<div>Planetary rings are, and have been, a common feature throughout the solar system.</div><div>Rings have been observed orbiting each of the giant planets, several Trans-Neptunian Objects, and debris rings are thought to have orbited both Earth and Mars.</div><div>The bright, massive planetary rings orbiting Saturn have been observed for centuries, and the Cassini Mission has given researchers a recent and extensive closeup view of these rings.</div><div>The Saturn ring system has served as a natural laboratory for scientists to understand the dynamics of planetary ring systems, as well as their influence on satellites orbiting nearby.</div><div>Researchers have shown that planetary ring systems and nearby satellites can be tightly-coupled systems.</div><div><br></div><div>In this work, I discuss the physics which dominate the dynamical evolution of planetary ring systems, as well as the interactions with any nearby satellites.</div><div>Many of these dynamics have been incorporated into a one-dimensional mixed Eulerian-Lagrangian numerical model that I call "RING-MOONS," to simulate the long-term evolution of tightly coupled satellite-ring systems.</div><div>In developing RING-MOONS, I have discovered that there are three evolution regimes for tightly-coupled satellite-ring systems which I designate as the "Boomerang," "Torque-Dependent," and "Slingshot" regimes.</div><div>Each regime may be defined using the rotation period of the primary body and the bulk density of the ring material.</div><div><br></div><div>The slow rotation period of Mars places it in the Boomerang regime.</div><div>I hypothesize that a giant impact with Mars ejected material into orbit, forming a debris ring around the planet.</div><div>Using RING-MOONS, I demonstrate how Lindblad torques cause satellites which form at the edge of the ring to initially migrate away from the ring, but over time as the mass of the ring decreases, tidal torques always cause the satellites to migrate inwards.</div><div>Assuming the satellites rapidly tidally disrupt upon migrating to the rigid Roche limit, a new ring is formed.</div><div>I show that debris material cycles between orbiting Mars as a planetary ring, or as discrete satellites, and that Phobos may be a product of a repeated satellite-ring cycle.</div><div>Uranus, which has a faster rotation rate falls within the Torque-Dependent regime.</div><div>Hypothesizing that a massive ring once orbited Uranus, I use RING-MOONS to demonstrate how the satellite Miranda may have formed from such a ring, and migrated outwards to its current orbit, but that any other satellites would have migrated inwards overtime.</div><div><br></div><div>Lastly, I examine Trans-Neptunian Objects (TNOs) in binary systems.</div><div>Tidal torques exerted on each body can decrease the mutual semi-major axis of the system.</div><div>I outline the conditions for which a fully synchronous system may experience a complete decay of the mutual orbit due to tidal torques.</div><div>As the semi-major axis decreases, it is possible for the smaller of the two bodies to shed mass before coming into contact with the more massive to form a contact binary.</div><div>I hypothesize that Chariklo and Chiron are contact binaries that formed via the tidal collapse of a binary TNOs system, and demonstrate how mass shedding may have occurred to form the rings observed today.</div>

Ce manuscrit présente des travaux originaux sur la théorie de la formation des planètes.Le but fondamental est de connecter la composition chimique des planètes géantes etdes petits corps avec les processus physiques et chimiques prenant lieu dans le disqueprotoplanétaire.1. Dans le chapitre 1 j'introduis les propriétés fondamentales des disques protoplané-taires ainsi que les bases de la théorie de formation des planètes.2. Dans le chapitre 2 j'attaque le problème du rapport C/O supersolaire mesurérécemment dans WASP 12b. J'élabore un modèle qui suit la distribution et transportde l'eau et du CO gazeux et solides à travers leurs di_usion, condensation,coagulation, gaz drag et sublimation afin de quantifer la variation du rapport C/Odans le disque en fonction du temps et de la distance. Mon modèle montre que,au fur et à mesure du temps, les vapeurs vont être enlever de l'intérieur de leurlignes de glaces respectives, avec le vapeur CO enlevé beaucoup plus lentement quela vapeur d'eau. Cette effet va augmenter le rapport C/O à l'intérieur de la lignede glace de l'eau d'une valeur initiale solaire (0.55) vers une valeur au voisinagede l'unité, permettant de former des planètes géantes avec des rapports C/O _ 1,comme WASP 12b. Je fnis ce chapitre en discutant les preuves observationnellesde cette enlèvement des vapeurs à l'intérieur des lignes de glaces.3. Dans le chapitre 3 j'utilise le même modèle pour interpréter la composition chimiqued'Uranus et Neptune. Je montre comment la formation de ces deux planètessur la sur-densité de glaces prédite par mon modèle sur la ligne de glace de CO peutexpliquer pourquoi ces planètes sont à la fois riches en carbone, pauvres en azote etavec des valeurs D/H sous-cométaires.4. Dans le chapitre 4 je change de sujet vers les propriétés chimiques des météoriteschondritiques, surtout leurs rapports D/H. J'utilise un modèle de disques à 2 couches(actif et morte) avec une code d'évolution D/H pour vérifier si les profiles thermiquesnon monotone trouvés dans ces disques peuvent expliquer la large gamme des valeursD/H trouvé entre les différents familles chondritiques. Je finis ce chapitre en discutantles implications de ce modèle des disques contenant des zones mortes sur laformation de Jupiter.5. Finalement je résume nos résultats dans Conclusions & perspectives, et finis enposant des questions que j'espère voir résolus prochainement. / In this manuscript I present multiple original works on planets formation theory. Themain goal is to connect the chemical composition of giant planets and small bodies to thephysical and chemical processes taking place in the protoplanetary disk.1. In chapter 1 I introduce the fundamental properties of disks and the basics ofplanets formation theory.2. In chapter 2 I tackle the supersolar C/O and subsolar C/H ratios measured recentlyin WASP 12b. I elaborate a model that tracks water and CO vapors and icesevolution through di_usion, condensation, coagulation, gas drag and sublimation inorder to quantify the variation of the C/O ratio as a function of distance and time.My model shows that, over time, vapors will get permanently depleted inside oftheir respective snowlines with CO getting depleted much slower than water. Thiswill increase the C/O ratio inside of the water snowline from the solar value of 0.55to near unity, allowing the formation of giant planets with C/O _ 1, such as WASP12b. I end this chapter by discussing the observational proofs for the existence ofsuch vapor depletions inside the icelines3. In chapter 3 I use the same model to interpret the chemical composition of Uranusand Neptune. I show how the formation of both planets on the CO snowline's icesoverdensity predicted by this model can explain why both planets are rich in carbon,poor in nitrogen and have subcometary D/H ratios.4. In chapter 4 I shift the discussion to the chemical properties of chondritic meteorites,mainly their D/H ratios. I use a snapshot from a layered (active + dead)zones disk model with a D/H ratio evolution code to check if the non monotonicthermal pro_les in these disks can explain the wide range of D/H ratios measuredin the di_erent chondritic families. I end this chapter by discussing the implicationsof the dead zone disk models for the formation of Jupiter.5. I _nally summarize my results in Conclusions & perspectives, and _nish bypointing out several relevant open questions to be hopefully resolved soon.

Uranus is one of the least explored planets in our solar system. Event though the Uranian Ly-α emission has been a subject of study for decades, there is not a consensus on the sources contribution to the total signal. This thesis aims to analyse the contribution from scattering of the solar flux to the Uranian Ly-α dayglow by solving the radiative transfer equation in a parameter study for the atmosphere. The sources are solar Ly-α resonant scattering and Rayleigh scattering by atomic and molecular hydrogen respectively. The radiative transfer equation is solved using the Feautrier Method Program, a program written by Randall G. Gladstone. The program was adjusted to the Uranian atmosphere and modelled with different variations in parameters, including the atmospheric temperature and particle density of Ly-α scatterers and absorbers. A parameter study is performed to investigate the dependency on the Ly-α signal on these parameters. The results showed a significant Ly-α limb brightening with a maximum intensity located around 400 km outside one planetary radius as seen from the disk center. The contributions to the Ly-α dayglow from Rayleigh scattering by H2 was calculated to be 160 R whereas the contribution from resonant scattering by H was 550 R. One feature that prevents direct comparison to observed data with this thesis is that some sources that contributes to Uranus Ly-α signal are omitted in the simulations. / Uranus är en av solsystemets minst utforskade planeter. Även om dess Ly-α-strålning har undersökt, råder ännu inte konsensus kring de olika källornas bidrag till den totala Ly-α signalen. Genom att lösa ekvationen för strålningstransport i en parameterstudie ämnar examensarbetet att studera bidraget från solens två källor till Uranus Ly-α- signal. De två källorna är resonant- och Rayleigh strålningsspridning från atomärt och molekulärt väte. Ekvationen för strålningstransport beräknas av ett program som heter Feautrier Method Program, skapat av Randall G. Gladstone. Programmet har justeras till Uranus atmosfär för att kunna beräkna strålningstransport för olika atmosfärersmodeller i en parameterstudie. Parameterna som ändras är temperaturen, partikeldensiteten hos spridare och absorberare i atmosfären. Från resultaten kan parameterstudien svara på beroendet av de olika källorna till Ly-α-signalen från Uranus. Resultaten visar en tydlig ökning av ljusintensitet vid Uranus kanter med maximum runt 400 km utanför planetens radie, sett från planetens mitt. Bidraget till Ly-α-signalen från Rayleigh stålningsspridning beräknades till 160 R och från resonant strålningsspridning till 550 R. En egenskap som hindrar direkt jämförelse med resultaten från detta examensarbete och observerad data är att alla bidragande källor till Uranus Ly-α signal inte simulerats.