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Table 17:

Results from the abundance analysis of HD 36430 (B2 V).

HD 36430
$T_{\rm eff}$ = 18 400 K, log g = 4.1 dex $\xi_{\rm t}$(Si)=3.5

Line
EW $\Delta$EW $\epsilon_{\rm Si}$ $\Delta\epsilon_{\rm Si}$
  (mÅ) (mÅ) (dex) (dex)

SiII3862
61 5 7.43 0.13
SiII6347 100 10 7.57 0.16
SiII6371 74 6 7.49 0.12
SiIII4552 77 3 7.55 0.06
SiIII4567 53 2 7.40 0.05
SiIII4574 28 5 7.37 0.19
SiIII5739 25 2 7.47 0.08
  $\epsilon_{\rm Si}$ =  7.47 $\Delta\epsilon_{\rm Si}$($\sigma $) = 0.08
  $\Delta$ $\xi_{\rm t}$(Si) = 1.0 $\Rightarrow$ $\Delta\epsilon_{\rm Si}$( $\xi_{\rm t}$) = 0.07

HD 36430
$T_{\rm eff}$ = 18 400 K, log g = 4.1 dex $\xi_{\rm t}$(O)=6.3

OII3954
19 5 8.77 0.26
OII4317 20 5 8.75 0.24
OII4319 20 5 8.76 0.25
OII4366 18 4 8.64 0.21
OII4414 33 3 8.78 0.10
OII4416 26 7 8.85 0.29
OII4641 27 5 8.74 0.20
OII4650 36 2 8.66 0.06
OII4661 18 3 8.72 0.16
OII4676 18 4 8.78 0.21
OII4069 37 3 8.86 0.09
OII4072 27 4 8.82 0.18
  $\epsilon_{\rm O}$ =  8.76 $\Delta\epsilon_{\rm O}$($\sigma $) = 0.07
  $\Delta$ $\xi_{\rm t}$(O) = 2.2 $\Rightarrow$ $\Delta\epsilon_{\rm O}$( $\xi_{\rm t}$) = 0.08


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