Fluorescence study of N-(3-pyrene)maleimide conjugated to rabbit skeletal F-actin and plasmodium actin polymers

The influence of divalent cations on the dynamic properties of actin filaments: a spectroscopic study

The principal aim of this investigation was to study the change of the protein flexibility and/or conformational properties of actin filaments upon the replacement of Ca2+ by Mg2+. The temperature dependence of the fluorescence lifetime and the anisotropy decay of N-(iodoacetyl)-N'-(5-sulfo-1-naphthyl)ethylenediamine (IAEDANS) attached covalently to the Cys374 residue of actin were measured. Saturation transfer electron paramagnetic resonance (ST-EPR) experiments were also carried out using N-(1-oxyl-2,2,6, 6-tetramethyl-4-piperidinyl)-maleimide (MSL) attached to the same residue (Cys374). The Arrhenius analysis of the temperature dependence of the fluorescence lifetimes shows that for Mg-F-actin, both the activation energy (E*) and the frequency factor (A) are smaller than they are for Ca-F-actin. The longer rotational correlation times resolved in the fluorescence experiments are larger in the Mg2+-loaded form of the actin filament between 6 degreesC and 28 degreesC, but this difference becomes negligible above 28 degreesC. The results of saturation transfer electron paramagnetic resonance measurements on maleimide spin-labeled actin filaments indicate that the replacement of Ca2+ by Mg2+ induced a decrease of the mobility of the label on the sub-millisecond time scale. Based upon these results, we concluded that the filaments polymerized from Ca-actin are more flexible than the filaments of Mg-actin.

Relationship between cellular uptake rate and chemical behavior of diammine/diaminocyclohexane platinum (II) complexes with oxygen-ligating anionic groups

The uptake kinetics of the platinum (II) complexes of the formula Pt(NH3)2X, Pt(dach)X by human erythrocyte in the plasma isotonic buffer was studied. The results showed that across-membrane transport of all the platinum complexes studied follows a first-order kinetic process. The uptake rate constants decrease with the change of oxygen-ligating anionic group in the sequence: sulfato > selenato > anion of squaric acid > oxalato > anion of demethylcantharic acid > malonato and increase with increasing lipophilicity of carrier group. The relationship between uptake rate and reactivity of these complexes was established. The stereochemistry of dach isomers was shown without effect on the reactivity and the sequence.

Torsional motion of eosin-labeled F-actin as detected in the time-resolved anisotropy decay of the probe in the sub-millisecond time range

The internal motion of F-actin in the time range from 10(-6) to 10(-3) second has been explored by measuring the transient absorption anisotropy of eosin-labeled F-actin using laser flash photolysis. The transient absorption anisotropy of eosin-F-actin at 20 degrees C has a component that decays in the submicrosecond time scale to an anisotropy of about 0.3. This anisotropy then decays with a relaxation time of about 450 microseconds to a residual anisotropy of about 0.1 after 2 ms. When the concentration of eosin-F-actin was varied in the range from 7 to 28 microM, the transient absorption anisotropy curves obtained were almost indistinguishable from each other. These results show that the anisotropy decay arises from internal motion of eosin-F-actin. Analysis of the transient absorption anisotropy curves indicates that the internal motion detected by the decay in anisotropy is primarily a twisting of actin protomers in the F-actin helix; bending of the actin filament makes a minor contribution only to the measured decay. The torsional rigidity calculated from the transient absorption anisotropy is 0.2 X 10(-17) dyn cm2 at 20 degrees C, which is about an order of magnitude smaller than the flexural rigidity determined from previous studies. Thus, we conclude that F-actin is more flexible in twisting than in bending. The calculated root-mean-square fluctuation of the torsional angle between adjacent actin protomers in the actin helix is about 4 degrees at 20 degrees C. We also found that the torsional rigidity is approximately constant in the temperature range from 5 to approximately 35 degrees C, and that the binding of phalloidin does not appreciably affect the torsional motion of F-actin.

Fluorescence spectroscopic studies of pyrene-actin adducts

Reaction kinetic studies of the sulfhydryl-directed fluorescent probes N-(1-pyrene)maleimide (PM) and N-(1-pyrenyl)iodoacetamide with actin from rabbit skeletal muscle showed that there were three accessible sulfhydryl groups in actin. Fluorescence spectral studies showed energy transfer from aromatic amino acid residues to fluorophore reacted at Cys-373, as well as weak excimer fluorescence probably due to doubly labeled molecules at Cys-10 and Cys-373. These results provide further evidence that trytophan and tyrosine residues are located near the probe attached to Cys-373 or Cys-10 and the latter two thiols are in close proximity. In age PM-labeled F-actin, the succinimido ring of PM underwent intramolecular aminolysis, resulting in large emission spectral changes and increased excimer fluorescence. Solvent perturbation studies indicate that the probes were located in a hydrophobic environment; their quantum yield and spectrum properties were very sensitive to changes in the microenvironment. Nanosecond-pulse fluorimetry studies revealed complex fluorescence emission decays with three intrinsic lifetimes in adducts with low molecular weight thiols as well as in labeled proteins. Fluorescence lifetimes were 17, 48 and 111 ns for the pyrenemaleimide adduct of actin, and 3, 14 and 60 ns for the pyrenyliodoacetamide adduct. Supporting evidence is given for the argument that multiple fluorescence lifetimes are an intrinsic property of the pyrene derivatives and are not due to the presence of impurity or heterogeneity in the protein reaction sites. Because of their high sensitivity and long lifetimes, pyrene derivatives are extremely useful.

Fluorescence photobleaching recovery in solutions of labeled actin

We have demonstrated that the technique of fluorescence photobleaching recovery (FPR) can be used to examine the state of a single component in complex self-assembling macromolecular systems. Polymerization of actin, initiated by addition of salt or Mg+2 to a low-ionic-strength solution of G-actin, has been observed by sequential measurement of FPR with the aid of fluorescein-labeled actin. Solutions of actin which had been labeled using 5-iodoacetamido fluorescein (5-IAF) showed anomalous recovery of fluorescence above the initial value, which indicates a photoinduced increase in local polymerization. No such anomaly was observed with actin that had been labeled with fluorescein isothiocyanate (FITC). The FPR data are directly interpretable in terms of the fraction of labeled protein that is immobilized in the supramolecular assembly and in terms of the average diffusion coefficient of the mobile fraction. Our data are consistent with the "treadmill" model of actin polymerization, in that they show that actin is present under polymerizing conditions either as a high polymer or as monomer or low oligomer. We believe that the FPR technique can be applied to the study of many types of reconstituted motile or cytoskeletal systems in vitro or in vivo.

Detection of actin assembly by fluorescence energy transfer

Fluorescence energy transfer was used to measure the assembly and disassembly of actin filaments. Actin was labeled at cysteine 373 with an energy donor (5-iodoacetamidofluorescein) or an energy acceptor (tetramethylrhodamine iodoacetamide or eosin iodoacetamide). Donor-labeled actin and acceptor-labeled actin were coassembled. The dependence of the transfer efficiency on the mole fraction of acceptor-labeled actin showed that the radial coordinate of the label at cysteine 373 is approximately 35 A, which means that this site is located near the outer surface of the filament. The distance between a donor and the closest acceptor in such a filament is 58 A. The increase in fluorescence after the mixing of actin filaments containing both donor and acceptor with unlabeled filaments showed that there is a slow continuous exchange of actin units. The rate of exchange was markedly accelerated when the filaments were sonicated. The rapid loss of energy transfer caused by mechanical shear probably resulted from an increase in the number of filament ends, which in turn accelerated the exchange of monomeric actin units. Energy transfer promises to be a valuable tool in characterizing the assembly and dynamics of actin and other cytoskeletal and contractile proteins in vitro and in intact cells.

Pulse-fluorometry study on actin and heavy meromyosin using F-actin labelled with N-(1-pyrene)maleimide

The single-photoelectron counting technique was used for measurement of the fluorescence decay kinetics of N-(1-pyrene)maleimide conjugated to the fast reactive cysteine of actin. The fluorescence decay curve of the labelled G-actin could not be described by a single-exponential function but by a double-exponential function. Polymerization of actin was accompanied by significant changes in the decay parameters of the two decay components. We found that the ionic strength, which plays an important role in the G-F equilibrium, scarcely affected these parameters provided that the labelled actin exists in the monomeric state. Thus it is suggested that the conformational change of actin protomer occurs at the time of association. When heavy meromyosin was added to the labelled F-actin, the decay parameter changed monotonically on increasing saturation of binding of heavy meromyosin and it levelled-off around a ratio of heavy meromyosin:actin of 0.5 mol/mol. Decay parameters under the influence of heavy meromyosin had values intermediate between those observed for the labelled G-actin and for the labelled F-actin. Therefore, it is suggested that binding of heavy meromyosin to F-actin alters the conformation of actin protomer towards that similar to G-actin.

Study of actin and its interactions with heavy meromyosin and the regulatory proteins by the pulse fluorimetry in polarized light of a fluorescent probe attached to an actin cysteine

The decay of anisotropy of the N-iodoacetyl-N'-(5-sulfo-1-naphthyl)-ethylenediamine fluorescence attached to cysteine-373 of actin can be characterized by two correlation times theta1 and theta2. theta1 has a value of several nanoseconds and is thought to represent some local protein motion. theta2 is of the order of several hundreds of nanoseconds. Its value increases with actin concentration. It represents an average of the G and F actin correlation times. When actin interacts with heavy meromyosin, theta2 increases and becomes infinite at a molar ratio of one heavy meromyosin molecule per four actin protomers. It is concluded that a definite complex is then formed between F actin and heavy meromyosin. In the same time, G actin concentration becomes equal to zero. Finally, when F actin forms a complex with the regulatory proteins tropomyosin and troponin, the value of theta2 is greater in the absence than in the presence of Ca2+. This result indicates that micromolar concentrations of Ca2+ induces a conformation change of the complex of F actin with the regulatory proteins.

Fluorescence energy transfer between epsilon-ATP at the nucleotide binding site and N-(4-dimethylamino-3,5-dinitrophenyl)-maleimide at Cys-373 of G-actin

The method of fluorescence energy transfer is used to measure the distance from the nucleotide binding site to Cys-373 of G-actin. The fluorescent ATP analogue 1-N6-ethenoadenosine 5'-triphosphate was used as donor and N-(4-dimethylamino-3,5-dinitrophenyl)-maleimide was used as acceptor. From the measurements of the efficiency of fluorescence energy transfer by both static and time resolved fluorometries, the distance between nucleotide binding site and Cys-373 residue of G-actin was calculated to be about 30 A.