Melting of myosin rod as revealed by electron microscopy. I. Effects of glycerol and anions on length and stability of myosin rod

The length of the rods of intact myosin molecules and of isolated myosin rods were determined under a variety of conditions by electron microscopy. In all experiments, except for freeze-drying, the temperature and pH were kept at 20 degrees C and 7.0. Glycerol was found to have a marked effect on the stability of myosin especially for air-dried molecules. In the presence of 0.3 M of volatile buffer salts, e.g., ammonium acetate, -formate, -benzoate, -bicarbonate, -carbamate, 30 to 50% of glycerol were needed to get average lengths of myosin rods comparable to published values and to the values of freeze-dried molecules (145-149 nm). Below 10% glycerol the average length of rods was shorter by about 10 and 20 nm in intact myosin and isolated rods, respectively. Chloride caused a significant concentration-dependent shortening of myosin rods due to destabilization of the alpha-helical double coiled rod structure. Similar or higher concentrations of volatile salts, not containing chloride as an anion, had no shortening effect. Thus, subtle influences depending on the composition of the dispersion solution on the final appearance and lengths of myosin rods have to be considered, before studying temperature- and pH-dependent changes of myosin rod structure [15].     

Rabbit cardiac myosin. II. Proteolytic fragmentation with insolubilized papain.

The substructure of the cardiac myosin molecule was examined by the limited proteolytic digestion of the parent molecule with (dialdehyde starch)-methylenedianiline-mercuripapain, S-MDA-mercuripapain, at low temperatures and neutral pH, using moderate enzyme to myosin rations. Pertinent properties of the insoluble enzyme complex were also examined. Kinetic, ultracentrifugal, and chromatographic observations of the fragmentation process revealed that a single type of lytic reaction occurs during the early stages, predominately releasing heavy meromyosin subfragment 1 (HMM-S1) and myosin rods. With further time digestion, the rods are additionally cleaved yielding light meromyosin and HMM-S2, and HMM-S1 is found to be partially degraded. The major proteolytic subfragments were isolated, purified, and characterized with respect to their enzymatic, optical, amino acid, and physicochemical properties. Only HMM-S1 exhibited Ca-2+-activated ATPase activity, and at a level three- to fourfold higher than that of native myosin. Moreover, its hydrohynamic properties suggest that it is globular in structure. On the other hand, light meromyosin-A (LMM-A) (which consists mainly of rods), and HMM-S2 appear to be highly asymmetric, rigid, alpha-helical molecules devoid of the amino acid proline. Strong similarities were evident in all aspects upon comparison of these results with documented information concerning the skeletal system. On the basis of the physical and chemical properties of the proteolytic subfragments relative to that of native myosin, it was further concluded that the cardiac myosin molecule is a double-stranded, alpha-helical rod ending in tow subfragment 1 globules, of which only one may be enzymatically active at a time.     

Substructure of the myosin molecule. 3. Preparation of single-headed derivatives of myosin

Native myosin has two globular regions attached to an a-helical rod. Papain is able to cleave the globular “heads” from the rod, leading to the formation of a variety of single-headed molecules. Among these subfragments are isolated globules (HMM S-1) and single globules attached to helical rods of lengths varying from 500 to 1400 Å. These subfragments can be separated from the other products of the proteolytic digestion by salt elution from a DEAE-cellulose column. Some of the properties of single-headed heavy meromyosin and myosin have been determined by hydrodynamic methods, and shadow-cast preparations of these subfragments have been directly visualized by electron microscopy. In addition to providing further evidence for the presence of two similar halves in myosin, these new subfragments can be used in studies related to the question of why myosin has two active “heads”.     

Conformational stability of the myosin rod

Chymotryptic cleavage patterns of myosin rods from pig stomach, chicken gizzard, and rabbit skeletal muscle indicate that short (approximately 45 nm) heavy meromyosin subfragment 2 (SF2) is a consistent product of all three rods, whereas long (approximately 60 nm) SF2 is derived only from skeletal muscle myosin. Differential scanning calorimetry was used to follow the thermally induced melting transition of the rods and certain of their subfragments. In 0.12 M KCl, sodium phosphate buffer, pH 6.2-7.6, the light meromyosin (LMM) and SF2 domains of each rod had essentially identical conformational stabilities. Temperature midpoints for the melting transitions were 54-56 degrees C for the two smooth muscle myosin rods and 50-53 degrees C for the skeletal muscle myosin rod. In 0.6 M K Cl buffer, melting transitions for the smooth muscle myosin rods were essentially unchanged, but skeletal muscle myosin rods showed multiphase melting, with major transitions at 43 degrees C and 52 degrees C. The first of these was tentatively attributed to LMM, and the second to SF2. In 0.12 M K Cl buffer, the LMM transition was stabilised so that it superimposed on that of SF2. No melting was observed in any of the rods at physiological temperature. These results indicate that, excluding a possible but only narrow hinge region, the entire myosin rod has essentially uniform conformational stability at physiological pH and ionic strength, and thus that the contractile and elastic properties of the cross-bridge exist in the heavy meromyosin subfragment 1 (SF1) domains of the molecule.     

Flexibility of Acanthamoeba myosin rod minifilaments.

Previous electric birefringence experiments have shown that the actin-activated Mg2+-ATPase activity of Acanthamoeba myosin II correlates with the ability of minifilaments to cycle between flexible and stiff conformations. The cooperative transition between conformations was shown to depend on Mg2+ concentration, on ATP binding, and on the state of phosphorylation of three serines in the C-terminal end of the heavy chains. Since the junction between the heavy meromyosin (HMM) and light meromyosin (LMM) regions is expected to disrupt the alpha-helical coiled-coil structure of the rod, this region was anticipated to be the flexible site. We have now cloned and expressed the wild-type rod (residues 849-1509 of the full-length heavy chain) and rods mutated within the junction in order to test this. The sedimentation and electric birefringence properties of minifilaments formed by rods and by native myosin II are strikingly similar. In particular, the Mg2+-dependent flexible-to-stiff transitions of native myosin II and wild-type rod minifilaments are virtually superimposable. Mutations within the junction between the HMM and LMM regions of the rod modulate the ability of Mg2+ to stabilize the stiff conformation. Less Mg2+ is required to induce minifilament stiffening if proline-1244 is replaced with alanine. Deleting the entire junction region (25 amino acids) results in a even greater decrease in the Mg2+ concentration necessary for the transition. The HMM-LMM junction does indeed seem to act as a Mg2+-dependent flexible hinge.     

The myosin filament. XIII. The sensitivity of LMM assembly to Mg.ATP

An LMM fragment (Mr 62,000) of myosin has been prepared which has aggregation properties that are sensitive to the presence of Mg.ATP. Aggregation of the LMM by reducing the ionic strength in the presence of 1 mM Mg.ATP produces non-periodic aggregates which gradually rearrange to paracrystals with a 43 nm axial repeat pattern. This fragment includes the C-terminal end of the myosin rod starting at residue 1376. Therefore, at least one of the Mg.ATP binding sites responsible for this effect is located somewhere along this region of the myosin rod. Although assembly of the rod fragment of myosin into paracrystals does not show sensitivity to Mg.ATP, assembly of intact myosin molecules to form filaments does show sensitivity to Mg.ATP. For myosin filaments, assembly initially gives a broad distribution around a mean length of 1.5 microns, which sharpens around the mean length with time. The rearrangement of the LMM rods and intact myosin molecules both induced by the presence of Mg.ATP are probably related. These findings highlight the complexity of the cooperative interactions between different portions of the myosin molecule that are involved in determining the assembly properties of the intact molecule.     

The carboxyl-terminal isoforms of smooth muscle myosin heavy chain determine thick filament assembly properties.

The alternatively spliced SM1 and SM2 smooth muscle myosin heavy chains differ at their respective carboxyl termini by 43 versus 9 unique amino acids. To determine whether these tailpieces affect filament assembly, SM1 and SM2 myosins, the rod region of these myosin isoforms, and a rod with no tailpiece (tailless), were expressed in Sf 9 cells. Paracrystals formed from SM1 and SM2 rod fragments showed different modes of molecular packing, indicating that the tailpieces can influence filament structure. The SM2 rod was less able to assemble into stable filaments than either SM1 or the tailless rods. Expressed full-length SM1 and SM2 myosins showed solubility differences comparable to the rods, establishing the validity of the latter as a model for filament assembly. Formation of homodimers of SM1 and SM2 rods was favored over the heterodimer in cells coinfected with both viruses, compared with mixtures of the two heavy chains renatured in vitro. These results demonstrate for the first time that the smooth muscle myosin tailpieces differentially affect filament assembly, and suggest that homogeneous thick filaments containing SM1 or SM2 myosin could serve distinct functions within smooth muscle cells.     

Electric birefringence study of the solution structure of chymotrypsin-cleaved Acanthamoeba myosin II

After removal of the 66 COOH-terminal amino acids from each of its two heavy chains by chymotrypsin digestion, Acanthamoeba myosin II forms only parallel dimers under conditions in which native myosin II forms bipolar filaments (Kuznicki, J., Cote, G. P., Bowers, B., and Korn, E. D. (1985) J. Biol. Chem. 260, 1967-1972). We have studied the solution structure of the chymotrypsin-cleaved myosin II by electric birefringence. Only two species, known to be monomer and parallel dimer from previous studies, were detected. The contribution to the birefringence decay from dimer increased from about 10 to 70% as the KCl concentration was lowered from 100 mM to 0 in 50% glycerol. At all ionic strengths, the monomer had a relaxation time corrected to water at 20 degrees C of 8.2 microseconds, whereas a relaxation time of 10.3 microseconds was expected for monomers with straight rigid rods. This strongly indicates that the myosin rod in solution is bent. On the assumption that there is a single bend 26 nm from the tip of the tail, as suggested by electron microscopy, it was calculated that the average bend angle would be 110 degrees, in solution, if as seems most likely, the average angle between the two globular heads were 180 degrees. The observed relaxation time of the dimer corrected to water at 20 degrees C was 25 microseconds, independent of ionic strength, which, if the motion of the heads were unrestricted, is consistent with a structure for a parallel dimer in which either the two monomer subunits have straight rigid rods and are staggered by about 28 nm or only one is bent and the stagger is 30 nm. As described in the accompanying Appendix, either of these dimers can be assembled into a bipolar filament compatible with the apparent structure of filaments of native myosin II (Pollard, T.D. (1982) J. Cell Biol. 95, 816-825).     

Electric birefringence study of rabbit skeletal myosin subfragments HMM, LMM, and rod in solution.

Electric birefringence measurements and depolarized light scattering experiments were performed with HMM, LMM, and rod, the three fragments of myosin, under conditions (0.3 M KCl, 0.02 M PO4, pH 7.3) the medium currently used for biochemical assays of myosin in its native state as well as of its subfragments. The comparison of myosin and rod relaxation times (17.2 and 22.8 microseconds, respectively) suggests that the average bend angle in the tail is sharper in intact myosin (90 degrees) whereas rod, when detached from the heads, is a more elongated species with an average bend angle of 120-135 degrees. The LMM relaxation time (6.4 microseconds) is consistent with a rigid linear stick model of length 78 nm. Flexibility in myosin tail is thus confirmed as located in the HMM-LMM hinge. LMM and rod did not exhibit any significant variation of their apparent relaxation times with concentration and the decay curves were best fitted by a single exponential, evidence that the concentration of parallel staggered dimers was negligible in the concentration range studied here (0-7 g/l). This observation lends support to previous results obtained with myosin. Respective HMM, LMM, and rod molecular weights and homogeneity as evaluated by SDS-PAGE analysis were correlated to the Kerr constants of their solutions. Large variations in LMM Kerr constants could be related to the loss of a COOH-terminal peptide on prolonged chymotryptic digestion. Electric birefringence combined with depolarized light scattering is presented as a potential method for net charge distribution studies.     

Myosin and paramyosin of Caenorhabditis elegans: biochemical and structural properties of wild-type and mutant proteins.

Myosin and paramyosin have been purified from the nematode, Caenorhabditis elegans. The properties of the myosin in general resemble those of other myosins. The native molecule is a dimer of heavy (210,000 dalton) polypeptide chains and contains 18,000 and 16,000 dalton light chains. When rapidly precipitated from solution, it forms small, bipolar aggregates, about 150 nm long, consistent with the expected molecular structure of a rigid rod with a globular head region at one end. Its ATPase activity is stimulated by Ca2+ and EDTA. The myosin binds to F actin in a polar and ATP-sensitive manner, and the Mg2+-ATPase is activated by either F actin or nematode thin filaments. Dialysis of myosin to low ionic strength produces very long filaments. When a myosin-paramyosin mixture is dialyzed under the same condtions, co-filaments form which consist of a myosin cortex, surrounding a paramyosin core. Some properties of myosin from the mutants E675 and E190, which have functionally and structurally altered body wall muscles, are compared with those of wild-type myosin. These myosins of these results are discussed in terms of the myosin heavy chain composition.     

Molecular properties of rhodopsin and rod function

Signal transduction in rod cells begins with photon absorption by rhodopsin and leads to the generation of an electrical response. The response profile is determined by the molecular properties of the phototransduction components. To examine how the molecular properties of rhodopsin correlate with the rod-response profile, we have generated a knock-in mouse with rhodopsin replaced by its E122Q mutant, which exhibits properties different from those of wild-type (WT) rhodopsin. Knock-in mouse rods with E122Q rhodopsin exhibited a photosensitivity about 70% of WT. Correspondingly, their single-photon response had an amplitude about 80% of WT, and a rate of decline from peak about 1.3 times of WT. The overall 30% lower photosensitivity of mutant rods can be explained by a lower pigment photosensitivity (0.9) and the smaller single-photon response (0.8). The slower decline of the response, however, did not correlate with the 10-fold shorter lifetime of the meta-II state of E122Q rhodopsin. This shorter lifetime became evident in the recovery phase of rod cells only when arrestin was absent. Simulation analysis of the photoresponse profile indicated that the slower decline and the smaller amplitude of the single-photon response can both be explained by the shift in the meta-I/meta-II equilibrium of E122Q rhodopsin toward meta-I. The difference in meta-III lifetime between WT and E122Q mutant became obvious in the recovery phase of the dark current after moderate photobleaching of rod cells. Thus, the present study clearly reveals how the molecular properties of rhodopsin affect the amplitude, shape, and kinetics of the rod response.     

Analysis of the chicken fast myosin heavy chain family. Localization of isoform-specific antibody epitopes and regions of divergence.

cDNAs encoding the rod region of four different fast myosin heavy chains (MYCHs) in the chicken were identified, using anti-MYCH monoclonal antibodies, in two expression libraries prepared from 19-day embryonic and adult chicken muscle. These clones were used to determine the amino acid sequences that encompass the epitopes of five anti-MYHC monoclonal antibodies. Additionally, the amino acid sequences were compared to each other and to a full length embryonic MYHC. Although there is extensive homology in the chicken fast myosin rods, sequences within the hinge, within the central portion of the light meromyosin fragment, and at the carboxy terminus exhibit the largest number of amino acid substitutions. We propose that divergence within these subdomains may contribute to isoform-specific properties associated with skeletal myosin rods.     

Paramyosin gene (unc-15) of Caenorhabditis elegans. Molecular cloning, nucleotide sequence and models for thick filament structure

Paramyosin is a major structural component of thick filaments isolated from many invertebrate muscles. The Caenorhabditis elegans paramyosin gene (unc-15) was identified by screening with specific antibodies an "exon-expression" library containing lacZ/nematode gene fusions. Short probes recovered from the library were used to identify bacteriophage lambda and cosmid clones that encompass the entire paramyosin (unc-15) gene. From these clones, numerous subclones containing epitopes reacting with anti-paramyosin sera were obtained, providing strong evidence that the initial cloned fragment was, in fact, derived from the structural gene for paramyosin. The complete nucleotide sequence of a 12 x 10(3) base-pair region spanning the gene was obtained. The gene is composed of ten short exons encoding a protein of 866 [corrected] amino acid residues. Paramyosin is highly similar to residues 267 to 1089 of myosin heavy chain rods. For most of its length, paramyosin appears to form an alpha-helical coiled-coil and shows the expected heptad repeat of hydrophobic amino acid residues and the 28-residue repeat of charged amino acids characteristic of myosin heavy chain rods. However, paramyosin differs from myosin in having non-helical extensions at both the N and C termini and an additional "skip" residue that interrupts the 28-residue repeat. The distribution of charges along the length of the paramyosin rod is also significantly different from that of myosin heavy chain rods. Potential charge-mediated interactions between paramyosin rods and between paramyosin and myosin rods were calculated using a model successfully applied previously to the analysis of the myosin rod sequences. Myosin rods aligned in parallel show optimal charge-charge interactions at multiples of 98 residue staggers (i.e. at axial displacements of multiples of 143 A). Paramyosin rods, in contrast, appear to interact optimally at parallel staggers of 493 residues (i.e. at axial displacements of 720 A) but show only weak interaction peaks at 98 or 296 residues. Similar calculations suggest optimal interactions between paramyosin molecules and myosin rods and in their anti-parallel alignments. The implications of these results for the structure of the bare zone and the assembly of nematode thick filaments are discussed.     

Dynamics of the Coiled-Coil Unfolding Transition of Myosin Rod Probed by Dissipation Force Spectrum

The motor protein myosin II plays a crucial role in muscle contraction. The mechanical properties of its coiled-coil region, the myosin rod, are important for effective force transduction during muscle function. Previous studies have investigated the static elastic response of the myosin rod. However, analogous to the study of macroscopic complex fluids, how myosin will respond to physiological time-dependent loads can only be understood from its viscoelastic response. Here, we apply atomic force microscopy using a magnetically driven oscillating cantilever to measure the dissipative properties of single myosin rods that provide unique dynamical information about the coiled-coil structure as a function of force. We find that the friction constant of the single myosin rod has a highly nontrivial variation with force; in particular, the single-molecule friction constant is reduced dramatically and increases again as it passes through the coiled-uncoiled transition. This is a direct indication of a large free-energy barrier to uncoiling, which may be related to a fine-tuned dynamic mechanosignaling response to large and unexpected physiological loads. Further, from the critical force at which the minimum in friction occurs we determine the asymmetry of the bistable landscape that controls uncoiling of the coiled coil. This work highlights the sensitivity of the dissipative signal in force unfolding to dynamic molecular structure that is hidden to the elastic signal.     

Packing of myosin molecules in muscle thick filaments

The backbone of the myosin filament is an aggregate of alpha-helical coiled coil myosin rods. Its surface forms a three-stranded helix composed of myosin heads. Currently there is no adequate model to describe the organization of the myosin filament. It is proposed here that, in cross-section the light meromyosin (LMM) of 18 myosin molecules form an outer tube, with nine S2 forming the interior core. At the surface of the thick filament, myosin heads are arranged in three rows, giving the filament a periodicity of 14.3 nm per three myosin molecules. Two of these molecules are organized at an angle of 120 degrees to each other on the same level, while the third is shifted 7.2 nm along the filament axis. This packing gives a striation pattern of 7.2 nm by electron microscopy. An alternative model is also possible, in which the heads of the myosin molecules are uniformly spaced at an interval of 14.3 nm along the filament axis. The packing of individual molecules within the myosin filament is based on a regular pattern of charge on the 28 amino-acid repeat in the rod domain.     

A general method for evaluation of diffusion constants,dilute-solution viscoelasticity,and the dielectric property of a rigid macromolecule with an arbitrary configuration. I

As the first part of the study on relaxational behavior of rigid macromolecules in solution, a general method for evaluating diffusion constants of a rigid macromolecule with an arbitrary configuration in a viscous solvent is presented. The evaluation is made by modeling the molecule with a rigid assembly of Stokes spheres. The diffusion constants are expressed by a 6 × 6 matrix which consists of translational, rotational, and cross constants, each being a 3 × 3 submatrix. Procedures of numerical calculation are presented for a given configuration of the molecule, together with some exemplifying results for the rigid rod, rigid sphere, and myosin molecule. The results for the rod and the sphere are compared with analytical results.     

General model of myosin filament structure. 3. Molecular packing arrangements in myosin filaments

Following the original proposals about myosin filament structure put forward as part of a general myosin filament model (Squire, 1971, 1972) it is here shown what the most likely molecular packing arrangements within the backbones of certain myosin filaments would be assuming that the model is correct. That this is so is already indicated by recently published experimental results which have confirmed several predictions of the model (Bullard and Reedy, 1972; Reedy et al., 1972; Tregear and Squire, 1973).The starting point in the analysis of the myosin packing arrangements is the model for the myosin ribbons in vertebrate smooth muscle proposed by Small &; Squire (1972). It is shown that there is only one reasonable type of packing arrangement for the rod portions of the myosin molecules which will account for the known structure of the ribbons and which is consistent with the known properties of myosin molecules. The dominant interactions in this packing scheme are between parallel myosin molecules which are related by axial shifts of 430 Å and 720 Å. In this analysis the myosin rods are treated as uniform rods of electron density and only the general features of two-strand coiled-coil molecules are considered.Since the general myosin filament model is based on the assumption that the structures of different types of myosin filament must be closely related, the packing scheme derived for the myosin ribbons is used to deduce the structures of the main parts (excluding the bare zones) of the myosin filaments in a variety of muscles. It is shown in each case that there is only one packing scheme consistent with all the available data on these filaments and that in each filament type exactly the same interactions between myosin rods are involved. In other words the myosin-myosin interactions involved in filament formation are specific, they involve molecular shifts of either 430 Å or 720 Å, and are virtually identical in all the different myosin filaments which have been considered. Apart from the myosin ribbons, these are the filaments in vertebrate skeletal muscle, insect flight muscle and certain molluscan muscles.In the case of the thick filaments in vertebrate skeletal muscle the form of the myosin packing arrangement in the bare zone is considered and a packing scheme proposed which involves antiparallel overlaps between myosin rods of 1300 Å and 430 Å. It is shown that this scheme readily explains the triangular profiles of the myosin filaments in the bare zone (Pepe, 1967, 1971) and many other observations on the form of these myosin filaments.Finally it is shown that the cores of several different myosin filaments, assuming they contain protein, may consist of different arrangements of one or other of two types of core subfilament.     

Role of the COOH-terminal nonhelical tailpiece in the assembly of a vertebrate nonmuscle myosin rod

A short nonhelical sequence at the COOH-terminus of vertebrate nonmuscle myosin has been shown to enhance myosin filament assembly. We have analyzed the role of this sequence in chicken intestinal epithelial brush border myosin, using protein engineering/site-directed mutagenesis. Clones encoding the rod region of this myosin were isolated and sequenced. They were truncated at various restriction sites and expressed in Escherichia coli, yielding a series of mutant myosin rods with or without the COOH-terminal tailpiece and with serial deletions from their NH2-termini. Deletion of the 35 residue COOH-terminal nonhelical tailpiece was sufficient to increase the critical concentration for myosin rod assembly by 50-fold (at 150 mM NaCl, pH 7.5), whereas NH2-terminal deletions had only minor effects. The only exception was the longest NH2-terminal deletion, which reduced the rod to 119 amino acids and rendered it assembly incompetent. The COOH-terminal tailpiece could be reduced by 15 amino acids and it still efficiently promoted assembly. We also found that the tailpiece promoted assembly of both filaments and segments; assemblies which have different molecular overlaps. Rod fragments carrying the COOH-terminal tailpiece did not promote the assembly of COOH-terminally deleted material when the two were mixed together. The tailpiece sequence thus has profound effects on assembly, yet it is apparently unstructured and can be bisected without affecting its function. Taken together these observations suggest that the nonhelical tailpiece may act sterically to block an otherwise dominant but unproductive molecular interaction in the self assembly process and does not, as has been previously thought, bind to a specific target site(s) on a neighboring molecule.     

Structure of the myosin head in solution and the effect of light chain 2 removal.

Structural properties of rabbit skeletal myosin head (S1) and the influence of the DTNB light chain (LC2) on the size and shape of myosin heads in solution were investigated by small angle x-ray scattering. The LC2 deficient myosin head, S1 (-LC2), and the S1 containing LC2 light chain, S1 (+LC2) were studied in parallel. The respective values of the radius of gyration were found to be (40.2 +/- 0.5) A and (46.7 +/- 1) A, while the maximum dimension was (190 +/- 15) A for both species. The large difference between the two Rg values suggest that LC2 is located close to one extremity of the myosin head, in agreement with most electron microscopy observations. All models derived from the x-ray scattering pattern of the native myosin head share a common overall morphology, showing two main regions, an asymmetric globular portion which tapers smoothly into a thinner domain of roughly equivalent length making an angle of approximately 60 degrees, with a contour length of approximately 210 A.     

A visual pigment expressed in both rod and cone photoreceptors.

Rods and cones contain closely related but distinct G protein-coupled receptors, opsins, which have diverged to meet the differing requirements of night and day vision. Here, we provide evidence for an exception to that rule. Results from immunohistochemistry, spectrophotometry, and single-cell RT-PCR demonstrate that, in the tiger salamander, the green rods and blue-sensitive cones contain the same opsin. In contrast, the two cells express distinct G protein transducin alpha subunits: rod alpha transducin in green rods and cone alpha transducin in blue-sensitive cones. The different transducins do not appear to markedly affect photon sensitivity or response kinetics in the green rod and blue-sensitive cone. This suggests that neither the cell topology or the transducin is sufficient to differentiate the rod and the cone response.