Title: Chapter 14
1Chapter 14 Chemical Analysis
- Review of curves of growth
- How does line strength depend on excitation
potential, ionization potential, atmospheric
parameters (temperature and gravity),
microturbulence - Differential Analysis
- Fine Analysis
- Spectrum Synthesis
2The Curve of Growth
- The curve of growth is a mathematical relation
between the chemical abundance of an element and
the line equivalent width - The equivalent width is expressed independent of
wavelength as log W/l
Wrubel COG from Aller and Chamberlin 1956
3Curves of Growth
- Traditionally, curves of growth are described
in three sections - The linear part
- The width is set by the thermal width
- Eqw is proportional to abundance
- The flat part
- The central depth approaches its maximum value
- Line strength grows asymptotically towards a
constant value - The damping part
- Line width and strength depends on the damping
constant - The line opacity in the wings is significant
compared to kn - Line strength depends (approximately) on the
square root of the abundance
4The Effect of Temperature on the COG
- Recall
- (under the assumption that Fn comes from a
characteristic optical depth tn) - Integrate over wavelength, and let lnrNa
- Recall that the wavelength integral of the
absorption coefficient is - Express the number of absorbers in terms of
hydrogen - Finally,
5The COG for weak lines
Changes in log A are equivalent to changes in log
gfl, qc, or kn For a given star curves of growth
for lines of the same species (where A is a
constant) will only be displaced along the
abcissa according to individual values of gfl, c,
or kn. A curve of growth for one line can be
scaled to be used for other lines of the same
species.
6A Thought Problem
- The equivalent width of a 2.5 eV Fe I line in
star A, a star in a star cluster is 25 mA. Star
A has a temperature of 5200 K. - In star B in the same cluster, the same Fe I line
has an equivalent width of 35 mA. - What is the temperature of star B, assuming the
stars have the same composition - What is the iron abundance of star B if the stars
have the same temperature?
7The Effect of Surface Gravity on the COG for Weak
Lines
- Both the ionization equilibrium and the opacity
depend on surface gravity - For neutral lines of ionized species (e.g. Fe I
in the Sun) these effects cancel, so the COG is
independent of gravity - For ionized lines of ionized species (e.g Fe II
in the Sun), the curves shift to the right with
increasing gravity, roughly as g1/3
8Effect of Pressure on the COG for Strong Lines
- The higher the damping constant, the stronger the
lines get at the same abundance. - The damping parts of the COG will look different
for different lines
9The Effect of Microturbulence
- The observed equivalent widths of saturated lines
are greater than predicted by models using just
thermal and damping broadening. - Microturbulence is defined as an isotropic,
Gaussian velocity distribution x in km/sec. - It is an ad hoc free parameter in the analysis,
with values typically between 0.5 and 5 km/sec - Lower luminosity stars generally have lower
values of microturbulence. - The microturbulence is determined as the value of
x that makes the abundance independent of line
strength.
10Microturbulence in the COG
5 km/sec
0 km/sec
Questions At what line strength do lines
become sensitive to microturbulence? Why is it
hard to determine abundances from lines on
the flat part of the curve of growth?
11Determining Abundances
- Classical curve of growth analysis
- Fine analysis or detailed analysis
- computes a curve of growth for each individual
line using a model atmosphere - Differential analysis
- Derive abundances from one star only relative to
another star - Usually differential to the Sun
- gf values not needed
- Spectrum synthesis
- Uses model atmosphere, line data to compute the
spectrum
12Jargon
- m/H log N(m)/N(H)star log N(m)/N(H)Sun
- Fe/H -1.0 is the same as 1/10 solar
- Fe/H -2.0 is the same as 1/100 solar
- m/Fe log N(m)/N(Fe)star log N(m)/N(Fe)Sun
- Ca/Fe 0.3 means twice the number of Ca atoms
per Fe atom
13Solar Abundances from Grevesse and Sauval
14Basic Methodology for Solar-Type Stars
- Determine initial stellar parameters
- Composition
- Effective temperature
- Surface gravity
- Microturbulence
- Derive an abundance from each line measured using
fine analysis - Determine the dependence of the derived
abundances on - Excitation potential adjust temperature
- Line strength adjust microturbulence
- Ionization state adjust surface gravity
15Projects!
- You may work in teams (1, 2 or 3 students)
- Perform an analysis of the spectrum
- Confirm the atmospheric parameters
- (optional) Measure the abundance of the atomic
species in homework 3 - Use Moog
- Chris Sneden MOOG
- or use the computers in Rm 311 with Moog already
installed
16Data
- Select one of the data archives
- FTS archive
- Wallace Hinkle 1996, APJS, 107, 312
- DPP NOAO Digital Library
- ELODIE archive
- Prugniel Soubiran 2001, AA, 369, 1048
- The ELODIE archive
- Others?
- Work with published EQW data
- Select a sample of stars, at least one per team
member
17Whats known?
- Review the literature for your selected object
- extant photometry
- 2MASS, ISO data?
- radial velocity measurements?
- IUE/STIS spectra?
- previous atmospheric analyses?
- metallicity determinations? (see Catalogue of
Fe/H (Cayrel de Strobel, 1997)
18Step 3
- Measure equivalent widths/detailed COG
- Spectrum Synthesis?
- Use Thevenin line data
- wavelength
- e.p.
- gf
- may work differentially to Arcturus (optical or
IR) or the Sun if needed