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Asteroseismology of Sun-like Stars

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Presentation on theme: "Asteroseismology of Sun-like Stars"— Presentation transcript:

1 Asteroseismology of Sun-like Stars
Travis Metcalfe (HAO)

2 The Internal Constitution of the Stars
“At first sight it would seem that the deep interior of the sun and stars is less accessible to scientific investigation than any other region of the universe. Our telescopes may probe farther and farther into the depths of space; but how can we ever obtain certain knowledge of that which is hidden behind substantial barriers? What appliance can pierce through the outer layers of a star and test the conditions within?” (written in 1926) Sir Arthur Eddington (1882 – 1944)

3 Seismology: seeing with sound
Convection creates acoustic noise – some of it resonates

4 Motivation New opportunities to probe the fundamental physics of solar and stellar models. Understanding the solar structure and evolution in a broader physical context.

5 1D oscillations: violin strings
Fundamental Third overtone First overtone Second overtone

6 2D oscillations: drums Radial modes Non-radial modes

7 2D oscillations: drums Radial modes Non-radial modes

8 3D oscillations: stars Radial modes Non-radial modes

9 3D oscillations: stars Radial modes Non-radial modes

10 Pulsations cause variations in spectral lines and brightness
Observations Pulsations cause variations in spectral lines and brightness

11 Space missions will soon revolutionize the observations

12 Space missions will soon revolutionize the observations

13 Space missions will soon revolutionize the observations

14 Matching models to observations is an optimization problem
Epistemology Matching models to observations is an optimization problem

15 Optimization Easy

16 Optimization Hard

17 Evolution as optimization
“Evolution is cleverer than you are.” – Francis Crick

18 Evolution as optimization
“Evolution is cleverer than you are.” – Francis Crick

19 Genetic algorithms Generate N random trial sets of parameter values.
Evaluate the model for each trial and calculate the variance. Assign a “fitness” to each trial, inversely proportional to the variance. Select a new population from the old one, weighted by the fitness. Encode-Breed-Mutate-Decode Loop to step 2 until the solution converges.

20 Evolutionary operators

21 Parallel computing Genetic algorithms are intrinsically parallelizable
Each iteration typically has 128 model evaluations Number of processors sets the number of models that can be evaluated in parallel Also need multiple runs with different random initialization

22 Stellar parameters Total Mass Surface Temperature Chemical composition
Convective efficiency Internal chemical gradients Rotation rate Age / Evolutionary status

23 The Future: Eddington et al.
2007 and beyond: a flood of unprecedented observations


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