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In dieser Arbeit werden nichtlineare Kopplungsmechanismen von akustischen Oszillatoren untersucht, die zu Synchronisation führen können. Aufbauend auf die Fragestellungen vorangegangener Arbeiten werden mit Hilfe theoretischer und experimenteller Studien sowie mit Hilfe numerischer Simulationen die Elemente der Tonentstehung in der Orgelpfeife und die Mechanismen der gegenseitigen Wechselwirkung von Orgelpfeifen identifiziert. Daraus wird erstmalig ein vollständig auf den aeroakustischen und fluiddynamischen Grundprinzipien basierendes nichtlinear gekoppeltes Modell selbst-erregter Oszillatoren für die Beschreibung des Verhaltens zweier wechselwirkender Orgelpfeifen entwickelt. Die durchgeführten Modellrechnungen werden mit den experimentellen Befunden verglichen. Es zeigt sich, dass die Tonentstehung und die Kopplungsmechanismen von Orgelpfeifen durch das entwickelte Oszillatormodell in weiten Teilen richtig beschrieben werden. Insbesondere kann damit die Ursache für den nichtlinearen Zusammenhang von Kopplungsstärke und Synchronisation des gekoppelten Zwei-Pfeifen Systems, welcher sich in einem nichtlinearen Verlauf der Arnoldzunge darstellt, geklärt werden. Mit den gewonnenen Erkenntnissen wird der Einfluss des Raumes auf die Tonentstehung bei Orgelpfeifen betrachtet. Dafür werden numerische Simulationen der Wechselwirkung einer Orgelpfeife mit verschiedenen Raumgeometrien, wie z. B. ebene, konvexe, konkave, und gezahnte Geometrien, exemplarisch untersucht. Auch der Einfluss von Schwellkästen auf die Tonentstehung und die Klangbildung der Orgelpfeife wird studiert. In weiteren, neuartigen Synchronisationsexperimenten mit identisch gestimmten Orgelpfeifen, sowie mit Mixturen wird die Synchronisation für verschiedene, horizontale und vertikale Pfeifenabstände in der Ebene der Schallabstrahlung, untersucht. Die dabei erstmalig beobachteten räumlich isotropen Unstetigkeiten im Schwingungsverhalten der gekoppelten Pfeifensysteme, deuten auf abstandsabhängige Wechsel zwischen gegen- und gleichphasigen Sychronisationsregimen hin. Abschließend wird die Möglichkeit dokumentiert, das Phänomen der Synchronisation zweier Orgelpfeifen durch numerische Simulationen, also der Behandlung der kompressiblen Navier-Stokes Gleichungen mit entsprechenden Rand- und Anfangsbedingungen, realitätsnah abzubilden. Auch dies stellt ein Novum dar. In this work non-linear coupling mechanisms in acoustic oscillator systems are examined which can lead to synchronization phenomena. This mechanisms are investigated in particular on organ pipes. Building up on the questions of preceding works the elements of the sound generation are identified using detailed experimental and theoretical studies, as well as numerical simulations. Furthermore the organ pipes interaction mechanisms of the mutual coupling are developed. This leads to a non-linear coupled oscillator model which is developed on the aeroacoustical and fluiddynamical first principles. The carried out model calculations are compared to the experimental results from preceding works. It appears that the sound generation and the coupling mechanisms are properly described by the developed nonlinear coupled model of self-sustained oscillators. In particular the cause can be cleared with it for the non-linear edges of the Arnold tongue of the coupled two-pipe system. With the new knowledge the influence of various space geometries on the sound generation of organ pipes is investigated. With numerical simulations the interaction of an organ pipe and different space geometries, like plane, convex, concave, and ridged geometry is studied. Also the influence of so called swell boxes on the sound generation and the sound pattern of the organ pipe is studied. In further new synchronization experiments with precisely equally tuned pairs of organ pipes, as well as with mixtures the synchronization is examined for various grids of horizontal and vertical pipe distances in the 2D-plane of sound radiation. The spatial discontinuities observed in the oscillation behaviour of the coupled pipe systems, point to changes between anti-phase and in-phase regimes of sychronization depending on pipes distances. Finally the possibility is documented to describe the phenomenon of the synchronization of two organ pipes realisticaly by solving the compressible Navier-Stokes equations numerically.

Colloids are widely considered as model systems to elucidate fundamental processes in atomic systems. However, there is one feature truly specific to colloidal suspensions that distinguishes them fundamentally from atomic systems: hydrodynamic interactions, which can lead to fascinating collective behavior.In this thesis, we present analytical work and simulation results for several micron-scale colloidal and biological systems where the dynamics is predominantly governed by hydrodynamic interactions.The first part deals with hydrodynamic interactions in two-point microrheology, a method to explore the viscoelastic behavior of soft materials (such as biological tissue) on the micron scale. We consider the overdamped motion of two birefringent colloidal beads immersed in a Newtonian fluid. The particles are assumed to be trapped by optical tweezers with respect to both their position and orientation. On the basis of a Langevin description of this system, we analyze the thermal fluctuations and obtain a rich spectrum of correlation functions. In particular, we focus on the rotational degrees of freedom and how they couple to translation, thus extending recent investigations restricted to translational correlations. An important feature of our system is the self-coupling of translation and rotation of one particle mediated by the neighboring particle. It thus shows a characteristic time delay that is clearly visible in the appropriate self-correlation function. Finally, we compare our analytical results with correlation functions determined both from Brownian-dynamics simulations that we performed and from available experimental data.In the second part, we study the dynamics of spherical particles circling in a ring-shaped harmonic trap. Hydrodynamic interactions completely determine their characteristic collective behavior. At first, the particles are driven by constant forces. A linear stability analysis for regular clusters of circling particles is performed, and we illustrate the periodic limit cycle to which the system converges. We clarify that drafting of particle doublets is essential to interpret this limit cycle. When we apply a spatially periodic sawtooth potential along the circular trap, in addition to the constant force, we find a novel caterpillar-like motional sequence that is dominated by the long-range hydrodynamic interactions and that promotes the surmounting of potential barriers by the particles. Our numerical findings are in good agreement with experiments. Such collective effects in sawtooth potentials may also be relevant in thermal ratchets that are commonly used to describe, e.g., biological motors.The issue of the third part is locomotion of microorganisms. Many types of bacteria use several rotating helical flagella to swim. Typically, the flagellar filaments form bundles, which means that their rotations must be synchronized. The central question of our study is whether hydrodynamic interactions are capable of such a synchronization. In a first approach, we consider two stiff helices that are modeled by rigidly connected beads, neglecting any elastic deformations. They are driven by constant and equal torques, and they are fixed in space by anchoring their ends in harmonic traps. For finite anchoring strength, we do indeed observe a synchronization of the helix rotations. However, the speed of phase synchronization decreases with increasing trap stiffness, and in the limit of infinite trap stiffness, the helices do not synchronize. This leads to the conclusion that some kind of flexibility is essential. Thus, as a second step, we refine our model and consider elastic deformations of the helices within the nontrivial theory of helical elastic rods. Again, we observe that the rotations of the two helices are synchronized. In particular, the additional flexibility of the helices further increases the synchronization speed. Besides the phase locking of the helices, we furthermore observe the "onset" of flagellar bundling.