The junctional delay time between contiguous cells in a chain was about 0.2-0.5 ms. A significant negative cleft potential develops in the narrow junctional clefts, whose magnitude depends on several factors, including the radial cleft resistance (Rjc). The cleft potential (Vjc) depolarizes the postjunctional membrane to threshold by a patch-clamp action. Therefore, one mechanism for the transfer of excitation from one cell to the next is by the electric field (EF) that is generated in the junctional cleft when the prejunctional membrane fires. Propagation velocity increased with elevation of Rjc. With electrical stimulation of the first cell of the first strand (cell A1), propagation rapidly spread down that chain and then jumped to the second strand (B chain), followed by jumping to the third strand (C chain) when present. The rapidity by which the parallel chains became activated depended on the longitudinal resistance of the narrow extracellular cleft between the parallel strands (Rol2). The higher the Rol2 resistance, the faster the propagation (lower propagation time) over the cardiac muscle sheet (2-dimensional). The transverse resistance of the cleft had no effect. When the first cell of the second strand (cell B1) was stimulated, propagation spread down the B chain and jumped to the other two strands (A and C) nearly simultaneously. When cell C1 was stimulated, propagation traveled down the C chain and jumped to the B chain, followed by excitation of the A chain. Thus, there was transverse propagation of excitation as longitudinal propagation was occurring. Therefore, transmission of excitation by the EF mechanism can occur between myocardial cells lying closely parallel to one another without the requirement of a specialized junction.     

甲壳动物横纹肌的收缩蛋白质与调节机制

甲壳动物横纹肌肌原纤维的肌丝陈列,收缩蛋白质和收缩的Ca²⁺依赖性调节机制与脊椎动物横纹肌有不少差异.脊椎动物横纹肌、甲壳动物快肌与慢肌的粗丝与细丝的数量比依次为1:2,1:3和1:6,肌丝阵列各异.甲壳动物粗肌丝由肌球蛋白和副肌球蛋白组成,其分子装配与脊椎动物不同.细肌丝含有肌动蛋白、原肌球蛋白和肌钙蛋白,肌钙蛋白-T分子量较高,肌钙蛋白-C仅1个Ca²⁺结合位点.甲壳动物横纹肌兼有细肌丝调节与粗肌丝调节.     

两种类型栓皮栎软木细胞微观排列与形态特征

采用扫描电镜对秦岭北坡楼观台地区的厚皮、薄皮两种类型栓皮栎软木进行细胞微观构造观察分析,并与欧洲栓皮槠进行比较,以阐明厚皮、薄皮栓皮栎软木的相关特性,为中国栓皮栎软木的合理利用提供依据。结果表明:(1)两种类型栓皮栎软木细胞的排列结构较一致,均由内部中空的封闭型薄壁细胞紧密排列组成;在弦切面上呈蜂窝状排列,径切面和横切面上呈砖墙状排列;在径切面上,软木细胞侧高整齐地排列成行,且与树干轴向垂直;在横切面上,软木细胞侧高整齐地处于以树干轴为中心散发出来的射线上。(2)栓皮栎软木细胞大小、细胞壁和侧壁褶皱等受生长季节的影响;从软木细胞形态特征上看,厚皮类型软木细胞壁薄、细胞体积大,其软木质量优于薄皮类型。(3)与欧洲栓皮槠比较,发现厚皮类型栓皮栎早软木细胞棱柱高较小(20.6μm vs.(对比)30~40μm),软木细胞壁略厚(1.7μm vs.1~1.5μm),细胞实体积(细胞壁体积占细胞总体积比例)略大(18.75%vs.10%),厚皮类型栓皮栎软木比欧洲栓皮槠的软木质量差一些。(4)受树皮生长应力的影响,两种类型栓皮栎软木细胞侧高壁上多发生褶皱,早软木细胞褶皱严重,晚软木细胞没有褶皱,但在早晚软木交界或含有杂质处褶皱特别严重,表明厚皮类型软木细胞的侧壁褶皱程度高于薄皮类型。(5)对细胞形态特征及软木特性等的分析表明,薄皮类型栓皮栎软木质量比厚皮类型差,未来对软木资源的开发利用应更注重厚皮类型。