Lab 8 Packet, Pruyn
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Sam Houston State University *
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1404
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Astronomy
Date
Dec 6, 2023
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Extrasolar Planets
A
NNA
‘C
AT
’ P
RUYN
10/27/2023
E
XTRASOLAR
P
LANETS
P
ROCEDURES
C
OMPUTER
SIMULATIONS
:
This lab makes use of a number of computer simulations created as part of the Nebraska Astronomy Applet Project (NAAP). You will use two different simulation programs, which can be found at the following URLs:
HELPFUL HINT: I can only successfully run these simulators in Microsoft Internet Explorer/Edge. Be sure you have flash enabled. Exoplanet Radial Velocity Simulator
– http://astro.unl.edu/naap/esp/animations/radialVelocitySimulator.html
It should look like THIS when you launch it:
This lab is adapted from the NAAP lab “Extrasolar Planets”
Extrasolar Planets
Exoplanet Transit Simulator, which looks like this when you launch it
– http://astro.unl.edu/naap/esp/animations/transitSimulator.html
2
Extrasolar Planets
L
AB
E
XERCISE
P
ART
I: E
XOPLANET
R
ADIAL
V
ELOCITY
S
IMULATOR
I
NTRODUCTION
Open up the exoplanet radial velocity simulator. You should note that there are several distinct panels:
A 3D Visualization
panel in the upper left where you can see the star and the
planet (magnified considerably). Note that the orange arrow labeled earth view
shows the perspective from which we view the system.
o
The Visualization Controls
panel allows one to check
show multiple
views
. This option expands the 3D Visualization panel so that it shows the
system from three additional perspectives:
A Radial Velocity Curve
panel in the upper right where you can see the graph of
radial velocity versus phase for the system. The graph has show theoretical curve
in default mode. A readout lists the system period
and a cursor allows one to
measure radial velocity and thus the curve amplitude
(the maximum value of
radial velocity) on the graph. The scale of the y-axis renormalizes as needed and
the phase of periastron (closest approach to the star) is assigned a phase of zero.
Note that the vertical red bar indicates the phase of the system presently displayed
in the 3D Visualization panel. This bar can be dragged and the system will update
appropriately.
There are three panels that control system properties. o
The Star Properties
panel allows one to control the mass of the star. Note
that the star is constrained to be on the main sequence – so the mass
selection also determines the radius and temperature of the star.
o
The Planet Properties
panel allows one to select the mass of the planet
and the semi-major axis and eccentricity of the orbit.
o
The System Orientation
panel controls the two perspective angles.
Inclination
is the angle between the Earth’s line of sight and the
plane of the orbit. Thus, an inclination of 0º corresponds to looking
directly down on the plane of the orbit and an inclination of 90º is
viewing the orbit on edge.
Longitude
is the angle between the line of sight and the long axis
of an elliptical orbit. Thus, when eccentricity is zero, longitude will
not be relevant.
There are also panels for Animation Controls
(start/stop, speed, and phase) and
Presets
(preconfigured values of the system variables).
E
XERCISES
Select the preset labeled Option A and click set. This will configure a system with the following parameters – inclination: 90º, longitude: 0º, star mass: 1.00 M
sun
, planet mass: 3
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Extrasolar Planets
1.00 M
jup
, semimajor axis: 1.00 AU, eccentricity: 0 (effectively Jupiter in the Earth’s orbit). 1.
Describe the radial velocity curve. What is its shape? What is its amplitude? What
is the orbital period? The radial velocity curve is sinusoidal in shape with an amplitude of 29 miles per
second. The orbital period is one year.
Increase the planet mass to 2.0 M
jup
and note the effect on the system. Now increase the planet mass to 3.0 M
jup
and note the effect on the system. 2.
In general, how does the amplitude of the radial velocity curve change when the
mass of the planet is increased? Does the shape change? Explain. The shape of the curve does not change, however as the mass of the planet
increases, the amplitude of the curve increases. In this instance, increasing the
mass of the planet at 1.0Mjup resulted in the amplitude increased from 29
miles per second at 2.0Mjup, to 58 miles per second at 3.0Mjup.
Return the simulator to the values of Option A. Increase the mass of the star to 1.2 M
sun
and note the effect on the system. Now increase the star mass to 1.4 M
sun
and note the effect on the system.
3.
How is the amplitude of the radial velocity curve affected by increasing the star
mass? Explain. The amplitude of the radial velocity curve decreases as the mass of the star
increases. When the mass of the star increased from 1.0Msun, the amplitude of
the curve decreased from 29 miles per second at 1.0Msun to 26 miles per second
at 1.2Msun, and 24 miles per second at 1.4Msun.
Return the simulator to the values of Option A.
4.
How is the amplitude of the radial velocity curve affected by decreasing the semi-
major axis of the planet’s orbit? How is the period of the system affected?
Explain. As the semi-orbital major axis of the planet’s orbit is decreased, the amplitude
increases and the orbital period decreases.
4
Extrasolar Planets
Return the simulator to the values of Option A
so that we can explore the effects of system orientation. It is advantageous to check show multiple views
. Note the appearance
of the system in the earth view
panel for an inclination of 90º.
Decrease the inclination to 75º and note the effect on the system. Continue decreasing inclination to 60º and then to 45º. 5.
In general, how does decreasing the orbital inclination affect the amplitude and
shape of the radial velocity curve? Explain. As the orbital inclination decreases the amplitude decreases. When inclination
was decreased from 90 degrees the amplitude decreased from 29 miles per second
to 28 miles per second at 75 degrees, 25 miles per second at 60 degrees, and 20
miles per second at 45 degrees. The shape of the radial velocity curve becomes
flatter the smaller the degree of orbital inclination.
6.
Assuming that systems with greater amplitude are easier to observe are we more
likely to observe a system with an inclination near 0° or 90°. Explain. It would be more likely for us to observe a system with an inclination of 90
degrees. A system with a 90-degree inclination will have a greater amplitude than
a system near 0 degrees. At 0 or near zero degrees, the radial velocity curve
becomes nearly flat with an amplitude nearly 0 miles per second.
Return the simulator to Option A. Note the value of the radial velocity curve amplitude. Increase the mass of the planet to 2 M
Jup
and decrease the inclination to 30°. What is the value of the radial velocity curve amplitude? Can you find other values of inclination and planet mass that yield the same amplitude?
At a mass of 2.0 Mjup and an inclination of 30 degrees, the amplitude is 29 miles per second. The same can be said for a planet with a mass of 1.0 Mjup and inclination of 90 degrees.
7.
Suppose the amplitude of the radial velocity curve is known but the inclination of
the system is not. Is there enough information to determine the mass of the
planet? 5
Extrasolar Planets
No, there is not enough information given to determine the mass because there
could be multiple values that give the same information.
8.
Typically astronomers don’t know the inclination of an exoplanet system. What
can astronomers say about a planet's mass even if the inclination is not known?
Explain. Without the inclination, astronomers can still speculate the mass of the planet and
apply other determined information to narrow down the possible mass.
Select the preset labeled Option B
and click set
. This will configure a system with the following parameters – inclination: 90º, longitude: 0º, star mass: 1.00 M
sun
, planet mass: 1.00 M
jup
, semimajor axis: 1.00 AU, eccentricity: 0.4. Thus, all parameters are identical to
the system used earlier except eccentricity.
In the orbit view box below indicate the earth viewing direction. Sketch the shape of the radial velocity curve in the box at right. Now set the longitude to 90°. Again indicate the earth’s viewing direction and sketch the shape of the radial velocity curve.
6
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Extrasolar Planets
7
Extrasolar Planets
9.
Does changing the longitude affect the curve in the example above? Yes.
10. Describe what the longitude parameter means. Does longitude matter if the orbit
is circular? The longitude parameter determines the angle between the observer and the
minor-axis of the orbit. The radial velocity curve of a planet with a circular
orbit is unaffected by longitude.
Select the preset labeled HD 39091 b
and click set
. Note that the radial velocity curve has
a sharp peak.
11. Determine the exact phase at which the maximum radial velocity occurs for HD
39091 b. Is this at periastron? Does the minimum radial velocity occur at
apastron? Explain. (Hint: Using the show multiple views
option may help you.) The maximum radial velocity occurs at 0.017, at periastron, when HD 30901 b is
closest to its parent star. The minimum radial velocity occurs near apastron
when HD 39091 b is farthest from its parent star. This is due to the fact that
when a planet nears its planet star its velocity will increase due to
gravitational force.
This simulator has the capability to include noisy radial velocity measurements. What we call ‘noise’ in this simulator combines noise due to imperfections in the detector as well as natural variations and ambiguities in the signal. A star is a seething hot ball of gas and not a perfect light source, so there will always be some variation in the signal.
Select the preset labeled Option A
and click set
once again. Check show simulated measurements
, set the noise to 3 m/s, and the number of observations to 50. 12. The best ground-based radial velocity measurements have an uncertainty (noise)
of about 3 m/s. Do you believe that the theoretical curve could be determined
from the measurements in this case? (Advice: check and uncheck the show
theoretical curve
checkbox and ask yourself whether the curve could reasonably
be inferred from the measurements.) Explain. 8
Extrasolar Planets
The theoretical curve could be determined from the measurements. There are also
enough data points with no extreme outliers to simulate the curve.
Select the preset labeled Option C
and click set
. This preset effectively places the planet Neptune (0.05 M
Jup
) in the Earth’s orbit.
13. Do you believe that the theoretical curve shown could be determined from the
observations shown? Explain. The theoretical curve could not be drawn from the observed data points due to
there being too many extreme outliers to generate a reliable curve.
Select the preset labeled Option D and click set. This preset effectively describes the Earth
(0.00315 M
Jup
at 1.0 AU). Set the noise to 1 m/s.
14. Suppose that the intrinsic noise in a star’s Doppler shift signal – the noise that we
cannot control by building a better detector – is about 1 m/s. How likely are we to
detect a planet like the earth using the radial velocity technique? Explain. The radial velocity method is not anticipated to discover a similar planet to Earth.
This is due to the fact that Earth orbits the Sun at a relatively large distance
despite it’s relatively small mass.
You have been running an observing program hunting for extrasolar planets in circular orbits using the radial velocity technique. Suppose that all of the target systems have inclinations of 90°, stars with a mass of 1.0 M
sun
, and no eccentricity. Your program has been in operation for 8 years and your equipment can make radial velocity measurements with a noise of 3 m/s. Thus, for a detection to occur the radial velocity curve must have a sufficiently large amplitude and the orbital period of the planet should be less than the duration of the project (astronomers usually need to observe several cycles to confirm the existence of the planet). Use the simulator to explore the detectability of each of the following systems. Describe the detectability of the planet by checking Yes, No, or Maybe. If the planet is undetectable, check a reason such as “period too long” or “amplitude too small”. Complete the following table. Two examples have been completed for you. 9
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Extrasolar Planets
Mass
Radius
Amplitude
Period
Detectable
Rationale
(M
Jup
)
(AU)
(m/s)
(days)
Y
N
M
A too
small
P too
big
0.1
0.1
8.9
11
X
1
0.1
89.9
11.5
X
5
0.1
450
11.5
X
0.1
1
2.86
365
X
X
1
1
28.8
365
X
5
1
144.1
364
X
0.1
5
1.28
4,080
X
X
X
1
5
12.82
4,080
X
X
5
5
63.4
4070
X
X
0.1
10
0.898
11,500
X
X
X
1
10
8.99
11,500
X
X
5
10
44.9
11,500
X
X
15. Use the table above to summarize the effectiveness of the radial velocity
technique. What types of planets is it effective at finding? Specifically, the radial velocity technique is very useful for discovering exoplanets..
However, it has proven to be problematic when attempting to discover every other
kind of planet. Using the table it is apparent that radial velocity can easily detect
planets with large masses and orbital periods, but has more difficulty detecting
planets with smaller masses and long orbital periods. PART
II: E
XOPLANET
T
RANSIT
S
IMULATOR
I
NTRODUCTION
Open the exoplanet transit simulator. Note that most of the control panels are identical to those in the radial velocity simulator. However, the panel in the upper right now shows the
variations in the total amount of light received from the star. The visualization panel in 10
Extrasolar Planets
the upper left shows what the star’s disc would look like from earth if we had a sufficiently powerful telescope. The relative sizes of the star and planet are to scale in this simulator (they were exaggerated for clarity in the radial velocity simulator.) Experiment with the controls until you are comfortable with their functionality. E
XERCISES
Select Option A and click set. This option configures the simulator for Jupiter in a circular
orbit of 1 AU with an inclination of 90°.
16. Determine how increasing each of the following variables would affect the depth
and duration of the eclipse. (Note: the transit duration is shown underneath the
flux plot.)
Radius of the planet: When increased, the duration and the depth of the eclipse increases. When
decreased, the duration and depth of the eclipse also decreases.
Semimajor axis: When increased, the duration of the eclipse as well as the orbital period will
increase. When decreased, the duration of the eclipse as well as the orbital period
will decrease. However, it doesn’t have an effect on the depth of the eclipse.
Mass (and thus, temperature and radius) of the Star: When increased, the duration of the eclipse increases but the depth of the eclipse
decreases. Similarly, when decreased, the duration of the eclipse decreases while
the depth increases.
Inclination: Changing the inclination would result in there being no eclipse.
The Kepler space probe (
http://kepler.nasa.gov
, launched in 2009) photometrically detects
extrasolar planets during transit. It has a photometric accuracy of 1 part in 50,000 (a noise
of 0.00002).
17. Select Option B
and click set
. This preset is very similar to the Earth in its orbit.
Select show simulated measurements
and set the noise to 0.00002. Do you think
Kepler will be able to detect Earth-sized planets in transit? Yes. He would be able to detect them using the transit method.
11
Extrasolar Planets
18. How long does the eclipse of an earth-like planet take? How much time passes
between eclipses? What obstacles would a ground-based mission to detect earth-
like planets face? The eclipse of a planet similar to Earth would take approximately 13 hours and
the time in-between eclipses would be 1 year. Obstacles in a ground-based
mission on the planet would likely involve its atmosphere. 12
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