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Circumstellar Habitable Zones/Extrasolar Planets
Image of the Kepler Space Telescope's Search Range inside this arm of the Milky Way
Image Courtesy of: www.dailygalaxy.com
The Milky Way Galaxy is populated with billions of stars like our Sun, and long before we had the scientific capability to prove the existence of other planets around those stars, we dreamed of those foreign worlds. With no evidence outside our own solar system, we dreamed of the extraterrestrial terrains explorers might encounter. Science Fiction and fantasy is filled with fantastic fictional encounters with alien civilizations on those worlds. The idea of extrasolar planetary travel intrigues the human inclination to explore.
Sadly, technology has not caught up to science fiction with respect to space exploration, but it has achieved positive proof of the existence of other worlds.
1
Artist's Impression of the Planets around
Pulsar, PSR B1257+12. The first
confirmed extrasolar planets.
Image By: NASA/JPL-Caltech/R. Hurt
(SSC)
The first extra solar planet was actually discovered in 1992, when several planets were detected orbiting a pulsar. The first extrasolar planet orbiting a main sequence star came three years later, and is from a class that came to be referred to as a 'hot jupiter' planet, being so close to its star that it may reach as high as a roaring 1200 Kelvin on the day side. Since those first discoveries though, astronomers have found thousands of extrasolar planets,
largely by the work of the Kepler Spacecraft and team. These discoveries range in mass from approximately Earth sized to nearly star sized (these objects are called brown dwarfs). Since that discovery, we've also established several other methods for Extrasolar planet detection that have broadened the search parameters to include Earth-scale planets. Current statistical estimates made by extrapolating from the density of extrasolar planets in nearby star regions, indicate that each star in the Milky Way should have at least one planet orbiting it.
In January 2013, the Harvard-Smithsonian Center for Astrophysics announced the expectation of at least 17 billion Earth sized planets in the Milky Way alone. The key to detecting these planets is to employ a variety of
search methods over widely different parts of the galaxy, because each method of extrasolar planetary detection has its' own strengths and weaknesses.
2
Graphic of Transit Method of Extrasolar Planetary Detection
Image Courtesy Of: http://www.novacelestia.com/images/extrasolar_photometric_transit_method_medium.jpg
Transit Method and Kepler
Planets do not emit their own light, so when an Extrasolar planet passes in front of its host star, the light we see is actually dimmed very slightly by the planetary eclipse. By observing stars for long periods at high accuracy, astronomers can record the little decreases in brightness, and so indirectly observe the planet. This is the method employed by the Kepler Space Telescope, an internationally funded spacecraft. The telescope, launched in 2006 is in orbit above the Earth staring at stars in the central band of the Milky Way waiting for them to 'blink'. In this way, Kepler has produced 2,740 planetary candidates to be confirmed by ground based observatories, and 114 confirmed extrasolar planets to date.
The transit method has provided scientists with many planets from the 100,000 stars being studied by Kepler, but it is biased towards finding large planets orbiting close to their stars. So the majority of Kepler discoveries are hot Neptune to Jupiter-mass planets.
Gravitational Wobble / Radial Velocity Method
An important feature of gravity is that the force of attraction is mutual and in
the radial direction. To illustrate this, think of yourself standing on the surface of the Earth. You know that you stay attached to the surface because
the Earth's gravity is pulling you down towards the Earth's core. What you 3
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may not immediately realize is that just as you are being pulled down to the Earth, the Earth is being pulled towards you. The reason this reaction on the Earth isn't immediately noticeable is the Earth has a mass of 5.97x10
24
kg, and you might have a mass of 100 kg. So you could never measure the tiny acceleration your gravity causes on the Earth.
The same feature applies to stellar gravity. As the Sun pulls on the Earth and
other planets to keep them in orbit, the planets pull on the Sun. But in this case, the combined masses of the planets is actually enough to make a measurable force on the Sun. Saying that the planets orbit the Sun is actually a simplification. Really, the Sun and planets both orbit their combined center of mass, in a sort of massively complex dance. That center of mass is still inside the Sun's radius,
for our Solar system, but this means that an outside observer would see that the Sun wobbles around while the planets orbit! Therefore, if scientists want to find other stellar systems, they can watch for the star to wobble as it dances gravitationally with its planets!
Graphic of Radial Velocity Method
Image by: http://www.scienceinschool.org/2011/issue19/exoplanet
Detecting the wobble of the star becomes a matter of looking for the Doppler
Effect in its light spectrum. When a light source is moving radially away from us, the light appears to have a longer wavelength, this is known as red-
shifting because red has the longer wavelengths in the visible spectrum. As the light source moves towards us radially, its light appears to have shorter wavelengths, known as blue-shifting. So by watching the spectrum of the star as it dances with its planets, we can see the whole spectrum shift towards the red when it's moving away, and to the blue when it's moving towards us.
Circumstellar Habitable Zone
4
Image by:Planetary Habitablility Laboratory at University of Puerto Rico, at Arecibo. http://phl.upr.edu/
In the field of extrasolar planetary hunting, it is an exciting achievement to discover a planet of any description. The true treasure that every team is hunting for though, is another planet that can support life as we know it. As far as biologists have been able to tell, there is only one feature of the Earth that every one of its organisms requires for survival: the presence of liquid water at its' surface. Thus the hunt is on for extrasolar planets with conditions that allow liquid water at their surface. Such a planet is in the Circumstellar Habitable Zone (CHZ), or “Goldilock's Zone” around its star. It's
far enough from its star so that water wouldn't boil away (not too hot), close enough that water wouldn't freeze to ice at its surface (not too cold), and the
right size to allow molecular hydrogen to be trapped on its surface by gravity
(just right). There are a lot of complications to this idea. Firstly, that the CHZ around a star would change dramatically as the star ages in its life cycle, changing luminosity and size. Secondly, that size and composition of atmosphere for a planet can dramatically change the temperature at its surface. However, as a means of ruling out planets where life as we know it could not possible exist, the concept of the CHZ is extremely useful.
5
The very general formula for calculating the CHZ of a main-sequence star is:
Where L
star is the Intrinsic Luminosity of the star, R
inner is the radius of the innermost circle of a star's habitable zone (in AU), and R
outer is the outermost circle of the star's habitable zone (in AU). The area in between makes up a disk where liquid water won't be frozen or boiled away by the host star. The numbers 1.1 and 0.53 represents the stellar flux at those orbital radii.
The first part appears to have a lot of math, but don't get bogged down by the formulas. Feel free to use Excel to complete the calculations for you! Part 1
1)
Using the data in table 1, select any 10 planetary systems downloaded from the NASA maintained database of confirmed Extrasolar Planets. Enter the data in the answer sheet for the systems you select.
2)
Find the Luminosities of the Host Stars The “Stellar Luminosity” value is used to calculate L
star
in solar units. Note that the value in the Stellar Luminosity column is in the units “logL
solar
”. In other words, it is the base 10 log (i.e., log
10
) of the solar luminosity. To convert it to solar units, you’ll need to take the inverse log of the value from the table. This is done by using the 10
x
function on your scientific calculator. For example, if the Stellar Luminosity value is 2, the inverse log is calculated by the following:
Enter 2 in your calculator
Select the 10
x
option
The answer will be 100. So, L
star
= 100 L
solar
(i.e., 100 solar luminosities).
Example 2: log(solar) = -0.2.
Enter -0.2 in your calculator
Select the 10
x
option
Answer: 0.63; So, L
star
= 0.63 L
solar
(i.e., 0.63 luminosities).
Convert the luminosities for the stars you’ve chosen and record in the answer table.
6
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3)
Calculate the Habitable Zone inner and outer boundaries for each chosen star. This is done using the following equations. Record your results in the
table and again, show your work for credit:
4)
Now look back at the Semi-Major Axes for each star that you recorded from NASA's database. Which of the exrasolar planets in each system fall in the Circumstellar Habitable Zone for their star? Hint: Identify which stars have a semi-major axis that lies between R
inner
and R
outer
.
Note: We are ignoring the fact that several of these planets have highly elliptical orbits. Although the semimajor axis may (or may not) lie in the CHZ, a large eccentricity may take the planet in and out of the CHZ during a full orbit.
Part 2
5)
The Sun
We will use the information available to determine which, if any, of the planets in our own Solar System are in the habitable zone of the Sun. Use the data in Table 2 and find the inner and outer boundaries for the habitable zone for the Sun. 6)
Determine whether Venus, Earth, and Mars are in the Sun’s habitable zone using this method and record your data in the answer sheet.
7
Table 1: Extrasolar Planet Data
Star Name
Planet
Letter
Discovery
Method
Orbital
Period
(days)
Stellar
Distance
(pc)
Semi-
Major
Axis
(AU)
Eccentricity
Planet
Mass
(Jupiter
Mass)
Stellar
Mass
Spectral
Type
Stellar
Luminosity
(logL
solar
)
55 Cnc
f
Radial Velocity
262
12.53
0.788
0.305
0.141
0.91
G8 V
-0.235
61 Vir
c
Radial Velocity
38.021
8.52
0.218
0.14
0.057
0.94
G5 V
-0.095
BD+14 4559
b
Radial Velocity
268.94
50.03
0.777
0.29
1.47
0.86
K2 V
-0.32
BD+48 738
b
Radial Velocity
392.6
1
0.2
0.91
0.74
K0 III
1.69
BD-17 63
b
Radial Velocity
655.6
37.54
1.34
0.54
5.1
0.74
K5 V
-0.678
GJ 667 C
c
Radial Velocity
28.14
6.8
0.125
0.02
0.012
0.33
M1.5 V
-1.863
GJ 667 C
f
Radial Velocity
39.026
6.8
0.156
0.03
0.008
0.33
M1.5 V
-1.863
GJ 687
b
Radial Velocity
38.14
4.53
0.164
0.04
0.058
0.41
M3 V
-1.672
GJ 832
c
Radial Velocity
35.68
4.94
0.163
0.18
0.017
0.45
M1.5
-1.585
GJ 876
c
Radial Velocity
30.088
1
4.7
0.13
0.25591
0.7142
0.33
M4
-1.886
GSC 06214-
00210
b
Imaging
145
320
16
0.9
K7
-0.42
HD 100777
b
Radial Velocity
383.7
52.8
1.03
0.36
1.16
1.01
G8 V
0.021
HD 125612
b
Radial Velocity
559.4
52.83
1.37
0.46
3
1.09
G3 V
0.037
HD 137388 A
b
Radial Velocity
330
38.45
0.89
0.36
0.223
0.86
K2 IV
-0.337
HD 13908
c
Radial Velocity
931
66.89
2.03
0.12
5.13
1.29
F8 V
0.602
HD 141937
b
Radial Velocity
653.22
33.46
1.488
0.41
9.316
1.03
G2/3 V
0.022
HD 142415
b
Radial Velocity
386.3
34.57
1.05
0.5
1.62
1.03
G1 V
0.06
HD 147513
b
Radial Velocity
528.4
12.87
1.32
0.26
1.21
1.11
G3/5 V
-0.01
HD 1502
b
Radial Velocity
431.8
167.5
1.31
0.101
3.1
1.61
K0
1.064
8
Star Name
Planet
Letter
Discovery
Method
Orbital
Period
(days)
Stellar
Distance
(pc)
Semi-
Major
Axis
(AU)
Eccentricity
Planet
Mass
(Jupiter
Mass)
Stellar
Mass
Spectral
Type
Stellar
Luminosity
(logL
solar
)
HD 1605
c
Radial Velocity
2111
84.6
3.52
0.098
3.48
1.31
K1 IV
0.82
HD 16175
b
Radial Velocity
995.4
59.84
2.148
0.637
4.77
1.34
G0
0.508
HD 181720
b
Radial Velocity
956
55.93
1.78
0.26
0.37
0.92
G1 V
0.288
HD 218566
b
Radial Velocity
225.7
29.94
0.688
0.3
0.21
0.85
K3 V
-0.452
HD 221287
b
Radial Velocity
456.1
52.88
1.25
0.08
3.09
1.25
F7 V
0.22
HD 25171
b
Radial Velocity
1845
56.05
3.02
0.08
0.95
1.09
F8 V
0.276
HD 40307
g
Radial Velocity
197.8
12.83
0.6
0.29
0.0223
0.77
K3 V
-0.639
HD 4113
b
Radial Velocity
526.62
44.05
1.28
0.903
1.56
0.99
G5
0.086
HD 43197
b
Radial Velocity
327.8
56.3
0.92
0.83
0.6
0.96
G8 V
-0.137
HD 44219
b
Radial Velocity
472.3
50.4
1.19
0.61
0.58
1
G2 V
0.26
HD 4732
b
Radial Velocity
360.2
56.5
1.19
0.13
2.37
1.74
K0 IV
1.19
HD 4732
c
Radial Velocity
2732
56.5
4.6
0.23
2.37
1.74
K0 IV
1.19
Kepler-22
b
Transit
289.86
23
190
0.849
0
0.113
0.97
G5 V
-0.102
Kepler-442
b
Transit
112.30
53
342
0.409
0.04
0.61
-0.932
Kepler-443
b
Transit
177.66
93
779
0.495
0.11
0.74
-0.664
Kepler-428
b
Transit
3.5256
3254
720
0.043
0.22
1.27
0.87
K1 V
-0.39
Kepler-47
c
Transit
303.13
7
1500
0.991
0.411
28
1.05
-0.076
Kepler-68
d
Radial Velocity
580
135
1.4
0.18
0.947
1.08
0.194
9
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Table 2" Orbital Data for the Solar System Inner Planets
Planet Eccentricity
Semi-Major Axis
(AU)
Stellar Luminosity (logL
solar
)
Venus
0.0
0.7
0.0
Earth
0.0
1.0
0.0
Mars
0.0
1.52
0.0
10
Answer Sheet
Selected Extra-Solar Planets
Star
Name
Planet
Letter
L
Star (Solar)
Semi-
Major
Axis
(AU)
R
inner
(AU)
R
outer
(AU)
In
Habitable
Zone?
Yes/No
1
BD-17 63
b
10
-0.678
= 0.21
1.34
√(0.21/1.1)=
0.44
√(0.21/.53)=
0.63
NO
2
GSC
06214-
00210
b
10
-0.42
= 0.38
320
√(0.38/1.1)=
0.588
√(0.38/.53)=
0.847
NO
3
HD
100777
b
10
0.021
= 1.05
1.03
√(1.05/1.1)=
0.977
√(1.05/.53)=
1.41
YES
4
HD
147513
b
10
-0.01
= 0.98
1.32
√(0.98/1.1)=
0.944
√(0.98/.53)=
1.36
YES
5
HD
218566
b
10
-0.452
= 0.35
0.688
√(0.35/1.1)=
0.56
√(0.35/.53)=
0.813
NO
6
HD 40307
b
10
-0.639
= 0.23
0.6
√(0.23/1.1)=
0.457
√(0.23/.53)=
0.659
NO
7
HD 4113
b
10
0.086
=1.22
1.28
√(1.22/1.1)=
1.053
√(1.22/.53)=
1.52
YES
8
HD 44219
g
10
0.26
= 1.82
1.19
√(1.82/1.1)=
1.286
√(1.82/.53)=
1.85
NO
9
Kepler-
443
b
10
-0.664
= 0.22
0.495
√(0.22/1.1)=
0.447
√(0.22/.53)=
0.64
YES
10
Kepler-47
c
10
-0.076
= 0.84
0.991
√(0.84/1.1)=
0.874
√(0.84/.53)=
1.259
YES
11
The Solar System
Star Name
Planet
Semi-
Major Axis
(AU)
L
Star (Solar)
R
inner
(AU)
R
outer
(AU)
In Habitable
Zone?
(Yes/No)
1
Sun
Venus
0.7
1
√(1/1.1)=
0.95
√(1/0.53)=
1.37
NO
2
Sun
Earth
1.0
1
√(1/1.1)=
0.95
√(1/0.53)=
1.37
YES
3
Sun
Mars
1.5
1
√(1/1.1)=
0.95
√(1/0.53)=
1.37
NO
12
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