The fate of S-AGB stars

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The fate of S-AGB stars Why won’t my code converge? or

description

The fate of S-AGB stars. Why won’t my code converge?. or. Work in Progress! No answer yet!. Herbert Lau Pilar Gil Pons Carolyn Doherty Me. Overview. Numerical problem ?. Massive AGBs fail to converge when M env about 2 M ʘ. Physical problem ?. Overview. Numerical problem ?. - PowerPoint PPT Presentation

Transcript of The fate of S-AGB stars

Page 1: The fate of S-AGB stars

The fate of S-AGB stars

Why won’t my code converge?

or

Page 2: The fate of S-AGB stars

Work in Progress!No answer yet!

Herbert Lau Pilar Gil Pons Carolyn Doherty Me

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Overview

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Overview

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Looking at the facts:when does it happen?

The divergence happens for different evolution codes (EVOLV, MONSTAR)

Can be delayed by increasing alpha (MLR)=>

increasing mixing efficiency (Herwig et al., Althaus et al,…)

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Looking at the facts:when does it happen?

Comparison: the last two TPs

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Pg < 0

Code dies with negative gas pressure T and P are dependent variables

So values chosen by matrix solution Prad = 1/3aT4 then known Pgas = P – Prad is known Then the e.o.s. tells us

So a Pg < 0 error means Prad provides all of P ie < 0 and L > LEdd

See Wood and Faulkner 1986!!

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Looking at the facts: contribution P/Prad in the hydrostatic case

Radiative case:

Edd

rad

L

L

P

P 1

then:

r

rrad

cGM

L

dP

dP

4

with:

cGMLEdd

4

Convective case:

Edd

rad

L

L

P

P'

1

then:

rr

rrad

cGM

L

dP

dP

4

with:

rEdd

cGML

4'

0

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Looking at the facts

ρe, Pe, Teρ+Δρ P+ΔPT+ΔT

ρ, P, T

g

H

C

acTU p

mp

8322

3

re U9

82/3

Conductivity radiation-to-convection

U >> convection inefficient

U << convection efficientρe, Pe, Te

ar

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After last TP

We have very inefficient convection here…

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What pushes L > LEdd ?

rEdd

cGML

4'

Reduce LEdd by increasing <> ???

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Petrovic et al (2006) OPAL opacity tables display a peak due to presence of Fe,

Ni at T aprox. 250000 K This peak causes huge inflation and departure of

hydrostatic equilibrium in WR stars Could this be our case?

Hypothesis κ-peak

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Testing the κ-peak hypothesis:We do find the κ-peak

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Look at that radius!

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We smoothed out the peak

and the code keeps converging!

The star lost a further 0.5 Msun

Before it died again!.

Testing the κ-peak hypothesis:

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But there is another larger opacity peak…

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And another!

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Hypothesis κ-peak

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Multiple κ-peaks We doubt the star can avoid its fate… Deep envelope and low density mean a region of

increasing opacity The high luminosity drives dramatic expansion In our hydrostatic case its supersonic!

103 – 104 R per year!

What does a REAL star do? We think the energy involved < binding energy of the

envelope But it might drive periodic, enhanced mass-loss at

least?

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We need to sort this out!

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The general picture

L>LEddLoss of hydrostatic eq

extreme low ρ-high T zone

code converges

Energy released after K peak

If we avoid the K peak