The Standard Solar Model and Its Evolution Marc Pinsonneault Ohio State University Collaborators: Larry Capuder Scott Gaudi.

Slides:



Advertisements
Similar presentations
1 The structure and evolution of stars Lecture 2: The equations of stellar structure Dr. Stephen Smartt Department of Physics and Astronomy
Advertisements

Standard Solar Model Calculation of Neutrino Fluxes Aldo Serenelli Institute for Advanced Study NOW 2006 Conca Specchiulla 11-Sept-2006.
Stellar Evolution. A Closer Look at the Sun Our goals for learning: Why was the Sun’s energy source a major mystery? Why does the Sun shine? What is the.
Chapter 11: Our Star © 2015 Pearson Education, Inc.
Copyright © 2012 Pearson Education, Inc. Chapter 10 Our Star 1.
Star Birth How do stars form? What is the maximum mass of a new star? What is the minimum mass of a new star?
Reminder: Reading Assignment Read Chapter 17 (“Star Birth”). Ensure that you: know the items listed in the “Summary Of Key Concepts”. Expect a quiz on.
Cosmic Chemistry: The Sun and Solar Wind Models in Science: Modeling the Sun.
Angular momentum evolution of low-mass stars The critical role of the magnetic field Jérôme Bouvier.
Stellar Evolution Stars must evolve because they shine.
The Independency of Stellar Mass-Loss Rates on Stellar X-ray Luminosity and Activity Space Telescope Science Institute – 2012.
Stars and the HR Diagram Dr. Matt Penn National Solar Observatory
Stellar Evolution. Basic Structure of Stars Mass and composition of stars determine nearly all of the other properties of stars Mass and composition of.
The Life History of Stars – Young Stars The Importance of Mass The entire history of a star depends on its mass and almost nothing else The more mass.
ASTR100 (Spring 2008) Introduction to Astronomy Our Star Prof. D.C. Richardson Sections
The birth of a star Chapter 11 1.Where are the birth places of stars? 2.What are the main components of a protostar? 3.When and how a new is born? 4.What.
© 2010 Pearson Education, Inc. Chapter 21 Galaxy Evolution.
Announcements Angel Grade update Friday April 2 Reading for next class: 17.4, chapter 18 Star Assignment 7, due Monday April 5 ÜDo Angel quiz, ÜAstronomy.
The Formation and Structure of Stars Chapter 9. Stellar Models The structure and evolution of a star is determined by the laws of: Hydrostatic equilibrium.
Properties of stars during hydrogen burning Hydrogen burning is first major hydrostatic burning phase of a star: Hydrostatic equilibrium: a fluid element.
The Formation and Structure of Stars
Stellar Structure Section 6: Introduction to Stellar Evolution Lecture 14 – Main-sequence stellar structure: … mass dependence of energy generation, opacity,
The Sun Astronomy 311 Professor Lee Carkner Lecture 23.
1 B.Ricci* What have we learnt about the Sun from the measurement of 8B neutrino flux? Experimental results SSM predictions SSM uncertainties on  (8B)
The Sun The Sun in X-rays over several years The Sun is a star: a shining ball of gas powered by nuclear fusion. Luminosity of Sun = 4 x erg/s =
Marc Pinsonneault (OSU).  New Era in Astronomy  Seismology  Large Surveys  We can now measure things which have been assumed in stellar modeling 
Properties of stars during hydrogen burning Hydrogen burning is first major hydrostatic burning phase of a star: Hydrostatic equilibrium: a fluid element.
Interesting News… Regulus Age: a few hundred million years Mass: 3.5 solar masses Rotation Period:
The formation of stars Learning Objective: How do stars form?
8. Solar System Origins Chemical composition of the galaxy
Formation of the Solar System
© 2004 Pearson Education Inc., publishing as Addison-Wesley Our Star.
The Sun. Our Nearest Stellar Neighbor Officially known as Sol, as in Solar System. Each star in the sky would be referred to as a sun by (hypothetical)
We are “star stuff” because the elements necessary for life were made in stars.
Astronomy 1020-H Stellar Astronomy Spring_2015 Day-33.
Chapter 9 The Sun. 9.4 The Active Sun Sunspots: appear dark because slightly cooler than surroundings:
Physics 681: Solar Physics and Instrumentation – Lecture 19 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Star Formation. Introduction Star-Forming Regions The Formation of Stars Like the Sun Stars of Other Masses Observations of Brown Dwarfs Observations.
Charles Hakes Fort Lewis College1. Charles Hakes Fort Lewis College2 Solar Interior/ Nuclear Fusion.
Science and Creationism 4. Planetary Science © Colin Frayn,
The Sun and other stars. The physics of stars A star begins simply as a roughly spherical ball of (mostly) hydrogen gas, responding only to gravity and.
© 2010 Pearson Education, Inc. Chapter 21 Galaxy Evolution.
1B11 Foundations of Astronomy Sun (and stellar) Models Silvia Zane, Liz Puchnarewicz
Composition and Mass Loss. 2 Two of the major items which can affect stellar evolution are Composition: The most important variable is Y – the helium.
Lecture 19: The Sun Our Star Some Facts about the Sun  distance from Earth: 1.5 x 10 8 km  luminosity: 3.86 x W  mass: 1.98 x kg (3.33.
© 2010 Pearson Education, Inc. 1. The Sun appears bright orange because of the extremely hot fires that are constantly burning carbon. TRUE or FALSE 2.
The Sun. Discussion What does it mean to say the Sun is in hydrostatic equilibrium?
© Colin Frayn, The Heavy Elements in Planets Where did they come from? –Heavy element fusion in massive stars –Supernova explosions.
The Fundamental Problem in studying the stellar lifecycle
Quiz #6 Most stars form in the spiral arms of galaxies Stars form in clusters, with all types of stars forming. O,B,A,F,G,K,M Spiral arms barely move,
Chapter 10 Our Star A Closer Look at the Sun Our goals for learning: Why does the Sun shine? What is the Sun’s structure?
M.R. Burleigh 2601/Unit 4 DEPARTMENT OF PHYSICS AND ASTRONOMY LIFECYCLES OF STARS Option 2601.
6 - Stellar Evolution-I. The life history of a star is determined by its mass…..
The Sun: Part 2. Temperature at surface = 5800 K => yellow (Wien’s Law) Temperature at center = 15,000,000 K Average density = 1.4 g/cm 3 Density at center.
Annoucements Go observing! Soon! The next exam is on Friday, October 8. –That is only 9 days from today.
Homework #10 Cosmic distance ladder III: Use formula and descriptions given in question text Q7: Luminosity, temperature and area of a star are related.
Lecture 12 Stellar structure equations. Convection A bubble of gas that is lower density than its surroundings will rise buoyantly  From the ideal gas.
Reading Unit 31, 32, 51. The Sun The Sun is a huge ball of gas at the center of the solar system –1 million Earths would fit inside it! –Releases the.
Death of Stars. Lifecycle Lifecycle of a main sequence G star Most time is spent on the main-sequence (normal star)
The Sun. Properties M = 2 X kg = 300,000 M Earth R = 700,000 km > 100 R Earth 70% H, 28% He T = 5800 K surface, 15,000,000 K core.
Novae and Supernovae - Nova (means new) – A star that dramatically increases in brightness in a short period of time. It can increase by a factor of 10,000.
12.1 Star Birth Our Goals for Learning How do stars form? How massive are newborn stars?
Evolution of Stars Evolution of protostars onto main sequence –Gravitational contraction –Luminosity versus temperature and radius Properties of stars.
The Sun.
Stellar Evolution and the Habitable Zone
Star Chapter 19: A Traumatic Birth
Modeling Stars.
Low Mass Stars (< 8 MSun) - Outline
Stellar Evolution.
Composition and Mass Loss
Presentation transcript:

The Standard Solar Model and Its Evolution Marc Pinsonneault Ohio State University Collaborators: Larry Capuder Scott Gaudi

Summary The Sun is predicted to become brighter as it ages for fundamental stellar structure reasons This luminosity evolution is extremely insensitive to assumptions about the input physics, except mass loss… …and the rotation of the Sun, and by extension mass loss, was very similar to the current values for the last 4 Gyr

Standard Solar Model Initial Conditions: Mass, Composition, Evolutionary State Equations of Stellar Structure –Conservation Laws The Solar Calibration –Reproduce current solar properties, adjust model uncertainties

In the Beginning… There are interesting problems around the formation of the Sun –Rotation: Hydrodynamic assembly phase Protostar-disk interaction –Mixing and Light Element Depletion –However, subsequent solar evolution is insensitive to the initial conditions (Vogt- Russell theorem)

Standard Model Assumptions and Ingredients Equation of State: OPAL; close to ideal gas Energy Generation: Adelberger et al. 2010; primarily pp Opacities: OP or OPAL; radiative core Convection Theory: MLT; convective envelope Gravitational settling included Rotation, rotational mixing, mass loss not included

Standard Luminosity Evolution Early transient phase (~30 Myr) when the Sun contracts and heats up Steady core H burning phase where the Sun steadily brightens

Why does the Sun brighten as it ages? Pressure gradient balances gravity Sun remains hot through H fusion 4 1 H => 1 4 He has a necessary implication: –8 particles -> 3 particles –To balance gravity fewer particles must move faster and the density must rise –These factors drive higher energy generation rates and luminosities in stars

Hotter More Luminous

Structural and Luminosity Changes Bahcall, Pinsonneault & Basu 2001

What Tools Do We Have to Test the Sun? Current Solar Properties: M, L, age, composition, solar wind… NeutrinosHelioseismology –Sound speed profile –Core helium profile –Scalar constraints: convection zone depth, surface helium

Good Agreement! Solar neutrinos Helioseismology implies a high O abundance –Disagreement with some recent models claiming a lower solar O, but only at ~ 2  –Sound speed agreement to 0.1 – 1% in any case

How Reliable is Solar Evolution? Vary input ingredients within error ranges Vary sources of input physics (opacities, equation of state, heavy element mixture) to test systematic errors

Net Result: Almost a Perfect Invariant! Solar L(t) is within 0.5% or better at all points during MS evolution

What About Mass Loss? Any change to solar evolution would require a drastic alteration… The current solar mass loss rate ~1.3 x g/s is far too small to impact evolution What properties of the ancient Sun could have been very different? –Look at rotation

Young Stars Can Be Rapid Rotators Denissenkov, Pinsonneault & Terndrup 2010

Link With Mass Loss More rapid rotation is linked with higher coronal X-ray luminosities and mass loss rates (Wood et al. 2005) –dM/dt ~ Lx –Lx measures coronal heating, and is observed to up to 1000x larger than solar for young stars –Higher past mass loss is reasonable

Lx is a strong function of mass and rotation rate Pizzolato et al Rossby numberRotation Period

Angular Momentum Evolution Protostellar initial state Star-disk coupling Core-envelope coupling Epstein & Pinsonneault 2012 Denissenkov, Pinsonneault & Terndrup 2010

Simple Extension of the Standard Model with Mass Loss Evolve assuming…. –dM/dt = (  /  sun )^a *(dM/dt) sun –  evolution from standard assumptions –Observed saturation in X-ray flux

Solar Evolution With Mass Loss Some Early Changes Possible However…. Rapid spin down  Solar wind rapidly converges to present-day value

What About More Severe Mass Loss? Basic issue: –Enhanced solar mass loss is most naturally driven by more rapid rotation in the younger Sun –Solar analogs are observed to reach a few times solar rotation in a few hundred Myr –Implies mass loss rates of order 10x solar or less for 90% of the solar age Sackmann & Boothroyd 2003

Tests and Future Directions Important tests of rotational history from Kepler and CoRoT will be arriving soon –Crucial check on old field stars Experimental tests of solar interiors physics Improved Wind Models