MEMBRANE AND PROTOPLASM RESISTANCE IN THE SQUID GIANT AXON

The direct current longitudinal resistance of the squid giant axon was measured as a function of the electrode separation. Large sea water electrodes were used and the inter-electrode length was immersed in oil. The slope of the resistance vs. separation curve is large for a small electrode separation, but becomes smaller and finally constant as the separation is increased. An analysis of the resistance vs. length curves gives the following results. The nerve membrane has a resistance of about 1000 ohm cm.² The protoplasm has a specific resistance of about 1.4 times that of sea water. The resistance of the connective tissue sheath outside the fiber corresponds to a layer of sea water about 20µ in thickness. The characteristic length for the axon is about 2.3 mm. in oil and 6.0 mm. in sea water.     

ACETYLCHOLINE CONTENT OF THE SCHWANN CELL AND AXON IN THE GIANT NERVE FIBRE OF THE SQUID

Abstract— Acetylcholine and choline were identified and their concentrations measured, by means of gas chromatography/mass spectrometry, in extracts obtained from nerve fibers of the hindmost stellar nerve of the squid Sepioteuthis sepioidea. These compounds were quantitated in samples of stellar nerve devoid of giant fiber, intact giant nerve fiber, extruded axoplasm, and axoplasm-free giant nerve fiber sheaths. In 11 samples of stellar nerve devoid of giant fiber, weighing an average of 20.8 ± 2.3 mg ( s.e.m. ), 756 ± 91 pmol ACh and 8.65 ± 0.62 nmol of choline were found. The total ACh content of the largest fibre in this group (10 μ m in diameter), for a 5 cm length of nerve, is in the order of 0.16 pmol. The average wet weights of a single giant nerve fiber (270-420 μ m in diameter) and its separate components ( s.e.m .; in mg; number of fibers in parentheses) were: intact fiber, 4.58 ± 0.19 (25); extruded axoplasm, 3.38 ± 0.13 (20); sheaths, 1.21 ± 0.11 (16). The average ACh content per unit weight of sample was about 2-3 times higher in the sheaths (5-13 pmol-mg⁻¹) than in the axoplasm (2-4 pmol mg⁻¹), whereas the ACh concentrations estimated per unit volume of cellular water were about 40 times higher in the Schwann cell (107-222 μ m ) than in the axon (2-5 μ m ). These experimental findings establish the presence of ACh in the giant nerve fiber of S. sepioidea. They also indicate the Schwann cells themselves as the main source for the release of ACh, responsible for their long-lasting hyperpolarizations following the conduction of nerve impulse trains by the axon.     

ELECTRIC IMPEDANCE OF THE SQUID GIANT AXON DURING ACTIVITY

Alternating current impedance measurements have been made over a wide frequency range on the giant axon from the stellar nerve of the squid, Loligo pealii, during the passage of a nerve impulse. The transverse impedance was measured between narrow electrodes on either side of the axon with a Wheatstone bridge having an amplifier and cathode ray oscillograph for detector. When the bridge was balanced, the resting axon gave a narrow line on the oscillograph screen as a sweep circuit moved the spot across. As an impulse passed between impedance electrodes after the axon had been stimulated at one end, the oscillograph line first broadened into a band, indicating a bridge unbalance, and then narrowed down to balance during recovery. From measurements made during the passage of the impulse and appropriate analysis, it was found that the membrane phase angle was unchanged, the membrane capacity decreased about 2 per cent, while the membrane conductance fell from a resting value of 1000 ohm cm.² to an average of 25 ohm cm.² The onset of the resistance change occurs somewhat after the start of the monophasic action potential, but coincides quite closely with the point of inflection on the rising phase, where the membrane current reverses in direction, corresponding to a decrease in the membrane electromotive force. This E.M.F. and the conductance are closely associated properties of the membrane, and their sudden changes constitute, or are due to, the activity which is responsible for the all-or-none law and the initiation and propagation of the nerve impulse. These results correspond to those previously found for Nitella and lead us to expect similar phenomena in other nerve fibers.     

MEMBRANE POTENTIAL OF THE SQUID GIANT AXON DURING CURRENT FLOW

The squid giant axon was placed in a shallow narrow trough and current was sent in at two electrodes in opposite sides of the trough and out at a third electrode several centimeters away. The potential difference across the membrane was measured between an inside fine capillary electrode with its tip in the axoplasm between the pair of polarizing electrodes, and an outside capillary electrode with its tip flush with the surface of one polarizing electrode. The initial transient was roughly exponential at the anode make and damped oscillatory at the sub-threshold cathode make with the action potential arising from the first maximum when threshold was reached. The constant change of membrane potential, after the initial transient, was measured as a function of the total polarizing current and from these data the membrane potential is obtained as a function of the membrane current density. The absolute value of the resting membrane resistance approached at low polarizing currents is about 23 ohm cm.². This low value is considered to be a result of the puncture of the axon. The membrane was found to be an excellent rectifier with a ratio of about one hundred between the high resistance at the anode and the low resistance at the cathode for the current range investigated. On the assumption that the membrane conductance is a measure of its ion permeability, these experiments show an increase of ion permeability under a cathode and a decrease under an anode.     

TRANSVERSE IMPEDANCE OF THE SQUID GIANT AXON DURING CURRENT FLOW

The change in the transverse impedance of the squid giant axon caused by direct current flow has been measured at frequencies from 1 kc. per second to 500 kc. per second. The impedance change is equivalent to an increase of membrane conductance at the cathode to a maximum value approximately the same as that obtained during activity and a decrease at the anode to a minimum not far from zero. There is no evidence of appreciable membrane capacity change in either case. It then follows that the membrane has the electrical characteristics of a rectifier. Interpreting the membrane conductance as a measure of ion permeability, this permeability is increased at the cathode and decreased at the anode.     

CALCIUM-CONTAINING ELECTRON-DENSE STRUCTURES IN THE AXONS OF THE SQUID GIANT SYNAPSE

Following the Oschman and Wall technique, electron-dense structures (EDS) were found on unstained, unosmicated membranes of squid giant synapse axons. These densities contain high concentrations of calcium and phosphorus as identified by energy dispersive X-ray analysis. Based on the signal strength, the quantity is significantly greater than that of other regions of the membrane or tissue spaces. The calcium EDS occur as plaques or globules along the axonic membrane, and small globules are found between sheath cell processes. EDS also occur at the synaptic site. These densities were correlated with the opacity change seen in giant axons. It is proposed that these structures represent sites where the calcium-binding protein found by other investigators has become nearly saturated with calcium.     

PROTEIN DEGRADATION IN SQUID GIANT AXONS

Axoplasm extruded from giant axons of the Chilean squid, Dosidicus gigas, contained a low level of neutral proteinase-like activity, equivalent to 4 × 10^?6 mg of chymotrypsin per mg of axoplasmic protein. The enzyme was active at physiological pH and ionic strength. Activity was completely inhibited by 1 mM-para-hydroxymercuribenzoate and was enhanced by divalent metal cations, especially Ca²⁺. Axoplasm also exhibited proteinase activity at pH 4.8. Both neutral and acid proteinase like activities were also present in the axonal sheath containing Schwann cells, but their specific activities relative to those in the axoplasm were different. A physiological role, related to the axoplasmic flow of protein, is discussed for the axoplasmic neutral proteinase-like activity.     

ASSOCIATION OF CALCIUM WITH MEMBRANES OF SQUID GIANT AXON : Ultrastructure and Microprobe Analysis

Giant axons from the squid, Loligo pealei, were fixed in glutaraldehyde and postfixed in osmium tetroxide. Calcium chloride (5 mM/liter) was added to all aqueous solutions used for tissue processing. Electron-opaque deposits were found along the axonal plasma membranes, within mitochondria, and along the basal plasma membranes of Schwann cells. X-ray microprobe analysis (EMMA-4) yielded signals for calcium and phosphorus when deposits were probed, whereas these elements were not detected in the axoplasm.     

THE SYNTHESIS OF CHOLINE PHOSPHOGLYCERIDES IN THE GIANT FIBRE SYSTEM OF THE SQUID

The mechanisms and pathways of synthesis of phosphatidylcholine in the giant fibre system of the squid (Loligo vulgaris) have been examined by incubating the stellate ganglion-nerve preparation or its separated compartments in an artificial bathing solution with labelled choline. Other experiments were done by dissecting the whole stellate ganglion into axoplasm, axon sheath, giant fibre lobe, small fibres and ganglion residue, after incubation. The initial rate of choline incorporation into choline phosphoglycerides was severalfold higher in the lobe than in the axon. Higher lipid radioactivity was recovered in the axon sheath as compared to the axoplasm, and in the small fibres as compared to the ganglion residue which contains its cell bodies. The production of phosphorylcholine and CDP-choline in the intact ganglion-nerve preparation during incubation with choline points to the occurrence of the net synthesis pathway for phosphatidylcholine in this material. Base-exchange activity was also observed in the axon and giant fibre lobe preparations in vitro, but no indication can yet be given whether it also takes place in intact preparations. Electrical stimulation and‘depolarizing’conditions enhance choline phosphorylation in the squid axon and lobe, but decrease phosphatidylcholine labelling.     

SITE OF BIOSYNTHESIS OF BRAIN-SPECIFIC PROTEINS IN THE GIANT FIBRE SYSTEM OF THE SQUID

The synthesis of brain-specific proteins has been examined in perikaryal and axonal regions of the giant fibre system of the squid. After in vitro incubation of stellate ganglia, stellate nerves and isolated giant axons with radioactive amino acids, the labelled soluble proteins have been extracted from the giant fibre lobe, the axoplasm and the axonal sheath of the giant axon and have been separated by gel electrophoresis on a continuous system. In addition, they have been challenged with antisera prepared against the cephalopod brain-specific proteins L1 and L2 and the resulting precipitate has been resolved by sodium dodecyl sulphate-gel electrophoresis. Synthesis of these two proteins appears to be restricted to the giant fibre lobe, while an additional discrete protein band (L5) also becomes clearly labelled in the isolated giant axon. Radioactive components migrating in the region of the L1 and L2 proteins are synthesized in the isolated giant axon. They can be distinguished from tbese proteins on the basis of electrophoretic and immunochemical criteria.     

INCORPORATION OF LABELLED PHOSPHATE INTO PHOSPHOLIPIDS IN SQUID GIANT AXONS

Inorganic phosphate labelled with ³²P was applied to giant axons excised from squid (Loligo pealeii) by addition of ³²Pi to the bathing solution, by injection into the axon, or by addition to axoplasm which had been separated from the sheath. The preparations were kept at 10 to 25° for various times up to 4 hr. When ³²P_i was supplied by way of the bathing solution, axoplasm and sheath were usually separated at the end of incubation before extraction of the lipids. Lipids were extracted with chloroform-methanol and resolved by paper chromatography. The lipids which became labelled appeared to be the same in sheath and axoplasm. They were identified by cochromatography with known lipids and by chromatography of products formed from them by mild alkaline hydrolysis. They included phosphatidylinositol, phosphatidylethanolamine, phosphatidic acid, and probably somelysophosphatidylethanolamine. Some labelled components remained unidentified. Phosphatidylcholine was apparently present, but did not become significantly labelled either in sheath or in axoplasm, or in a squid's stellate ganglion. There was no evidence that separation from the sheath impaired the capacity of the axoplasm for lipid synthesis.     

IDENTIFICATION OF A CALCIUM-BINDING, BRAIN SPECIFIC PROTEIN IN THE AXOPLASM OF SQUID GIANT AXONS

Abstract— An acidic protein has been isolated from the optic lobes of two cephalopods, Sepia officinalis and Loligo vulgaris. The protein has been obtained in pure form by fractionation with ammonium sulphate and chromatography on DEAE-cellulose and Sephadex G 100. Its apparent molecular weight is 13,000–15,000. Glutamic and aspartic acids account for 35 per cent of the amino acid residues. The protein binds Ca²⁺ ions with an apparent dissociation constant of 2·5 × 10⁻⁵ M at physiological concentrations of KCI. Antibodies have been prepared against the protein purified from Sepia officinalis. By the micro-complement fixation technique it has been shown that the protein is highly concentrated in the nervous system of cephalopods and that the amount in the axoplasm of squid giant axons is eight to nine-fold higher than in the optic lobes of the same animal.     

THE AXON HILLOCK AND THE INITIAL SEGMENT

Axon hillocks and initial segments have been recognized and studied in electron micrographs of a wide variety of neurons. In all multipolar neurons the fine structure of the initial segment has the same pattern, whether or not the axon is ensheathed in myelin. The internal structure of the initial segment is characterized by three special features: (a) a dense layer of finely granular material undercoating the plasma membrane, (b) scattered clusters of ribosomes, and (c) fascicles of microtubules. A similar undercoating occurs beneath the plasma membrane of myelinated axons at nodes of Ranvier. The ribosomes are not organized into Nissl bodies and are too sparsely distributed to produce basophilia. They vanish at the end of the initial segment. Fascicles of microtubules occur only in the axon hillock and initial segment and nowhere else in the neuron. Therefore, they are the principal identifying mark. Some speculations are presented on the relation between these special structural features and the special function of the initial segment.     

CONFIGURATION OF A FILAMENTOUS NETWORK IN THE AXOPLASM OF THE SQUID (LOLIGO PEALII L.) GIANT NERVE FIBER

High-resolution electron microscopy is integrated with physicochemical methods in order to investigate the following preparations of the giant nerve fibers of the squid (Loligo pealii L.): (1) Thin sections of fibers fixed in four different fixatives; (2) fresh axoplasm stained negatively in solutions of different pH and composition; (3) chemically isolated threadlike elements of the axoplasm. A continuous, three-dimensional network can be identified in all these preparations of the axoplasm. The network is composed of coiled or looped unit-filaments ~30 A wide. The unit-filaments are intercoiled in strands ~ 70–250 A wide. The strands are oriented longitudinally in the axoplasm, often having a sinuous course and cross-associations. Microtubules are surrounded by intercoiled unit-filaments and filamentous strands. Calcium ions cause loosening and disintegration of the network configuration. UO₂⁺⁺ ions of a 1% uranyl acetate solution at pH 4.4 display a specific affinity for filamentous protein structures of the squid giant nerve fiber axoplasm, segregating the filamentous elements of the axoplasm in a coiled, threadlike preparation. The uranyl ions combine probably with the carboxyl groups of the main amino acids of the protein—glutamic and aspartic acids. It is proposed that by coiling/decoiling and folding/unfolding of the unit-filaments, shifts in physicochemical properties of the axoplasm are maintained.     

POTENTIAL,IMPEDANCE, AND RECTIFICATION IN MEMBRANES

Impedance and potential measurements have been made on a number of artificial membranes. Impedance changes were determined as functions of current and of the composition of the environmental solutions. It was shown that rectification is present in asymmetrical systems and that it increases with the membrane potential. The behavior in pairs of solutions of the same salt at different concentrations has formed the basis for the studies although a few experiments with different salts at the same concentrations gave results consistent with the conclusions drawn. A theoretical picture has been presented based on the use of the general kinetic equations for ion motion under the influence of diffusion and electrical forces and on a consideration of possible membrane structures. The equations have been solved for two very simple cases; one based on the assumption of microscopic electroneutrality, and the other on the assumption of a constant electric field. The latter was found to give better results than the former in interpreting the data on potentials and rectification, showing agreement, however, of the right order of magnitude only. Although the indications are that a careful treatment of boundary conditions may result in better agreement with experiment, no attempt has been made to carry this through since the data now available are not sufficiently complete or reproducible. Applications of the second theoretical case to the squid giant axon have been made showing qualitative agreement with the rectification properties and very good agreement with the membrane potential data.     

ACTION OF POTASSIUM AND NARCOTICS ON RECTIFICATION IN NERVE AND MUSCLE

Electrical rectification was demonstrated in whole sartorius muscle and sciatic nerve of Rana pipiens and also in the single giant nerve fiber of the northern squid, Ommastrephes illecibrossus. It is probably a property of the plasma membrane. Rectification decreases reversibly under the influence of increased concentrations of the potassium ion and with chloroform, veratrine sulfate and isoamyl carbamate. No effect was found with lack of calcium, excess calcium, or barium chloride. Decrease in rectification is invariably accompanied by simultaneous decrease in resting potential. A proposed explanation of the mechanism of rectification is discussed. Rectification in a living membrane, viz. a change in resistance with change in direction of current flow, may possibly be explained in terms of a change in the concentration of potassium ions in the membrane.