In vitro assays demonstrate that pollen tube organelles use kinesin-related motor proteins to move along microtubules

The movement of pollen tube organelles relies on cytoskeletal elements. Although the movement of organelles along actin filaments in the pollen tube has been studied widely and is becoming progressively clear, it remains unclear what role microtubules play. Many uncertainties about the role of microtubules in the active transport of pollen tube organelles and/or in the control of this process remain to be resolved. In an effort to determine if organelles are capable of moving along microtubules in the absence of actin, we extracted organelles from tobacco pollen tubes and analyzed their ability to move along in vitro-polymerized microtubules under different experimental conditions. Regardless of their size, the organelles moved at different rates along microtubules in the presence of ATP. Cytochalasin D did not inhibit organelle movement, indicating that actin filaments are not required for organelle transport in our assay. The movement of organelles was cytosol independent, which suggests that soluble factors are not necessary for the organelle movement to occur and that microtubule-based motor proteins are present on the organelle surface. By washing organelles with KI, it was possible to release proteins capable of gliding carboxylated beads along microtubules. Several membrane fractions, which were separated by Suc density gradient centrifugation, showed microtubule-based movement. Proteins were extracted by KI treatment from the most active organelle fraction and then analyzed with an ATP-sensitive microtubule binding assay. Proteins isolated by the selective binding to microtubules were tested for the ability to glide microtubules in the in vitro motility assay, for the presence of microtubule-stimulated ATPase activity, and for cross-reactivity with anti-kinesin antibodies. We identified and characterized a 105-kD organelle-associated motor protein that is functionally, biochemically, and immunologically related to kinesin. This work provides clear evidence that the movement of pollen tube organelles is not just actin based; rather, they show a microtubule-based motion as well. This unexpected finding suggests new insights into the use of pollen tube microtubules, which could be used for short-range transport, as actin filaments are in animal cells.     

Single microtubules from squid axoplasm support bidirectional movement of organelles

Single filaments, dissociated from the extruded axoplasm of the squid giant axon and visualized by video-enhanced differential interference contrast microscopy, transport organelles bidirectionally. Organelles moving in the same or opposite directions along the same filament can pass each other without colliding, indicating that each transport filament has several tracks for organelle movement. In order to characterize transport filaments, organelle movements were first examined by video microscopy, and then the same filaments were examined by electron microscopy after rapid-freezing, freeze-drying, and rotary-shadowing. Transport filaments that supported bidirectional movement of organelles are 22 nm to 27 nm in diameter and have a substructure indicative of a single microtubule. Immunofluorescence showed that virtually all transport filaments contain tubulin. These results show that single microtubules can serve as a substratum for organelle movement, and suggest that an interaction between organelles and microtubules is the basis of fast axonal transport.     

Bundling of microtubules in vitro by a high molecular weight protein prepared from the squid axon

A high molecular weight protein has been partially purified from sheaths of squid giant axons. This protein fraction was capable of restoring the membrane excitability of the squid axon which had been destroyed by internal perfusion of microtubule poison, when perfused along with microtubule proteins (Matsumoto et al. (1979) J. Biochem. 86, 1155-1158). This protein, designated as 260 K protein, was purified by gel filtration and Con A-Sepharose affinity chromatography. The apparent molecular weight of the axonal protein was estimated to be 260,000 by electrophoresis in the presence of sodium dodecylsulfate. This protein was revealed to be a glycoprotein. When phosphocellulose-purified tubulin was incubated with 260 K protein at 36 degrees C in the presence of dimethylsulfoxide, turbidity of the solution was much increased. 260 K protein co-sedimented with microtubles assembled from purified tubulin. Light microscopic and electron microscopic observations revealed that the high turbidity was due to bundling of microtubules which was caused by 260 K protein. On the other hand, the effect of this protein on the turbidity increase was not so prominent when microtubules were assembled from microtubule proteins consisting of tubulin and microtubule-associated proteins. High shear and low shear viscometry and co-sedimentation experiments revealed that 260 K protein had little effect on actin polymerization under the same medium conditions as used in tubulin polymerization.     

Movement of organelles along filaments dissociated from the axoplasm of the squid giant axon

Cytoplasmic filaments, separated from the axoplasm of the squid giant axon and visualized by video-enhanced differential interference contrast microscopy, support the directed movement of organelles in the presence of ATP. All organelles, regardless of size, move continuously along isolated transport filaments at 2.2 +/- 0.2 micron/sec. In the intact axoplasm, however, movements of the larger organelles are slow and saltatory. These movements may reflect a resistance to movement imposed by the intact axoplasm. The uniform rate of all organelles along isolated transport filaments suggests that a single type of molecular motor powers fast axonal transport. Organelles can attach to and move along more than one filament at a time, suggesting that organelles have multiple binding sites for this motor.     

Plus-end motors override minus-end motors during transport of squid axon vesicles on microtubules

Plus- and minus-end vesicle populations from squid axoplasm were isolated from each other by selective extraction of the minus-end vesicle motor followed by 5'-adenylyl imidodiphosphate (AMP-PNP)- induced microtubule affinity purification of the plus-end vesicles. In the presence of cytosol containing both plus- and minus-end motors, the isolated populations moved strictly in opposite directions along microtubules in vitro. Remarkably, when treated with trypsin before incubation with cytosol, purified plus-end vesicles moved exclusively to microtubule minus ends instead of moving in the normal plus-end direction. This reversal in the direction of movement of trypsinized plus-end vesicles, in light of further observation that cytosol promotes primarily minus-end movement of liposomes, suggests that the machinery for cytoplasmic dynein-driven, minus-end vesicle movement can establish a functional interaction with the lipid bilayers of both vesicle populations. The additional finding that kinesin overrides cytoplasmic dynein when both are bound to bead surfaces indicates that the direction of vesicle movement could be regulated simply by the presence or absence of a tightly bound, plus-end kinesin motor; being processive and tightly bound, the kinesin motor would override the activity of cytoplasmic dynein because the latter is weakly bound to vesicles and less processive. In support of this model, it was found that (a) only plus-end vesicles copurified with tightly bound kinesin motors; and (b) both plus- and minus-end vesicles bound cytoplasmic dynein from cytosol.     

Neurofilament protein is phosphorylated in the squid giant axon

We have observed the phosphorylation of neurofilament protein from squid axoplasm. Phosphorylation is demonstrated by 32P labeling of protein during incubation of axoplasm with [gamma-32P]ATP. When the labeled proteins are separated by SDS-polyacrylamide gel electrophoresis (SDS-PAGE), two bands, at 2.0 x 10(5) daltons and greater than 4 x 10(5) daltons, contain the bulk of the 32P. The 2.0 x 10(5)-dalton phosphorylated polypeptide comigrates on SDS-PAGE with one of the subunits of squid neurofilament protein. Both major phosphorylated polypeptides co-fractionate with neurofilaments in discontinuous sucrose gradient centrifugation and on gel filtration chromatography on Sepharose 4B. The protein-phosphate bond behaves like a phospho-ester, and labeled phospho-serine is identified in an acid hydrolysate of the protein. The generality of this phenomenon in various species and its possible physiological significance are discussed.     

Kinesin-3 is an organelle motor in the squid giant axon

Conventional kinesin (Kinesin-1), the founding member of the kinesin family, was discovered in the squid giant axon, where it is thought to move organelles on microtubules. In this study, we identify a second squid kinesin by searching an expressed sequence tag database derived from the ganglia that give rise to the axon. The full-length open reading frame encodes a 1753 amino acid sequence that classifies this protein as a Kinesin-3. Immunoblots demonstrate that this kinesin, unlike Kinesin-1, is highly enriched in chaotropically stripped axoplasmic organelles, and immunogold electron microscopy (EM) demonstrates that Kinesin-3 is tightly bound to the surfaces of these organelles. Video microscopy shows that movements of purified organelles on microtubules are blocked, but organelles remain attached, in the presence Kinesin-3 antibody. Immunogold EM of axoplasmic spreads with antibody to Kinesin-3 decorates discrete sites on many, but not all, free organelles and localizes Kinesin-3 to organelle/microtubule interfaces. In contrast, label for Kinesin-1 decorates microtubules but not organelles. The presence of Kinesin-3 on purified organelles, the ability of an antibody to block their movements along microtubules, the tight association of Kinesin-3 with motile organelles and its distribution at the interface between native organelles and microtubules suggest that Kinesin-3 is a dominant motor in the axon for unidirectional movement of organelles along microtubules.     

Binding of radioactively labeled saxitoxin to the squid giant axon

Summary The binding of saxitoxin, a specific inhibitor of the sodium conductance in excitable membranes, has been measured in giant axons from the squid,Loligo pealei. Binding was studied by labeling saxitoxin with tritium, using a solvent-exchange technique, and measuring the toxin uptake by liquid scintillation counting. Total toxin binding is the sum of a saturable, hyperbolic binding component, with a dissociation constant at 2–4°C of 4.3±1.7nm (meanse), and a linear, nonsaturable component. The density of saturable binding sites is 166±20.4 m^–2. From this density and published values of the maximum sodium conductance, the conductance per toxin site is estimated to be about 7 pS, assuming sequential activation and inactivation processes (F. Bezanilla & C.M. Armstrong, 1977,J. Gen. Physiol. 70: 549). This single site conductance value of 7 pS is in close agreement with estimates of the conductance of one open sodium channel from measurements of gating currents and of noise on squid giant axons, and is consistent with the hypothesis that one saxitoxin molecule binds to one sodium channel.     

On the binding of labelled saxitoxin to the squid giant axon

Measurement of the maximum saturable binding capacity for 3H-labelled saxitoxin in well cleaned giant axons from Loligo forbesi gave a value of 290 +/- 65 (s.e.m.) binding sites per square micrometre of membrane. In samples of the fin nerve the total saturable uptake was 12.4 +/- 2.4 fmol mg-1 wet mass, corresponding to 94 sites per square micrometre for fibres whose mean diameter after fixation and embedding was estimated as 16 micron.     

Currents related to the sodium-calcium exchange in squid giant axon

We report the measurement of a Cai-activated membrane current in dialyzed squid axon under membrane potential control with a low-noise voltage clamp. Two additional voltage clamp systems were used to clamp the external guard plates to a value that prevented the establishment of potential differences between the central and lateral compartments of the experimental chamber. This reduced to a minimum the contribution of membrane currents generated at the axon ends to the current measured in the central pool. This latter current was reduced by using internal and external solutions designed to diminish at a maximum membrane currents, while maintaining the conditions for optimal operation of the Na+-Ca2+ exchange. Thus TTX was used to block Na+ channels and prolonged exposure to K+-free media was used to eliminate K+ conductance. The maximum concentration of external sodium was 200 mM. The addition of fixed amounts of free ionic calcium to the internal solution, activated a current whose direction and magnitude depended on the thermodynamic driving forces for calcium and sodium. When the experimental conditions determined an inwardly directed current, this depended on the presence of external sodium, and lithium could not substitute for it. The Cai-activated current, was blocked by external lanthanum and showed a high temperature dependence. In experiments in which the reversal potential was measured for the Cai-activated current, it was found to be strikingly similar to the value calculated according to Er = 3ENa - 2ECa, suggesting that the current is the electrical manifestation of the Na+-Ca2+ exchange operating with an stoichiometry of 3Na+:1Ca2+.     

Individual microtubules in the axon consist of domains that differ in both composition and stability

We have explored the composition and stability properties of individual microtubules (MTs) in the axons of cultured sympathetic neurons. Using morphometric means to quantify the MT mass remaining in axons after various times in 2 micrograms/ml nocodazole, we observed that approximately 48% of the MT mass in the axon is labile, depolymerizing with a t1/2 of approximately 5 min, whereas the remaining 52% of the MT mass is stable, depolymerizing with a t1/2 of approximately 240 min. Immunofluorescence analyses show that the labile MTs in the axon are rich in tyrosinated alpha-tubulin, whereas the stable MTs contain little or no tyrosinated alpha-tubulin and are instead rich in posttranslationally detyrosinated and acetylated alpha-tubulin. These results were confirmed quantitatively by immunoelectron microscopic analyses of the distribution of tyrosinated alpha-tubulin among axonal MTs. Individual MT profiles were typically either uniformly labeled for tyrosinated alpha-tubulin all along their length, or were completely unlabeled. Roughly 48% of the MT mass was tyrosinated, approximately 52% was detyrosinated, and approximately 85% of the tyrosinated MTs were depleted within 15 min of nocodazole treatment. Thus, the proportion of MT profiles that were either tyrosinated or detyrosinated corresponded precisely with the proportion of MTs that were either labile or stable respectively. We also observed MT profiles that were densely labeled for tyrosinated alpha-tubulin at one end but completely unlabeled at the other end. In all of these latter cases, the tyrosinated, and therefore labile domain, was situated at the plus end of the MT, whereas the detyrosinated, and therefore stable domain was situated at the minus end of the MT, and in each case there was an abrupt transition between the two domains. Based on the frequency with which these latter MT profiles were observed, we estimate that minimally 40% of the MTs in the axon are composite, consisting of a stable detyrosinated domain in direct continuity with a labile tyrosinated domain. The extreme drug sensitivity of the labile domains suggests that they are very dynamic, turning over rapidly within the axon. The direct continuity between the labile and stable domains indicates that labile MTs assemble directly from stable MTs. We propose that stable MTs act as MT nucleating structures that spatially regulate MT dynamics in the axon.     

Fluorescence of squid axon membrane labelled with hydrophobic probes

Summary Extrinsic fluorescence changes in squid giant axons were examined under a variety of experimental conditions using 2-p-toluidinylnaphthalene-6-sulfonate (TNS) and other fluorescent probes. Measurements of the degree of polarization of the fluorescent light (with the axis of the polarizer parallel to the longitudinal axis of the axon) indicated that the class of the TNS molecules in the axon membrane which participate in production of fluorescence signals have a definite orientation with their absorption and emission oscillators directed parallel to the long axis of the axon. Rectangular depolarizing voltage pulses produced a transient decrease in the fluorescent intensity, of which the early component is correlated tentatively with the rise in the membrane conductance. In response to hyperpolarizing pulses, there was an increase in fluorescence intensity which may be explained in terms of increased incorporation of TNS into the ordered structure in the membrane. Hyperpolarizing responses in KCl depolarized axons were accompanied by a change in fluorescent intensity. Tetrodotoxin appeared to suppress the initial component of the fluorescence signal produced by depolarizing clamping pulses. The technique for detecting these fluorescence changes and the physico-chemical properties of TNS are described in some detail.     

Interaction of n-alkylguanidines with the sodium channels of squid axon membrane

The effects of n-alkylguanidine derivatives on sodium channel conductance were measured in voltage clamped, internally perfused squid giant axons. After destruction of the sodium inactivation mechanism by internal pronase treatment, internal application of n-amylguanidine (0.5 mM) or n-octylguanidine (0.03 mM) caused a time-dependent block of sodium channels. No time-dependent block was observed with shorter chain derivatives. No change in the rising phase of sodium current was seen and the block of steady-state sodium current was independent of the membrane potential. In axons with intact sodium inactivation, an apparent facilitation of inactivation was observed after application of either n-amylguanidine or n-octylguanidine. These results can be explained by a model in which alkylguanidines enter and occlude open sodium channels from inside the membrane with voltage-independent rate constants. Alkylguanidine block bears a close resemblance to natural sodium inactivation. This might be explained by the fact that alkylguanidines are related to arginine, which has a guanidino group and is thought to be an essential amino acid in the molecular mechanism of sodium inactivation. A strong correlation between alkyl chain length and blocking potency was found, suggesting that a hydrophobic binding site exists near the inner mouth of the sodium channel.     

Interaction of deoxycholate with the sodium channel of squid axon membranes

Deoxycholate can react with sodium channels with a high potency. The apparent dissociation constant for the saturable binding reaction is 2 microM at 8 degrees C, and the heat of reaction is approximately -7 kcal/mol. Four independent test with Na-free media, K-free media, tetrodotoxin, and pancuronium unequivocally indicate that it is the sodium channel that is affected by deoxycholate. Upon depolarization of the membrane, the drug modified channel exhibits a slowly activating and noninactivating sodium conductance. The kinetic pattern of the modified channel was studied by increasing deoxycholate concentration, lowering the temperature, chemical elimination of sodium inactivation, or conditioning depolarization. The slow activation of the modified channel can be represented by a single exponential function with the time constant of 1--5 ms. The modified channel is inactivated only partially with a time constant of 1 S. The reversal potential is unchanged by the drug. Observations in tail currents and the voltage dependence of activation suggest that the activation gate is actually unaffected. The apparently slow activation may reflect an interaction betweem deoxycholate and the sodium channel in resting state.     

Light scattering spectroscopy of the squid axon membrane

Light scattering studies on the giant squid axon were done using the technique of optical mixing spectroscopy. This experimental approach is based on the use of laser light to detect the fluctuations of membrane macromolecules which are associated with conductance fluctuations. The light scattering spectra were similar to the Lorentzian-like behavior of conductance fluctuations, possibly reflecting an underlying conformational change in the specific membrane sites responsible for the potassium ion conductance. The amplitude of the spectra measured, increased when the membrane was depolarized and decreased on hyperpolarization. The spectra were fit to the sum of two terms, a (1/fcomponent and a simple Lorentzian term. Spectra from deteriorating axons did not show sensitivity to membrane potential changes. It is shown theoretically that fluctuations due to the voltage-dependent variable, n, of the Hodgkin-Huxley formalism are identical to the voltage fluctuations. The derived power spectrum is that of a second order system, capable of showing resonance peaking only if the voltage dependence of the potassium rate constants is included in the analysis. The lack of resonance peaking in the observed light scattering spectra, indicates that the data are best described by a damped second order system.     

Differential growth of the branches of a regenerating bifurcate axon is associated with differential axonal transport of organelles

Axonal trees display differential growth during development or regeneration; that is, some branches stop growing and often retract while other branches continue to grow and form stable synaptic connections. In this study, an in vitro model of differential growth is examined to identify the intracellular events responsible for this phenomenon. When the giant cerebral neuron of Aplysia californica is placed in culture, vigorous growth occurs from the ends of both branches of its bifurcate axon. If an appropriate target neuron is placed next to one branch, growth from that branch is unabated while growth from the other branch is suppressed. The bidirectional fast transport of membranous organelles was examined in the two branches by the use of high-resolution video microscopy. Transport was similar in the branches in the absence of a target cell but was much greater in the growing than in the nongrowing branch when a target was present. Electron microscopic examination of fixed specimens confirmed these findings. Differential growth may be initiated or sustained by a diversion from certain branches of materials used in growth which are supplied by fast axonal transport.