Les Céphéides sont des étoiles pulsantes utilisées pour calculer les distances dans l'univers (notamment dans le Groupe Local). Elle font partie de la bande d’instabilité du diagramme de Hertzsprung-Russell. Le mécanisme κ (où κ désigne l’opacité du milieu), proposé par Eddington en 1917 pour expliquer ces variations périodiques de rayon et luminosité, est encore mal connu dans lecas de Céphéides froides (bord rouge de la bande d’instabilité) présentant une zone convective en surface.Cette thèse consiste à effectuer des simulations 3D de ces étoiles afin d’étudier l’interaction entre leurs pulsations radiales acoustiques et la convection de surface. On se ramène à un cas simple : l’étude de la propagation de modes acoustiques dans une boite cartésienne dont une partie est convective.Nous utilisons le code Heracles développé au CEA par Édouard Audit, que nous avons complété (ajout d’une étape de dissipation, passage à l’ordre 2 en temps pour l’étape de conduction).Pour valider notre code et notre modèle de Céphéide, nous reproduisons les résultats de Gastine & Dintrans (2011b) à 1D (cas purement radiatifs) et 2D (avec convection) : certaines simulations instables au κ-mécanisme (avec une saturation non-linéaire aux temps longs à 1D) redeviennent stables à 2D à cause de l’influence de la convection. La bande d’instabilité théorique du diagramme de Hertzsprung-Russell est donc trop étroite à 2D.L’hypothèse à vérifier était alors que ces Céphéides retrouvent une certaine instabilité et une saturation non-linéaire lors de simulations 3D. En effet, il est connu que les simulations 2D et 3D de convection différent à bas nombre de Prandtl, ce qui est notre cas. Dès lors, nous montrons que les panaches de convection sont en effet moins forts à 3D et ne perturbent pas autant les pulsations. On retrouve ainsi des simulations instables. Le bord rouge de la bande d’instabilité théorique est donc plus proche du bord observé à 3D qu’à 2D.Enfin, nous montrons que les modèles 1D de convection dépendante du temps de Stellingwerf (1982) et de Kuhfuss (1986) donnent des résultats similaires lorsqu’il s’agit de reproduire le profil de flux convectif des simulations 3D, lorsque la simulation présente des mouvements d’ensemble de type κ-mécanisme. Les deux modèles peinent cependant à reproduire les valeurs de ce flux convectif de manière convaincante. Cela justifie l’importance des simulations 3D. / Cepheids are pulsating stars used to calculate distances in the universe (more precisely in the Local Group). They are part of the Hertzsprung-Russell diagram’s instability strip. Their periodic variations (of luminosity and radius) are well explained by κ-mechanism, first suggested by Eddington (1917). But cold Cepheids (red edge of the instability strip) have a convective zone near their surface that affects their pulsation properties.Therefore, this PhD. thesis aims at performing 3D simulations of simplified Cepheids to study the interaction between surface convection and radial pulsations. We actually study the propagation of acoustic modes in a cartesian box partially convective.For this, we use Heracles, a hydrodynamical code developed in CEA, France, by Edouard Audit. We had to complete the code with a dissipation step and a second order (in time) conduction step (which was already available as a first order method).To validate the code and the Cepheid model used, we reproduce Gastine & Dintrans (2011b) results in 1D (radiative cases) and 2D (with convection): some setups that are unstable for κ-mecanism (with nonlinear saturation in 1D simulations) are stable in 2D thanks to convection. The theoretical Hertzsprung-Russell diagram’s instability strip is then too narrow in 2D.The hypothesis for this work was that those Cepheids would be unstable again (with saturation) in 3D due to the fact that convection grows weaker when convective plumes are 3D. 2D and 3D simulations are indeed different when Prandtl number is low as it is in our simulations. We show that pulsations are indeed not quenched anymore and that simulations are unstable. Theoretical 3D instability strip is then closer to the observed one than 2D strip was.Finally, we show that the 1D models of time-dependant convection from Stellingwerf (1982) and Kuhfuß (1986) give similar results for the convective flux of 3D convection with κ-mecanism. But none of them is able to give the exact values. That means that 3D simulations are indeed precious.

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In the current era of “precision cosmology”, measuring the expansion rate of the Universe (Hubble constant, or H0) more accurately and precisely helps to better constrain the properties of dark energy. Cepheid-based distances are a critical step in the Extragalactic Distance Scale and have been recently used to measure H0 with a total uncertainty of only 3.4%. I will present my work on Cepheid variables in three different galaxies as part of this effort. NGC 4258 is a galaxy with a very precise and accurate distance (3% uncertainty) based on radio interferometric observations of water masers orbiting its central massive black hole. Therefore, it can be used to obtain a robust absolute calibration of the Cepheid Period-Luminosity relation. I analyzed observations of NGC 4258 obtained at Gemini North over four years and increased the number of long-period Cepheids (P>45 days) known in this galaxy. NGC 5584 was the host of type Ia SN 2007af. I applied a difference imaging technique to Hubble Space Telescope (HST) observations of this galaxy and discovered several hundred Cepheids. I compared my results with previous work based on traditional PSF photometry. The distance estimates of the two samples matched within the errors of the measurements, and so the difference imaging technique was a success. Additionally, I validated the first “white-light” variability search with the HST F350LP filter for discovering Cepheids. NGC 4921 is located in the heart of the Coma cluster at a distance of about 100 Mpc. I conducted a search for Cepheid variables using HST, extending the reach of Hubble by a factor of 3 relative to previous Cepheid work. Since Coma is in the Hubble flow, this approach eliminates the need for a secondary distance indicator and enables a direct determination of H0 based exclusively on a Cepheid distance. I present preliminary results from this challenging project.

De automatiserade produktionslinjerna på Cepheid kallas Robal. Robal arbetar dygnet runt för attproducera så många patroner som möjligt. Produktionslinjen består av en grupp av stationer somtillsammans producerar patroner.Detta examensarbete är baserat på Pre-lid fyllningsstation på Robal som har syfte a dispensera enhögviskös vätska bestående av PEG, (poly etylenglykol) i patronerna. Mängden vätska somdispenseras är olika och kan skilja mellan 0.5 och 4 gram beroende på vilket recept på patron somanvänds. Receptet för CTNG patronen är fokus i detta arbete, CTNG är patronen vars har denlängsta cykeltiden, detta på grund av den kräver den största mängden vätska att dispenseras.Det praktiska arbetet för detta examensarbete var uppdelat i olika delar. Första uppgiften var attanalysera olika tryck och deras respektive dispenseringstid. Analysen utfördes genom att testaolika intervall av tryck på en dispenseringsstation placerad i labbet på Cepheid.Dispenseringsstation liknar Pre-lid stationen på Robal. Tryck mellan 40 och 400 Kpa analyseradesmed steg på 10 Kpa.Nästa uppgift var att validera om tryckkärlet som används i nuläget för att hitta det maximalatillåtna trycket som tryckkärlet får utsättas för. Uppgiften börjades med att samla ritningar påtryckkärlet för att ta fram korrekta mått som behövs i dem kommande beräkningarna.Med svenska standarden för tryckkärl [7] utfördes beräkningar på tryckkärlet. Eftersom locket äroerhört överdimensionerat så försummades locket i dessa beräkningar.När de teoretiska beräkningarna var slutförda modellerades tryckkärlet upp efter ritningar iSolidworks 2020. Med en komplett Cad-modell kunde en FEM-analys i samma mjukvara utföraspå tryckkärlet. På FEM-analysen analyserades hela tryckkärlet, inklusive locket.Tryckanalysen indikerar att dispenseringstiden drastiskt minskar med bara små ökande trycksteg.Resultat från valideringsberäkningarna visar att det trycksatta kärlet är dimensionerat enligtstandarder [7] för att hantera ett tryck högre än det inställda måltrycket.

Classical Cepheids and eclipsing binary systems are powerful probes for measuring stellar fundamental parameters and constraining stellar astrophysics. A Cepheid in an eclipsing binary system is even more powerful, constraining stellar physics, the distance scale and the Cepheid mass discrepancy. However, these systems are rare, only three have been discovered. One of these, OGLE-LMC-CEP1812, presents a new mystery: where the Cepheid component appears to be younger than its red giant companion. In this work, we present stellar evolution models and show that the Cepheid is actually product of a stellar merger during main sequence evolution that causes the Cepheid to be a rejuvenated star. This result raises new questions into the evolution of Cepheids and their connections to smaller-mass anomalous Cepheids.