Exploring Mesoscale Structures Using Chord Occultations of Saturn's Rings

Exploring Mesoscale Structures Using Chord Occultations of Saturn's Rings

University of Central Florida STARS Honors Undergraduate Theses UCF Theses and Dissertations 2021 Exploring Mesoscale Structures using Chord Occultations of Saturn's Rings Lamia Benyamine University of Central Florida Part of the The Sun and the Solar System Commons Find similar works at: https://stars.library.ucf.edu/honorstheses University of Central Florida Libraries http://library.ucf.edu This Open Access is brought to you for free and open access by the UCF Theses and Dissertations at STARS. It has been accepted for inclusion in Honors Undergraduate Theses by an authorized administrator of STARS. For more information, please contact [email protected]. Recommended Citation Benyamine, Lamia, "Exploring Mesoscale Structures using Chord Occultations of Saturn's Rings" (2021). Honors Undergraduate Theses. 915. https://stars.library.ucf.edu/honorstheses/915 EXPLORING MESOSCALE STRUCTURES USING CHORD OCCULTATIONS OF SATURN’S RINGS by LAMIA BENYAMINE A thesis submitted in partial fulfillment of the requirements for the Honors Undergraduate Thesis in Physics in the College of Sciences and in the Burnett Honors College at the University of Central Florida Orlando, Florida Spring Term 2021 ABSTRACT The intent of this thesis is to examine mesoscale structures found in stellar occultations of Saturn's rings. The Cassini spacecraft orbited Saturn for over 13 years and collected stellar occultations using an Ultraviolet Imaging Spectrograph (UVIS). Chord occultations were analyzed using autocorrelations at minimum ring plane radius to visualize the structure and correlation in the azimuthal direction. These particle tracking occultations cut a chord across the rings in the path of the star. By taking the autocorrelation of these chord occultations, 8 out of the 66 showed clumping within the first 3.0 km in azimuth representing signs of a structure. Six of those occultations could be moonlets or propellers as their minimum ring plane radii are in the Propeller Belt region. The Fast Fourier Transform Power Spectrum of the autocorrelation was also taken, and 6 of the 8 had high peak power outputs at certain wavelengths. It is also observed that five of the occultations may contain self-gravity wakes. ii LIST OF FIGURES Figure 1a: Cassini UVIS mechanical characteristics with the four different channels (Esposito et al., 2004) ......................................................................................................................................... 2 Figure 1b: (Top) UVIS stellar occultations showing optical depth of Saturn’s main rings (A, B, C) and Cassini Division) at about 10 km radial resolution as a function of ring plane radius. (Bottom) A mosaic of the main rings from ISS (Colwell et al., 2009). .......................................... 3 Figure 1.1a: The star ε Canis Majoris is occulted by the shadowed rings of Saturn indicated by the stippling. Also, the FUV occultation slit and HSP are shown around the star. The stippling indicated shadowed regions of Saturn and its rings (Esposito et al., 1998). The blue curve illustrates a potential path of a star behind the rings as seen from Cassini, and the red arrow shows the minimum ring plane radius sampled by this occultation. At this turnaround point, the star’s distance from Saturn changes very slowly and the occultation samples change in the azimuthal or orbital direction. ......................................................................................................... 5 Figure 1.2a: Data from a UVIS particle tracking occultation of the star KapOri279 taken from rmin123,211 km, located in the Cassini Division. Ingress (blue) and egress (red) portions of the chord occultation. ............................................................................................................................ 6 Figure 1.3a: Near the Encke Gap of the A ring, a propeller 5 km in radial dimension, 60 km in azimuthal dimension (Sremcevic et al., 2013). ............................................................................... 8 Figure 1.3b: Number of propellers against radius in the Propeller Belt regions of the A ring. Resolved propellers are noted by solid bars, and the cross-hatched bars indicate unresolved features (Tiscareno et al., 2008). ..................................................................................................... 8 Figure 1.4a: Geometric model of self-gravity wakes displaying the parameters that affect the ring opacity. ϕ-ϕwake is the viewing angle ϕ with respect to the wake alignment (Colwell et al., 2006). .............................................................................................................................................. 9 Figure 2.3a: Graph of cosine of x with a lag of 1. ....................................................................... 11 Figure 2.3b: Autocorrelation of cosine of x with a lag of 1. ....................................................... 11 Figure 2.4a: An example FFT PS of the autocorrelation of cosine. ............................................ 12 Figure 3.1a: The data of AlpCru100 within 5 km of the minimum ring plane radius in azimuthal distance. ........................................................................................................................................ 13 Figure 3.1b: The data of AlpCru100 at the minimum ring plane radius with separated ingress and egress data. ............................................................................................................................. 14 Figure 3.2a: The autocorrelation of AlpAra085 at the turnaround point with a lag of 20,000, displaying 0.3 km in the azimuthal direction. ............................................................................... 15 Figure 3.2b: The autocorrelation of KapOri280 at the turnaround point with the same lag and distance as 3.2a. ............................................................................................................................ 15 iii Figure 3.2c: The autocorrelation of AlphaCru100 at the turnaround point with a lag of 20,000, displaying 3.0 km in the azimuthal direction. ............................................................................... 15 Figure 3.2e: The autocorrelation of AlpVir008 at the turnaround point with a lag of 20,000, displaying 0.3 km in the azimuthal direction. ............................................................................... 17 Figure 3.2f: The autocorrelation of AlpVir008 turnaround point with the same lag as 3.2e, but 3.0 km in azimuth. ........................................................................................................................ 17 Figure 3.2g: The autocorrelation of ZetCMa169 turnaround point with a lag of 20,000 displaying 0.3 km in the azimuthal direction. ............................................................................... 17 Figure 3.3a: The FFT fractional power spectral density taken of the autocorrelation of AlphaCru100 and displaying the power output at each wavelength. ............................................ 19 Figure 3.3b: The same FFT fractional power spectral density done in 3.3a zooming in to 3.0 km in wavelength. ............................................................................................................................... 19 Figure 3.3c: The FFT fractional power spectral density taken of the autocorrelation of ZetCMa169 and displaying the power output at each wavelength zooming in to 3.0 km in wavelength. ................................................................................................................................... 19 Figure 4a: Displaying the main rings along ring plan radius with labeled possible structures in the observed. occultations ............................................................................................................. 22 iv LIST OF TABLES Table 3.1: Lists the length in meters of azimuth that it takes for the autocorrelation to drop to zero at ����. “*” indicates occultations that showed humps in the autocorrelation. “#” indicates occultations where the ingress and egress data at ���� are not similar. ...................................... 16 Table 3.3: Peak fractional power outputs of the FFT of the autocorrelation function. ................ 18 v TABLE OF CONTENTS 1. INTRODUCTION ...................................................................................................................... 1 1.1 Chord Occultations ...................................................................................................................................................... 4 1.2 Ingress and Egress ....................................................................................................................................................... 6 1.3 Moonlets/Propellers .................................................................................................................................................... 7 1.4 Self Gravity Wakes ....................................................................................................................................................... 9 2. METHODS ............................................................................................................................... 10 2.1 Dataset ....................................................................................................................................................................... 10 2.2 Mapping ....................................................................................................................................................................

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