Module 09 Colour Index TABLE of CONTENTS 1. Learning Outcomes

Total Page:16

File Type:pdf, Size:1020Kb

Module 09 Colour Index TABLE of CONTENTS 1. Learning Outcomes Module 09 Colour Index TABLE OF CONTENTS 1. Learning Outcomes 2. Introduction 3. Dependence of magnitudes on wavelength 3.1. UBV System of Johnson and Morgan 3.2. Colour Index 3.3. Colour-Colour Diagrams 3.4. Colour Excess 3.5. Reddening and Redshift 4. Summary 1. Learning Outcomes After studying this module, you should be able to Appreciate that the magnitude depends on the wavelength at which it is measured Understand the need of UBV photometric system Realize that the UBV system at present measures magnitudes at various wavelength bands other than the visual region Understand why magnitudes of stars at various wavelength bands of their spectra are not equal Grasp the concept of colour index Understand that the colour index follows the surface temperature of the star Realize the importance of colour-colour diagrams in describing stars 2. Introduction In the last module we introduced the concept of magnitudes. Apparent magnitude is a number assigned to a star (or any other celestial object) to indicate its brightness. Brighter stars are assigned lower magnitudes and fainter stars are characterized by higher magnitudes. Only stars brighter than 6th magnitude are visible to the unaided eye. Since brightness is a function of distance and the intrinsic brightness of a star, apparent magnitude does not allow us to compare stars with respect to their intrinsic brightness. Therefore, to compare brightness all stars are thought to be at a standard distance of 10 pc. The apparent magnitude at this distance is called the absolute magnitude of the star. It turns out that the difference between the absolute magnitudes of two stars is proportional to the ratio of their luminosities. So, in absolute magnitude, we have now a handle to estimate the luminosity of as star. We also found that the difference between the apparent and absolute magnitudes of a star, the distance modulus, allows us to determine the distance of the star. It was pointed out that overwhelming majority of stars in the sky are faint stars; there is real paucity of bright stars. The number of stars brighter than 6th magnitude, those visible to the naked eye, is only about 5000. Also most stars are less luminous than the Sun; very few stars have luminosity greater than the Sun. We know that stars radiate in many wavelengths. Therefore, we now turn to the dependence of magnitudes on wavelength and introduce an important quantity: colour index. 3. Dependence of magnitudes on wavelength If the radiation of stars were monochromatic, magnitude differences would be entirely independent of the instruments used to determine them. But stellar radiation is not monochromatic. Moreover, the measuring instruments select a band of wavelengths rather than a single wavelength (Fig. 9.1). Therefore, magnitude becomes instrument dependent. However, this is not the case with the instruments which are nonselective, such as radiometers, bolometers and thermocouples. These instruments measure the true luminosities of stars once they have been corrected for absorption of radiation in the atmosphere of the earth. Unfortunately, these instruments are rather insensitive and, therefore, are not used for determining stellar luminosities. Instead one uses an indirect method which employs the idea of bolometric correction, as we shall see later. 3.1. UBV System of Johnson and Morgan Magnitudes are measured these days with special filters attached to the telescopes. The filters belong to what is called the UBV Johnson Morgan photometric system. The V band was provided to approximate to the visual magnitude system. The B band approximated to the photographic magnitude. The peak sensitivity of the filter in the visual region (denoted by V), for example, centres around a wavelength to which the eye is most sensitive, 훌545 nm in the yellow-green region of the spectrum. Similarly, filters for blue (B) and ultraviolet (U) have their peak sensitivities centred around 훌435 nm and 훌350 nm, respectively (Fig. 9.1). A filter in the red region (푹) has its peak sensitivity around 훌640 nm, and the one in the infrared region has peak around 훌800 nm (Fig. 9.2). ) 훌 Sensitivity S( Fig. 9.1. Sensitivity functions of the U, B and V filters (Johnson and Morgan, 1953). The magnitudes determined with these filters are denoted as 푚푉, 푚퐵, and 푚푈, or simply as 푉, 퐵, and 푈. Notice that these are all apparent magnitudes. The corresponding absolute magnitudes are denoted by 푀푉, 푀퐵, and 푀푈. Fig. 9.2. Modern system of filters. (Source: Bessell, Annu. Rev. Astron. Astrophys., 2005). All the magnitudes of a star in various wavelength bands are not equal, because each filter samples a different region of the blackbody spectrum corresponding to the surface temperature Blue Filter Yellow Green Filter Black Body Curve at Star’s Temperature Higher Intensity Temperature Lower Temperature Wavelength Fig. 9.3. Blue band and yellow-green band filters sample different regions of the spectrum. The blue magnitude of the star at higher temperature is lower than the yellow-green magnitude. Opposite is the case with the star at lower temperature. of the star. Referring to Fig. 9.3, the blue filter samples higher intensity region of the spectrum at higher temperature while yellow-green filter samples region of lower intensity of the same curve. At lower temperature the blue filter samples the lower intensity and the yellow-green filter samples the higher intensity. Since higher brightness is associated with a lower magnitude, and vice versa, the blue magnitude of the star at higher temperature in Fig. 9.3 is lower than its visual magnitude. On the other hand, for the star at lower temperature in the same figure, the blue magnitude will be slightly higher than the yellow-green magnitude. 3.2. Colour Index The difference between the magnitudes of a star at different wavelengths is called its colour index (C.I.), or just the colour, of the star. It is obvious that the colour index is a measure of the surface temperature of the star. That is why instead of the temperature of the star, many times its colour index is stated. We shall state the precise relationship between the temperature and the colour index a little later. One kind of colour index is defined as C. I. = 푚퐵 − 푚푉 = 퐵 − 푉. (9.1) The colour index is stated in units of magnitude. Another colour index is 푈 − 퐵: 푚푈 − 푚퐵 = 푈 − 퐵. (9.2) The reference star for measuring colour indices is star Vega (Surface temperature, 9602 K; Apparent magnitude, 0.03; Luminosity, 50 푳ʘ; Distance, 7.68 pc). For this star, by definition, all the three indices are equal, that is, 푼 = 푩 = 푽, which implies that 푩 − 푽 = ퟎ. ퟎ and 푼 − 푩 = ퟎ. ퟎ. So, star Vega is a white star. A star with 푩 − 푽 < ퟎ has higher intensity in the blue region than Vega. We usually say that the star is bluer than Vega; a star with 푩 − 푽 > ퟎ is redder than Vega. Table 9.1 shows the sample calibration of various colour indices for stars of various surface temperatures, 푻풆풇풇. The first column in the Table shows the spectral class of the star. We shall study spectral classification of stars later. For the present, you can ignore the first column. Table 9.1. Sample Calibration Colour Indices of Stars of various Surface Temperatures Class 푩– 푽 푼– 푩 푽– 푹 푹– 푰 푻풆풇풇 (K) O5V –0.33 –1.19 –0.15 –0.32 42,000 B0V –0.30 –1.08 –0.13 –0.29 30,000 A0V –0.02 –0.02 0.02 –0.02 9,790 F0V 0.30 0.03 0.30 0.17 7,300 G0V 0.58 0.06 0.50 0.31 5,940 K0V 0.81 0.45 0.64 0.42 5,150 M0V 1.40 1.22 1.28 0.91 3,840 Source of data: Zombeck, Martin V. (1990). "Calibration of MK spectral types". Handbook of Space Astronomy and Astrophysics (2nd ed.). Cambridge University Press. p. 105. ISBN 0-521-34787-4. Look at the 퐵 − 푉 colour index of stars of temperatures 42000 K and 30000 K. They have very high intensity in the blue colour of their spectra. These are called blue stars. Stars of temperature ~ 1000, of the type of star Vega, are white. Stars of lower temperatures are redder than Vega, redness increasing as the temperature decreases. Sun, with a surface temperature ~ 6000 K is yellowish in colour, while stars with temperatures ~ 4000 K are red stars. Colour index (푩 − 푽) for the Sun has been estimated as 0.656. A category of dwarf stars are red dwarf stars. These stars actually outnumber all other categories of stars. Their surface temperatures are low and their masses are a fraction of solar mass while -4 their luminosities are typically 10 L⨀. There are also stars which are many times larger in size than the Sun. These, the so-called red giants and red supergiants are also red because of their low surface temperatures. Another collection of red stars is a globular cluster. Globular clusters are very old clusters, 10 billion years or older. They contain very old, therefore, red stars. There are about 150 of such clusters in the Milky way galaxy. The new-born stars are blue because of their high surface temperatures. Galaxies in which there is a burst of new stars, star burst galaxies, appear blue, because of preponderance of blue stars in them. An example of a blue star is the star Rigel, the brightest star in Orion constellation. Just like red giants, there exist also blue giant stars, stars of huge sizes and high surface temperatures.
Recommended publications
  • Information Bulletin on Variable Stars
    COMMISSIONS AND OF THE I A U INFORMATION BULLETIN ON VARIABLE STARS Nos November July EDITORS L SZABADOS K OLAH TECHNICAL EDITOR A HOLL TYPESETTING K ORI ADMINISTRATION Zs KOVARI EDITORIAL BOARD L A BALONA M BREGER E BUDDING M deGROOT E GUINAN D S HALL P HARMANEC M JERZYKIEWICZ K C LEUNG M RODONO N N SAMUS J SMAK C STERKEN Chair H BUDAPEST XI I Box HUNGARY URL httpwwwkonkolyhuIBVSIBVShtml HU ISSN COPYRIGHT NOTICE IBVS is published on b ehalf of the th and nd Commissions of the IAU by the Konkoly Observatory Budap est Hungary Individual issues could b e downloaded for scientic and educational purp oses free of charge Bibliographic information of the recent issues could b e entered to indexing sys tems No IBVS issues may b e stored in a public retrieval system in any form or by any means electronic or otherwise without the prior written p ermission of the publishers Prior written p ermission of the publishers is required for entering IBVS issues to an electronic indexing or bibliographic system to o CONTENTS C STERKEN A JONES B VOS I ZEGELAAR AM van GENDEREN M de GROOT On the Cyclicity of the S Dor Phases in AG Carinae ::::::::::::::::::::::::::::::::::::::::::::::::::: : J BOROVICKA L SAROUNOVA The Period and Lightcurve of NSV ::::::::::::::::::::::::::::::::::::::::::::::::::: :::::::::::::: W LILLER AF JONES A New Very Long Period Variable Star in Norma ::::::::::::::::::::::::::::::::::::::::::::::::::: :::::::::::::::: EA KARITSKAYA VP GORANSKIJ Unusual Fading of V Cygni Cyg X in Early November :::::::::::::::::::::::::::::::::::::::
    [Show full text]
  • A Study of Two Open Clusters Containing Wolf-Rayet Stars
    A STUDY OF TWO OPEN CLUSTERS CONTAINING WOLF-RAYET STARS by Stephen L. Shorlin A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE DEPARTMENT OF ASTRONOlMY AND PHYSICS SAINT MARY'S UMNERSITY MAY 1998 HALIFAX, NOVA SCOTIA Ostephen L. Shorlin, 1998 National Library Bibliothèque nationale I*m of Canada du Canada Acquisitions and Acquisitions et Bibliographie Services services bibliographiques 395 Wellington Street 395. nie Wellington Ottawa ON K1A ON4 Ottawa ON KIA ON4 Canada Canada The author has granted a non- L'auteur a accordé une licence non exclusive licence allowing the exclusive permettant à la National Library of Canada to Bibliothèque nationale du Canada de reproduce, loau, distribute or seU reproduire, prêter, distribuer ou copies of this thesis in microfoq vendre des copies de cette thèse sous paper or electronic formats. la fome de microfiche/nIm, de reproduction sur papier ou sur format électronique. The author retains ownership of the L'auteur conserve la propriété du copyright in this thesis. Neither the droit d'auteur qui protège cette thèse. thesis nor substantial extracts fiom it Ni la thèse ni des extraits substantiels may be printed or otherwise de celle-ci ne doivent être imprimes reproduced *out the author's ou autrement reproduits sans son permission. autorisation- Abstract The results of UBV CCD photornetry are presented for a newly discovered open cluster, as well as new photornetry for thirty-seven members of the open cluster HM 1. The new open cluster, to be designated OCL 1104610, has a distance modulus of Vo - l'LIV = 15.5 & 0.2: corresponding to a distance of 12.61::: kpc, and is several Myr old.
    [Show full text]
  • Publications of the Astronomical Society of the Pacific 107: 945-958, 1995 October
    Publications of the Astronomical Society of the Pacific 107: 945-958, 1995 October Galaxy Colors in Various Photometric Band Systems M. Fukugita1 Institute for Advanced Study, Princeton, New Jersey 08540 Electronic mail: [email protected] K. Shimasaku2 Princeton University Observatory, Princeton, New Jersey 08544 Electronic mail: [email protected] T. ICHIKAWA Kiso Observatory, University of Tokyo, Kiso-gun, Nagano 397-01, Japan Electronic mail: [email protected] Received 1995 March 10; accepted 1995 June 14 ABSTRACT. A study is made of stellar and galaxy colors using a spectrophotometric synthesis technique. We show that use of good color response functions and a modem determination of the spectroscopic energy distribution for a Lyr gives synthetic stellar colors in a good agreement with photometric observations to about 0.05 mag. The synthetic method then is applied to study galaxy colors using the spectrophotometric atlas of Kennicutt (1992, ApJS, 79, 255), and a comparison is made with observed galaxy colors. The Κ correction is calculated and compared with that of Coleman, Wu, and Weedman (1980, ApJS, 43, 393). We then study colors of galaxies in various photometric band systems and obtain color transformation laws, which enable us to find offsets among different systems. We include 48 photometric bands in our study. 1. INTRODUCTION in addition to a good sample of galaxy SED over a wide range of wavelength. Continual efforts to obtain the SED of Colors of galaxies provide us with valuable information Vega (Oke and Schild 1970; Hayes and Latham 1975; Oke concerning their present-day composition of stars, and ac- and Gunn 1983; Kurucz 1979; Hayes 1985, hereafter re- cordingly it gives us hints about the formation and evolution ferred to as H85; Castelli and Kurucz 1994, hereafter re- of galaxies.
    [Show full text]
  • The ∆A Photometric System
    Ernst Paunzen (Autor) The _a photometric system https://cuvillier.de/de/shop/publications/8305 Copyright: Cuvillier Verlag, Inhaberin Annette Jentzsch-Cuvillier, Nonnenstieg 8, 37075 Göttingen, Germany Telefon: +49 (0)551 54724-0, E-Mail: [email protected], Website: https://cuvillier.de 1 Summary This book describes the history, characteristics, observations, results and future prospects of the Δa photometric system. Up to now, it success- fully produced countless scientific output since its development and first appearance on the astronomical scene initiated by Hans-Michael Maitzen in 1976. It was intended to study the typical and unique flux depression at 5200 A˚ found in mainly magnetic chemically peculiar stars of the upper main sequence. Therefore the most important measurement is through the g2 filter centred at this wavelength region. In addition, one needs the information about the continuum flux of the same object. Originally, the g1 (centred at 5000A)˚ and Str¨omgren y (5500A)˚ was used to get the continuum flux. In principle, any other filters such as Johnson BV RI can be used. However, the closer it is measured to the 5200A˚ region and the narrower the used filters are, the results become more accurate. The a index is then defined as the flux in g2 compared to the continuum one. Because there is a general increase of opacity around 5200A˚ with decreasing temperature, one has to normalize a with the index a0 of a non-peculiar star of the same temperature, to compare different peculiar (or deviating) stars with each other (Δa index). With this photometric system it is possible to measure any peculiarities, such as abnormal absorption and emission lines, in the region of 5200A.˚ Soon, it was used to investigate metal-weak, Be/shell and supergiants in the Galactic field and open clusters.
    [Show full text]
  • Fundamental Stellar Photometry for Standards of Spectral Type on the Revised System of the Yerkes Spectral Atlas “
    COMMENTS ON THE PAPER “FUNDAMENTAL STELLAR PHOTOMETRY FOR STANDARDS OF SPECTRAL TYPE ON THE REVISED SYSTEM OF THE YERKES SPECTRAL ATLAS “ BY H.L. JOHNSON AND W.W. MORGAN (1953) SIDNEY VAN DEN BERGH Dominion Astrophysical Observatory Herzberg Institute of Astrophysics National Research Council of Canada 5071 West Saanich Road Victoria, British Columbia, V8X 4M6 Canada Received 1998, December 3 Photometry and spectroscopy are among the most important and fundamental types of astronomical observations. By the middle of the twentieth century most spectral classification was defined in terms of MKK type standards (Morgan, Keenan & Kellerman 1943). However, for a variety of reasons (Weaver 1947), the establishment of photometric standards remained problematic. Commission 25 (Photometry) of the International Astronomical Union devoted seemingly endless years to discussions on the establishment of an international photometric standard system. Weaver (1952) advocated that a new sub- commission should be created which would have as its task “The establishment of an ‘ideal’ photo-electric color and magnitude system.” A subsequent IAU resolution (Oosterhoff 1954) suggested that “La Commission recommende que soit constituJe une nouvelle sous-commission des Jtalons de magnitudes - 2 - stellaire....”. Additional problems were: (1) The Commission could not decide between monochromatic magnitudes and broad-band magnitudes, and (2) some advocated a two-color system (Hertzsprung 1950), whereas others (Becker 1946) favored a three-color (photographic, photovisual, red) photometric system. In his characteristically energetic fashion Johnson (Johnson & Morgan 1951) then took the bull by the horns and started to observe so many stars and clusters on his UBV system that it soon became the de facto international photometric system1.
    [Show full text]
  • Visualizing Large-Scale Uncertainty in Astrophysical Data
    Visualizing Large-Scale Uncertainty in Astrophysical Data Hongwei Li, Student Member, IEEE, Chi-Wing Fu, Member, IEEE, Yinggang Li, Member, IEEE, and Andrew J. Hanson, Member, IEEE Abstract— Visualization of uncertainty or error in astrophysical data is seldom available in simulations of astronomical phenomena, and yet almost all rendered attributes possess some degree of uncertainty due to observational error. Uncertainties associated with spatial location typically vary significantly with scale and thus introduce further complexity in the interpretation of a given visualization. This paper introduces effective techniques for visualizing uncertainty in large-scale virtual astrophysical environments. Building upon our previous transparently scalable visualization architecture, we develop tools that enhance the perception and comprehension of uncertainty across wide scale ranges. Our methods include a unified color-coding scheme for representing log-scale distances and percentage errors, an ellipsoid model to represent positional uncertainty, an ellipsoid envelope model to expose trajectory uncertainty, and a magic-glass design supporting the selection of ranges of log-scale distance and uncertainty parameters, as well as an overview mode and a scalable WIM tool for exposing the magnitudes of spatial context and uncertainty. Index Terms—Uncertainty visualization, large spatial scale, interstellar data, astronomy. F 1 INTRODUCTION Uncertainty and error are common and crucial entities in scientific representations is lacking in a large fraction of 3D astronomical visu- studies. As pointed out by Johnson [23, 24], if we look at leading alization products. In visually spectacular animations depicting nebula peer-reviewed science and engineering journals, we can see that the flythroughs or travel from the Earth through the Milky Way Galaxy majority of 2D graphs represent error or uncertainty in the experimen- produced for planetariums and television programs, rarely does the tal or simulated data.
    [Show full text]
  • Evaluating Stars Temperature Through the B-V Index Using a Virtual Real Experiment…
    Paper—Evaluating Stars Temperature Through the B-V Index Using a Virtual Real Experiment… Evaluating Stars Temperature Through the B-V Index Using a Virtual Real Experiment from Distance: A Case Scenario for Secondary Education. https://doi.org/10.3991/ijoe.v14i01.7842 Nikolaos Dintsios ! , Stamatia Artemi, Hariton Polatoglou Aristotle University! " of Thessaloniki, Thessaloniki, Greece [email protected] Abstract—In this paper we propose a scenario for secondary education at which students could estimate the temperature, the radius and the age of stars. To achieve this, we built a virtual real experiment which can be performed from distance on any portable device. Students can connect to a webpage and choose a star from a list. After applying B and V filters they obtain the B and V magni- tude. Consequently, they calculate the B-V index of a star and using a simple formula they estimate the star’s surface temperature. Furthermore, guided through a worksheet and with the use of Hertzsprung–Russell diagram they can estimate the radius and the age of the star. Keywords—remote virtual experiments, astronomy, remote experiments, star surface temperature 1 Introduction 1.1 Astronomy in Education Astronomy is a very interesting scientific subject and many students are highly mo- tivated to study it. Studying the literature on astronomy education we found that most studies have been focused on Earth, day/night cycle, Earth-Sun-Moon system, seasons and Moon phases [1], [2] while fewer studies were referring to stars. More specifical- ly, the great majority of studies which are focused on stars deal with the motion, the position and the origin of stars’ light [3]-[6].
    [Show full text]
  • 00 Oo Oo UBVRI PHOTOMETRIC STANDARD STARS AROUND THE
    O'! 00 THE ASTRONOMICAL JOURNAL VOLUME 88, NUMBER 3 MARCH 1983 oo UBVRI PHOTOMETRIC STANDARD STARS AROUND THE CELESTIAL EQUATOR8' ARLOU. LANDOLTb) LSU Observatory, Baton Rouge, Louisiana 70803 1983AJ. Received 8 November 1982 ABSTRACT UBVRI photoelectric observations have been made of 223 stars mostly in an approximate two degree band centered on the celestial equator. The observing program was planned to provide new UBVRI standard stars, available to telescopes of a variety of sizes in both hemispheres, on an internally consistent homogeneous system around the sky. Most of the stars are in Selected Areas 92-115. The stars average 20.7 measures each on 12.2 different nights. The stars in this paper fall in the range 1SVS 12.5 and — 0.35(5 — V)S + 2.0. I. INTRODUCTION ble to telescopes of all sizes in both hemispheres. The observational data were tied into the UBV standard Accurate, internally consistent, and readily accessi- stars of Landolt (1973) and the RI standards of Cousins ble standard star photometric sequences are necessary (1976). for the calibration of the intensity and color data that The observing plan by necessity focused on a boot- astronomers obtain at the telescope. The most used pho- strapping theme. The Cousins (1976) R/standard stars tometric system during the past twenty-five years has available at the time that the project began were bright, been the UBV system, developed by Johnson and Mor- mostly V <1.0. Therefore, it was necessary to begin the gan (1953). Additional refinements were published by manufacture of new standard stars at the 0.4-m tele- Johnson and Harris (1954) and by Johnson (1955).
    [Show full text]
  • An Effective Temperature Calibration for Main-Sequence B- to F-Type Stars
    An effective temperature calibration for main-sequence B- to F-type stars using VJHKs colors Ernst Paunzen1, Martin Netopil1, and Andreas Herdin2 1 Department of Theoretical Physics and Astrophysics, Masaryk University, Kotl´aˇrsk´a 2, 611 37 Brno, Czech Republic 2 Universit¨atssternwarte, T¨urkenschanzstr. 17, 1180 Wien, Austria [email protected] (Submitted on 29.08.2016. Accepted on 12.09.2016) Abstract. The effective temperature is an important parameter that is needed for numerous astrophysical studies, in particular to place stars in the Hertzsprung-Russell diagram, for example. Although the availability of large spectroscopic surveys increased significantly in the last decade, photometric data are still much more frequent. Homoge- neous photometric (all-sky) surveys provide the basis to derive the effective temperature with reasonable accuracy also for objects that are not covered by spectroscopic surveys, or are out of range for the current spectroscopic instrumentations because of too faint magnitudes. We use data of the Two Micron All Sky Survey (2MASS) and broadband visual photometric measurements to derive effective temperature calibrations for the in- trinsic colors (V − J), (V − H), (V − Ks), and (J − Ks), valid for B2 to F9 stars. The effective temperature calibrations are tied to the Str¨omgren-Crawford uvbyβ photometric system and do not depend on metallicity or rotational velocity. Key words: stars: early-type – stars: fundamental parameters – techniques: photometric Introduction With the development of high quality and stable astronomical infrared ar- ray technology, between 1997 and 2001, the Two Micron All Sky Survey (2MASS) provided a full-sky census with millijansky sensitivity and arcsec- ond resolution (Skrutskie et al., 2006).
    [Show full text]
  • CCD Photometry of Standard Stars at Maidanak Astronomical
    Journal of The Korean Astronomical Society 41: 1 ∼ 12, 2009 CCD Photometry of Standard Stars at Maidanak Astronomical Observatory in Uzbekstan: Transformations and Comparisons Beomdu Lim1, Hwankyung Sung1, M. S. Bessell2, R. Karimov3, M. Ibrahimov3 1 Department of Astronomy and Space Science, Sejong University,Seoul,Korea e-mail: [email protected], [email protected] 2 Research School of Astronomy & Astrophysics, Australian National University, Private Bag, Weston Creek PO, ACT 2611, Australia e-mail: [email protected] 3 Ulugh Beg Astronomical Institute, 33 Astronomical Street, Tashkent 700052, Uzbekistan e-mail: [email protected], [email protected] () ABSTRACT Observation of standard stars is of crucial importance in stellar photometry. We have studied the standard transformation relations of the UBV RI CCD photometric system at the Maidanak Astronom- ical Observatory in Uzbekistan. All observations were made with the AZT-22 1.5m telescope, SITe 2k CCD or Fairchild 486 CCD, and standard Bessell UBV RI filters from 2003 August to 2007 September. We observed many standard stars around the celestial equator observed by SAAO astronomers. The atmospheric extinction coefficients, photometric zero points, and time variation of photometric zero points of each night were determined. Secondary extinction coefficients and photometric zero points were very stable, while primary extinction coefficients showed a distinct seasonal variation. We also determined the transformation coefficients for each filter. For B, V , R, and I filters, the transformation to the SAAO standard system could be achieved with a straight line or a combination of two straight lines. However, in the case of the U filter and Fairchild 486 CCD combination, a significant non-linear correction term - related to the size of Balmer jump or the strength of the Balmer lines - of up to 0.08 mags was required.
    [Show full text]
  • Exploring the Population of Compact Stellar X-Ray Sources in Our Milky Way
    AUTHOR: Sandra Magdy Kamel Greiss DEGREE: MSc TITLE: Exploring the population of compact stellar X-ray sources in our Milky Way DATE OF DEPOSIT: .............................. I agree that this thesis shall be available in accordance with the regulations governing the University of Warwick theses. I agree that the summary of this thesis may be submitted for publication. I agree that the thesis may be photocopied (single copies for study purposes only). Theses with no restriction on photocopying will also be made available to the British Library for microfilming. The British Library may supply copies to individuals or li- braries. subject to a statement from them that the copy is supplied for non-publishing purposes. All copies supplied by the British Library will carry the following statement: \Attention is drawn to the fact that the copyright of this thesis rests with its author. This copy of the thesis has been supplied on the condition that anyone who consults it is understood to recognise that its copyright rests with its author and that no quotation from the thesis and no information derived from it may be published without the author's written consent." AUTHOR'S SIGNATURE: ..................................................... USER'S DECLARATION 1. I undertake not to quote or make use of any information from this thesis without making acknowledgement to the author. 2. I further undertake to allow no-one else to use this thesis while it is in my care. DATE SIGNATURE ADDRESS ............................................................................
    [Show full text]
  • An Analysis of the Long-Term Photometric Behavior of Ε Aurigae
    Kloppenborg et al., JAAVSO Volume 40, 2012 1 An Analysis of the Long-term Photometric Behavior of e Aurigae Brian K. Kloppenborg Department of Physics and Astronomy, University of Denver, 2112 East Wesley Avenue, Denver, CO 80208; [email protected] Jeffrey L. Hopkins Hopkins Phoenix Observatory, 7812 West Clayton Drive, Phoenix, AZ 85033; [email protected] Robert E. Stencel University of Denver, Department of Physics and Astronomy, 2112 E. Wesley Avenue, Denver, CO 80208; [email protected] Received June 1, 2012; revised October 4, 2012; accepted October 4, 2012 Abstract The lure of a 50% reduction in light has brought a multitude of observers and researchers to e Aur every twenty-seven years, but few have paid attention to the system outside of eclipse. As early as the late 1800s, it was clear that the system undergoes some form of quasi-periodic variation outside of totality, but few considered this effect in their research until the mid-1950s. In this work we focus exclusively on the out-of-eclipse (OOE) variations seen in this system. We have digitized twenty-seven sources of historic photometry from eighty-one different observers. Two of these sources provide twenty-seven years of inter- eclipse UBV photometry which we have analyzed using modern period finding techniques. We have discovered the F-star variations are multi-periodic with at least two periods that evolve in time at DP ≈ –1.5 day/year. These periods are detected when they manifest as near-sinusoidal variations at 3,200-day intervals. We discuss our work in an evolutionary context by comparing the behavior found in e Aur with bona-fide supergiant and post-AGB stars of similar spectral type.
    [Show full text]