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Christian Altenbach

Publications and source records attributed to Christian Altenbach.

10 recordsLinked to original sources
PubMed2006

Hydrophobic loop dynamics and actin filament stability.

It has been postulated that the hydrophobic loop of actin (residues 262-274) swings out and inserts into the opposite strand in the filament, stabilizing the filament structure. Here, we analyzed the hydrophobic loop dynamics utilizing four mutants that have cysteine residues introduced at a single location along the yeast actin loop. Lateral, copper-catalyzed disulfide cross-linking of the mutant cysteine residues to the native C374 in the neighboring strand within the filament was fastest for S265C, followed by V266C, L267C, and then L269C. Site-directed spin labeling (SDSL) studies revealed that C265 lies closest to C374 within the filament, followed by C266, C267, and then C269. These results are not predicted by the Holmes extended loop model of F-actin. Furthermore, we find that disulfide cross-linking destroys L267C and L269C filaments; only small filaments are observed via electron microscopy. Conversely, phalloidin protects the L267C and L269C filaments and inhibits their disulfide cross-linking. Combined, our data indicate that, in solution, the loop resides predominantly in a "parked" position within the filament but is able to dynamically populate other conformational states which stabilize or destabilize the filament. Such states may be exploited within a cell by filament-stabilizing and -destabilizing factors.

Actin Cytoskeleton↗
PubMed2006

Conformational dynamics of loop 262-274 in G- and F-actin.

According to the original Holmes model of F-actin structure, the hydrophobic loop 262-274 stabilizes the actin filament by inserting into a pocket formed at the interface between two protomers on the opposing strand. Using a yeast actin triple mutant, L180C/L269C/C374A [(LC)(2)CA], we showed previously that locking the hydrophobic loop to the G-actin surface by a disulfide bridge prevents filament formation. We report here that the hydrophobic loop is mobile in F- as well as in G-actin, fluctuating between the extended and parked conformations. Copper-catalyzed, brief air oxidation of (LC)(2)CA F-actin on electron microscopy grids resulted in the severing of thin filaments and their conversion to amorphous aggregates. Disulfide, bis(methanethiosulfonate) (MTS), and dibromobimane (DBB) cross-linking reactions proceeded in solution at a faster rate with G- than with F-actin. Cross-linking of C180 to C269 by DBB (4.4 A) in either G- or F-actin resulted in shorter and less stable filaments. The cross-linking with a longer MTS-6 reagent (9.6 A) did not impair actin polymerization or filament structure. Myosin subfragment 1 (S1) and tropomyosin inhibited the disulfide cross-linking of phalloidin-stabilized F-actin. Electron paramagnetic resonance measurements with nitroxide spin-labeled actin revealed strong spin-spin coupling and a similar mean interspin distance ( approximately 10 A) in G- and in F-actin, with a broader distance distribution in G-actin. These results show loop 262-274 fluctuations in G- and F-actin and correlate loop dynamics with actin filament formation and stability.

Actin Cytoskeleton↗
PubMed2006

Conformational states and dynamics of rhodopsin in micelles and bilayers.

Nitroxide sensors were placed in rhodopsin at sites 140, 227, 250, and 316 to monitor the dynamics and conformation of the receptor at the cytoplasmic surface in solutions of dodecyl maltoside (DM), digitonin, and phospholipid bilayers of two compositions. The EPR spectra reveal a remarkable similarity of rhodopsin structure and the activating conformational change in DM and bilayers, the hallmark of which is an outward tilt of transmembrane helix VI. This conformational change is blocked in solutions of digitonin, although changes in optical absorbance accompany activation, showing that absorbance and structural changes are not necessarily coupled. In DM and bilayers, the receptor is apparently in equilibrium between conformational substates whose populations are modulated by activation. Despite the general similarity in the two environments, the receptor conformations have increased flexibility in DM relative to bilayers. For the activated receptor in DM and bilayers, a pH-dependent conformational equilibrium is identified that may correspond to the optically characterized MII(a)()-MII(b)() equilibrium. No specific effects of headgroup composition on receptor conformation in lipid bilayers were found.

Amino Acid Substitution↗
PubMed2005

Accessibility and dynamics of nitroxide side chains in T4 lysozyme measured by saturation recovery EPR.

Long pulse saturation recovery electron paramagnetic resonance spectroscopy is applied to the investigation of spin-labeled side chains placed along a regular helix extending from 128 to 135 in T4 lysozyme. Under an argon atmosphere, analysis of the exponential saturation recovery curves gives the spin-lattice relaxation rates of the nitroxides, which depend on the nitroxide side-chain dynamics. In the presence of the fast-relaxing paramagnetic reagents O(2) or NiEDDA, global analysis of the saturation recovery provides the spin-lattice relaxation rates as well as the Heisenberg exchange rates of the nitroxide with the reagents. As previously shown with power saturation methods, such exchange rates are direct measures of the solvent accessibility of the nitroxide side chains in the protein structure. The periodic dependence of the spin-lattice relaxation rates and the exchange rates along the 128-135 sequence reveal the presence of the helical structure, demonstrating the use of these parameters in structure determination. In general, multiple exponentials are required to fit the saturation recovery data, thus identifying multiple states of the side chain. In one case, multiple conformations detected in the spectrum are not evident in the saturation recovery, suggesting rapid exchange on the timescale of spin-lattice relaxation.

Argon↗
PubMed2005

Accessibility of nitroxide side chains: absolute Heisenberg exchange rates from power saturation EPR.

In site-directed spin labeling, the relative solvent accessibility of spin-labeled side chains is taken to be proportional to the Heisenberg exchange rate (W(ex)) of the nitroxide with a paramagnetic reagent in solution. In turn, relative values of W(ex) are determined by continuous wave power saturation methods and expressed as a proportional and dimensionless parameter Pi. In the experiments presented here, NiEDDA is characterized as a paramagnetic reagent for solvent accessibility studies, and it is shown that absolute values of W(ex) can be determined from Pi, and that the proportionality constant relating them is independent of the paramagnetic reagent and mobility of the nitroxide. Based on absolute exchange rates, an accessibility factor is defined (0 < rho < 1) that serves as a quantitative measure of side-chain solvent accessibility. The accessibility factors for a nitroxide side chain at 14 different sites in T4 lysozyme are shown to correlate with a structure-based accessibility parameter derived from the crystal structure of the protein. These results provide a useful means for relating crystallographic and site-directed spin labeling data, and hence comparing crystal and solution structures.

Bacteriophage T4↗
PubMed2004

Structural origins of constitutive activation in rhodopsin: Role of the K296/E113 salt bridge.

The intramolecular interactions that stabilize the inactive conformation of rhodopsin are of primary importance in elucidating the mechanism of activation of this and other G protein-coupled receptors. In the present study, site-directed spin labeling is used to explore the role of a buried salt bridge between the protonated Schiff base at K296 in TM7 and its counterion at E113 in TM3. Spin-label sensors are placed at positions in the cytoplasmic surface of rhodopsin to monitor changes in the structure of the helix bundle caused by point mutations that disrupt the salt bridge. The single point mutations E113Q, G90D, and A292E, which were previously reported to cause constitutive activation of the apoprotein opsin, are found to cause profound movements of both TM3 and TM6 in the dark state, the latter of which is similar to that caused by light activation. The mutant M257Y, which constitutively activates opsin but does not disrupt the salt bridge, is shown to cause related but distinguishable structural changes. The double mutants E113Q/M257Y and G90D/M257Y produce strong activation of the receptor in the dark state. In the E113Q/M257Y mutant investigated with spin labeling, the movement of TM6 and other changes are exaggerated relative to either E113Q or M257Y alone. Collectively, the results provide structural evidence that the salt bridge is a key constraint maintaining the resting state of the receptor, and that the disruption of the salt bridge is the cause, rather than a consequence, of the TM6 motion that occurs upon activation.

Animals↗
PubMed2002

A model for the structure of the Escherichia coli SOS-regulated UmuD2 protein.

The ubiquitous Y-family of DNA polymerases, exemplified by the Escherichia coli UmuC protein (the catalytic subunit of DNA Pol V), possess the remarkable ability to replicate imperfect DNA templates that cannot be replicated by other types of DNA polymerases. Since this ability comes at the cost of a reduced fidelity, it is important that organisms manage these unique polymerases to coordinate their actions with those of the replication machinery. In E. coli, it is becoming evident that a sophisticated series of protein-protein interactions involving the two forms of the umuD gene product, UmuD and UmuD' and components of the replicative DNA polymerase serve to manage the actions of the umuC-encoded DNA polymerase. The purpose of this study was to better understand how structural differences between UmuD2 and UmuD2' help to determine which biological role the umuDC gene products will play; the UmuD2C complex functions as a DNA damage checkpoint effector, while the UmuD2'C complex participates in translesion DNA synthesis, which serves as the mechanistic basis for most chemical and UV light mutagenesis. Based on the results of a combination of disulfide cross-linking experiments, measurements of solvent accessibility and electron paramagnetic spin resonance (EPR) studies, we have developed a refined model for the structure of the UmuD2 homodimer. In the model that we are proposing, the N-terminal arms of UmuD (residues 1-39) form an extended interface in the UmuD2 homodimer by folding down over the globular domains of their intradimer partners. As a result, significant portions of the surface of each globular domain are buried in the UmuD2 homodimer. Based on the structure of the UmuD2' homodimer, both in the crystal and in solution, these same surfaces are exposed. Implications of these structural differences between the UmuD2 and the UmuD2' homodimers with respect to their roles in managing the actions of the umuC-encoded DNA polymerase are discussed.

Binding Sites↗
PubMed2002

Arrangement of subunits and ordering of beta-strands in an amyloid sheet.

Amyloid fibrils are associated with several disease states, but their structures have yet to be fully defined. Here we use site-directed spin labeling to explain some of the specific interactions that are formed between subunits when the protein transthyretin (TTR) assembles into amyloid fibrils, which are associated with both spontaneous and familial amyloid diseases in humans. The results suggest that fibrils are formed when a major conformational change displaces the terminal beta-strand from the edge of a beta-sheet in the native structure, exposing the penultimate strand. The newly exposed strand then allows a novel beta-sheet interaction to form between the TTR subunits. This interaction and another previously identified subunit association lead to a plausible model for the specific sequence of beta-strands in one of the indefinitely repeating beta-sheets of TTR amyloid, which is formed by a head-to-head, tail-to-tail arrangement of subunits.

Amyloid↗
PubMed2002

Site-directed spin labeling of a bacterial chemoreceptor reveals a dynamic, loosely packed transmembrane domain.

We used site-directed spin labeling and electron paramagnetic resonance spectroscopy to investigate dynamics and helical packing in the four-helix transmembrane domain of the homodimeric bacterial chemoreceptor Trg. We focused on the first transmembrane helix, TM1, particularly on the nine-residue sequence nearest the periplasm, because patterns of disulfide formation between introduced cysteines had identified that segment as the region of closest approach among neighboring transmembrane helices. Along this sequence, mobility and accessibility of the introduced spin label were characteristic of loosely packed or solvent-exposed side chains. This was also the case for eight additional positions around the circumference and along the length of TM1. For the continuous nine-residue sequence near the periplasm, mobility and accessibility varied only modestly as a function of position. We conclude that side chains of TM1 that face the interior of the four-helix domain interact with neighboring helices but dynamic movement results in loose packing. Compared to transmembrane segments of other membrane proteins reconstituted into lipid bilayers and characterized by site-directed spin labeling, TM1 of chemoreceptor Trg is the most dynamic and loosely packed. A dynamic, loosely packed chemoreceptor domain can account for many experimental observations about the transmembrane domains of chemoreceptors.

Diffusion↗