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M. A. Al-Wardat

Publications and source records attributed to M. A. Al-Wardat.

5 recordsLinked to original sources

Narrowing the solar surface flux transport parameter space through nonlinear feedbacks

The surface flux transport (SFT) model describes the evolution of the Sun's large-scale photospheric magnetic field. While linear transport processes are relatively well constrained, nonlinear feedbacks such as tilt and latitude quenching remain less explored, despite their potential role in regulating the solar cycle. We aim to determine how nonlinear quenching mechanisms and flux decay influence the admissible parameter space of the SFT model, and to identify parameter combinations that reproduce the observed characteristics of the solar polar magnetic field. We extend the parameter-space optimisation by introducing analytic prescriptions for tilt quenching (TQ) and latitude quenching (LQ) in the source term, together with a tunable flux-decay term. The model is solved numerically over a grid of meridional flow speeds ($u_{0}$), surface diffusivities ($η$), and decay timescales ($τ$). Admissible solutions are defined by agreement with {observationally motivated constraints on the {polar-field minimum-to-extremum amplitude ratio}, reversal timing, and the latitude of the polar cap boundary. Both TQ and LQ reduce the admissible parameter domain, with LQ exerting the stronger influence. Their combined action produces a pronounced saturation ("ceiling") that limits axial dipole amplification. The inclusion of a finite flux-decay timescale ($τ\simeq 8$--$10$~yr) further narrows the admissible domains within the present parameterised source formulation, whereas the non-decaying case may lead to unrealistically persistent dipole fields in this modelling framework. Correlations between $u_{0}$, $η$, and $τ$ reveal a coupled balance between advection, diffusion, and phenomenological flux loss.

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Physical and Geometrical Parameters of the Evolved Binary System HD6009

Atmospheric modeling and dynamical analysis of the components of the visually close binary system (VCBS) HD6009 were used to estimate their individual physical and geometrical parameters. Model atmospheres were constructed using a grid of Kurucz solar metalicity blanketed models and used to compute the individual synthetic spectral energy distribution (SED) for each component separately. These SEDs were combined together to compute the entire SED for the system from the net luminosities of the components $a$ and $b$ located at a distance $d$ from the Earth. %The entire observational SED of the system was used as a reference for the comparison with the synthetic ones. We used the feedback modified parameters and iteration method to get the best fit between synthetic and observational entire SEDs. The physical and geometrical parameters of the system's components were derived as: $T_{\rm eff}^{a} =5625\pm75$\,K, $T_{\rm eff}^{b} =5575\pm75$\,K, log $g_{a}=3.75\pm0.25$, log $g_{b}=3.75\pm0.25$, $R_{a}=2.75\pm0.30 R_\odot$, $R_{b}=2.65\pm0.30 R_\odot$, $M_v^{a}= 2\fm80\pm0.30$, $M_v^{b}=2\fm93\pm0.30$, $M_a= 1.42\pm0.15 M_{\odot}$, $M_b=1.40\pm0.15 M_{\odot}$, $L_a=6.80\pm0.75 L_\odot$, $L_b=6.09\pm0.75 L_\odot$ and $π=14.43$mas dynamical parallax. The system is shown to be consist of G6 IV primary and G6 IV secondary components.

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A Study of the Abundance of Low-Z Elements in the Sun During its Whole Predicted Life

The study of the elemental composition of stars and galaxies is a key topic for understanding their origin and evolution. In this study, we present the results of the calculation of solar abundances of the isotopes $^{1}$H, $^{4}$He, $^{12}$C, $^{14}$N, $^{15}$O, $^{16}$O, $^{17}$O, and $^{18}$O during the four phases of the solar life; Hydrogen burning, Onset of rapid growth and red giant, Helium burning and Helium exhaustion. The open source package nucnet-tools from the Webnucleo Group in Clemson University, SC, USA was used for this purpose. The results for all isotopes are listed in tables for future use. Abundances found, globally, agree fairly well with those predicted in the literature. Results obtained for the last two phases have no equivalent elsewhere.

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Physical and Geometrical Parameters of CVBS XII: Fin 350 (Hip 64838)

A complete astrophysical and dynamical study of the close visual binary system (CVBS) (A7V + F0V), Finsen 350, is presented. Beginning with the entire observational spectral energy distribution (SED) and the magnitude difference between the subcomponents, Al-Wardat's complex method for analyzing close visual binary stars (CVBS) was applied as a reverse method of building the individual and entire synthetic SEDs of the system. This was combined with Docobo's analytic method to calculate the new orbits. Although possible short ($\approx$ 9 years) and long period ($\approx$ 18 years) orbits could be considered taking into account the similar results of the stellar masses obtained for each of them (3.07 and 3.41 $M_{\odot}$, respectively), we confirmed that the short solution is correct. In addition, other physical, geometrical and dynamical parameters of this system such as the effective temperatures, surface gravity accelerations, absolute magnitudes, radii, the dynamical parallax, etc., are reported. The main sequence phase of both components with age around 0.79 Gy is approved.

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The visually close binary system HD375; Is it a sub-giant binary?

Atmospheric modeling is used to build synthetic spectral energy distributions (SEDs) for the individual components of the speckle interferometric binary system HD375. These synthetic SEDs are combined together for the entire system and compared with its observational SED in an iterated procedure to achieve the best fit. Kurucz blanketed models with the measurements of magnitude differences were used to build these SED's. The input physical elements for building these best fitted synthetic SEDs represent adequately enough the elements of the system. These elements are: $T_{\rm eff}^{a} =6100\pm50$\,K, $T_{\rm eff}^{b} =5940\pm50$\,K, log $g_{a}=4.01\pm0.10$, log $g_{b}=3.98\pm0.10$, $R_a=1.93\pm0.20 R_\odot$, $R_b=1.83\pm0.20 R_\odot$ $M_{v}^{\rm a}=3.26\pm0.40$, $M_{v}^{\rm b}=3.51\pm0.50$, $L_a= 4.63\pm0.80 L_\odot$ and $ L_b= 3.74\pm0.70 L_\odot$ depending on new estimated parallax $π=12.02 \pm 0.60$ mas. A modified orbit of the system is built and compared with earlier orbits and the masses of the two components are calculated as $M_a =1.35M_{\odot}$ and $M_b=1.25M_{\odot}$. Depending on the estimated physical and geometrical elements of the system, which are assured by synthetic photometry, we suggest that the two components are evolved subgiant (F8.5 IV & G0 IV) stars with age of 3.5 Gy formed by fragmentation.

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