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Observational Constraints on The Evolution of Dust in ...

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2 Introducti<strong>on</strong><br />

planets may eventually form) are thus ejected <strong>in</strong>to space, where they <strong>in</strong>term<strong>in</strong>gle with<br />

the surround<strong>in</strong>g Interstellar Medium (ISM). This “enriched” ISM subsequently provides<br />

the material for the next generati<strong>on</strong> <strong>of</strong> stars, eventually lead<strong>in</strong>g to the creati<strong>on</strong><br />

<strong>of</strong> the planetary systems <strong>in</strong> which life <strong>in</strong> the universe has become possible.<br />

In our own Milky Way, <strong>on</strong>e theory is that a supernova explosi<strong>on</strong> has triggered<br />

the formati<strong>on</strong> <strong>of</strong> our Sun and its protoplanetary disk, around 4.6 billi<strong>on</strong> years ago<br />

(e.g., Camer<strong>on</strong> 1962). Eight planets (Mercury, Venus, Earth, Mars, Jupiter, Saturn,<br />

Uranus, and Neptune) and countless smaller bodies (e.g. dwarf planets, comets,<br />

asteroids) were formed from the material <strong>in</strong> this pre-solar nebula. <strong>The</strong> structure and<br />

compositi<strong>on</strong> <strong>of</strong> these Solar System bodies has given the first clues to the development<br />

<strong>of</strong> models <strong>of</strong> how planets are formed.<br />

This thesis focuses <strong>on</strong> the <strong>in</strong>terplay <strong>of</strong> the young star and its protoplanetary disk,<br />

<strong>on</strong> the evoluti<strong>on</strong> <strong>of</strong> the dust particles that make up the protoplanetary disk surround<strong>in</strong>g<br />

the young star, and thus <strong>on</strong> the very first stage <strong>of</strong> the formati<strong>on</strong> <strong>of</strong> planets like<br />

those that compose our own Solar system.<br />

1.1 Low-mass Star Formati<strong>on</strong><br />

<strong>The</strong> most comm<strong>on</strong> type <strong>of</strong> stellar objects are stars <strong>of</strong> low mass (∼0.5 M ⊙ ), that dom<strong>in</strong>ate<br />

both <strong>in</strong> number and <strong>in</strong> total mass. Low-mass stars form <strong>in</strong>side relatively dense<br />

c<strong>on</strong>centrati<strong>on</strong>s <strong>of</strong> <strong>in</strong>terstellar gas and dust known as molecular clouds (Stahler & Palla<br />

2004), with the dust mak<strong>in</strong>g up ∼1 % <strong>of</strong> the mass <strong>of</strong> the cloud (Tielens 2005). This<br />

dust is believed to be sub-µm <strong>in</strong> size and to c<strong>on</strong>sist <strong>of</strong> almost completely amorphous<br />

silicate- and carb<strong>on</strong>-based gra<strong>in</strong>s (Kemper et al. 2004). <strong>The</strong>se regi<strong>on</strong>s are mostly selfgravitat<strong>in</strong>g,<br />

c<strong>on</strong>f<strong>in</strong>ed by an external pressure, magnetized and extremely cold (T ∼<br />

10 K). Under these c<strong>on</strong>diti<strong>on</strong>s, most elements are <strong>in</strong> molecular form, as revealed by<br />

observati<strong>on</strong>s <strong>of</strong> CO emissi<strong>on</strong> (Ungerechts & Thaddeus 1987). <strong>The</strong>se dense regi<strong>on</strong>s<br />

are opaque to visible light due to their high ext<strong>in</strong>cti<strong>on</strong>, but translucent at l<strong>on</strong>ger<br />

wavelengths. <strong>The</strong>refore observati<strong>on</strong>s at l<strong>on</strong>ger wavelengths can probe the <strong>in</strong>ternal<br />

structure <strong>of</strong> clouds and study star formati<strong>on</strong>.<br />

Star formati<strong>on</strong> beg<strong>in</strong>s when a regi<strong>on</strong> <strong>in</strong> the cloud cools and reaches a sufficient<br />

density <strong>of</strong> matter to satisfy the criteria for Jeans <strong>in</strong>stability, beg<strong>in</strong>n<strong>in</strong>g to collapse<br />

under its own gravity (Shu et al. 1993; Myers et al. 2000). Matter accretes toward the<br />

center at a c<strong>on</strong>stant rate. As the gas and dust c<strong>on</strong>tract from the <strong>in</strong>side-out (Shu 1977),<br />

gravitati<strong>on</strong>al energy is released through radiati<strong>on</strong> and quickly re-absorbed by the<br />

opaque envelope <strong>of</strong> material that is still collaps<strong>in</strong>g. Short wavelength radiati<strong>on</strong> from<br />

deep <strong>in</strong>side the core is then obscured when captured by the dust <strong>in</strong> the envelope, reprocessed<br />

and re-emitted at <strong>in</strong>frared or sub-millimeter wavelengths, thereby provid<strong>in</strong>g<br />

<strong>in</strong>formati<strong>on</strong> <strong>on</strong> the dusty outer envir<strong>on</strong>ment. Furthermore, when gravitati<strong>on</strong>al energy<br />

is transformed <strong>in</strong>to k<strong>in</strong>etic energy dur<strong>in</strong>g the collapse, gas particles speed up and<br />

collide, <strong>in</strong>creas<strong>in</strong>g the temperature <strong>of</strong> the form<strong>in</strong>g star and its immediate surround<strong>in</strong>gs.<br />

As a result, thermal pressure builds up, which serves to support the cloud structure<br />

aga<strong>in</strong>st further collapse.

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