| A Comparison of Some Quantities in Spectral Type G2 Giants and Dwarfs | ||
| Quantity | Dwarfs (Luminosity Class V) | Giants (Luminosity Class III) |
| Electron Pressure, Pe [dyn cm-2] | 37.2 | 5.13 |
| Effective Temperature, T [K] | 5720 | 5200 |
| N1/N0 for Fe | 7.86 | 9.08 |
| N1/N0 for Sr | 696 | 1364 |
|
A Comparison of Some Quantities Characterizing Fe and Sr in G2 V and III |
|||||||||
| Quantity | I [ev] | ΘIIII | ΘVI | u0(TV) | u0(TIII) | u1(TV) | u1(TIII) | log(2u1(TV)/u0(TV) | log(2u1(TIII)/u0(TIII) |
| Fe | 7.87 | 7.63 | 6.93 | 31.09 | 28.86 | 47.08 | 44.77 | 0.481 | 0.492 |
| Sr | 5.69 | 5.52 | 5.01 | 1.42 | 1.24 | 2.30 | 2.22 | 0.510 | 0.554 |
Note that:
(1) N(SrII)/N(SrI) increases much more rapidly with luminosity than does N(FeII)/N(FeI). This is mostly because of the
smaller ionization potential of Sr which makes it less sensitive to the small T decline with increasing luminosity. Fe is
more T sensitive. (Note: II(Fe) = 7.87 eV, II(Sr) = 5.695 eV.)
(2) In Fe the small drop in T with increasing luminosity, almost cancels the increase in N(FeII)/N(FeI) which results from
decreasing Pe.
(3) Therefore the line strength ratio λ4077(SrII)/λ4045(FeI) increases significantly with luminosity class in F, G and K
stars, since λ4077 increases appreciably with increasing luminosity class, while λ4045 slightly decreases.