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^{2}

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We present the dependence of electron temperature fluctuations of O
^{++} and H
^{+} by the chemical abundances of oxygen and nitrogen. Models assume that hydrogen density is uniform in one case and non uniform in the second case, which vary with the distance from the central star. The abundances of oxygen and nitrogen change by scale factor 5 and 1/5. Our analysis suggests that temperature fluctuations are consistent with photoionization. Using the cloudy photoionization code, we found a reasonable close agreement of the computed value with the one that was done before this work. Our simulation also shows that how change of abundances affects temperature fluctuations and its value is less than 0.01.

Accurate abundances of heavy metals are essential for solving astrophysical problems, including stellar and galactic chemical evolution. This was tested by different authors like [

The gas temperature obtained from the observed O[III] line ratio is greater than the one from the Balmer discontinuity [^{2} on photoionization in H II region. These values in H II region varying from 0.02 to 0.09 were found and yielded significant effects on element abundances.

The abundance determination in H II region and the planetary nebula have positive impacts of temperature fluctuations given by [

Cloudy is an impressive code offering a vast amount of possibilities to model wide variety of objects. The contents of physics and the basic numerical framework of the codes are explained in the documents given by [

In this paper, we will try to analyze the effect of hydrogen density and chemical abundances on temperature structure of electrons and its temperature fluctuations of both hydrogen and oxygen ions. In §2, we present the problem formulation of temperature fluctuations. In §3 we describe the models and present our calculations. In §4 we present the results and finally we present the conclusion.

Temperature in homogeneities on the emission lines, based on statistical approximation introduced by [_{0} and is given by

For homogeneous metalicity nebulae characterized by small temperature in homogeneities, n_{e} is the electron density, T is the electron temperature, and V is the volume over which the integration is carried out. The rms amplitude t of the temperature in homogeneities is defined as

We simplified the expression presented by [^{2} depends on the density of ionic species considered while in the above equation. We implicitly consider only ionized H (by setting

The nature of temperature fluctuations is one of the important question in nebular astrophysics. CLOUDY predicts that they should be very small because of the abundance of cooling function of temperature, while some observations indicate a very large value of t^{2} [^{2} [

We consider two different models for this photoionized region in H II regions. The first one correspond to a dense nebulae ionized by a star that is very hot and its temperature is ^{4} cm^{−}^{3}. The second correspond to a more diluted nebulae ionized by a hot star. We assumed the density of the gas in neutral medium within the galaxy is that of power law decrease in the gas density with the distance from the center given by

where n_{o} is the gas density at r = r_{o} and r_{o} is the scale length describing the rate of decay of this with radius. We have chosen hydrogen density, n(H) = 10^{3} cm^{−}^{3}, change by^{5} K. The stars are assumed to radiate as a blackbody. The inner radius of the nebulae is chosen to be 10^{16} cm for the former case and 5 × 10^{16} cm for the latter one. In both cases we assume that the total number of H Lyman continuum photons emitted by the star, Q(H) = 10^{48} photons per second and the filling factor is unit.

An additional set of a nebular parameters is the chemical composition of gas, usually taken to be 10^{5}, 776, 437, 182, 110, 75, and 36 atoms of He, C, O, N, Ne, S, and Ar, respectively per 10^{6} H atoms is shown in

We can easily observe from the result given in

H | He | O | C | N | Ne | S | Ar |
---|---|---|---|---|---|---|---|

10^{6} | 10^{5} | 437 | 776 | 182 | 110 | 18 | 16 |

0.00 | −1.00 | −3.36 | −3.11 | −3.74 | −3.96 | −4.75 | −4.79 |

^{−1} | ^{−3} | O (abundance) increase scale by 5 | N (abundance) increase scale by 5 | ||
---|---|---|---|---|---|

10^{48} | 75,000 K | 10^{4} | 10^{16} | 2188 | 912 |

100,000 K | 10^{3} | 5 × 10^{16} |

^{−1} | ^{−3} | O (abundance by scale factor of 1/5) | N (abundance by scale factor 1/5) | ||
---|---|---|---|---|---|

10^{48} | 100,000 K | 10^{4} | 5 × 10^{16} | 689 | 145.6 |

75,000 K | 10^{3} | 10^{16} |

Abundances | ||||

9760 K | 9340 K | 0.0083 | 0.006 | |

7430 K | 6860 K | 0.01 | 0.007 | |

11,200 K | 10,900 K | 0.0036 | 0.004 | |

9760 K | 9340 K | 0.0083 | 0.006 | |

9850 K | 9410 K | 0.01 | 0.007 | |

9410 K | 9050 K | 0.005 | 0.0032 |

lower than the normal abundances given by [^{2} ≈ 0.007 whereas t^{2} ≈ 0.004 when the O abundances decrease by scale factor 1/5. This result shows that there is slight variation with the result obtained by [^{++}), the rise of the abundances and temperature of ionized O are in the contrary. When it increases by scale factor its temperature is 7430 K and drops by 1/5, its temperature rises to 11,200 K.

When the abundances of O is increased by a scale factor 5, the temperature of H (T(H^{+})) is decreased by 26.5% and its temperature fluctuation t^{2}(O^{++}) is slightly increased by 0.001. But it drops by scale factor 1/5, temperature of H rises to 10 900 K and its fluctuation is t^{2}(H^{+}) = 0.004.

Similarly, when the abundance of nitrogen increases by scale factor 5, its temperature of T(O^{++}) decreases by 3.7%. This is much smaller than the previous one. Its temperature fluctuation t^{2}(H^{+}) of H and O when the abundances of N increases by scale factor 5 are 0.05 and 0.0032 respectively. But when the abundance of nitrogen drops by scale factor 1/5, its temperature is slightly greater than the normal abundances given by [

In the first model, we have more diluted nebulae ionized by a hot star. We have chosen hydrogen density n(H) = 10^{4} cm^{−}^{3}, change by

Abundances | ||||

9476 K | 8950 K | 0.013 | 0.008 | |

7550 K | 5270 K | 0.043 | 0.003 | |

11,100 K | 10,800 K | 0.006 | 0.003 | |

9470 K | 8950 K | 0.001 | 0.008 | |

9710 K | 9210 K | 0.02 | 0.007 | |

8490 K | 7830 K | 0.0013 | 0.009 |

temperature of electrons drops when the abundances of the most cooling elements increase by scale factor 5. The higher the abundances of oxygen elements, its peak temperature drops faster than the other two cases. Similarly the abundances of nitrogen shown in

In the second model, we have more diluted nebulae ionized by a hot star and we have chosen hydrogen density n(H) = 10^{3} cm^{−}^{3}, change by^{5} K. The result shown in

describe the temperature of electron is greatest when the abundances of both O and N are smallest. Since these elements are the main cooling agents, its temperature structure shows that through the processes temperature drops in both cases. Temperature fluctuations of O and N are smaller in this model.

In this paper we present a study of temperature fluctuation on two different cases, for uniform and non uniform hydrogen density at two different temperatures of 75,000 and 100,000 K. This was done by in homogeneities on the emission lines, based on statistical approximation introduced by [_{0} described by Equation (1). The main results are based on the analysis of chemical abundances of oxygen and nitrogen on different mechanism to test such change. Temperature fluctuations are obtained from the photoionization models generated by the spectral synthesis code CLOUDY (C10.00), calculated using the recombination theory for hydrogenic ions. Accurate t^{2} values have been obtained by comparing the O^{++} abundances derived from recombination lines with those derived from collisionally excited lines. It is clear from the result that temperature variations t^{2} < 0.01 value as described in [

We thank our supervisor Prof. Dreck Smith, the Editor and the referee for their comments. This research is funded by the Dire-Dawa University and My Friend Mr. Yared Ayele who arrived at the right time. This support is greatly appreciated.