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thesis - IRS, The Infrared Spectrograph

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2.6. Analysis 23O IV 140.0 nm25.9 µ mTe (K)N II 575.5 nm658.4 nmO III 436.3 nm500.7 nmNe V 342.6 nm24.3 µ mMg V 278.3 nm5.61 µ mFigure 2.3–. Electron temperature versus ionization potential. <strong>The</strong> lines used for each ion are indicated.<strong>The</strong>re is a correlation of T e with IP, represented by the curve.2.6.3 AbundancesIn order to be able to compute abundances, values of N e and T e are needed for each ion.<strong>The</strong>y are derived from the relations presented in Fig. 2.2 and 2.3. Once the N e and T e areknown the relative ionic abundances can be determined. <strong>The</strong>n, applying an ICF the elementabundances are derived. Ionic abundances are normalized to hydrogen. <strong>The</strong> equation used todetermine the ionic abundances is:N ionN p= I ionI HβN eλ ulλ Hβα HβA ul(NuN ion) −1(2.2)In the equation N p is the density of the ionized hydrogen; I ion /I Hβ is the measuredintensity of the ionic line, normalized to H β ; λ ul is the wavelength of the line and λ Hβ is thewavelength of H β ; α Hβ is the effective recombination coefficient for H β ; A ul is the Einsteinspontaneous transition rate for the line and finally N u /N ion is the ratio of the population ofthe level from which the line originates to the total population of the ion.All abundance values are shown in Table 2.6. <strong>The</strong> ICF is unity in four cases, becauseall important ionization states have been measured. In most cases it is between 1.0 and1.25, and only in three cases is it above 1.25 (S, Mg and K with ICF’s of 1.27, 2 and 1.35respectively). In Keyes et al. (1990), the ICF is normally between 1.2 and 5, and only in afew cases is under 1.2. This shows that the present abundance determination is an importantimprovement. <strong>The</strong> ICF were calculated on a purely empirical basis. For a given element theionization potential where the maximum ionic abundance is reached was taken into accountusing the known distribution of neon ions (with varying IP) as an example. For some ionslike potassium, no information on the high sixth stage of ionization was found, thus an upper

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