the classification of stellar spectra

21
The Hertszprung-Russell diagram plots the luminosities (absolute magnitudes) of stars as a function of their spectral type, and reveals that stars with the same spectral type can have very different luminosities. In addition, the spectra of stars with the same effective temperature but different luminosities show subtle differences in line widths. Today, we know that the spectra of stars depend on both their effective temperature (reflecting the temperature dependence in the excitation and ionization of atoms/ions) and their luminosity (reflecting pressure broadening of atomic/ionic spectral lines). The Harvard scheme The Classification of Stellar Spectra

Upload: ahanu

Post on 23-Feb-2016

36 views

Category:

Documents


0 download

DESCRIPTION

The Classification of Stellar Spectra. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: The Classification of Stellar Spectra

The Hertszprung-Russell diagram plots the luminosities (absolute magnitudes) of stars as a function of their spectral type, and reveals that stars with the same spectral type can have very different luminosities. In addition, the spectra of stars with the same effective temperature but different luminosities show subtle differences in line widths. Today, we know that the spectra of stars depend on both their effective temperature (reflecting the temperature dependence in the excitation and ionization of atoms/ions) and their luminosity (reflecting pressure broadening of atomic/ionic spectral lines). The Harvard scheme classifies stars according to their effective temperatures. The Morgan-Keenan scheme extends the Harvard classification to further classify stars according to their luminosities.

The Classification of Stellar Spectra

Page 2: The Classification of Stellar Spectra

Learning Objectives Stellar Evolution Early and

Late Spectral Type Stars Stellar Luminosities and Sizes

Hertzprung-Russel Diagram Morgan-Keenan Classification

Luminosity classesPressure broadening of spectral lines

Spectroscopic Parallax

Page 3: The Classification of Stellar Spectra

Learning Objectives Stellar Evolution Early and

Late Spectral Type Stars Stellar Luminosities and Sizes

Hertzprung-Russel Diagram Morgan-Keenan Classification

Luminosity classesPressure broadening of spectral lines

Spectroscopic Parallax

Page 4: The Classification of Stellar Spectra

By the early 20th century, astronomers had some notion of the -luminosities of stars (distances measured through trigonometric parallaxes) -masses of stars (from studies of binary systems) -effective temperatures of stars (from studies of stellar spectral lines)

At the time, astronomers believed that stars began their lives as hot and luminous O stars and ended their lives as cool and dim M stars. (Today, we know this idea to be incorrect.)

Astronomers therefore referred to stars with spectral types O, B, and A as early spectral types (under the notion that these stars were relatively young) and F, G, K, and M as late spectral types (under the notion that these stars were relatively old). This tradition remains in the language of astronomers.

Stellar Evolution

Oh Be A Fine Girl/Guy Kiss Me Age ➙

{ }Early-type stars

Late-type stars

Page 5: The Classification of Stellar Spectra

If the idea of stellar cooling was correct, there should therefore be a relation between a star’s luminosity (absolute magnitude) and its spectral type.

Stellar Luminosities and Sizes

In 1905, A Danish engineer and amateur astronomer, Ejnar Hertzsprung, compared the absolute magnitudes and spectral types of stars for which both quantities had been accurately determined.

Independently, an astronomer at Princeton University, Henry Norris Russell, was conducting a similar study.

Ejnar Hertzsprung, 1873-1965

Henry Norris Russell, 1877-1957

Page 6: The Classification of Stellar Spectra

Russell published the following plot based on more than 200 stars.

Stellar Luminosities and Sizes

Lum

inos

ity

Later Spectral Type Does this plot support the argument that

earlier spectral types are more luminous than later spectral types?

Page 7: The Classification of Stellar Spectra

Russell published the following plot based on more than 200 stars.

Stellar Luminosities and Sizes

Lum

inos

ity

Later Spectral Type Does this plot support the argument that

earlier spectral types are more luminous than later spectral types? To a degree yes, in the sense that there seems to be a trend of higher luminosity towards earlier spectral types.

Page 8: The Classification of Stellar Spectra

Russell published the following plot based on more than 200 stars.

Stellar Luminosities and Sizes

Lum

inos

ity

Later Spectral Type Does this plot support the argument that

earlier spectral types are more luminous than later spectral types? To a degree yes, in the sense that there seems to be a trend of higher luminosity towards earlier spectral types.

Looking at all the points as a whole, does this plot support the argument that earlier spectral types are more luminous than later spectral types?

Page 9: The Classification of Stellar Spectra

Russell published the following plot based on more than 200 stars.

Stellar Luminosities and Sizes

Lum

inos

ity

Later Spectral Type Does this plot support the argument that

earlier spectral types are more luminous than later spectral types? To a degree yes, in the sense that there seems to be a trend of higher luminosity towards earlier spectral types.

Looking at all the points as a whole, does this plot support the argument that earlier spectral types are more luminous than later spectral types? No, in the sense that the maximum luminosity does not appear to vary much across spectral types.

Page 10: The Classification of Stellar Spectra

Stellar Luminosities and Sizes Hertzsprung was puzzled by the discovery that

stars of type G and later had a range of luminosities despite the same spectral types.

Stars of the same spectral types but different luminosities must have different sizes, as dictated by the Stefan-Boltzmann law

Hertzsprung therefore referred to the brighter stars as giants.

Independently, Russell came to the same conclusion. He also called the stars in the upper right corner giants.

He called stars in the strip bounded by the diagonal line, containing most (80%-90%) of the stars studied, dwarfs.

Lum

inos

ity

Later Spectral Type

GiantsDwarfs

Page 11: The Classification of Stellar Spectra

Learning Objectives Stellar Evolution Early and

Late Spectral Type Stars Stellar Luminosities and Sizes

Hertzprung-Russel Diagram Morgan-Keenan Classification

Luminosity classesPressure broadening of spectral lines

Spectroscopic Parallax

Page 12: The Classification of Stellar Spectra

A modern version of the Hertzsprung-Russel (H-R) diagram.

The Hertzsprung-Russel Diagram

This diagram shows a simple relation between a stars’s luminosity and temperature on the main sequence.

A star’s position on the main sequence is governed by a single factor: its mass.

Page 13: The Classification of Stellar Spectra

Learning Objectives Stellar Evolution Early and

Late Spectral Type Stars Stellar Luminosities and Sizes

Hertzprung-Russel Diagram Morgan-Keenan Classification

Luminosity classesPressure broadening of spectral lines

Spectroscopic Parallax

Page 14: The Classification of Stellar Spectra

Hertzsprung wondered whether there might be some differences in the spectra of stars of the same spectral type but vastly different luminosities. He found just such a variation in spectra among the stars cataloged by Antonia Maury.

The worked developed by Hertzsprung and Maury, and continued by other astronomers, culminated in the 1943 publication of the Atlas of Stellar Spectra by William W. Morgan and Phillip C. Keenan of the Yerkes Observatory.

Their atlas consists of 55 prints of spectra that clearly display the effect of temperature and luminosity (different stellar radii for a given spectral type) on stellar spectra.

Morgan and Keenan also described their criteria for the classification of each spectrum and extended the Harvard classification by introducing a luminosity class.

Morgan-Keenan Luminosity Classes

William W. Morgan, 1906-1994

Phillip C. Keenan, 1908-2000

Page 15: The Classification of Stellar Spectra

A page from the Atlas of Stellar Spectra.

Morgan-Keenan Luminosity Classes

Page 16: The Classification of Stellar Spectra

Morgan-Keenan Luminosity Classes The spectral lines of stars with the same effective

temperature but different luminosities have different widths.

In general, for stars of the same spectral type (effective temperature), narrower lines are produced by stars with higher luminosities.

Page 17: The Classification of Stellar Spectra

Spectral Line Profile Recall the three components that contribute to the profiles of spectral lines:

- natural broadening due to Heisenberg’s uncertainty principle (Lorentz profile) - Doppler broadening due to the random motion of hot gas (Gaussian profile) - pressure broadening due to the perturbation of atomic orbitals via collisions with neutral atoms or the electric fields of ions (Lorentz profile)

Page 18: The Classification of Stellar Spectra

Pressure Broadening Larger stars have lower photospheric gas pressures, resulting

in weaker pressure broadening and therefore narrower lines.

Page 19: The Classification of Stellar Spectra

Learning Objectives Stellar Evolution Early and

Late Spectral Type Stars Stellar Luminosities and Sizes

Hertzprung-Russel Diagram Morgan-Keenan Classification

Luminosity classesPressure broadening of spectral lines

Spectroscopic Parallax

Page 20: The Classification of Stellar Spectra

Spectroscopic Parallax The M-K classification scheme enables astronomers to locate a star’s position on

the Hertzsprung-Russell diagram based entirely on the appearance of its spectrum.

Once the star’s absolute magnitude, M, has been read from the vertical axis of the H-R diagram, the distance to the star can be calculated from its apparent magnitude, m, using Eq. (3.5)

where d is in units of parsecs.

Page 21: The Classification of Stellar Spectra

Spectroscopic Parallax The M-K classification scheme enables astronomers to locate a star’s position on

the Hertzsprung-Russell diagram based entirely on the appearance of its spectrum.

Once the star’s absolute magnitude, M, has been read from the vertical axis of the H-R diagram, the distance to the star can be calculated from its apparent magnitude, m, using Eq. (3.5)

where d is in units of parsecs. This method of determining stellar distances is known as spectroscopic parallax,

and is the primary way of determining the distances to stars with no measurable trigonometric parallax.

The intrinsic scatter of roughly ±1 magnitude for a specific luminosity class renders such distance estimates uncertain by a factor of about 101/5 = 1.6.