• Title/Summary/Keyword: limb darkening

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Variation in Solar Limb Darkening Coefficient Estimated from Solar Images Taken by SOHO and SDO

  • Moon, Byeongha;Jeong, Dong-Gwon;Oh, Suyeon;Sohn, Jongdae
    • Journal of Astronomy and Space Sciences
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    • v.34 no.2
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    • pp.99-103
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    • 2017
  • The sun is not equally bright over the whole sphere, but rather is darkened toward the limb. This effect is well-known as limb darkening. The limb darkening coefficient is defined by the ratio of the center intensity to limb intensity. In this study, we calculate the limb darkening coefficient using the photospheric intensity estimated from solar images taken by solar and helispheric observatory (SOHO) and solar dynamics observatory (SDO). The photospheric intensity data cover almost two solar cycles from May 1996 to December 2016. The limb darkening coefficient for a size of 0.9 diameter is about 0.69 and this value is consistent with solar limb darkening. The limb darkening coefficient estimated from SOHO shows a temporal increase at solar maximum and a gradual increase since the solar minimum of 2008. The limb darkening coefficient estimated from SDO shows a constant value of about 0.65 and a decreasing trend since 2014. The increase in the coefficient reflects the effect of weakened solar activity. However, the decrease since 2014 is caused by the aging effect.

ILLUMINANCE DURING A SOLAR ECLIPSE WITH LIMB DARKENING: A MATHEMATICAL MODEL

  • Lee, Sung Hwan;Lee, Siyul
    • Journal of The Korean Astronomical Society
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    • v.45 no.5
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    • pp.111-116
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    • 2012
  • We present a mathematical model that predicts the variation of illuminance during a solar eclipse, considering continuous effects of limb darkening. We assume that (1) the Sun and the Moon constitute perfect spheres, (2) the Moon crosses the Sun with a constant apparent velocity, and (3) sunspots, prominences, and coronae can be neglected. We compare predictions of this model with actual measurements made by M$\ddot{o}$llmann & Vollmer (2006) during a total solar eclipse in Turkey, and with predictions of existing models. The new model is shown to describe the actual phenomenon more accurately than existing models.

AN APPLICATION OF WD MODEL TO EB TYPE CONTACT BINARY SYSTEM (EB형 접촉식쌍성에 대한 WD 모델 적용에 관한 분석)

  • 오규동;오수연
    • Journal of Astronomy and Space Sciences
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    • v.17 no.2
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    • pp.163-172
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    • 2000
  • The EB type contact binaries show large temperature difference $(\mid\bigtriangleup T\mid\geq1,000K)$ between two components. Thus we have modified the mode 3 of the WD program to adjust albedos, limb darkening coefficients and gravity darkening exponents for both components of such binaries, while the values for those parameters should be same for both components in the original WD program. Both of the modified and the original versions have been applied to the EB type contact binaries such as DO Cas, GO Cyg, and FS Lup. The computed light curves with modified version fit better to the observations.

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타이탄 대기의 주연증광에 haze의 성질변화가 미치는 영향

  • Sim, Chae-Gyeong;Kim, Sang-Jun
    • The Bulletin of The Korean Astronomical Society
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    • v.36 no.1
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    • pp.43.1-43.1
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    • 2011
  • 근적외영역의 타이탄 측광영상에서 나타나는 주연감광(Limb Darkening) 및 주연증광(Limb Brightening) 현상의 원인을 설명하기 위해 구면기하(spherical geometry)에 의한 효과 외에 헤이즈(haze) 자체의 성질 변화량을 추정해 본다. 근적외영역의 강한 메탄 흡수 밴드 부근에서 타이탄의 대기를 관측하면 파장에 따라 표면 부근에서 성층권 사이의 정보를 얻을 수 있으며, 이를 복사전달모델과 비교해 대기 중에 존재하는 연무 입자의 성질을 유추할 수 있다. 관측자료는 2006년 2월 Gemini/North Observatory의 Near-Infrared Integral Field Spectrometer(NIFS)를 이용해 얻은 측 분광 자료를 사용하였다. NIFS의 공간분해능은 화소당 0.05"로, 타이탄의 적도부분을 약 17화소로 분해할 수 있으므로, 각 지역별로 분광선 모델을 만들어 관측자료와 비교하는 데에 용이하였다.

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Observation of transiting exoplanet TrES-2b at Maidanak Observatory in Uzbekistan

  • Yang, Yun-A;Lee, Sang-Gak;Kang, Won-Seok
    • The Bulletin of The Korean Astronomical Society
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    • v.36 no.1
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    • pp.28.1-28.1
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    • 2011
  • We observed the transiting exoplanet, TrES-2b, with 1.5m telescope at Maidanak Observatory in Uzbekistan. We observed TrES-2 system for six nights, which contained two orbital periods of the planet. Therefore, we obtained the entire light curve of TrES-2b, which covered not only the whole primary transit containing both ingress and egress part, but also non-transit region. We used both R and Y band filters. Especially, Y filter is used first for transit observation and covers relatively longer wavelength ($1.02{\mu}m$ of center wavelength), to provide the light curve less affected by limb darkening. By fitting best model light curve for the obtained one, we determined these observables, transit depth, transit length, and planet's orbital period, which led to the determination of five physical parameters, stellar radius R*, stellar mass M*, inclination i, semi-major axis a, and planetary radius Rp. We will discuss of these results.

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Physical Properties of Transiting Planetary System TrES-3

  • Lee, Jae-Woo;Youn, Jae-Hyuck;Kim, Seung-Lee;Lee, Chung-Uk;Koo, Jae-Rim;Park, Byeong-Gon
    • The Bulletin of The Korean Astronomical Society
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    • v.35 no.2
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    • pp.65.2-65.2
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    • 2010
  • We present four new transits of the planetary system TrES-3 observed between 2009 May and 2010 June. Among those, the third transit by itself indicates possible evidence for brightness disturbance, which could originate from a starspot or an overlapping double transit. A total of 107 transit times, including our measurements, were used to determine the improved ephemeris with a transit epoch of $2454185.910950\pm0.000073$ HJED (Heliocentric Julian Ephemeris Date) and an orbital period of $1.30618698\pm0.00000016$ d. We analyzed the transit light curves using the JKTEBOP code and adopting the quadratic limb-darkening law. In order to derive the physical properties of the TrES-3 system, the transit parameters are combined with the empirical relations from eclipsing binary stars and stellar evolutionary models, respectively. The stellar mass and radius obtained from a calibration using $T_{eff}$, log $\rho$ and [Fe/H] are in good agreement with those from the isochrone analysis within the uncertainties. We found that the exoplanet TrES-3b has a mass of $1.93\pm0.07\;M_{Jup}$, a radius of $1.30\pm0.04\;R_{Jup}$, a surface gravity of $28.2\pm1.1\;m\;s^{-1}$, a density of $0.82\pm0.06\;\rho_{Jup}$, and an equilibrium temperature of $1641\pm23K$.

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Heat-Flux Analysis of Solar Furnace Using the Monte Carlo Ray-Tracing Method (몬테카를로 광선추적법을 이용한 태양로의 열유속 해석)

  • Lee, Hyun-Jin;Kim, Jong-Kyu;Lee, Sang-Nam;Kang, Yong-Heack
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.35 no.10
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    • pp.989-996
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    • 2011
  • An understanding of the concentrated solar flux is critical for the analysis and design of solar-energy-utilization systems. The current work focuses on the development of an algorithm that uses the Monte Carlo ray-tracing method with excellent flexibility and expandability; this method considers both solar limb darkening and the surface slope error of reflectors, thereby analyzing the solar flux. A comparison of the modeling results with measurements at the solar furnace in Korea Institute of Energy Research (KIER) show good agreement within a measurement uncertainty of 10%. The model evaluates the concentration performance of the KIER solar furnace with a tracking accuracy of 2 mrad and a maximum attainable concentration ratio of 4400 sun. Flux variations according to measurement position and flux distributions depending on acceptance angles provide detailed information for the design of chemical reactors or secondary concentrators.