O free-electron laser (FEL) surgiu como uma nova fonte de radiação eletromagnética. O presente trabalho trata do efeito de carga em um FEL específico: de passagem única; e, sendo que as interações relevantes são entre o feixe e o campo magnético e entre os elétrons (não são estudados os campos auto consistentes do laser). Encontram-se as equações de movimento de cada partícula dentro do poço e comparam-se os resultados analíticos com os resultados obtidos por simulação computacional, para os limites de povoamento dos elétrons em uma situação de equilíbrio. Posteriormente, se analisa o efeito de carga através dos mapas de Poincaré, introduzindo partículas com uma determinada distribuição inicial, dentro do potencial aprisionador. Conclui-se que a introdução de cargas aumenta o número de graus de liberdade do sistema, fazendo com que os mapas de Poincaré não sejam mais uma boa ferramenta para analisar a dinâmica do sistema. Observa-se, também, o fenômeno de quebra de onda no FEL através do efeito do balanço do potencial e de uma distribuição inicial de elétrons diferente da distribuição de equilíbrio. / Free-electron laser (FEL) was first created as a new source of electromagnetic radiation. The present work is about the charge effect on a specific FEL: single pass; and, with interactions between the beam and the magnetic field and between electrons (laser self consistent fields are not studied). Motion equations of each particle inside ponderomotive well are discovered, and then analytic results for the limits of electronic population are compared with simulated ones, in the situation of equilibrium. Afterwards, particles are introduced in the trapping potential, respecting a defined initial distribution, so the charge effect is analyzed through Poincaré maps. In conclusion, the introduction of charges raises the number of freedom degrees of the system. This makes the Poincaré maps not such a good tool to analyze the system dynamics. The wave breaking phenomenon is also observed in FEL through oscillation balance effect and an initial electronic distribution distinct of the equilibrium one.

O free-electron laser (FEL) surgiu como uma nova fonte de radiação eletromagnética. O presente trabalho trata do efeito de carga em um FEL específico: de passagem única; e, sendo que as interações relevantes são entre o feixe e o campo magnético e entre os elétrons (não são estudados os campos auto consistentes do laser). Encontram-se as equações de movimento de cada partícula dentro do poço e comparam-se os resultados analíticos com os resultados obtidos por simulação computacional, para os limites de povoamento dos elétrons em uma situação de equilíbrio. Posteriormente, se analisa o efeito de carga através dos mapas de Poincaré, introduzindo partículas com uma determinada distribuição inicial, dentro do potencial aprisionador. Conclui-se que a introdução de cargas aumenta o número de graus de liberdade do sistema, fazendo com que os mapas de Poincaré não sejam mais uma boa ferramenta para analisar a dinâmica do sistema. Observa-se, também, o fenômeno de quebra de onda no FEL através do efeito do balanço do potencial e de uma distribuição inicial de elétrons diferente da distribuição de equilíbrio. / Free-electron laser (FEL) was first created as a new source of electromagnetic radiation. The present work is about the charge effect on a specific FEL: single pass; and, with interactions between the beam and the magnetic field and between electrons (laser self consistent fields are not studied). Motion equations of each particle inside ponderomotive well are discovered, and then analytic results for the limits of electronic population are compared with simulated ones, in the situation of equilibrium. Afterwards, particles are introduced in the trapping potential, respecting a defined initial distribution, so the charge effect is analyzed through Poincaré maps. In conclusion, the introduction of charges raises the number of freedom degrees of the system. This makes the Poincaré maps not such a good tool to analyze the system dynamics. The wave breaking phenomenon is also observed in FEL through oscillation balance effect and an initial electronic distribution distinct of the equilibrium one.

O free-electron laser (FEL) surgiu como uma nova fonte de radiação eletromagnética. O presente trabalho trata do efeito de carga em um FEL específico: de passagem única; e, sendo que as interações relevantes são entre o feixe e o campo magnético e entre os elétrons (não são estudados os campos auto consistentes do laser). Encontram-se as equações de movimento de cada partícula dentro do poço e comparam-se os resultados analíticos com os resultados obtidos por simulação computacional, para os limites de povoamento dos elétrons em uma situação de equilíbrio. Posteriormente, se analisa o efeito de carga através dos mapas de Poincaré, introduzindo partículas com uma determinada distribuição inicial, dentro do potencial aprisionador. Conclui-se que a introdução de cargas aumenta o número de graus de liberdade do sistema, fazendo com que os mapas de Poincaré não sejam mais uma boa ferramenta para analisar a dinâmica do sistema. Observa-se, também, o fenômeno de quebra de onda no FEL através do efeito do balanço do potencial e de uma distribuição inicial de elétrons diferente da distribuição de equilíbrio. / Free-electron laser (FEL) was first created as a new source of electromagnetic radiation. The present work is about the charge effect on a specific FEL: single pass; and, with interactions between the beam and the magnetic field and between electrons (laser self consistent fields are not studied). Motion equations of each particle inside ponderomotive well are discovered, and then analytic results for the limits of electronic population are compared with simulated ones, in the situation of equilibrium. Afterwards, particles are introduced in the trapping potential, respecting a defined initial distribution, so the charge effect is analyzed through Poincaré maps. In conclusion, the introduction of charges raises the number of freedom degrees of the system. This makes the Poincaré maps not such a good tool to analyze the system dynamics. The wave breaking phenomenon is also observed in FEL through oscillation balance effect and an initial electronic distribution distinct of the equilibrium one.

In the Thesis, two important theoretical problems arising in the theory of one-dimensional defocusing nonlinear Schrödinger (NLS) flows are investigated analytically and numerically: (i) the resonant generation of dispersive shock waves (DSWs) in one-dimensional NLS flow past a broad repulsive penetrable barrier; and (ii) the interaction of counter-propagating DSW and a simple rarefaction wave (RW), which is referred to as the DSW refraction problem. The first problem is motivated by the recent experimental observations of dark soliton radiation in a cigar-shaped BEC by sweeping through it a localised repulsive potential; the second problem represents a dispersive-hydrodynamic counterpart of the classical gas-dynamics problem of the shock wave refraction on a RW, and, apart from its theoretical significance could also find applications in superfluid dynamics. Both problems also naturally arise in nonlinear optics, where the NLS equation is a standard mathematical model and the `superfluid dynamics of light' can be used for an all-optical modelling of BEC flows. The main results of the Thesis are as follows: (i) In the problem of the transcritical flow of a BEC through a wide repulsive penetrable barrier an asymptotic analytical description of the arising wave pattern is developed using the combination of the localised ``hydraulic'' solution of the 1D Gross-Pitaevskii (GP) equation with repulsion (the defocusing NLS equation with an added external potential) and the appropriate exact solutions of the Whitham-NLS modulation equations describing the resolution of the upstream and downstream discontinuities through DSWs. We show that the downstream DSW effectively represents the train of dark solitons, which can be associated with the excitations observed experimentally by Engels and Atherton (2008). (ii) The refraction of a DSW due to its head-on collision with the centred RW is considered in the frameworks of two one-dimensional defocusing NLS models: the standard cubic NLS equation and the NLS equation with saturable nonlinearity, the latter being a standard model for the light propagation through photorefractive optical crystals. For the cubic nonlinearity case we present a full asymptotic description of the DSW refraction by constructing appropriate exact solutions of the Whitham modulation equations in Riemann invariants. For the NLS equation with saturable nonlinearity, whose modulation system does not possess Riemann invariants, we take advantage of the recently developed method for the DSW description in non-integrable dispersive systems to obtain key parameters of the DSW refraction. In both problems, we undertake a detailed analysis of the flow structure for different parametric regimes and calculate physical quantities characterising the output flows in terms of relevant input parameters. Our modulation theory analytical results are supported by direct numerical simulations of the corresponding full dispersive initial value problems (IVP).

To understand and to predict the weather and climate, numerical models are important tools and it is crucial that the controlling processes are described correctly. Since 70% of the global surface is covered with water the description how the ocean and atmosphere communicates has a considerable impact. The ocean–atmosphere exchange occurs through transport of momentum (friction) and heat, governed by turbulent eddies. The sea surface is also an important source of turbulence in both directions. The scales of the turbulent eddies cannot be resolved in ocean and climate models. Therefore, the turbulent exchanges have to be related to mean variables, such as wind speed and temperature differences. By using measurements, new methods to describe the air–sea exchange during two specific processes were developed. These processes are the so-called UVCN-regime (Unstable Very Close to Neutral stratification) and swell, i.e. waves which are not produced by the local wind. These processes were included in an ocean model and in a regional atmospheric climate model and the impact was investigated. The UVCN-regime enhances the heat transport significantly during the autumn and winter months in the ocean model. This results in a shallower well-mixed surface layer in the ocean. Wind-following swell reduces the surface friction, which is very important for the atmosphere. Some secondary effects in the climate model are reduced low-level cloud cover and reduced precipitation by more than 10% over sea areas. Locally and for short periods the impact is large. It is important to include the UVCN-regime and the swell impact in models, to make simulations more reliable.

Στην παρούσα διατριβή διερευνάται η επίδραση παράκτιων μη-θραυόμενων κυματισμών στη μορφολογική ισορροπία αμμώδους πυθμένα με πτυχώσεις, η θραύση εκχείλισης κυμάτων πάνω από πυθμένα σταθερής κλίσης, καθώς και τα συνεπαγόμενα κυματογενή ρεύματα στη ζώνη απόσβεσης. Για το σκοπό αυτό αναπτύσσονται μοντέλα αριθμητικής προσομοίωσης, τα οποία πραγματοποιούν επίλυση των δισδιάστατων και τρισδιάστατων εξισώσεων ασυμπίεστης, συνεκτικής ροής με ελεύθερη επιφάνεια. Η αριθμητική επίλυση των εξισώσεων ροής, Navier-Stokes, επιτυγχάνεται με τη χρήση κλασματικής μεθόδου για τη χρονική ολοκλήρωση, ενώ η χωρική διακριτοποίηση πραγματοποιείται μέσω ενός υβριδικού σχήματος πεπερασμένων διαφορών και ψευδο-φασματικών μεθόδων προσέγγισης. Στις προσομοιώσεις της θραύσης εκχείλισης κύματος γίνεται χρήση της μεθόδου προσομοίωσης μεγάλων κυμάτων LWS, σύμφωνα με την οποία επιλύονται μόνο οι μεγάλες χωρικές διακυμάνσεις της ταχύτητας και της ελεύθερης επιφάνειας, ενώ η επίδραση των μικρότερων διακυμάνσεων περιγράφεται μέσω ενός μοντέλου διατμητικών τάσεων υποκλίμακας (SGS), ανάλογα με ότι ισχύει στη μέθοδο προσομοίωσης μεγάλων δινών, LES. Ένα ανεξάρτητο μοντέλο για την προσομοίωση της μεταβολής μορφολογίας πυθμένα, μέσω μεταφοράς φορτίου πυθμένα, αναπτύσσεται και χρησιμοποιείται σε σύζευξη με τα μοντέλα προσομοίωσης δισδιάστατης ροής. H παροχή του φορτίου πυθμένα υπολογίζεται μέσω τροποποίησης γνωστών εμπειρικών σχέσεων, σε συνδυασμό με τη στιγμιαία διατμητική τάση πυθμένα από τη μονάδα προσομοίωσης της ροής. Από τις προσομοιώσεις ροής πάνω από πυθμένα με πτυχώσεις, προκύπτει ότι η παρουσία των πτυχώσεων επηρεάζει σημαντικά το κυματογενές οριακό στρώμα, ενώ οι μορφολογικές προσομοιώσεις οδηγούν στο συμπέρασμα ότι, η μακροπρόθεσμη ισορροπία των πτυχώσεων επέρχεται για συγκεκριμένη τιμή της γωνίας/συντελεστή δυναμικής τριβής, η οποία συσχετίζεται με τις διαστάσεις των πτυχώσεων και τα χαρακτηριστικά του κύματος. Για τη θραύση εκχείλισης εξετάζονται οι περιπτώσεις κάθετης αλλά και υπό γωνία, ως προς την ακτογραμμή, διάδοσης κυμάτων πάνω από πυθμένα σταθερής κλίσης 1/35. Τα αποτελέσματα για τα χαρακτηριστικά της κάθετης θραύσης (ύψος και βάθος θραύσης, Ηb και db, αντίστοιχα) και του συνεπαγόμενου υποβρύχιου ρεύματος, συγκρίνονται με δημοσιευμένες πειραματικές μετρήσεις και η συμφωνία είναι ικανοποιητική. Το μοντέλο είναι σε θέση να προσομοιώσει την ανάπτυξη του επιφανειακού στροβίλου στο μέτωπο του θραυόμενου κύματος, η οποία συνοδεύεται από αύξηση της ισχύος των SGS τάσεων (μέχρι βάθους d/db ≈ 0.75) και διαδοχική μείωσή τους, μέχρι μηδενισμού, στα ρηχά της ζώνης απόσβεσης. Από τα αποτελέσματα για το πεδίο στροβιλότητας και τις SGS τάσεις, κατά την προσομοίωση της υπό γωνία θραύσης, παρατηρείται η σταδιακή θραύση του κύματος κατά μήκος της κορυφογραμμής, ενώ προκύπτει ότι οι τελευταίες παραμένουν ενεργές για περίπου δύο μήκη κύματος. Επίσης, η μέση ταχύτητα του παράλληλου ρεύματος προκύπτει πιο ενισχυμένη σε ρηχά βάθη στη ζώνη απόσβεσης (d/db < 0.5), ενώ η κατακόρυφη κατανομή του παρουσιάζεται σαφώς επηρεασμένη από την παρουσία του υποβρύχιου ρεύματος κοντά στον πυθμένα. / In the present thesis, the impact of nearshore, non-breaking waves on the morphological equilibrium of small scale patterns that appear in sandy beds, well-known as ripples, the spilling wave breaking over a bed of constant slope and the wave-induced currents developing in the surf zone, are investigated. Numerical models are developed for the simulation of the aforementioned phenomena, based on the numerical solution of the two/three-dimensional, incompressible, viscous, free-surface flow. The numerical solution of the flow equations, i.e. the Navier-Stokes equations, is accomplished by means of a time-splitting scheme of three stages for the temporal discretization and a hybrid scheme for the spatial discretization, with central finite differences along the streamwise direction and pseudo-spectral approximations, with Fourier modes and Chebyshev polynomials along the spanwise and vertical directions, respectively. The simulations of spilling wave breaking are performed employing the so-called large-wave simulation (LWS) method, according to which, large velocity and free-surface scales are fully resolved, while the effect of subgrid scales is modeled by eddy-viscosity stresses, similar to large-eddy simulation (LES) methodology. The bed morphology evolution, driven by the bed load sediment transport, is simulated by a morphology model, which performs the numerical solution of the sediment mass conservation equation, utilized coupled with the two-dimensional flow model. The bed load transport rate, is computed inserting bed shear stress timeseries (by the flow model) into published empirical formulas that have been modified to fit the characteristics of the investigated cases. For the case of rippled bed, it was found that the structure of the wave boundary layer is substantially influenced by the presence of the ripples, and that for a certain value of the dynamic friction angle/coefficient, which is correlated to the ripple dimensions and the wave characteristics, the ripples remain in quasi-steady equilibrium after each wave period. Wave breaking is investigated by the simulation of normal and oblique to the shoreline propagation, transformation and spilling breaking of incoming Stokes waves, over a bed of constant slope, tanβ = 1/35. Our numerical results are compared to published experimental measurements, and it is found that the LWS model predicts adequately the wave breaking parameters - breaking height, Ηb, and depth, db- and the distribution of the undertow current in the surf zone. The development of the surface roller in the breaking wavefront is also captured, while is connected to the increase of the strength of the sub-grid (SGS) stresses in the outer surf zone (up to d/db ≈ 0.75) and their successive decrease at shallower depths close to the shoreline. For the case of oblique wave breaking, the vorticity and the SGS stresses distribution in the surf zone clearly indicate the gradual breaking along the wave crestline, while the latter (SGS stresses) remain active for about two wavelenghts. Finally, the magnitude of the longshore current is found to be enhanced at shallower depths in the surf zone (d/db < 0.5), while its vertical distribution is affected by the interaction with the undertow current.

Cette thèse présente une simulation, en canal à houle, des processus naturels hydrodynamiques etde transport sédimentaire de la zone de déferlement bathymétrique. L’analyse spatio-temporelle dela structure moyenne et instantanée de l’écoulement repose sur un jeu de mesures hauterésolutions.On effectue une étude des processus de couche limite et de l’impact des processus desurface libre sur le fond sédimentaire.Un profil de plage en forme de terrasse est engendré par le déferlement de séries de vagues irrégulières(JONSWAP) sur un fond mobile constitué de sédiments de faible densité (_ _ 1.19). Dans cesconditions, la mesure acoustique (ADVP) de profils de vitesse, de concentration et de flux de sédimentsest synchronisée à des séquences d’images vidéo et à des mesures de hauteurs de vagues.Une analyse de l’évolution des quantités moyennes hydrodynamiques et de transport solide est réaliséedans la zone de déferlement. Une analyse à l’échelle intra-vague aborde la structure del’écoulement sous le déferlement de vagues irrégulières. Enfin, on s’attache à une comparaison de lacontrainte au fond sous une vague déferlée calculée par des modèles physiques, à celle obtenue parmesures directes. / This thesis presents a wave channel simulation of the hydrodynamic and sediment transportprocesses in the wave breaking region. The spatio-temporal analysis of the mean and instantaneousflow structure relies on a full set of high resolution data. The study focuses on processes related tothe wave boundary layer and to the impact of surface breaking on the mobile bed.A terraced beach profile is generated by the breaking of irregular wave sequences (JONSWAP) on amobile bed constituted of low density sediments (_ _ 1.19). In these conditions, the acoustic measurementof velocity profiles, concentration profiles and sediment flux profiles are synchronised withsequences of video images and wave heights. An analysis of the evolution of mean hydrodynamicand sediment transport quantities is undertaken across the entire wave breaking zone. An intra-waveanalysis on the flow structure below irregular breaking waves is carried out. Finally, bed shear stressbelow a breaking wave predicted by different physical models and direct measurements, are comparedand discussed.

No description available.

Dans un contexte international, la prévision d'intensité des cyclones tropicaux connaît encore de graves déficiences tandis que la prévision de trajectoire de ces phénomènes météorologiques extrêmes s'est grandement améliorée ces dernières décennies. Une source d'erreur pour la prévision d'intensité est le manque de connaissance des processus physiques qui régissent l'évolution de la structure et de l'intensité des cyclones. Cette thèse, proposée dans le cadre des responsabilités du Centre Météorologique Régional Spécialisé (CMRS) de la Réunion et des axes de recherche du LACy et du CNRM, a pour but d'améliorer la prévision numérique et la compréhension des mécanismes de changement de structure et d'intensité des cyclones dans le sud-ouest de l'océan Indien. On observe statistiquement dans le bassin de fréquents déferlements d'ondes de Rossby qui correspondent à une intrusion des talwegs d'altitude depuis les moyennes latitudes vers les régions où évoluent les cyclones. Ces déferlements advectent dans la troposphère tropicale de l'air d'origine stratosphérique à fort tourbillon potentiel (PV). Le cœur d'un cyclone tropical étant caractérisé par un vortex cyclonique de fort PV, il est donc légitime de se demander si de tels talwegs sont capables de « nourrir » un cyclone en déferlant jusqu'à lui, et l'intensifier par superposition de PV. D'un autre côté, l'approche d'un talweg est associée à d'autres facteurs pouvant jouer en défaveur d'une intensification, comme un fort cisaillement vertical de vent. L'étude de processus est réalisée sur le cyclone Dora (2007) avec le modèle opérationnel du CMRS sur le bassin, Aladin-Réunion. Ce modèle hydrostatique à aire limitée bénéficie d'une résolution horizontale de 8 km et de son propre schéma d'assimilation 3Dvar avec bogus de vent. Un tel bogus permet d'affiner la structure du cyclone à l'instant initial en ajoutant des observations de vent déduites d'un profil analytique et des paramètres de structure du cyclone estimés par les images satellites. Des diagnostiques sur les variables thermodynamiques en sortie de modèle montrent que la phase d'intensification rapide de Dora est bien associée à l'advection de tourbillon potentiel (PV) en provenance du talweg. Bien que fortement cisaillé, le système parvient à s'intensifier grâce à la forte inclinaison du talweg qui advecte du PV au cœur du cyclone en 2 temps et à 2 niveaux (haute et moyenne troposphère). Lorsque le talweg est au plus proche du cyclone, il force un processus dynamique interne appelé « cycle de remplacement du mur de l'œil ». On observe une inclinaison et un renforcement des vitesses verticales à l'extérieur du mur de l'œil principal, associé à une accélération de la circulation cyclonique tangentielle par advection de moment angulaire sur toute l'épaisseur de la troposphère dans cette zone annulaire (mis en évidence par les flux d'Eliassen-Palm). Un second maximum de vent relatif apparaît alors et une deuxième phase d'intensification rapide s'ensuit avec la contraction du mur secondaire. Le forçage de processus internes par une influence externe (un talweg) semble donc être le moteur de l'intensification rapide de Dora dans un environnement cisaillé, et potentiellement celui d'autres cyclones dans le bassin qui sont approchés par des talwegs d'altitude. Les prévisionnistes du CMRS sont invités à surveiller les champs de PV de tels systèmes, en attendant que de plus amples diagnostiques soient réalisés avec l'outil d'inversion du tourbillon potentiel développé sur le modèle global Arpège. / Despite significant improvements in Tropical Cyclone (TC) track forecasts over the past few decades, anticipating the sudden intensity changes of TCs remains a major operational issue. The main purpose of this thesis is to analyze TC rapid intensification processes in relation with external forcing induced by upper-level troughs originating from the mid-latitudes. The impact of initial storm structure on storm evolution and prediction is also documented. An objective definition for rapid intensification in the southwest Indian Ocean is first proposed. The location and frequency of TC-trough interactions are identified, as well as TC-trough arrangements conducive to TC intensification. An interesting study case, TC Dora (2007), is chosen to run numerical simulations initialized with synthetic TC observations blended in a global analysis. The simulated TC-trough interaction is intricate with potential vorticity (PV) advection from the trough into the TC core at mid and upper levels. Vortex intensification first occurs inside the eyewall and results from PV superposition. Further intensification is associated with a subsequent secondary eyewall formation triggered by external forcing from the trough. The numerical model is able to reproduce the main features associated with outer eyewall spin-up, inner eyewall spin-down, and their effects on vortex intensity changes. Another numerical study examines typhoons in the northwest Pacific and demonstrates the critical role played by initial vortex structure in TC track and intensity prediction. Upgrading the initial specification of a TC inner-core structure in numerical models is recommended for future TC prediction improvements.

Une étude numérique de la dynamique d'ondes internes de gravité en fluide stablement stratifié est menée. On décrit un algorithme pseudo-spectral<br />parallèle permettant d'intégrer les équations de Navier-Stokes sur une machine paralèele. En deux dimensions d'espace, on analyse la dynamique d'un<br />champ d'ondes internes propagatives, d'amplitude modérée et initialement plan et monochromatique. Le champ d'ondes est instable et déferle. Le déferlement produit une turbulence de petites échelles spatiales influencées par la stratification. L'étude<br />est étendue au cas tridimensionnel, plus réaliste. En trois dimensions, on étudie le même champ d'ondes internes, que l'on perturbe par un bruit infinitésimal ondulatoire tridimensionnel, mais on considère des ondes statiquement stables et<br />instables (grandes amplitudes). On montre que le déferlement d'une onde interne est un processus intrinsèquement tridimensionnel, y compris pour les ondes de faible amplitude. La tridimensionalisation du champ d'ondes s'opère dans les zones de l'espace où le champ de densité devient statiquement instable. L'effondrement gravitationnel d'une zone est de structure transverse au plan de propagation de l'onde. Les effets de la turbulence des petites échelles sur la production de la composante non propagatrice de l'écoulement, le mode de vorticité potentielle et la production d'un écoulement moyen, permet de conclure que seule une petite proportion de l'énergie mécanique initiale est convertie sous ses deux formes, la majeure partie étant dissipée par la dissipation visqueuse et conduction thermique. On reconsidère le mode de vorticiée potentielle par une approche Hamiltonienne non-canonique du fluide parfait stratifié. La dérivation d'un système de dynamique modifiée permet d'étudier la relaxation d'un écoulement stratifié, conservant sa vorticité potentielle et sa densité, vers un état stationnaire d'énergie minimale, correspondant au mode de vorticité potentielle.