The Cosmic Distance Ladder - ak.
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School
Utah State University *
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Course
1040
Subject
Astronomy
Date
Feb 20, 2024
Type
Pages
4
Uploaded by HighnessFireAnteater8
The Cosmic Distance Ladder – Student Guide
Exercises
The
Cosmic
Distance
Ladder
Module
consists
of
material
on
seven
different
distance
determination
techniques. Four of the techniques have external simulators in addition to the background pages. You are
encouraged to work through the material for each technique before moving on to the next technique.
Radar Ranging
Question 1: Over the last 10 years, a large number of iceballs have been found in the outer solar system out
beyond Pluto. These objects are collectively known as the Kuiper Belt. An amateur astronomer suggests using
the radar ranging technique to learn the rotation periods of Kuiper Belt Objects. Do you think that this plan
would be successful? Explain why or why not? No, I don't think this plan would be successful because the
radar ranging technique would only be useful if you want to find its distance but it wouldbt be able to determine
the rotational period.
Parallax
In addition to astronomical applications, parallax is used for measuring distances in many other disciplines
such as surveying. Open the
Parallax Explorer
where techniques very similar to those used by surveyors are
applied to the problem of finding the distance to a boat out in the middle of a large lake by finding its position
on a small scale drawing of the real world. The simulator consists of a map providing a scaled overhead view
of the lake and a road along the bottom edge where our surveyor represented by a red X may be located. The
surveyor is equipped with a theodolite (a combination of a small telescope and a large protractor so that the
angle of the telescope orientation can be precisely measured) mounted on a tripod that can be moved along
the road to establish a baseline. An
Observer’s View
panel shows the appearance of the boat relative to trees
on the far shore through the theodolite.
Configure the simulator to
preset A
which allows us to see the location of the boat on the map. (This is a
helpful simplification to help us get started with this technique
– normally the main goal of the process is to learn the position of the boat on the scaled map.) Drag the
position of the surveyor around and note how the apparent position of the boat relative to background objects
changes. Position the surveyor to the far left of the road and click
take measurement
which causes the
surveyor to sight the boat through the theodolite and measure the angle between the line of sight to the boat
and the road. Now position the surveyor to the far right of the road and click
take measurement
again. The
distance between these two positions defines the baseline of our observations and the intersection of the two
red lines of sight indicates the position of the boat.
We now need to make a measurement on our scaled map and convert it back to a distance in the real world.
Check
the ruler
and use this ruler to measure the distance from the baseline to the boat in an arbitrary unit.
Then use the map scale factor to calculate the perpendicular distance from the baseline to the boat.
Question 2: Enter your perpendicular distance to the boat in map units 7.5
Show your calculation of the distance to the boat in meters in the box below.
Configure the simulator to
preset B
. The parallax explorer now assumes that our surveyor can make angular
observations with a typical error of 3. Due to this error we will now describe an area where the boat must be
located as the overlap of two cones as opposed to a definite location that was the intersection of two lines.
This preset is more realistic in that it does not illustrate the position of the boat on the map.
Question 3: Repeat the process of applying triangulation to determine the distance to the boat and then
answer the following:
What
is
your
best
estimate for
the perpendicular
distance to the boat?
7 x 20 = 140m
What is the greatest distance to the boat that is still consistent with
your observations?
8 x 20 = 160m
What is the smallest distance to the boat that is still consistent with
your observations?
6 x 20 = 120m
Configure the simulator to
preset C
which limits the size of the baseline and has an error of 5 in each angular
measurement.
Question 4: Repeat the process of applying triangulation to determine the distance to the boat and then
explain how accurately you can determine this distance and the factors contributing to that accuracy. After
repeating this process it's not very accurate when it comes to determining the distance and other factors.
Distance Modulus
Question 5: Complete the following table concerning the distance modulus for several objects.
Objec
t
Apparent Magnitude
m
Absolute
Magnitude M
Distance Modulus
m-M
Distance
(pc)
Star A
2.4
2.4
0
10
Star B
6.02
5
1.02
16
Star C
10
8.01
1.99
25
Star D
8.5
0.5
8
398.1
Question 6: Could one of the stars listed in the table above be an RR Lyrae star? Explain why or why not.Yes,
one of the stars in the table could be an RR Lyrae star because both star d and the RR Lyrae star share the
same magnitude of 0.5 which is necessary trait an RR Lyrae star contains
Spectroscopic Parallax
Open up the
Spectroscopic Parallax Simulator
. There is a panel in the upper left entitled
Absorption Line
Intensities
– this is where we can use information on the types of lines in a star’s spectrum to determine its
spectral type. There is a panel in the lower right entitled
Star Attributes
where one can enter the luminosity
class based upon information on the thickness of line in a star’s spectrum. This is enough information to
position the star on the HR Diagram in the upper right and read off its absolute magnitude.
Let’s work through an example. Imagine that an astronomer observes a star to have an apparent magnitude of
4.2 and collects a spectrum that has very strong helium and moderately strong ionized helium lines – all very
thick. Find the distance to the star using spectroscopic parallax.
Let’s first find the spectral type. We can see in the Absorption Line Intensities panel that for the star to have
any helium lines it must be a very hot blue star. By dragging the vertical cursor we can see that for the star to
have very strong helium and moderate ionized helium lines it must either be O6 or O7. Since the spectral lines
are all very thick, we can assume that it is a main sequence star.
Setting the star to luminosity
class V in the Star Attributes panel then determines its position on the HR Diagram and identifies its absolute
magnitude as -4.1. We can complete the distance modulus calculation by setting the apparent magnitude
slider to 4.2 in the Star Attributes panel. The distance modulus is 8.3 corresponding to a distance of 449 pc.
Students should keep in mind that spectroscopic parallax is not a particularly precise technique even for
professional astronomers. In reality, the luminosity classes are much wider than they are shown in this
simulation and distances determined by this technique probably have uncertainties of about 20%.
Question 7: Complete the table below by applying the technique of spectroscopic parallax.
Obser
vatio
nal
Data
Analysis
m
Description of spectral
lines
Description of
line thickness
M
m-
M
d
(pc)
6.2
strong hydrogen lines
moderate helium lines
very thin
4.8
1.4
18.6
13.1
strong molecular lines
very thick
4.8
8.3
447
7.2
strong ionized metal
lines moderate hydrogen
lines
very thick
4.8
2.4
29.5
Main Sequence Fitting
Open up the Cluster Fitting Explorer. Note that the main sequence data for nearby stars whose distances are
known are plotted by absolute magnitude in red on the HR Diagram. In the Cluster Selection Panel,
choose the Pleiades cluster. The Pleiades data are then added in apparent magnitude in blue. Note that the
two y-axes are aligned, but the two main sequences don’t overlap due to the distance of the Pleiades (since it
is not 10 parsecs away).
If you move the cursor into the HR diagram, the cursor will change to a handle, and you can shift the apparent
magnitude scale by clicking and dragging. Grab the cluster data and drag it until the two main sequences are
best overlapped as shown to the right.
We can now relate the two y-axes. Check
the horizontal bar
which will automate the process of determining
the offset between the m and M axes. Note that it doesn’t matter where you compare the m and M values, at
all points they will give the proper distance modulus. One set of values gives m –
M = 1.6 – (-4.0) = 5.6 which corresponds to a distance of 132 pc.
Question 8: Note that there are several stars that are above the main sequence in the upper left. Can you
explain why these stars are not in the main sequence?
These stars aren't in the main sequence due to their
low core energy which means that they won't fit into the sequence because the other stars have a higher
energy.
Question 9: Note that there are several stars below the main sequence especially near temperatures of about
5000K. Can you explain why these stars are not in the main sequence?These stars aren't in the main
sequence due to their higher temperatures which affect the stars that fall under the main sequence.
Question 10: Determine the distance to the Hyades cluster.
Apparent magnitude
m
Absolute Magnitude
M
Distance
(pc)
2
5
2.51
Question 11: Determine the distance to the M67 cluster.
Apparent magnitude
m
Absolute Magnitude
M
Distance
(pc)
5
6
6.31
Cepheids
Question 12: A type II Cepheid has an apparent magnitude of 12 and a pulsation period of 3 days. Determine
the distance to the Cepheid variable and explain your method in the box below?
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Supernovae
Open up the
Supernovae Light Curve Explorer
. It functions similarly to the Cluster Fitting Explorer. The red
line illustrates the expected profile for a Type I supernovae in terms of Absolute Magnitude. Data from various
supernovae can be graphed in terms of apparent magnitude. If the data represents a Type I Supernovae it
should be possible to fit the data to the Type I profile with the appropriate shifts in time and magnitude. Once
the data fit the profile, then the difference between apparent and absolute magnitude again gives the distance
modulus.
As an example load the data for 1995D. Grab and drag the data until it best matches the Type I profile as
shown. One can then use the
show horizontal bar
option to help calculate the distance modulus. One pair of
values is m – M = 13-(-20) = 33 which corresponds to a distance of 40 Mpc.
Question 13: Determine the distance to Supernovae 1994ae and explain your method in the box below?
Question 14: Load the data for Supernova 1987A. Explain why it is not possible to determine the distance to
this supernova? It's not possible to determine the distance of this supernova because absolute magnitude and
apparent magnitude both are different.