The 3-satisfiability Problem (3-SAT) is a demanding combinatorial problem that is of central importance among the nondeterministic polynomial (NP) complete problems, with applications in circuit design, artificial intelligence, and logistics. Even with optimized algorithms, the solution space that needs to be explored grows exponentially with the increasing size of 3-SAT instances. Thus, large 3-SAT instances require excessive amounts of energy to solve with serial electronic computers. Network-based biocomputation (NBC) is a parallel computation approach with drastically reduced energy consumption. NBC uses biomolecular motors to propel cytoskeletal filaments through nanofabricated networks that encode mathematical problems. By stochastically exploring possible paths through the networks, the cytoskeletal filaments find possible solutions. However, to date, no NBC algorithm for 3-SAT has been available. Herein, an algorithm that converts 3-SAT into an NBC-compatible network format is reported and four small 3-SAT instances (with up to three variables and five clauses) using the actin–myosin biomolecular motor system are experimentally solved. Because practical polynomial conversions to 3-SAT exist for many important NP complete problems, the result opens the door to enable NBC to solve small instances of a wide range of problems.

No description available.

Motores moleculares são proteínas capazes de transportar objetos tais como vesículas, organelas e macromoléculas ao longo do citoesqueleto. Tratam-se de dispositivos bastante interessantes do ponto de vista físico, pois produzem trabalho em um ambiente extremamente ruidoso. Recentemente, diversos experimentos realizados in vivo têm revelado que objetos transportados por motores moleculares ao longo dos microtúbulos apresentam movimento bidirecional. Embora o movimento unidirecional dos motores envolvidos no transporte destes objetos seja bem caracterizado tanto experimentalmente quanto teoricamente, o movimento bidirecional das partículas transportadas pelos motores ainda não é bem entendido. Contudo, acredita-se que este fenômeno seja causado pela cooperatividade dos motores moleculares. Existem na literatura diversos trabalhos que visam descrever o comportamento coletivo de partículas locomovendo-se sobre uma rede unidimensional com interações de volume excluído e taxas de transição assimétricas. Estes modelos são conhecidos como TASEP (Totally asymmetric simple exclusion processes ) ou ASEP (Asymmetric simple exclusion processes ) e fazem parte de uma classe de modelos denominados sistemas difusivos dirigidos_. Embora alguns autores tenham utilizado modelos do tipo ASEP e TASEP para descrever o movimento dos motores moleculares exclusivamente [37], [38], não há ainda nesta visão microscópica, extensões deste modelo para incorporar as partículas cuja dinâmica depende exclusivamente da presença de motores. No presente trabalho propomos um modelo de exclusão, desenvolvido com o intuito de descrever o movimento conjunto de motores moleculares e das partículas carregadas pelos mesmos, as quais por simplicidade denominamos vesículas. Neste modelo, as vesículas não possuem dinâmica própria, ou seja, dependem da interação com os motores moleculares para se movimentarem. Procuramos soluções analíticas para este modelo para o 1 RESUMO 2 caso em que há apenas uma vesícula locomovendo-se sobre a rede. Utilizando o método das matrizes [32], calculamos a velocidade média da vesícula no estado estacionário e analisamos seu comportamento em situações de interesse. / Molecular motors are proteins that transport objects such as vesicles, organelles and macromolecules along the cytoskeletum of cells. For physics, they are very interesting devices because they are able to generate work in an extremely viscous environment. Recently, many in vivo experiments have revealed that objects transported by molecular motors move bidirectionally along microtubules. Although the unidirectional movement of such molecular motors is experimentally and theoretically well characterized, the movement of particles transported by these motors is not well understood yet. However, this fenomenum is believed to be caused by the cooperativity of molecular motors. A great number of works are found in literature, which were formulated to describe the collective behaviour of many particles moving in a one-dimensional lattice with a preferred hop rate and exclusion. These models are known as TASEP (Totally asymmetric simple exclusion processes) or ASEP (Asymmetric simple exclusion processes) and are part of a class of models named _driven di_usive systems_. Although some authors made use of ASEP and TASEP models to describe the movement of molecular motors [37], [38], there is not yet, in this microscopic point of view, extensions of these models capable of incorporate particles which the dynamics depends exclusivaly from the presence of motors. In this work we propose a exclusion model developed to describe the joint movement of molecular motors and particles, generally called vesicles. In this model, vesicles do not have a proper dynamics, that is, they on the interaction with molecular motors to move. We look after analytical solutions of this model when there is only one vesicle moving on the lattice. We use a matrix formulation [32] to obtain the mean velocity of the vesicle and analyse its behaviour in situations of interest.

Motores moleculares são proteínas capazes de transportar objetos tais como vesículas, organelas e macromoléculas ao longo do citoesqueleto. Tratam-se de dispositivos bastante interessantes do ponto de vista físico, pois produzem trabalho em um ambiente extremamente ruidoso. Recentemente, diversos experimentos realizados in vivo têm revelado que objetos transportados por motores moleculares ao longo dos microtúbulos apresentam movimento bidirecional. Embora o movimento unidirecional dos motores envolvidos no transporte destes objetos seja bem caracterizado tanto experimentalmente quanto teoricamente, o movimento bidirecional das partículas transportadas pelos motores ainda não é bem entendido. Contudo, acredita-se que este fenômeno seja causado pela cooperatividade dos motores moleculares. Existem na literatura diversos trabalhos que visam descrever o comportamento coletivo de partículas locomovendo-se sobre uma rede unidimensional com interações de volume excluído e taxas de transição assimétricas. Estes modelos são conhecidos como TASEP (Totally asymmetric simple exclusion processes ) ou ASEP (Asymmetric simple exclusion processes ) e fazem parte de uma classe de modelos denominados sistemas difusivos dirigidos_. Embora alguns autores tenham utilizado modelos do tipo ASEP e TASEP para descrever o movimento dos motores moleculares exclusivamente [37], [38], não há ainda nesta visão microscópica, extensões deste modelo para incorporar as partículas cuja dinâmica depende exclusivamente da presença de motores. No presente trabalho propomos um modelo de exclusão, desenvolvido com o intuito de descrever o movimento conjunto de motores moleculares e das partículas carregadas pelos mesmos, as quais por simplicidade denominamos vesículas. Neste modelo, as vesículas não possuem dinâmica própria, ou seja, dependem da interação com os motores moleculares para se movimentarem. Procuramos soluções analíticas para este modelo para o 1 RESUMO 2 caso em que há apenas uma vesícula locomovendo-se sobre a rede. Utilizando o método das matrizes [32], calculamos a velocidade média da vesícula no estado estacionário e analisamos seu comportamento em situações de interesse. / Molecular motors are proteins that transport objects such as vesicles, organelles and macromolecules along the cytoskeletum of cells. For physics, they are very interesting devices because they are able to generate work in an extremely viscous environment. Recently, many in vivo experiments have revealed that objects transported by molecular motors move bidirectionally along microtubules. Although the unidirectional movement of such molecular motors is experimentally and theoretically well characterized, the movement of particles transported by these motors is not well understood yet. However, this fenomenum is believed to be caused by the cooperativity of molecular motors. A great number of works are found in literature, which were formulated to describe the collective behaviour of many particles moving in a one-dimensional lattice with a preferred hop rate and exclusion. These models are known as TASEP (Totally asymmetric simple exclusion processes) or ASEP (Asymmetric simple exclusion processes) and are part of a class of models named _driven di_usive systems_. Although some authors made use of ASEP and TASEP models to describe the movement of molecular motors [37], [38], there is not yet, in this microscopic point of view, extensions of these models capable of incorporate particles which the dynamics depends exclusivaly from the presence of motors. In this work we propose a exclusion model developed to describe the joint movement of molecular motors and particles, generally called vesicles. In this model, vesicles do not have a proper dynamics, that is, they on the interaction with molecular motors to move. We look after analytical solutions of this model when there is only one vesicle moving on the lattice. We use a matrix formulation [32] to obtain the mean velocity of the vesicle and analyse its behaviour in situations of interest.

DNA provides an ideal substrate for nanoscale construction and programmable dynamic mechanisms. DNA mechanisms can be used to produce DNA motors which do mechanical work, e.g. transportation of a substrate along a track. I explore a method for control of a DNA mechanism ubiquitous in DNA motor designs, toehold-mediated strand displacement, by which one strand in a duplex can be swapped for another. My method uses a mismatch between a pair of nucleotides in the duplex, which is repaired by displacement. I find that displacement rate can be fine-tuned by adjusting the position of the mismatch in the duplex, enabling the design of complex kinetic behaviours. A bipedal motor [1, 2] is designed to walk along a single-stranded DNA track. Previously the motor has only taken a single step, due to a lack of designs to extend the single-stranded track. I present a novel design for track held under tension using a 3D DNA origami tightrope, and verify its assembly. The bipedal motor design is adapted and a method to specifically place motors on tightropes is demonstrated. Motor operation is investigated on truncated tracks and tightrope tracks by electrophoresis and spectrofluorometry. The motor does not accumulate appreciably at the track end; this is tentatively attributed to rearrangement of the motor between track sites without interaction with fuel. Tightrope origami can hold single-stranded DNA under pN tension. I use tightropes to study hybridization kinetics under tension and find dramatic, non-monotonic changes in hybridization rate constants and dissociation constants with tension in the range ∼0-15 pN. Extended tracks for a 'burnt-bridges' motor which destroys its track as it moves [3] are created on the inside of DNA nanotubes, which can be polymerised to create tracks up to a few mm in length, and on tiles which I attempt to join in a specific order. Crossing of the motor between tubes is verified, and microscopy experiments provide some evidence that track is being cleaved by the motor, a requirement for movement along the track. Tile based tracks are imaged by super-resolution DNA PAINT [4], providing proof-of-principle for track observation to infer motor movement.

La maladie de Huntington (MH) est une maladie neurodégénérative héréditaire autosomique dominante. Elle résulte d’une expansion anormale de glutamines (polyQ) dans la partie N-terminale de la protéine huntingtine (HTT ; codé par HTT). La MH est caractérisée par la dysfonction et la mort de cellules neuronales dans le cerveau, entraînant l’apparition de symptômes cognitifs, psychiatriques et moteurs, dévastateurs chez les patients. De nombreuses études sur des modèles animaux et cellulaires montrent que l’expansion polyQ dans la protéine mutante conduit à un gain de nouvelles fonctions toxiques, ainsi qu’à la perte de fonctions neuroprotectives de la protéine sauvage. Pendant ma thèse, je me suis intéressée à la description et à la validation fonctionnelle d’un nouvel outil pour étudier la HTT : pARIS-htt. pARIS-htt est un gène synthétique construit pour faciliter le clonage et le marquage de la protéine HTT totale. En utilisant différentes approches cellulaires, nous avons montré que pARIS-htt peut remplacer le rôle de la HTT endogène dans le transport de vésicules du Golgi ainsi que du brain derived neurotrophic factor (BDNF). La version mutante de pARIS-htt ne peut pas restaurer cette fonction. Parallèlement, nous avons généré deux variants de pARIS-htt avec soit une délétion dans la région d’interaction de la HTT avec la dynéine, moteur moléculaire se dirigeant vers l'extrémité négative des microtubules, soit avec la huntingtin associated protein 1 (HAP1), l’un de ses interacteurs. Dans les expériences de remplacement du gène, aucun des deux mutants n’a restauré le transport vésiculaire.Un autre aspect de ma thèse a été d’étudier le rôle de la HTT au cours de la mitose. Nous avons mis en évidence l’importance de la HTT dans le contrôle de l’orientation du fuseau. Cette fonction est perdue lorque la HTT est mutée, mais restaurée lorsque celle-ci est phosphorylée par Akt à la sérine 421. Le contrôle de l’orientation du fuseau est particulièrement important durant la neurogénèse puisque cette orientation ainsi que le mode de division sont impliqués dans la détermination des devenirs cellulaires. Cette fonction de la HTT est conservée chez la D. melanogaster.Cette étude a donc permis de mieux comprendre les fonctions de la HTT, et de proposer de nouvelles cibles thérapeutiques pour traiter la MH. / Huntington disease (HD) is an autosomal-dominant neurodegenerative disorder caused by the pathogenic expansion of the poly-glutamine (polyQ) N-terminal stretch in the huntingtin protein (HTT; encoded by HTT). HD is characterized by the dysfunction and death of neurons in the brain, leading to devastating cognitive, psychiatric, and motor symptoms in patients. Studies in multiple cell and animal model systems support the notion that polyQ expansion in mutant HTT leads to the gain of new toxic functions and loss of the neuroprotective functions of the wild-type HTT. During my thesis, I focused on the description and functional validation of a new tool to study HTT: pARIS-htt. pARIS-htt is a synthetic gene built to facilitate cloning and tagging of full-length HTT. Using different cellular approaches, we showed that pARIS-htt can replace endogenous HTT in the transport of Golgi and brain derived neurotrophic factor (BDNF) containing vesicles. pARIS-htt mutant version could not restore vesicular transport when endogenous HTT was knocked-down. Moreover, we generated pARIS-htt deletion mutants for HTT interaction domain with dynein, a minus-end directed motor protein, and huntingtin associated protein 1 (HAP1), a HTT interactor. Both deletion mutants failed to restore vesicular transport in gene replacement assays. Another aspect of my thesis was the study of HTT during mitosis. We showed that HTT monitors spindle orientation though its interaction with diverse proteins involved in cell division. This function is lost when HTT is mutated and can be reverted by Akt phosphorylation at serine 421. The control of spindle orientation is particularly important during neurogenesis since spindle orientation and the mode of division of apical progenitors are implicated in the determination of cell fate. This function of HTT is conserved in D. melanogaster. This study contributes to the understanding of HTT functions and suggests new therapeutical approaches to treat HD.

Bewegungen von prozessiven molekularen Motoren des Zytoskeletts sind durch ein Wechselspiel von gerichteter Bewegung entlang von Filamenten und Diffusion in der umgebenden Lösung gekennzeichnet. Diese eigentümlichen Bewegungen werden in der vorliegenden Arbeit untersucht, indem sie als Random Walks auf einem Gitter modelliert werden. Ein weiterer Gegenstand der Untersuchung sind Effekte von Wechselwirkungen zwischen den Motoren auf diese Bewegungen. <br /> <br /> Im einzelnen werden vier Transportphänomene untersucht: <br /> (i) Random Walks von einzelnen Motoren in Kompartimenten verschiedener Geometrien, <br /> (ii) stationäre Konzentrationsprofile, die sich in geschlossenen Kompartimenten infolge dieser Bewegungen einstellen,<br /> (iii) randinduzierte Phasenübergänge in offenen röhrenartigen Kompartimenten, die an Motorenreservoirs gekoppelt sind, und <br /> (iv) der Einfluß von kooperativen Effekten bei der Motor-Filament-Bindung auf die Bewegung. Alle diese Phänomene sind experimentell zugänglich, und mögliche experimentelle Realisierungen werden diskutiert. / Movements of processive cytoskeletal motors are characterized by an interplay between directed motion along filament and diffusion in the surrounding solution. In the present work, these peculiar movements are studied by modeling them as random walks on a lattice. An additional subject of our studies is the effect of motor-motor interactions on these movements. <br /> <br /> In detail, four transport phenomena are studied: <br /> (i) Random walks of single motors in compartments of various geometries, <br /> (ii) stationary concentration profiles which build up as a result of these movements in closed compartments, <br /> (iii) boundary-induced phase transitions in open tube-like compartments coupled to reservoirs of motors, and <br /> (iv) the influence of cooperative effects in motor-filament binding on the movements. All these phenomena are experimentally accessible and possible experimental realizations are discussed.

In biological cells, the long-range intracellular traffic is powered by molecular motors which transport various cargos along microtubule filaments. The microtubules possess an intrinsic direction, having a 'plus' and a 'minus' end. Some molecular motors such as cytoplasmic dynein walk to the minus end, while others such as conventional kinesin walk to the plus end. Cells typically have an isopolar microtubule network. This is most pronounced in neuronal axons or fungal hyphae. In these long and thin tubular protrusions, the microtubules are arranged parallel to the tube axis with the minus ends pointing to the cell body and the plus ends pointing to the tip. In such a tubular compartment, transport by only one motor type leads to 'motor traffic jams'. Kinesin-driven cargos accumulate at the tip, while dynein-driven cargos accumulate near the cell body. We identify the relevant length scales and characterize the jamming behaviour in these tube geometries by using both Monte Carlo simulations and analytical calculations. A possible solution to this jamming problem is to transport cargos with a team of plus and a team of minus motors simultaneously, so that they can travel bidirectionally, as observed in cells. The presumably simplest mechanism for such bidirectional transport is provided by a 'tug-of-war' between the two motor teams which is governed by mechanical motor interactions only. We develop a stochastic tug-of-war model and study it with numerical and analytical calculations. We find a surprisingly complex cooperative motility behaviour. We compare our results to the available experimental data, which we reproduce qualitatively and quantitatively. / In biologischen Zellen transportieren molekulare Motoren verschiedenste Frachtteilchen entlang von Mikrotubuli-Filamenten. Die Mikrotubuli-Filamente besitzen eine intrinsische Richtung: sie haben ein "Plus-" und ein "Minus-"Ende. Einige molekulare Motoren wie Dynein laufen zum Minus-Ende, während andere wie Kinesin zum Plus-Ende laufen. Zellen haben typischerweise ein isopolares Mikrotubuli-Netzwerk. Dies ist besonders ausgeprägt in neuronalen Axonen oder Pilz-Hyphen. In diesen langen röhrenförmigen Ausstülpungen liegen die Mikrotubuli parallel zur Achse mit dem Minus-Ende zum Zellkörper und dem Plus-Ende zur Zellspitze gerichtet. In einer solchen Röhre führt Transport durch nur einen Motor-Typ zu "Motor-Staus". Kinesin-getriebene Frachten akkumulieren an der Spitze, während Dynein-getriebene Frachten am Zellkörper akkumulieren. Wir identifizieren die relevanten Längenskalen und charakterisieren das Stauverhalten in diesen Röhrengeometrien mit Hilfe von Monte-Carlo-Simulationen und analytischen Rechnungen. Eine mögliche Lösung für das Stauproblem ist der Transport mit einem Team von Plus- und einem Team von Minus-Motoren gleichzeitig, so dass die Fracht sich in beide Richtungen bewegen kann. Dies wird in Zellen tatsächlich beobachtet. Der einfachste Mechanismus für solchen bidirektionalen Transport ist ein "Tauziehen" zwischen den beiden Motor-Teams, das nur mit mechanischer Interaktion funktioniert. Wir entwickeln ein stochastisches Tauzieh-Modell, das wir mit numerischen und analytischen Rechnungen untersuchen. Es ergibt sich ein erstaunlich komplexes Motilitätsverhalten. Wir vergleichen unsere Resultate mit den vorhandenen experimentellen Daten, die wir qualitativ und quantitativ reproduzieren.

Cargo transport by molecular motors is ubiquitous in all eukaryotic cells and is typically driven cooperatively by several molecular motors, which may belong to one or several motor species like kinesin, dynein or myosin. These motor proteins transport cargos such as RNAs, protein complexes or organelles along filaments, from which they unbind after a finite run length. Understanding how these motors interact and how their movements are coordinated and regulated is a central and challenging problem in studies of intracellular transport. In this thesis, we describe a general theoretical framework for the analysis of such transport processes, which enables us to explain the behavior of intracellular cargos based on the transport properties of individual motors and their interactions. Motivated by recent in vitro experiments, we address two different modes of transport: unidirectional transport by two identical motors and cooperative transport by actively walking and passively diffusing motors. The case of cargo transport by two identical motors involves an elastic coupling between the motors that can reduce the motors’ velocity and/or the binding time to the filament. We show that this elastic coupling leads, in general, to four distinct transport regimes. In addition to a weak coupling regime, kinesin and dynein motors are found to exhibit a strong coupling and an enhanced unbinding regime, whereas myosin motors are predicted to attain a reduced velocity regime. All of these regimes, which we derive both by analytical calculations and by general time scale arguments, can be explored experimentally by varying the elastic coupling strength. In addition, using the time scale arguments, we explain why previous studies came to different conclusions about the effect and relevance of motor-motor interference. In this way, our theory provides a general and unifying framework for understanding the dynamical behavior of two elastically coupled molecular motors. The second mode of transport studied in this thesis is cargo transport by actively pulling and passively diffusing motors. Although these passive motors do not participate in active transport, they strongly enhance the overall cargo run length. When an active motor unbinds, the cargo is still tethered to the filament by the passive motors, giving the unbound motor the chance to rebind and continue its active walk. We develop a stochastic description for such cooperative behavior and explicitly derive the enhanced run length for a cargo transported by one actively pulling and one passively diffusing motor. We generalize our description to the case of several pulling and diffusing motors and find an exponential increase of the run length with the number of involved motors. / Lastentransport mittels Motorproteinen ist ein grundlegender Mechanismus aller eukaryotischen Zellen und wird üblicherweise von mehreren Motoren kooperativ durchgeführt, die zu einer oder zu verschiedenen Motorarten wie Kinesin, Dynein oder Myosin gehören. Diese Motoren befördern Lasten wie zum Beispiel RNAs, Proteinkomplexe oder Organellen entlang Filamenten, von denen sie nach einer endlichen zurückgelegten Strecke abbinden. Es ist ein zentrales und herausforderndes Problem zu verstehen, wie diese Motoren wechselwirken und wie ihre Bewegungen koordiniert und reguliert werden. In der vorliegenden Arbeit wird eine allgemeine theoretische Herangehensweise zur Untersuchung solcher Transportprozesse beschrieben, die es uns ermöglicht, das Verhalten von intrazellularem Transport, ausgehend von den Transporteigenschaften einzelner Motoren und ihren Wechselwirkungen, zu verstehen. Wir befassen uns mit zwei Arten kooperativen Transports, die auch kürzlich in verschiedenen in vitro-Experimenten untersucht wurden: (i) gleichgerichteter Transport mit zwei identischen Motorproteinen und (ii) kooperativer Transport mit aktiv schreitenden und passiv diffundierenden Motoren. Beim Lastentransport mit zwei identischen Motoren sind die Motoren elastisch gekoppelt, was eine Verminderung ihrer Geschwindigkeit und/oder ihrer Bindezeit am Filament hervorrufen kann. Wir zeigen, dass solch eine elastische Kopplung im Allgemeinen zu vier verschiedenen Transportcharakteristiken führt. Zusätzlich zu einer schwachen Kopplung, können bei Kinesinen und Dyneinen eine starke Kopplung und ein verstärktes Abbinden auftreten, wohingegen bei Myosin Motoren eine verminderte Geschwindigkeit vorhergesagt wird. All diese Transportcharakteristiken, die wir mit Hilfe analytischer Rechnungen und Zeitskalenargumenten herleiten, können durch Änderung der elastischen Kopplung experimentell untersucht werden. Zusätzlich erklären wir anhand der Zeitskalenargumente, warum frühere Untersuchungen zu unterschiedlichen Erkenntnissen über die Auswirkung und die Wichtigkeit der gegenseitigen Beeinflussung der Motoren gelangt sind. Auf diese Art und Weise liefert unsere Theorie eine allgemeine und vereinheitlichende Beschreibung des dynamischen Verhaltens von zwei elastisch gekoppelten Motorproteinen. Die zweite Art von Transport, die in dieser Arbeit untersucht wird ist der Lastentransport durch aktiv ziehende und passiv diffundierende Motoren. Obwohl die passiven Motoren nicht zum aktiven Transport beitragen, verlängern sie stark die zurückgelegte Strecke auf dem Filament. Denn wenn ein aktiver Motor abbindet, wird das Lastteilchen immer noch am Filament durch den passiven Motor festgehalten, was dem abgebundenen Motor die Möglichkeit gibt, wieder an das Filament anzubinden und den aktiven Transport fortzusetzen. Für dieses kooperative Verhalten entwickeln wir eine stochastische Beschreibung und leiten explizit die verlängerte Transportstrecke für einen aktiv ziehenden und einen passiv diffundierenden Motor her. Wir verallgemeinern unsere Beschreibung für den Fall von mehreren ziehenden und diffundierenden Motoren und finden ein exponentielles Anwachsen der zurückgelegten Strecke in Abhängigkeit von der Anzahl der beteiligten Motoren.

Cells are the minimum unit of life. They are born, they eat, the may grow, they may move, and, eventually, they die. By contrast, from a physicist point of view, cells are systems out of equilibrium continuously transducing between matter, energy and information. This transduction is what grants the cell their active properties. In order to perform such tasks, cells have a set of macromolecules, a machinery, which are called, Molecular Motors or Molecular Machines. The operation of molecular motors is multiple. For instance, kinesins are molecular motors able to transport cargoes along the cell, or the Bacterial Flagellar Motor works as a nanometric ionic turbine transmitting its rotation to bacterial flagella propelling the cell. The energy input of such nanometric devices have two primary sources. On one hand the hydrolysis of nucleotide derivatives, such as ATP. On the other hand, molecular motors can also be found in biological membranes obtaining energy from the natural flux of ions crossing the membrane due to mechano-chemical energetic differences at each side. The recycling of ATP molecules takes place in another molecular machine, the F0F1 ATP synthase. F0F1 is made up of two subunits that can be separated themselves in two different molecular machines. This way, the F1 motor can couple a rotatory motor with the synthesis/hydrolysis of ATP. Understanding the working of molecular motors is not straightforward. The transduction processes result from a complex set of interactions of all the molecules conforming the motor plus all the interactions with the surrounding molecules. Thus, different approaches with different levels of abstraction are necessary. In the current thesis, molecular motors are studied through the identification of the energetic transduction cycles out of the trajectory of the motor. Trajectories allow to identify the different mechanical and chemical processes driving the motor and allow to propose a spatio-temporal potential for the motor that give information of the energetic performance of the motor such as power and efficiency. This analysis is performed on the F1 motor (in its hydrolysis regime). Such analysis allowed to identify the origin of two well differentiated mechanical and chemical processes that were quantified by means of the reaction kinetics theory and the overdamped dynamics associated with the nanometric biological scale. From this analysis resulted a prediction for the average velocity of the motor with the experimental control parameters. The resulting velocity matches experimental measures of the average velocity without fitting any parameter since all the parameters needed can be extracted from alternative experimental assays. The appealing results of the average velocity lead to a proposal of motor potential for the F1 motor consisting on two linear piece-wise potentials flashing between them. Each potential presenting the experimental characteristics observed when the catalytic site of the motor is empty or occupied. The potential also hold the substepping mechanism observed experimentally. Thus, the resulting potential can be tested, together with the overdamped dynamics of the potential and the thermal fluctuations characteristic of the biological cellular scale. This results in a Langevin equation leading the dynamics of the motor. Again, the stochastic dynamics proposed are able to reproduce the velocity of the motor returning a better approximation than the deterministic approach. As happened in the previous case, there is no fitting in the parameters to test the validity of the velocity expression. Actually, the model is able to predict the measured substep angle from optimisation arguments. The mismatch between the deterministic and the stochastic results was identified as a result of a loss of ATP hydrolysis events due to thermal fluctuations that has been also properly quantified through the Fokker-Planck formalism of the corresponding Langevin equation. The motor potential proposed was also used to study experimental assays of the F1 motor working against conservative forces. The effect of a conservative torque in the working of the motor contains contributions both mechanical and chemical. Altogether, this contributions were successfully addressed presenting again an analytical and stochastic prediction for the velocity of the motor that matches the experimental observations without the need of any parameter fitting. This analysis also entailed a study of the energetic performance of the motor which is unavailable experimentally. The results show a complete divergence between the stochastic and deterministic predictions. The divergence is specially dramatical near the stall force of the motor where the determenistic analysis predicts an efficiency maximum and the stochastic analysis returns a null efficiency. This points out that the stochastic effects are very relevant to the energetic performance of the motor and can not be missed in a proper energetic study of a molecular machine. Besides the study of the F1 motor, also a rotatory device working with an ionic flux was analised. The aim of the analysis was the devise of a minimal mechanistic turbine and the study of its main working features. Such a machine is composed by a mobile piston with periodic boundary conditions at both ends of a nanometric channel separating two particle reservoirs. Hence, the turbine is able to transduce energy between the flux of ions and an external force hindering the natural motion of the piston. Again, thermal fluctuations provide a stochastic dynamic that must be studied through a Langevin equation that can be tackled analytically. This study revealed that the velocity and the flux are not coupled. Specially, two different stall forces appear for the motor. One for the velocity and one for the flux. This results in an intermediate zone where there is a continuous leakage of ions that does not allow any energetic output. This effect is originated from thermal fluctuations. Thus, when the energetic performance is evaluated, a similar behaviour than the one obtained for the F1 motor is recuperated. This minimal model was extended with more complex turbines that take into account more thoroughly the biophysics of molecular machines. All of them result in the same energetic landscape where a minimum of efficiency is obtained near the stall of the motor. Additionally, a new formalism has been developed to simplify the resulting Langevin equations (Fokker-planck white noise limit) and a new algorithm has been devised able to integrate Langevin equations with non-continuous multiplicative noise / Los Motores Moleculares son macromoléculas biológicas que se encargan de hacer las transducciones energéticas necesarias dentro de las células. Este trabajo estudia la transformación de energía de motores moleculares rotatorios reales principalmente la F1-ATPasa, el Motor Flagelar de las Bacterias y el F0. Para estudiar la dinámica del motor se han utilizado ecuaciones de Langevin sobreamortiguadas que recogen la importancia de las fluctuaciones térmicas, así como las fuerzas externas aplicadas al motor (conservativas y disipativas) y el potencial interno del motor que contiene la información físico-química de su comportamiento. Este estudio se ha aplicado a la F1-ATPasa, que se puede estudiar tanto analíticamente, obviando las fluctuaciones térmicas como desde su naturaleza estocástica mediante potenciales intermitentes. En ambos casos, el modelo es capaz de describir la dinámica del motor y su dependencia con los diferentes parámetros controlables experimentalmente: Concentración de ATP, fuerza disipativa y fuerza conservativa. En el mismo sentido se ha diseñado una turbina nanoscópica que recoge los principios básicos de la interacción mecánica entre un flujo de iones y la rotación del motor. En ambos casos, tanto en la turbina como en el F1 se observa que el ruido térmico no afecta mucho a la velocidad del motor y en cambio produce cambios enormes en parámetros energéticos como la potencia o la eficiencia. Concretamente, el escenario clásico en que un máximo de eficiencia se obtiene para la fuerza de calado desaparece obteniendo nuevos regímenes óptimos de trabajo. Adicionalmente, se ha desarrollado un formalismo para simplificar las ecuaciones de Langevin obtenidas (límite de ruido blanco) y se ha diseñado un nuevo algoritmo para integrar ecuaciones de Langevin en las cuales el ruido multiplicativo es discontinuo en el espacio.