Lab 8
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Course
110L
Subject
Astronomy
Date
Dec 6, 2023
Type
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8
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1
Name:__________________________________________
Date:_________________
PHYS 110L Lab # 8
Sloan Digital Sky Survey Stellar Spectra Lab
1
Instructions:
Please read
carefully
and follow the steps described below and answer
all
questions. If confused, please ask your instructor for help.
Part #1 Introduction
Classification lies at the foundation of nearly every science. Scientists develop classification
systems based on the patterns they see. Classifying stellar spectra was a key step for astronomers
in discovering how stars work. Thus, in astronomy as well as other sciences, the seemingly
ordinary step of classifying things eventually yields critical insights into our world.
Useful Definitions:
•
Absorption line
‒
A
“
valley
”
that appears in a spectrum due to light being absorbed by
energy level transitions in atoms
•
Angstrom
‒
A unit of length measurement used for spectral wavelengths; one Angstrom
is one ten-billionth of a meter (1 Å = 10
−
10
m)
•
Balmer series
‒
The series of absorption lines resulting from transitions from low to high
energy starting at the second energy level (
n
=2) in the hydrogen atom
•
Continuum
‒
The smooth curve of a spectrum
•
Continuum peak wavelength
‒
The wavelength at which the spectral continuum is
greatest; it appears as the top of a broad hill in the spectrum
•
Emission line
‒
A
“
peak
”
that appears in a spectrum due to light being emitted from high
to low energy level transitions in atoms
1
Modified from Sloan Digital Sky Survey III,
http://skyserver.sdss.org/dr10/en/proj/teachers/basic/spectraltypes/lesson.aspx
Learning Objectives:
In this lab assignment you will conduct a series of inquiries to identify key features of spectra,
including the continuum peak and absorption lines. You will also explore how atomic energy
level transitions explain spectral absorption lines.
2
•
Energy level
‒
An amount of energy that an electron can have in an atom
•
Hydrogen alpha (Hα) line ‒
An absorption line associated with the transition from the
second energy level (
n
=2) to the third energy level (
n
=3) in the hydrogen atom
•
Noise
‒
Random variations in a spectrum that are not associated with the continuum or
emission or absorption lines
•
Spectrum
‒
A graph of the amount of light given off by an object at different wavelengths
•
Thermal radiation
‒
Radiation given off by hot objects, such as stars
Part #2 Spectra of Stars
A spectrum (the plural is spectra) is a graph of the amount of light something gives off (how
bright the object is) at different wavelengths. In analyzing the spectra of stars, we frequently do
not know the distances to the stars, so a star
’
s spectrum shows how bright it appears from Earth.
The Sloan Digital Sky Survey (SDSS) measures wavelength in units of Angstroms (symbol Å), 1
Angstrom = 10
−
10
meters. The wavelengths of SDSS spectra go from around 4000 Å (just into
ultraviolet light) to 9000 Å (just into infrared light). The scale for the amount of light is
complicated, but higher numbers are brighter.
The image below shows a typical SDSS spectrum with some labels to point out several features.
Study the image; the text on the next page describes some of its features.
3
Some features of the spectrum are:
•
Continuum peak
‒
the top of the broad
“
hill
”
in the spectrum
•
Absorption line
‒
one of the narrow
“
valleys
”
in the spectrum
•
Noise
‒
some small random fluctuation in the spectrum; noise is usually much smaller
than the absorption lines
The spectrum of a star is composed mainly of thermal radiation (blackbody) that produces a
continuous spectrum. The star emits light over the entire electromagnetic spectrum, from
gamma-rays to radio waves. However, stars do not emit the same amount of energy at all
wavelengths.
The peak emission of their thermal radiation (the continuum peak in the previous spectrum)
comes at a wavelength determined by the star
’
s surface temperature
‒
the hotter the star, the
bluer the continuum peak
(recall Wien’s law)
.
An ideal thermal spectrum is shown on the left below. A spectrum of an actual star is shown on
the right.
In addition to the continuous spectrum, a star
’
s spectrum includes dark lines (absorption lines).
Absorption lines are produced by atoms whose electrons absorb light at a specific wavelength,
causing the electrons to move from a lower energy level to a higher one. This process removes
some of the continuum being produced by the star and results in dark features in the spectrum.
In the actual stellar spectrum, shown above on the right, notice how the underlying shape (the
continuum) is a thermal radiation curve with roughly the same peak as the spectrum on the left.
The big difference between these two is that an actual stellar spectrum has absorption lines and
noise.
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4
Part #3 Exploring Spectra
Step 1.
The table below lists 14 stars. Click on each of the star numbers in the table below and
open the hyperlink to go to the Quick Look tool entry for that star. You will see a picture of the
star and its spectrum. Click on the spectrum for a larger view.
Star
Star
1
8
2
9
3
10
4
11
5
12
6
13
7
14
Step 2.
Examine each star and its spectrum and answer the questions below.
Question 1:
What do you notice about the spectra?
All the spectra have absorptions line, noise, continuum peak which are on different sides.
Also, #8 only has noise. Some look similar, but most of them look different.
Question 2:
What are the most important features they all have in common?
The most important features are absorption lines, noise, and continuum peak.
Question 3:
What differences do you notice among the spectra?
The continuum peak is almost always in a different spot. Some of them have it on the left
side, and some have the right side.
Question 4:
How do the features you identified in Question 1 and 2 change among the 14
spectra?
The continuum peak is on different sides, and they have different absorption lines.
5
When the continuum peak on the left side means the stars are hot and when the continuum
peak is on the right side it means the stars are cold. Most of the stars are hot in given
spectrum.
Part #4 Absorption and Emission Lines
In Part #3 you examined the spectra of 14 stars. You probably noticed two features that all the
spectra had in common. All the spectra have similar overall shapes, and all have peaks and
valleys of different heights.
These are the very same features astronomers use to classify stars. In fact, it was through
classifying stars that astronomers eventually realized what those features mean, and how they
relate.
The Hydrogen Atom
To begin to understand what the peaks and valleys mean, take a close look at a hydrogen atom. A
hydrogen atom has one proton and one electron. Its electron can only occupy certain energy
levels; think of energy levels as unequally spaced steps of a ladder. The higher up an electron is
on the ladder, the more energy it has. Astronomers use the letter
“
n
”
and a number to designate
each energy level. The lowest energy level is called the
“
n
=1
”
level, the second lowest level
“
n
=2
,”
the third
“
n
=3
,”
and so on.
Electrons can move from one level to another by absorbing energy or releasing energy. For
example, if an electron moves down from the 2
nd
energy level to the 1
st
(
n
=2 to
n
=1), then the
atom emits a photon of light. The emitted photon has an energy equal to the difference between
the 2
nd
and 1
st
energy levels. An electron can only move up from the 1
st
to 2
nd
energy level if it
gains the right amount of energy. The electron typically gains this energy if the atom absorbs a
photon of light with the right energy.
The animation
link to the right shows a hydrogen atom that
starts with its electron moving from the
n
=1 energy level to
n
=
2
after absorbing a photon. The electron then emits a
photon of the same energy to go back to
n
=1. Since a
photon
’
s wavelength is determined by its energy, if you
know the energy a photon has, you know its wavelength. To
go up from
n
=1 to
n
=2, an electron must absorb a photon
with an energy of 10.2 electron-volts (1.63 × 10
-18
Joules)
‒
this photon has a wavelength of 1216 Angstroms.
To go down from
n
=2 to
n
=1, the atom must emit a photon of 1216 Angstroms.
Question 4:
To go up in energy level from
n
=1 to
n
=2, what wavelength of light must a
hydrogen atom absorb?
It must absorb 1216 Angstroms of light.
6
How do you know? Hint: Re-read the previous paragraph.
It says that a photon’s wavelength is the same as its energy, and to go from n=1 to n=2, it
needs to absorb a photon with the energy of 1216 Angstrom.
Even though hydrogen has only one electron, the electron can jump between different energy
levels. The graph below shows some possible jumps in energy levels for the electron (arrows).
The transition that is most useful to astronomers is the one in the middle, with electrons jumping
up from
n
=2 or down into
n
=2. These transitions are called the Balmer series, after the physicist
who first studied them. The reason that they are so useful is that the wavelengths emitted or
absorbed are wavelengths of visible light.
How does this apply to spectra? Recalling the spectra you classified in the last activity, if you
look at one of the spectra again, you should notice an obvious valley at about 6500 Å
‒
the
wavelength of the first transition in the Balmer series (
n
=2 to
n
=3
). Astronomers call this the Hα
(Hydrogen-alpha) transition, and they call the
signature in a star’s spectrum the Hα line.
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Question 5:
The spectrum below is the spectrum of a typical star. Below the spectrum is a
zoomed-in view of the area around 6560 Å. You saw in the graph previously
that the Hα
transition is at 6563 Å. So, the zoomed-
in view shows the Hα line for the spectrum. Is the Hα
line in this spectrum an emission line or an absorption line?
It is an absorption line.
How do you know?
Because it has a valley which dips down. We know this is an absorption line because of
that.
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Conclusion.
Please provide feedback regarding the lab assignment. Are there things that you
liked or disliked? Thanks!!