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9.7 Option – Astrophysics: 3. Spectroscopy
| Syllabus reference (October 2002
version) |
|
3. Spectroscopy is a vital tool for astronomers and
provides a wealth of information
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Students learn to:
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Students:
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Extract from Physics Stage 6 Syllabus (Amended
October 2002). © Board of Studies, NSW.
[Edit: 12 Aug 08]
Prior learning:
Preliminary module 8.2 The World Communicates
Preliminary module 8.5 The Cosmic Engine
Background:
Spectroscopy is the analysis of spectra. There are three
types of spectra – continuous, emission (bright lines)
or absorption (black lines.) This website covers the history
of spectroscopy and what it has revealed:
Spectroscopy: Information concealed in
starlight
Brian von Konsky, Curtin University of
Technology, WA.

perform a
first-hand investigation to examine a
variety of spectra produced by discharge tubes, reflected
sunlight, or incandescent filaments
- Your teacher may have planned a first hand
investigation for you, or you could follow the
sample procedure below. Ensure that the plan you use
includes consideration of any safety aspects such as
dangers from high voltage or X-radiation from discharge
tubes or power supplies, and the brightness of the Sun. You
should include details of any safe work practices you adopt
as you perform this investigation in any report you write.
- Draw each spectrum you examine, noting any observable
features. As a result of your investigation you should be
able to group spectra into a small number of distinct
types, based on similarity of identifiable features. You
will find examples of what you would expect to see in
astronomy texts or by searching the Internet.
Sample Procedure
Safety note: Do not look directly at
the sun with your eyes or through any optical device unless
it has been designated as safe to use for this purpose.
Keep a safe working distance from any high voltage or spark
discharge apparatus.
Choose a variety of light sources for this experiment.
Include light from an incandescent lamp (i.e., one with a
filament), a fluorescent tube, a flame, light seen through
various coloured solutions, and various discharge tubes as
commonly found in school science laboratories. Since you
should not point the spectroscope directly at the Sun, you
could look at the sunlight reflected from a sheet of white
paper or card. Comment on what effect this might have on
the accuracy or validity of what you observe.
Examine the light from each source using a spectroscope.
You should describe and draw each spectrum, indicating
observable features of the spectrum. If it is possible to
vary the voltage of the incandescent lamp, examine the
light from this source at various power levels, commenting
on both the change in brightness and range of colours
observed. As an extension, you could use the scale in the
spectrometer to observe and record the wavelength of
features of each spectrum.
Group the spectra you have observed according to whether
they are continuous spectra, line spectra, absorption
spectra or a combination of these. Describe the common
features of each type of spectrum.

account
for the production of emission and absorption spectra and
compare
these with a continuous blackbody spectrum
- An emission spectrum consists only of radiation at a
number of discrete wavelengths, appearing as bright lines
against a dark background. This type of spectrum is
produced by hot diffuse gases, such as in a gas discharge
tube or in clouds of interstellar gas heated by hot young
stars nearby. Electrical energy or heat supplied to the gas
is absorbed by atoms or ions in the gas, raising the energy
level of electrons. As the electrons fall back to their
normal energy state, they give up a quantum of energy as a
photon corresponding to one of the observed wavelengths.
The emission spectrum is made up of lines corresponding to
all the possible electron transitions. The relative
intensity of each line depends on the composition of the
gas.
- An absorption spectrum consists of a continuous range
of wavelengths with discrete gaps at particular
wavelengths, appearing as dark lines against a continuous
background of colours. Absorption spectra are produced when
a continuous spectrum of light passes through a cloud of
cool gas. Atoms and ions in the gas absorb photons of
wavelengths corresponding to the quanta of energy involved
in possible transitions of electrons to higher energy
levels. The electrons quickly fall back to their original
energy level, re-emitting the absorbed wavelength in all
directions, thus reducing the intensity of light
transmitted at the corresponding wavelengths. These
wavelengths correspond to the dark lines of the absorption
spectrum. The relative darkness of each line depends on the
composition of the gas. The darkness of the lines against
the background spectrum depends on the size and density of
the cloud of gas.
- A continuous black body spectrum has no lines, either
dark or bright, but instead shows a continuous range of
frequencies. Continuous spectra are given off by hot
solids, liquids and high pressure gases. The intensity of
the spectrum varies smoothly with frequency, with a maximum
that depends on the temperature of the body.
An alternative way of comparing the three types of
spectrum is by using a table:
| Continuous black body spectrum |
Emission spectrum |
Absorption spectrum |
|
consists of a continuous range of frequencies
without either bright or dark lines, appearing as a
continuous range of colours
|
consists only of radiation at a number of discrete
wavelengths, appearing as bright lines against a dark
background
|
consists of a continuous range of wavelengths with
discrete gaps at particular wavelengths, appearing as
dark lines against a continuous background of
colours
|
|
given off by hot solids, liquids and high pressure
gases
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produced by hot diffuse gases
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produced when a continuous spectrum of light passes
through a cloud of cool gas
|
|
all wavelengths are produced at some intensity
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wavelengths produced depend on possible energy
transitions within atoms of the gas
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wavelengths absorbed depend on possible energy
transitions within atoms of the gas
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intensity varies smoothly with wavelength, with the
maximum depending on the temperature of the hot
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intensity of lines varies discretely with each
wavelength, depending on the composition of the gas
|
darkness of lines varies discretely with each
wavelength, depending on the composition and density of
the gas
|
on blackbody emission, that allows
you to specify different values of surface temperature, can
be found at:
Continuos Emission and Absorption Spectra
Center for Astrophysics, Harvard Smithsonian, USA. (This web site
last checked 12 August 2008)

describe
the technology needed to measure astronomical spectra
- An astronomical spectrum consists of the range of
wavelengths of light and other radiation emitted, reflected
or transmitted by an astronomical object such as a star, a
nebula, a galaxy or a quasar.
- Astronomical spectra can be viewed using a
spectroscope, or recorded and measured with a spectrograph,
mounted at the focus of a telescope. A spectrograph
consists of 3 parts:
- The first part, known as a collimator, uses a narrow
slit and one or more mirrors or lenses to form a parallel
beam of light from a single light source such as a star.
- The second part is known as the dispersive element as
it produces the spectrum by dispersing the beam into its
component wavelengths. It consists of either a triangular
prism or a diffraction grating. The grating consists of
many closely spaced parallel slits (transmission grating)
or ruled lines (reflection grating).
- The third part is a device to view or record the
different wavelengths. It may be a viewing telescope, a
focussing mirror with photographic plate or film, or an
electronic imaging device such as a charge coupled device
(CCD) detector. CCD detectors, like those used in video
cameras, have the advantage of being able to record very
faint light signals. Other modern enhancements include the
use of computer controlled positioning equipment in
conjunction with fibre optics, and multiple spectroscopes
to obtain the spectra of many objects in the viewing field
at once, or selectively examine various parts of a single
object concurrently.

identify
the general types of spectra produced by stars, emission
nebulae, galaxies and quasars
- Stars are masses of hot dense gas undergoing
thermonuclear fusion at their core. They behave as
approximate black bodies and so their spectrum is therefore
that of a black body corresponding to the temperature of
the star’s surface. Generally however there will also
be prominent dark absorption lines produced as a result of
the continuous black body light passing through the
star’s relatively cooler atmosphere that is above its
surface. For this reason stars are observed to produce
absorption spectra.
- Emission nebulae are regions of hot gas, mainly
hydrogen, and dust heated by the radiation from nearby
young stars. As excited electrons in the atoms and ions
within the nebula drop to lower energy levels, line spectra
are produced with emission lines in the ultraviolet,
visible, infrared and radio bands, characteristic of the
elements that make up the nebula.
- A galaxy is an aggregation of hundreds of thousands to
billions of stars. The spectrum of a galaxy is essentially
a composite of the various spectra from its components.
This generally consists of a continuous background
superimposed with absorption lines of type B and K stars,
along with emission lines due to hydrogen in gaseous
nebulae. As most galaxies are receding from our point of
view, the lines of galaxies are often strongly red-shifted.
- Quasars, are very distant objects that produce vast
quantities of continuous radiation at all wavelengths but
with most of their energy in the longer radio wavelengths.
Quasars have quite different spectra from those of close
galaxies, because they have broad, high intensity emission
lines superimposed on the continuous spectrum. These lines
show an extremely large red shift, which indicates that
they are moving at speeds up to 0.9 c. Some show absorption
lines with red shift near or less than those shown by
emission lines. It is thought that these absorption lines
could be caused by dim galaxies and interstellar gas
between Earth and the quasars.

describe
the key features of stellar spectra and describe how these
are used to classify stars
- A stellar spectrum is the spectrum of radiation emitted
by a star.
- A stellar spectrum consists of an approximate black
body radiation spectrum for the temperature of the stellar
surface, superimposed with absorption lines characteristic
of the elements present in the stellar atmosphere.
- The shape of the curve of intensity against wavelength
across a star’s black-body spectrum, and particularly
the position of the intensity maximum, identifies the
surface temperature of the star. When stars of different
surface temperature are compared, there is an increase in
luminosity along with a gradual change from red, for the
coolest stars, through orange, yellow, white and eventually
to blue for the hottest stars.
- Thus the spectral quality of stellar radiation can be
used to classify visible stars into several spectral class:
O, B, A, F, G, K, and M, from hottest to coolest. Each
spectral class has a characteristic colour and surface
temperature range, and each is characterised by specific
absorption line patterns, indicating the elements in the
star’s atmosphere. Each class is further subdivided
into ten sub classes, e.g. O1, O2, O3...O8, O9, B0, B1, B2
... There are also stars that radiate predominantly in the
ultra-violet (class W) and infra-red (classes R, N and S)
regions of the spectrum.
Table of spectral classes of visible
stars
| Spectral Class |
Colour |
Surface temperature (K) |
Elements evident in absorption lines |
| O |
blue |
over 30 000 |
ionised He, weak H |
| B |
blue-white |
30 000 – 15 000 |
neutral He, weak H |
| A |
white |
15 000 – 10 000 |
strong H |
| F |
white-yellow |
10 000 – 7 000 |
weak H, metals (Ca, Fe) |
| G |
yellow |
7000 - 5000 |
strong metals, esp. Ca |
| K |
orange |
5000 - 4000 |
strong metals; CH and CN |
| M |
red |
4000 - 3000 |
strong molecules (incl. TiO) |

describe
how spectra can provide information on surface temperature,
rotational and translational velocity, density and chemical
composition of stars
-
Surface temperature: The continuous
spectrum of a star is similar to that of a black body
radiator at the same surface temperature. By plotting the
intensity of a star’s radiation as a function of
its wavelength, the wavelength at which intensity is a
maximum can be found. Wien’s Law shows that this
wavelength is inversely proportional to the surface
temperature (K) of the star. This means that the redder a
star appears, the lower is its surface temperature, while
the bluer the star, the higher the surface temperature.
Wien’s Displacement Law: (not required by the
syllabus)
-
Rotational velocity: If a star is
rotating, then one side is travelling away from us while
the other side is coming toward us. Light emitted from
the receding side will be red-shifted, while light from
the approaching side will be blue-shifted by the same
amount. Light from other parts of the star will fall
within these two limits. Thus the individual spectral
lines will be broadened by an amount depending on the
rotational velocity of the star. The faster a star
rotates, the more broadening of spectral lines is
observed.

- Translational velocity: The component
of the translational velocity of a star parallel to the
observer’s line of sight can be determined by
observing the extent and direction of Doppler shift
exhibited by the star’s absorption lines. If a star
is approaching the observer, every absorption line in the
spectrum of the star is shifted toward the blue end of the
spectrum by the same amount. If the star is moving away,
all the lines are shifted towards the red end. The amount
by which all the lines are shifted depends on the component
of the velocity of the star along the line of sight.
The component of the translational velocity of a star
perpendicular to the observer’s line of sight cannot be
determined from the star’s spectrum, but only
photographically over a lengthy period of time.
- Density: Density, and therefore
pressure, at the surface of a star can also broaden
spectral lines, but the intensity varies across the line in
different way from the effect of rotation. In high density
(small and massive) stars the increased gas pressure
produces more rapid collision between atoms during the
emission or absorption of radiation. These collisions cause
changes in the electron orbits and hence produce a broader
spectral line. Rotational velocity and the density of a
star can both be deduced from the width and shape of the
spectral lines.
- Chemical composition: Each chemical
element has a unique emission spectrum consisting of lines
corresponding to the internal electronic transitions within
the element. These lines are in the same places as the
lines in an absorption spectrum for a cloud of the same
element. Elements in the star’s outer layers absorb
light from the continuous black-body spectrum of the star.
A comparison of a star’s absorption spectrum with the
spectra of known elements allows the chemical composition
of the star’s outer layers to be deduced.

analyse
information to predict
the surface temperature of a star from its
intensity/wavelength graph
- You may be provided with a graph of intensity against
wavelength for the spectrum of a star. Analyse the
information by first identifying the wavelength at
which the black body curve is at its highest intensity. You
will need to be able to justify your estimate of this
wavelength. This can best be done by drawing a vertical
line down from the peak of the curve so that it intercepts
the horizontal (wavelength) axis. You may need to
interpolate between divisions on the wavelength axis. Take
care to ensure that your answer is given in the correct SI
unit.
- In order to predict the surface
temperature of the star from the wavelength of maximum
intensity, you will probably be given the Wien’s Law
equation:
where (W = 2.89 x 10-3 m.K). Rearrange the equation so
that T is the subject of the equation, then substitute in the
value of wavelength from the graph.
Example:
The intensity/wavelength graph of a star is given below.
Use this curve to predict the star’s surface
temperature.
Solution:
From the curve the wavelength at which the intensity is
a maximum is approximately 5.8 x 10-7 m. The
star’s surface temperature is then:
