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Sirius and White Dwarf

The Hertzsprung-Russell (HR) Diagram

Posted in September 4, 2021 by David

Categories: Cosmology, Science

Tags: Cosmology

The Hertzsprung-Russell diagram is foundational to an understanding of stars and virtually everything astronomers have learned about stars, galaxies, and the universe.  The diagram plots the absolute magnitude of a star against its spectrum. Thus, to put any star on the diagram, we only need to know its surface temperature (which relates to its spectral type) and absolute brightness.

Astronomers can determine the spectral type for visible stars if the telescope can gather enough light.  The amount of light collected from a star can be increased with a larger telescope, longer collections time, or more sensitive equipment. In addition, astronomers can determine the absolute magnitude of a star if we know the parallax of the star (which can be difficult to measure) and its apparent brightness.

The H-R diagram relates the absolute brightness of a star to its surface temperature.

By Richard Powell – The Hertzsprung Russell Diagram, CC BY-SA 2.5, Link

The main sequence on the HR diagram is where most stars can be located. The band of stars goes from the faint red stars on the lower right to the brilliant blue stars on the upper left.  All the main sequence stars are called “dwarf” stars even though they come in many different sizes.

In the upper right of the diagram reside the red-giant stars, which are enormously big but with low surface temperatures.  The lower left part of the diagram shows a sparser collection of faint blue-white stars, the “white dwarf” stars.

We know the red giant stars in the upper right portion of the HR diagram are “giants,” huge stars with low surface temperatures but enormous sizes radiating lots of light.

Stars in the main sequence are referred to a “dwarfs” by convention.  How small can a star be and still be considered a star?

Alvin Clark and Sirius

The refractor was the main telescope design used in the 19th century.  This used the same design as a modern camera or binoculars to look through a lens.  The lenses used at that time were very difficult to make well and often required multiple attempts to make a perfect glass lens without any bubbles or imperfections.  Of course, these imperfections would adversely affect the quality of the image produced.

The lens type of telescope was that the glass would sag or change conformation when it was pointed in different directions.  This was due to the weight of the glass and was largely unavoidable. As a result, larger and larger lenses were being made, but they soon reached their maximum practical size.

The appearance of one of the largest refracting telescopes.

By W. J. Morgan & Co. – This image is available from the United StatesLibrary of Congress;’s Prints and Photographs division under the digital ID cph.3a13718. Link

The reflector is the type of telescope that is currently design type used in modern large telescopes where a mirror is used instead of a lensing system.  This is because the massive weight of the reflecting mirrors can be supported individually using computer guidance to produce a perfectly focused beam of light.  Large refractor telescopes are mostly now relics of the past.

Alvin Clark was busy testing the lens of the 36 inch Lick refractor seen on the right drawing.  The Lick observatory telescope was the largest in the world at the time of its completion in 1887.

Clark had made an 18.5-inch lens for the University of Mississippi in 1862.  He was testing the optics on the brightest star in the sky, Sirius.  During these observations, he discovered a faint companion star that had never been seen before.  Friedrich Bessel had proposed a “dark companion” of Sirius based on this faint wobble several decades earlier but sadly did not live to see that he was correct in his predictions.

Sirius and Its Companion Star

Under ideal observational conditions, Sirius can just be glimpsed during the daytime.  Its brightness is in contrast with its companion star which is much dimmer.  The question became, why is it dimmer?

The two stars are at approximately the same distance from the Earth, but Sirius appears 780 times brighter than its companion star.  The difference in their brightness represents a difference in their absolute brightness.  Sirius is just much brighter than its companion.

Sirius is about 23 times more bright than the Sun at the wavelength of visible light.  Astronomers determined the spectra of these two wars and were able to determine their surface temperature.  Sirius has a surface temperature of 9,900 K. In contrast, its companion has a surface temperature of 25,000 K.  Using the Stefan-Boltzman equation, the diameter of Sirius turns out to be 2,300,000 kilometers or 60% greater than the diameter of the Sun.

The real surprise came when the diameter of Sirius’ companion star was calculated.  The diameter was about 12,800 kilometers, the same as the Earth’s!  The dramatic conclusion of this exercise was that stars exist which are about the same size as the Earth!  These are now referred to as “white dwarfs.”

These conclusions all arise from an understanding that the star’s surface temperature determines the spectral types of various stars, and according to the HR diagram, the spectral type of a star determines its absolute brightness.

What astronomers next needed to determine the cause of these relationships.

Summary

The Hertzsprung-Russell diagram represents an amazing discovery.  Stars are so distant that even the closest star is (at least now) too far away for direct exploration.  It takes light from that star years to travel the immense distance to Earth.

Even though stars are so far away, we can learn much about them just by observation of their simple characteristics.  The spectrum of a star carries a tremendous amount of information as its internal structure and composition determine its spectral type.  By knowing its spectral type, we know the star’s surface temperature and absolute brightness.  Astronomers can then determine the size of a star through applications of the Stefan-Boltzman equation – truly a remarkable achievement.

The next puzzle was why all of this happens!


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