A model for processive movement of single-headed myosin-IX

Dynamics of ATP-dependent and ATP-independent steppings of myosin-V on actin: catch-bond characteristics

An analytical theory is presented for the dynamics of myosin-V molecular motor, where both ATP-dependent and ATP-independent steppings are taken into account. Specifically, the dependences of velocity, run length and unbinding rate upon both forward and backward loads and ATP concentration are studied, explaining quantitatively the diverse available single-molecule data and providing predicted results. The results show that the unbinding rate increases with the increase of ATP concentration and levels off at both low and high ATP concentrations. More interestingly, at an ATP concentration that is not very low, the unbinding rate exhibits characteristics of a catch-slip bond under backward load, with the unbinding rate decreasing rapidly with the increase of the backward load in the range smaller than about 2.5 pN and then increasing slowly with the further increase of the backward load. By contrast, under forward load the unbinding rate exhibits a slip-bond characteristic.

Class IX Myosins: Motorized RhoGAP Signaling Molecules

Class IX myosins are simultaneously motor and signaling molecules. In addition to myosin class-specific functions of the tail region, they feature unique motor properties. Within their motor region they contain a long insertion with a calmodulin- and a F-actin-binding site. The rate-limiting step in the ATPase cycle is ATP hydrolysis rather than, typical for other myosins, the release of either product. This means that class IX myosins spend a large fraction of their cycle time in the ATP-bound state, which is typically a low F-actin affinity state. Nevertheless, class IX myosins in the ATP-bound state stochastically switch between a low and a high F-actin affinity state. Single motor domains even show characteristics of processive movement towards the plus end of actin filaments. The insertion thereby acts as an actin tether. The motor domain transports as intramolecular cargo a signaling Rho GTPase-activating protein domain located in the tail region. Rho GTPase-activating proteins catalyze the conversion of active GTP-bound Rho to inactive GDP-bound Rho by stimulating GTP hydrolysis. In cells, Rho activity regulates actin cytoskeleton organization and actomyosin II contractility. Thus, class IX myosins regulate cell morphology, cell migration, cell-cell junctions and membrane trafficking. These cellular functions affect embryonic development, adult organ homeostasis and immune responses. Human diseases associated with mutations in the two class IX myosins, Myo9a and Myo9b, have been identified, including hydrocephalus and congenital myasthenic syndrome in connection with Myo9a and autoimmune diseases in connection with Myo9b.

A model for the chemomechanical coupling of myosin-V molecular motors

Herein, a model for the chemomechanical coupling of dimeric myosin-V motors is presented. Based on this model and the proposal that the rate constants of the ATPase activity of the two heads are independent of an external force in a range smaller than the stall force, we analytically studied the dynamics of the motor, such as the stepping ratio, dwell time between two mechanical steps, and velocity, under varying force and ATP concentrations. The theoretical results well reproduce the diverse available single-molecule experimental data. In particular, the experimental data showing that at a low ATP concentration, the dwell time and velocity have less force dependency than at a high ATP concentration is explained quantitatively. Moreover, the dependency of the chemomechanical coupling ratio on the force and ATP concentration was studied.

The paper presents a model of chemomechanical coupling of myosin-V motor, explaining the dynamics under varying force and ATP concentrations.

Investigating role of conformational changes of microtubule in regulating its binding affinity to kinesin by all-atom molecular dynamics simulation

Changes of affinity of kinesin head to microtubule regulated by changes in the nucleotide state are essential to processive movement of kinesin on microtubule. Here, using all-atom molecular dynamics simulations we show that besides the nucleotide state, large conformational changes of microtubule-tubulin heterodimers induced by strong interaction with the head in strongly binding state are also indispensable to regulate the affinity of the head to the tubulin. In strongly binding state the high affinity of the head to microtubule arises largely from mutual conformational changes of the microtubule and head induced by the specific interaction between them via an induced-fit mechanism. Moreover, the ADP-head has a much weaker affinity to the local microtubule-tubulin, whose conformation is largely altered by the interaction with the head in strongly binding state, than to other unperturbed tubulins. This indicates that upon Pi release the ADP-head temporarily has a much weaker affinity to the local tubulin than to other tubulins.

A model of processive movement of dimeric kinesin

Dimeric kinesin can move processively on microtubule filaments by hydrolyzing ATP. Diverse aspects of its movement dynamics have been studied extensively by using various experimental methods. However, the detailed molecular mechanism of the processive movement is still undetermined and a model that can provide a consistent and quantitative explanation of the diverse experimental data is still lacking. Here, we present such a model, with which we study the movement dynamics of the dimer under variations of solution viscosity, external load, ATP concentration, neck linker length, effect of neck linker docking, effect of a large-size particle attached to one kinesin head, etc., providing consistent and quantitative explanations of the available diverse experimental data. Moreover, predicted results are also provided.

Ankyrin domain of myosin 16 influences motor function and decreases protein phosphatase catalytic activity

The unconventional myosin 16 (Myo16), which may have a role in regulation of cell cycle and cell proliferation, can be found in both the nucleus and the cytoplasm. It has a unique, eight ankyrin repeat containing pre-motor domain, the so-called ankyrin domain (My16Ank). Ankyrin repeats are present in several other proteins, e.g., in the regulatory subunit (MYPT1) of the myosin phosphatase holoenzyme, which binds to the protein phosphatase-1 catalytic subunit (PP1c). My16Ank shows sequence similarity to MYPT1. In this work, the interactions of recombinant and isolated My16Ank were examined in vitro. To test the effects of My16Ank on myosin motor function, we used skeletal muscle myosin or nonmuscle myosin 2B. The results showed that My16Ank bound to skeletal muscle myosin (K D ≈ 2.4 µM) and the actin-activated ATPase activity of heavy meromyosin (HMM) was increased in the presence of My16Ank, suggesting that the ankyrin domain can modulate myosin motor activity. My16Ank showed no direct interaction with either globular or filamentous actin. We found, using a surface plasmon resonance-based binding technique, that My16Ank bound to PP1cα (K D ≈ 540 nM) and also to PP1cδ (K D ≈ 600 nM) and decreased its phosphatase activity towards the phosphorylated myosin regulatory light chain. Our results suggest that one function of the ankyrin domain is probably to regulate the function of Myo16. It may influence the motor activity, and in complex with the PP1c isoforms, it can play an important role in the targeted dephosphorylation of certain, as yet unidentified, intracellular proteins.

The loop2 insertion of type IX myosin acts as an electrostatic actin tether that permits processive movement

Although class IX myosins are single-headed, they demonstrate characteristics of processive movement along actin filaments. Double-headed myosins that move processively along actin filaments achieve this by successive binding of the two heads in a hand-over-hand mechanism. This mechanism, obviously, cannot operate in single-headed myosins. However, it has been proposed that a long class IX specific insertion in the myosin head domain at loop2 acts as an F-actin tether, allowing for single-headed processive movement. Here, we tested this proposal directly by analysing the movement of deletion constructs of the class IX myosin from Caenorhabditis elegans (Myo IX). Deletion of the large basic loop2 insertion led to a loss of processive behaviour, while deletion of the N-terminal head extension, a second unique domain of class IX myosins, did not influence the motility of Myo IX. The processive behaviour of Myo IX is also abolished with increasing salt concentrations. These observations directly demonstrate that the insertion located in loop2 acts as an electrostatic actin tether during movement of Myo IX along the actin track.

Molecular motors: how to make models that can be used to convey the concept of molecular ratchets and thermal capture

A wide variety of cellular processes use molecular motors, including processive motors that move along some form of track (e.g., myosin with actin, kinesin or dynein with tubulin) and polymerases that move along a template (e.g., DNA and RNA polymerases, ribosomes). In trying to understand how these molecular motors actually move, many apply their understanding of how man-made motors work: the latter use some form of energy to exert a force or torque on its load. However, quite a different mechanism has been proposed to possibly account for the movement of molecular motors. Rather than hydrolyzing ATP to push or pull their load, they might use their own thermal vibrational energy as well as that of their load and their environment to move the load, capturing those movements that occur along a desired vector or axis and resisting others; ATP hydrolysis is required to make backward movements impossible. This intriguing thermal capture or Brownian ratchet model is relatively more difficult to convey to students. In this report, we describe several teaching aids that are very easily constructed using widely available household materials to convey the concept of a molecular ratchet.