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Celestial Ceneus
basically a survey or count of celestial objects in the universe — like stars, planets, galaxies, nebulae, and other cosmic bodies → looks at different types number and distributions
Stellar Masses:
Determined through looking at binary star systems
1. Visual
Spectroscopic
Eclipsing
Ranges for masses
Stars: 1/12 < m < 250
BROWN Dwarfs: 1/100 < m < 1/12
Considered failed stars
Planets: m < 1/100
Binary Star Systems
a system of two stars orbiting a common center of mass
Visual method for determining mass
Both stars can be directly seen through a telescope as two separate points of light
Spectroscopic method for determining mass
Stars are too close to be resolved visually, but their spectral lines show Doppler shifts as they move toward or away from us
Shows two spectral line movements
Eclipsing method for determining mass
The orbital plane is edge-on to our line of sight, so the stars pass in front of each other, causing brightness variations
Looks similar to the transit graph
Mass-Luminosity Relationship
More massive a star the more luminous: L ~ M3.9
Stellar Mass Calculations: Newton’s Versions of Kepler’s third law
D3= (M1+ M2)P2
D = semimajor axis of the orbit of one with respect to the other in AU
P = period with which they go around each other in years
M1+M2 = Both masses are non-negligable and its their sum
Barycentre/ Centre of mass
The point about which the stars will orbit
The star with the higher mass will be closer to the barycentre and move with a slower velocity
Stellar Radii Ranges
Fainter stars are smaller than brighter stars
Star Sizes by Occultations
An occultation occurs when a larger object passes in front of a smaller, more distant object, temporarily blocking its light
Measure the time it takes for the star’s light to disappear and reappear
Using the speed of the occulting object the stars angular diameter can be calculated
By measuring the distance to the star its size can be measured
Star Sizes by Eclipsing Binaries
A binary star system where the orbital plane is aligned so that one star passes in front of the other as seen from Earth → causing a periodic dips in brightness
Primary Eclipse: Brighter star is partially or fully blocked → largest dip in brightness.
Secondary Eclipse: Dimmer star is blocked → smaller dip.
Contacts:
First Contact: Beginning of brightness drop.
Second Contact: Smaller star fully hidden (total eclipse starts).
Third Contact: Smaller star starts to reappear (total eclipse ends).
Fourth Contact: Eclipse fully over, brightness returns to normal.
T2 - t1 = second contact to first contact time
T3 - t1 = third contact to first contact time
Star Sizes by Stefan-Boltzmann Law:
Luminosity and Temperature of a star
L=4πR2σT4
Rewritten as:
Need luminosity from apparent brightness and distance (flux) and temperature from colour index (B-V) or spectral type
HR Diagrams
the relationship between a star's luminosity and its surface temperature
Axes
X-axis: Surface temperature (hot → cold from left to right or vice versa depending on convention)
Y-axis: Luminosity (brightness) increases upward
Observations from HR diagrams
Classification of the star
Determine its evolutionary stage
Estimate size
Estimate Temperature
Estimate luminosity
Mass determines a Star’s positions on the HR Diagrams:
Higher mass → hotter and more luminous → top-left
O, B, A
Medium Stars
F and G
Lower mass → cooler and dimmer → bottom-right
K and M
Main Sequence
A diagonal band from top-left (hot, luminous) to bottom-right (cool, dim)
This band is where 90% of stars lie showing a strong correlation
Where they spend most of their lives
These stars eventually become giants/ supergiants
Spectral Class vs luminosity
Giants/Supergiants: Above this main sequence → large radius and very luminous however they have cooler surfaces
Tend to become white dwarfs later on
Around 10% of stars
White dewars: Below the main sequence → Small radii but have high temperatures with lower luminosities
Better seen in UV