<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE dataset SYSTEM "http://tarantella.gsfc.nasa.gov/xml/dataset_048.dtd">
<dataset subject="astronomy" xmlns:xlink="http://www.w3.org/XML/XLink/0.9">
	<title>Evolutionary Sequences of Stellar Models with New Radiative 
Opacities. II. Z = 0.02</title>
	<altname type="ADC">J/A+AS/100/647</altname>
		<altname type="CDS">J/A+AS/100/647</altname>
		<altname type="brief">Evolutionary Sequences of Stellar Models with New</altname>
	<reference>
		<source>
<journal>
	<title>Evolutionary Sequences of Stellar Models with New Radiative 
Opacities. II. Z = 0.02</title>
	<author>
			<initial>A</initial>
			<lastName>Bressan</lastName></author>
	<author>
			<initial>F</initial>
			<lastName>Fagotto</lastName></author>
	<author>
			<initial>G</initial>
			<lastName>Bertelli</lastName></author>
	<author>
			<initial>C</initial>
			<lastName>Chiosi</lastName></author>
	<name>Astron. Astrophys. Suppl. Ser.</name>
	<volume>100</volume>
	<pageno>647</pageno>
		<date>
			<year>1993</year></date>
	<bibcode>1993A&amp;AS..100..647B</bibcode></journal></source></reference>
	<keywords parentListURL="http://messier.gsfc.nasa.gov/xml/keywordlists/apj_keywords.html">
			<keyword xlink:href="Hertzsprung-Russell_(HR_diagram).html">Hertzsprung-Russell (HR diagram)</keyword>
			<keyword xlink:href="stars_abundances.html">stars: abundances</keyword>
			<keyword xlink:href="stars_evolution.html">stars: evolution</keyword>
			<keyword xlink:href="stars_imaging.html">stars: imaging</keyword>
			<keyword xlink:href="stars_interiors.html">stars: interiors</keyword></keywords>
	<descriptions>
				<abstract>
					<para>
   A large grid of stellar models computed with the most recent radiative 
   opacities by Iglesias et al. (1992) is presented. The evolutionary tracks 
   have initial masses in the range 0.6 to 120 solar masses and extend from 
   the ZAMS to the beginning of the thermally pulsing regime of the AGB for 
   low and intermediate mass stars, and to the central C-ignition for higher 
   masses. Two smaller samples of stellar models are also presented. The 
   first deals with models of the same chemical composition and opacity but 
   calculated with the classical scheme of mixing. They are meant to provide 
   the necessary tool for discriminating among the two types of mixing. The 
   other sample contains models of the same composition calculated with 
   overshoot and classical radiative opacities by Huebner et al. (1977).</para></abstract>
                        <details/></descriptions>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="t1-0.6">
	<title>Table 1, M=0.60</title></tableLink>
				<tableLink xlink:href="t1-0.7">
	<title>Table 1, M=0.70</title></tableLink>
				<tableLink xlink:href="t1-0.8">
	<title>Table 1, M=0.80</title></tableLink>
				<tableLink xlink:href="t1-0.9">
	<title>Table 1, M=0.90</title></tableLink>
				<tableLink xlink:href="t1-1.0">
	<title>Table 1, M=1.00</title></tableLink>
				<tableLink xlink:href="t1-1.1">
	<title>Table 1, M=1.1</title></tableLink>
				<tableLink xlink:href="t1-1.2">
	<title>Table 1, M=1.2</title></tableLink>
				<tableLink xlink:href="t1-1.3">
	<title>Table 1, M=1.3</title></tableLink>
				<tableLink xlink:href="t1-1.4">
	<title>Table 1, M=1.4</title></tableLink>
				<tableLink xlink:href="t1-1.5">
	<title>Table 1, M=1.5</title></tableLink>
				<tableLink xlink:href="t1-1.6">
	<title>Table 1, M=1.6</title></tableLink>
				<tableLink xlink:href="t1-1.7">
	<title>Table 1, M=1.7</title></tableLink>
				<tableLink xlink:href="t1-1.8">
	<title>Table 1, M=1.8</title></tableLink>
				<tableLink xlink:href="t1-1.9">
	<title>Table 1, M=1.9</title></tableLink>
				<tableLink xlink:href="t1-2.0">
	<title>Table 1, M=2.0</title></tableLink>
				<tableLink xlink:href="t2-0.5">
	<title>Table 2, M=0.50</title></tableLink>
				<tableLink xlink:href="t2-0.55">
	<title>Table 2, M=0.55</title></tableLink>
				<tableLink xlink:href="t2-0.6">
	<title>Table 2, M=0.60</title></tableLink>
				<tableLink xlink:href="t2-0.7">
	<title>Table 2, M=0.70</title></tableLink>
				<tableLink xlink:href="t2-0.8">
	<title>Table 2, M=0.80</title></tableLink>
				<tableLink xlink:href="t2-0.9">
	<title>Table 2, M=0.90</title></tableLink>
				<tableLink xlink:href="t2-1.0">
	<title>Table 2, M=1.0</title></tableLink>
				<tableLink xlink:href="t2-1.1">
	<title>Table 2, M=1.1</title></tableLink>
				<tableLink xlink:href="t2-1.2">
	<title>Table 2, M=1.2</title></tableLink>
				<tableLink xlink:href="t2-1.3">
	<title>Table 2, M=1.3</title></tableLink>
				<tableLink xlink:href="t2-1.4">
	<title>Table 2, M=1.4</title></tableLink>
				<tableLink xlink:href="t2-1.5">
	<title>Table 2, M=1.5</title></tableLink>
				<tableLink xlink:href="t2-1.6">
	<title>Table 2, M=1.6</title></tableLink>
				<tableLink xlink:href="t2-1.8">
	<title>Table 2, M=1.7</title></tableLink>
				<tableLink xlink:href="t2-2.0">
	<title>Table 2, M=2.0</title></tableLink>
				<tableLink xlink:href="t3-2.2">
	<title>Table 3, M=2.2</title></tableLink>
				<tableLink xlink:href="t3-2.5">
	<title>Table 3, M=2.5</title></tableLink>
				<tableLink xlink:href="t3-3.0">
	<title>Table 3, M=3.0</title></tableLink>
				<tableLink xlink:href="t3-4.0">
	<title>Table 3, M=4.0</title></tableLink>
				<tableLink xlink:href="t3-5.0">
	<title>Table 3, M=5.0</title></tableLink>
				<tableLink xlink:href="t3-6.0">
	<title>Table 3, M=6.0</title></tableLink>
				<tableLink xlink:href="t3-7.0">
	<title>Table 3, M=7.0</title></tableLink>
				<tableLink xlink:href="t3-9.0">
	<title>Table 3, M=9.0</title></tableLink>
				<tableLink xlink:href="t5-2.5">
	<title>Table 5, M=2.5</title></tableLink>
				<tableLink xlink:href="t5-3.0">
	<title>Table 5, M=3.0</title></tableLink>
				<tableLink xlink:href="t5-4.0">
	<title>Table 5, M=4.0</title></tableLink>
				<tableLink xlink:href="t5-5.0">
	<title>Table 5, M=5.0</title></tableLink>
				<tableLink xlink:href="t5-7.0">
	<title>Table 5, M=7.0</title></tableLink>
				<tableLink xlink:href="t5-9.0">
	<title>Table 5, M=9.0</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>Age</name>
			<definition>Age of models</definition>
			<units>yr</units></field>
		<field>
			<name>log.L</name>
			<definition>log of total luminosity</definition>
			<units>Sun</units></field>
		<field>
			<name>log.Te</name>
			<definition>log of effective temperature</definition>
			<units>K</units></field>
		<field>
			<name>log.g</name>
			<definition>log of surface gravity</definition>
			<units>cm/s2</units></field>
		<field>
			<name>log.Tc</name>
			<definition>log of central temperature</definition>
			<units>K</units></field>
		<field>
			<name>log.rho_c</name>
			<definition>log of central density</definition>
			<units>g/cm3</units></field>
		<field>
			<name>Comp</name>
			<definition>central abundance (by mass) of H or He</definition>
			<units>---</units></field>
		<field>
			<name>XC</name>
			<definition>central abundance of 12 C</definition>
			<units>---</units></field>
		<field>
			<name>XO</name>
			<definition>central abundance of 16 O</definition>
			<units>---</units></field>
		<field>
			<name>Conv</name>
			<definition>fractionary mass of the convective core
                                    (inclusive of overshoot)</definition>
			<units>---</units></field>
		<field>
			<name>Q_disc</name>
			<definition>fractionary mass of the first mesh point where
                                    the chemical composition differs from the
                                    surface value</definition>
			<units>---</units></field>
		<field>
			<name>log.L_H</name>
			<definition>log of H luminosity</definition>
			<units>Sun</units></field>
		<field>
			<name>Q1_H</name>
			<definition>fractionary mass of the inner border of the
                                    H-rich region</definition>
			<units>---</units></field>
		<field>
			<name>Q2_H</name>
			<definition>fractionary mass of the outer border of the
                                    H-burning region. The boundary is taken
                                    where the nuclear energy generation rate
                                    becomes greater than a suitable value</definition>
			<units>---</units></field>
		<field>
			<name>log.L_He</name>
			<definition>log of He luminosity</definition>
			<units>Sun</units></field>
		<field>
			<name>Q1_He</name>
			<definition>fractionary mass of the inner border of the
                                    He-burning region  (when greater than zero
                                    He-burning is in a shell).  The boundary is
                                    taken where the nuclear energy generation
                                    rate becomes greater than a suitable value</definition>
			<units>---</units></field>
		<field>
			<name>Q2_He</name>
			<definition>fractionary mass of the upper border of the
                                    He-burning region. The boundary is taken
                                    as above.</definition>
			<units>---</units></field>
		<field>
			<name>log.L_C</name>
			<definition>log of C luminosity</definition>
			<units>Sun</units></field>
		<field>
			<name>log.L_nu</name>
			<definition>log of neutrinos luminosity (absolute value)</definition>
			<units>Sun</units></field>
		<field>
			<name>Q_Tmax</name>
			<definition>fractionary mass of the point where the
                                    temperature attains the maximum value</definition>
			<units>---</units></field></fields></tableHead>
	<tableHead>
		<tableLinks>
				<tableLink xlink:href="t4-12">
	<title>Table 4, M=12</title></tableLink>
				<tableLink xlink:href="t4-15">
	<title>Table 4, M=15</title></tableLink>
				<tableLink xlink:href="t4-20">
	<title>Table 4, M=20</title></tableLink>
				<tableLink xlink:href="t4-30">
	<title>Table 4, M=30</title></tableLink>
				<tableLink xlink:href="t4-40">
	<title>Table 4, M=40</title></tableLink>
				<tableLink xlink:href="t4-60">
	<title>Table 4, M=60</title></tableLink>
				<tableLink xlink:href="t4-100">
	<title>Table 4, M=100</title></tableLink>
				<tableLink xlink:href="t4-120">
	<title>Table 4, M=120</title></tableLink>
				<tableLink xlink:href="t5-12">
	<title>Table 5, M=12</title></tableLink>
				<tableLink xlink:href="t5-15">
	<title>Table 5, M=15</title></tableLink>
				<tableLink xlink:href="t5-20">
	<title>Table 5, M=20</title></tableLink></tableLinks>
	<fields>
		<field>
			<name>Age</name>
			<definition>Age of models</definition>
			<units>yr</units></field>
		<field>
			<name>M</name>
			<definition>current value of the Mass</definition>
			<units>Sun</units></field>
		<field>
			<name>log.L</name>
			<definition>log of total luminosity</definition>
			<units>Sun</units></field>
		<field>
			<name>log.Te</name>
			<definition>log of effective temperature</definition>
			<units>K</units></field>
		<field>
			<name>log.g</name>
			<definition>log of surface gravity</definition>
			<units>cm/s2</units></field>
		<field>
			<name>log.Tc</name>
			<definition>log of central temperature</definition>
			<units>K</units></field>
		<field>
			<name>log.rho_c</name>
			<definition>log of central density</definition>
			<units>g/cm3</units></field>
		<field>
			<name>Comp</name>
			<definition>central abundance (by mass) of H or He</definition>
			<units>---</units></field>
		<field>
			<name>XC</name>
			<definition>central abundance of 12 C</definition>
			<units>---</units></field>
		<field>
			<name>XO</name>
			<definition>central abundance of 16 O</definition>
			<units>---</units></field>
		<field>
			<name>Conv</name>
			<definition>fractionary mass of the convective core
                                    (inclusive of overshoot)</definition>
			<units>---</units></field>
		<field>
			<name>Q_disc</name>
			<definition>fractionary mass of the first mesh point where
                                    the chemical composition differs from the
                                    surface value</definition>
			<units>---</units></field>
		<field>
			<name>log.L_H</name>
			<definition>log of H luminosity</definition>
			<units>Sun</units></field>
		<field>
			<name>Q1_H</name>
			<definition>fractionary mass of the inner border of the
                                    H-rich region</definition>
			<units>---</units></field>
		<field>
			<name>log.L_He</name>
			<definition>log of He luminosity</definition>
			<units>Sun</units></field>
		<field>
			<name>log.Mdot</name>
			<definition>log of absolute value of mass loss rate</definition>
			<units>Sun/yr</units></field>
		<field>
			<name>X_sur</name>
			<definition>surface abundance (by mass) of 1 H</definition>
			<units>---</units></field>
		<field>
			<name>Y_sur</name>
			<definition>surface abundance (by mass) of 4 He</definition>
			<units>---</units></field>
		<field>
			<name>XC_sur</name>
			<definition>surface abundance (by mass) of 12 C</definition>
			<units>---</units></field>
		<field>
			<name>XN_sur</name>
			<definition>surface abundance (by mass) of 14 N</definition>
			<units>---</units></field>
		<field>
			<name>XO_sur</name>
			<definition>surface abundance (by mass) of 16 O</definition>
			<units>---</units></field></fields></tableHead>
	
			<textFile xlink:href="table1.tex"><name>table1.tex</name><description><para>Table 1, LaTeX</para></description></textFile>
			<textFile xlink:href="table2.tex"><name>table2.tex</name><description><para>Table 2, LaTeX</para></description></textFile>
			<textFile xlink:href="table3.tex"><name>table3.tex</name><description><para>Table 3, LaTeX</para></description></textFile>
			<textFile xlink:href="table4.tex"><name>table4.tex</name><description><para>Table 4, LaTeX</para></description></textFile>
			<textFile xlink:href="table5.tex"><name>table5.tex</name><description><para>Table 5, LaTeX</para></description></textFile>
	<history>
		<ingest>
	
			<creator>
				<staff/>
				<affiliation>CDS</affiliation></creator>
	<date>
		<year>1993</year><month>Feb</month><day>09</day></date></ingest>
		</history>
	<identifier>J_A+AS_100_647.xml</identifier></dataset>
