AST 300 Study Notes: Planet + Star Formation
AST 300 Study Notes: Planet + Star Formation
Overview of Solar System Formation
The formation of the Solar System involves several key processes and events.
Sun Ignition: The Sun ignites when nuclear fusion begins, clearing the protoplanetary disk of gas and dust.
Inner Planets: Despite the Sun igniting, objects in the Solar System were still in motion, leading to gravitational instability.
Late Heavy Bombardment (LHB): Occurred approximately 4 billion years ago, characterized by:
- A significant number of impact events on inner planets.
- Possible effects include:
- Delivery of water to Earth.
- Causing Venus to rotate retrograde.
- Displacing Uranus, resulting in an axial tilt.
- General chaos in the inner solar system.
Systems with Hot Jupiters
Migration Inward: Pertains to the movement of large gas giants towards their stars, influenced by several factors:
- Disk: The presence of a protoplanetary disk affects migration.
- Eccentricity: Planets can have varying eccentric orbits during and after migration.
- Ex Situ Formation: Planets that form beyond the frost line are later drawn in.
- In Situ Formation: Direct formation takes place in their current positions.
- Tidal Migration: Gravitational interactions with the disk can influence planetary orbits.
- Disk Disappearance: The phase when the protoplanetary disk dissipates.
Class Assignment: Star and Planet Formation Summary
Task: Write a narrative detailing the formation of the Sun and planets, using specified key terms:
- Key Terms: protostar, angular momentum, ices, optically thin, gravity, rocky planet, accretion, hydrogen, Jeans Mass, protoplanetary disk, condensation, Main-Sequence, metals, fragmentation, moons, density, fusion, gas giant, optically thick, pressure, Zero-Age Main Sequence (ZAMS), Giant Molecular Cloud (GMC), rocks, helium, free-fall.Hertzsprung-Russell (HR) Diagram Plot: Include a sketch representing the Sun's evolutionary track.
High Mass Stars and Star Formation
High Mass Stars: These stars reach the Main Sequence (MS) first, affecting the formation of other stars:
- Pros:
- Influence on surrounding gas dynamics, promoting more star formation.
- Create stellar winds that may help clear the region for cleaner stellar formations.
- Cons:
- Their strong radiation can inhibit the formation of new stars in their vicinity.
- They may disrupt forming systems with their supernova explosions.
Study of Stromgren Spheres
Definition: Regions around O-type stars where hydrogen gas is ionized, creating an optically thin area.
Key Parameters:
- Stromgren Radius (R_S): The size of the ionized region.
- Photon Production Rate (Q*): The rate at which the star produces ionizing photons, measured in photons/sec.
- Recombination Coefficient (α(T_e)): Determines how easily electrons and protons recombine to form neutral hydrogen.
- Electron Density (n_e): Represents the number of free electrons per unit volume.
In-Class Math Problem: Size of Stromgren Sphere
Given Data:
- Nebular Temperature: T_e = 10^4 K (104 K).
- Recombination Coefficient: α = 2.6 x 10^{-19} m³ s^{-1}.
- Rate of Ionizing Photons from O star: Q* = 5 x 10^{48} s^{-1}.
- Typical Nebular Density: n_e = 10^7 m^{-3}.Calculation: Solve for R_S using the Stromgren sphere formula:
Stellar Evolution
Stellar Evolution Tracks
As stars go through their life cycles, observable properties such as luminosity and temperature change, which are plotted in HR Diagrams.
Main Sequence Life:
- Stability: A star remains on the main sequence for about 80-90% of its life.
- Evolutionary Changes: Stars do not remain identical; core composition changes significantly during this phase.
- Core Fusion Process:
- Hydrogen converts to helium, raising mean molecular mass, leading to increased core pressure.
- The relationship described by the ideal gas law requires that either central temperature (T_c) or central density (ρ_c) must increase.
Main Sequence Characteristics
Stars increase in luminosity and radius during their main sequence lifetime while effective temperature decreases due to the core's heating dynamics.
For the Sun, this phase lasts roughly 9.8 Gyr after reaching ZAMS.
Evolution on the HR Diagram
Once the hydrogen core is depleted, hydrogen fusion transitions to occur in a shell around the core, leading to changes in luminosity and radius affecting the star's position on the HR diagram.
Shell Hydrogen Fusion Period
After the core depletes its hydrogen reserves, it becomes isothermal:
- Isothermal Region: The temperature remains constant for inner parts; density must increase towards the core to support material above in hydrostatic equilibrium.
- Schönberg-Chandrasekhar Limit: Defines the maximum mass fraction for an isothermal core.
Transition to Red Giant Branch
Key Changes:
- The core collapses if it exceeds the Schönberg-Chandrasekhar limit, leading to rapid stellar evolution.
- Characteristics of a 1 M¤ star on the Red Giant Branch:
- Radius: Approximately 170 R¤.
- Temperature of Photosphere: Approximately 3000 K.
- Luminosity: Approximately 2300 L¤.
Degeneracy in the Core
As the density in the core continues to rise, electrons become degenerate, influencing stellar behavior:
- Electron Degeneracy: Governed by the Pauli Exclusion Principle, restricting electron states.
- Pressure Dynamics: In degenerate gases, pressure does not depend on temperature; electron degeneracy pressure stabilizes the core as temperature rises.
Helium Flash
When temperature reaches about 10^8 K, helium fusion commences, initiating a helium flash:
- Rapid energy generation changes core dynamics significantly—heat spreads rapidly through conduction.
Horizontal Branch Star Phase
After beginning helium fusion, the Red Giant transitions to a Horizontal Branch status:
- Characteristics of a Horizontal Branch Star (1 M¤):
- Radius: Approximately 10 R¤.
- Temperature of Photosphere: Approximately 5000 K.
- Luminosity: Approximately 100 L¤.
Stellar Fusion Requirements
Fusion Minimum Conditions
Fusion Type | Fusion By-Product | Minimum Core Temp (K) | Min Core Density (g/cm³) | Minimum Stellar Mass (M¤) |
|---|---|---|---|---|
Hydrogen | Helium | 13 million K | 100 | 0.08 |
Helium | Carbon, Oxygen | 100 million K | 100,000 | 0.5 |
Carbon | Oxygen, Ne, Mg, Na | 500 million K | 200,000 | 4 |
Neon | Oxygen, Mg | 1.2 billion K | 4,000,000 | ~8 |
Oxygen | Mg, Si, S, P | 1.5 billion K | 10,000,000 | ~8 |
Silicon | Si, S, Ar, Ca, Ti, Cr, Fe, Ni | ~3 billion K | 30,000,000 | ~8 |
Russell-Vogt Theorem
It states that "A star’s properties are determined primarily by its mass." If the initial mass of a star is known, its evolution can be broadly predicted.
Stellar Fate Based on Mass Range
Different mass ranges dictate the series of fusion processes and the eventual fate of a star:
Mass Range
Fusion Process
Final Fate
M < 0.08 M¤ | NO FUSION | Brown Dwarf (failed star) | | 0.08 M¤ < M < 0.5 M¤ | H -> He only (Helium)
White Dwarf
0.5 M¤ < M < 5 M¤ | H -> He AND He -> C/O (Carbon/Oxygen)
White Dwarf
5 M¤ < M < 8 M¤ | H -> He, He -> C/O, C/O -> Ne/Mg
White Dwarf
M > 8 M¤
H -> He, He -> C/O, C/O -> Ne/Mg, Ne/Mg -> Si, Si -> Fe
Neutron Star; Black Hole
Stellar Evolution Timescales
Duration for Key Fusion Processes:
- Hydrogen burning: 7 million years
- Helium burning: 700,000 years
- Carbon burning: 600 years
- Neon burning: 1 year
- Oxygen burning: 6 months
- Silicon burning: 1 dayNuclear Reactions: Govern the evolution timescale of main sequence stars and post-main sequence stars, influenced by gravity and the Kelvin-Helmholtz timescale as fusion stops and the core contracts.