Could this hypothetical xoplanet support life?

AI Thread Summary
The created planet has a mass of 0.218 times that of Earth, a radius of 0.60 Earths, and a surface temperature averaging 305 Kelvin. It possesses one moon and orbits a sun-like star every 342 days, with a stable solar system located 50 light years from Earth. The planet's atmosphere could potentially support gases like carbon dioxide, nitrogen, and oxygen, but retention depends on various factors including temperature and gravity. A magnetic field could enhance atmospheric retention, while volcanic activity might replenish gases over time. Overall, the planet's conditions suggest it could harbor native life despite being inhospitable to Earth-like organisms.
KTevolved
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Here is a brief detail on the planet i created.

Mass .218 Earth's, density 5.62 g/cm3, radius .60 Earth's, surface gravity is .602 Earth's
It has 1 moon that has 5% the mass of the main world orbiting 300,000 miles above the surface.
It orbits a sun like star, same luminosity and mass every 342 days, eccentricity is .08
The average temperature is 305 Kelvin
It has 80% water and 20% land, the crust ranges from 5-30 miles thick

I am just wondering if this planet can support a thick atmosphere of carbon dioxide, nitrogen, oxygen, water vapor and some methane. I also need to know if the planet an generate a magnetic field.

The planet i created is currently 3.5 billion years old and it is in a stable solar system that is 50 light years from earth.
 
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Sure, although Earth like life would not survive on this planet i think native life could. It would be hot 305 Kelvin is 89 F and for a global temperature there would be no ice caps at all. There could be plant life if there is a lot of cloud cover to reduce the heat. I think your right on the edge of habitability when it comes to temperature.
 
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Quoting from another thread:

onomatomanic said:
A rule-of-thumb lower bound to atmosphere retention (derived here) is given by

rm ~ (3/2) (k/G) (1/m_proton) (R/M) T ~ 2*10^14 (R in m / M in kg) (T in K)

where R, M and T are the planet's radius, mass and surface temperature in SI units. The resultant number is the molecular mass, in atomic mass units, below which the thermal kinetic energy exceeds the gravitational binding energy.

Plugging in values for Earth, that yields rm ~ 0.06. Gases with a molecular mass below this value cannot be retained at all (which is meaningless here, since molecular masses are by definition integers). Gases between this value and ten times this value are lost quickly, i.e. within a year or so (still meaningless here). Gases between ten times and a hundred times this value are lost slowly, i.e. within a billion years or so. That means everything with a molecular mass below 6, which covers diatomic hydrogen and helium. Gases above a hundred times this value are retained almost indefinitely.

To get a long-lived Earth-like atmosphere, the lightest gas that has to be retained is diatomic nitrogen, I think, which means a molecular mass of 28 and thus rm ~ 0.3. In other words, you need a planet for which the quantity (R/M)*T is no more than five times higher than it is for Earth. If a shorter-lived atmosphere is sufficient, the quantity may be ten or twenty times higher (for reference, "twenty times higher" corresponds to the Moon, roughly).

As mentioned initially, this is a lower bound. It doesn't stop the atmosphere from, say, being chemically absorbed into the crust or being stripped away by solar wind or any number of other relevant processes which have already been discussed above.
mfb said:
If the planet has water, those molecules (atomic weight of 18) should stay in the atmosphere, too.

Some similar relations:
With the average density ρ, M scales with ρR^3, and the ratio becomes \frac{T}{\rho R^2}.

The surface gravity scales with g~M/R^2, and an equivalent ratio is T/(gR).
onomatomanic said:
^ Good point. Evaporating water straight into space doesn't sound very habitable.

And it occurs to me that methane would be again slightly lighter, and should probably be kept too, considering that it's a minor but not insignificant carbon cycle constituent and greenhouse gas.

So, better call it (rm < 2.5 rmEarth) for a long-lived and (2.5 rmEarth < rm < 10 rmEarth) for a short-lived atmosphere. Which means that the Moon isn't even marginally suitable - domed cities it is. :P

Using your values, one gets rm ~ (R/M)*T ~ (0.6/0.218)*(305 K/290 K) rmEarth ~ 2.9 rmEarth

If you're talking about colonization, that's definitely good enough. If you're talking about evolution, it's a little bit outside the stricter limits for water vapor and methane I derived at the end, but should still be close enough for the seepage to be of marginal significance at worst. *thumbs up*

Someone else will have to address magnetic fields, I'm afraid. :smile:
 


How far is it from the star?
 


^ 0.96 AU, unless I misinterpreted the OP.
 


The planet in question should be able to support an atmosphere of any gas, so long as it is not heavier than the material making up the planet itself.

whether or not a planet has a magnetic field depends on whether or not it's core rotates, and what it's inner and outer core consist of.
 


The core would be a iron/nickle and a bit of sulfur mix to lower melting point. The mantle would have more iron in it than Earth's. So with water vapor not being perminant any idea how long it could last in the atmosphere until total dissapearence?
So for the oceans if the atmosphere was thicker in CO2 or nitrogen say 3-6 bar would the liquid stay or seep also?
 


KTevolved said:
So with water vapor not being perminant any idea how long it could last in the atmosphere until total dissapearence?

Very roughly, the range from 2.5 rmEarth to 25 rmEarth corresponds to retention times of billions of years to days. Based on that, my best guess for 2.9 rmEarth would be several billion years for water and a billion years for methane. But the model is very simplistic, so those may be off by several orders of magnitude either way. Millions of years, you can rely on, I'd say.

KTevolved said:
So for the oceans if the atmosphere was thicker in CO2 or nitrogen say 3-6 bar would the liquid stay or seep also?

The way I'm thinking about this (which may be wrong), a thicker atmosphere would actually be counterproductive. The only thing that keeps the gases bound to the planet is gravity, and increasing the amount of atmosphere isn't going to increase the planetary mass in a significant way until it becomes a gas giant, more or less. Instead, more atmosphere means that it extends farther into space, which makes it more susceptible to stripping, and higher absolute losses due to similar relative loss rates. Bad all around, it seems to me.
 


LastTimelord said:
The planet in question should be able to support an atmosphere of any gas, so long as it is not heavier than the material making up the planet itself.

Care to elaborate? Hydrogen? Helium?
 
  • #10


It would be able to support any atmosphere that would realistically exist in large quantities. Of course, if the atmosphere were more dense than the planet, then the gas would sink and the rock would rise, although I severely doubt that any gas would realistically be this dense
 
  • #11


Make sense i could understand leakage in the upper atmosphere. There is one thing i don't get though leakage from the surface because the higher up you get in the troposphere the colder the temperature gets so i would think like 99% of the water vapor would sink back due to colder temps and less heat excitement of molecules That basically what I am confused about but i totally get leakage in the upper atmosphere.
 
  • #12


LastTimelord said:
It would be able to support any atmosphere that would realistically exist in large quantities. Of course, if the atmosphere were more dense than the planet, then the gas would sink and the rock would rise, although I severely doubt that any gas would realistically be this dense

Hard to deny.
 
  • #13


Though it would be cool because with a that leakage maybe some plants if they exist would be able to get water from the vapor instead of just relying on rain haha.
 
  • #14


Plus with a magetic field i would think there would be less escape of any gas but without it i doomed.
 
  • #15


While denser air does sink there would still be very minimal leakage in the upper reaches of the atmosphere. The colder air concept does play an important role though without the freezing temperatures water vapor would escape much quicker. I do believe that with a denser atmsphere and a magnetic field you would hold onto a thicker atmosphere that could last billions of years. Oxygen CO2 and nitrogen will be permenently retained as long as the temperature does not increase. Stay awesome :)
 
  • #16


While onomatomanic is right about adding more atmosphere would cause it to grow in height id think that f the molecules were more tightly paked it would be denser that way and the altitude wouldn't change. While the exosphere and thermospheres height may grow te stratosphere and troposphere might stay the same. Its very interesting to think about.
 
  • #17


KTevolved said:
There is one thing i don't get though leakage from the surface because the higher up you get in the troposphere the colder the temperature gets so i would think like 99% of the water vapor would sink back due to colder temps and less heat excitement of molecules That basically what I am confused about but i totally get leakage in the upper atmosphere.

Atmosphere_model.png


Temperature does drop with height in the region familiar to us (up to 10 km), but this trend doesn't continue indefinitely. Once you get above 100 km, the temperature begins to climb in earnest due to the absorption of hard UV light (which is why we don't get any of that down here).

Whether 99% of the water vapour sinks back isn't the issue at all. Sinking or no sinking, 99% of the atmosphere are close to the planet's surface, simply because density decreases with height. The issue is what happens to the 1% above that. If there is a mechanism which allows this fraction to rapidly escape, then another 1% of the remainder will have to rise to take its place, which will escape by the same mechanism, and so on until there is nothing left. One hundred times "rapidly" is still pretty rapid, if you see what I mean. :smile:

Anyway, I'm not sure I understand your thinking here. Why should water vapour sink down due to temperature decreasing with height? The decrease affects all gases, not just water, and since they can't all sink at the same time, none of them can sink at all, it seems to me. Obviously, if the water vapour gets the chance to precipitate into droplets, this no longer applies and it falls (as rain) rather than sink - maybe that's what you meant?

KTevolved said:
Though it would be cool because with a that leakage maybe some plants if they exist would be able to get water from the vapor instead of just relying on rain haha.

Space plants? I agree that the idea has a certain appeal, but if water leaks at that sort of rate, your planet is pretty much screwed, I think. :-p

KTevolved said:
Plus with a magetic field i would think there would be less escape of any gas but without it i doomed.

Yes, having a magnetic field reduces atmospheric escape, because it deters stripping of the upper layer by the solar wind. It's only one factor among several, either way, though.
 
  • #18


Yea i was trying to say rain but i didnt know if it would just eveaporate before it reached the surface. When you said earlier several billion years retining would that be with a magnetc field and the several million years without. I was just wondering cus billions vs millions is a huuuuge difference haha. I would think volcanic activity would help replenish water and other gases and if it had a longer bombardment with more icy based comets or asteroids but idk. Thinking about this stuff is really cool, cus we might observe it one day.
 
  • #19


KTevolved said:
When you said earlier several billion years retining would that be with a magnetc field and the several million years without. I was just wondering cus billions vs millions is a huuuuge difference haha.

No, the model only covers ordinary kinetic escape driven by heat, nothing else. The difference results from the simplicity of the model, which gives only one hard figure - the watershed between immediate escape and short-term retention. Beyond that, everything is gradual and has to be either intricately modeled or roughly estimated, and I only have the means to do the latter - thus, large error margins. Sorry.

KTevolved said:
I would think volcanic activity would help replenish water and other gases and if it had a longer bombardment with more icy based comets or asteroids but idk.

As I said, my best guess is that the seepage would be insignificant even over billions of years, but it's no more than a guess. If so, you don't need to do anything. If you want to err on the side of caution, give the planet more water than Earth had to start with, so that you can let some portion of it escape and still have enough left to go on with. :smile:
 
  • #20


Volcanic activity would help replenish Co2 levels and if there are plants that produce oxygen more oxygen in the atmosphere. The increased eccentricity is interesting. You would be closer and farther from the sun than Earth is to its own which will have minimal effects. On the close side you will be warmer having more solar enerfy and further less energy. The 80% water would definatly help stay put the water especially if your oceans and seas are deep.
 
  • #21


Yes the i was going for more eccentricity to vary the nvirnments more between hot and cold and i would think that the increase in eccentricity would heat the core a little more than if it were not.
 
  • #22


So how about nirtogen and oxygen can they stay for billions of years also? I also gave the atmosphere 1.5 bars to be realistic lol. Also how would the eccentricity affect the planet?
 
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  • #23


Yes oxygen and nitrogen can stay indefinetly. A 1.5 atmosphere on your planet would keep the oceans in a liquid state and it will rain and have weather systems due to the heating and cooling from the star.
 
  • #24
Eccentricity of 0.08 means that between perihelion and aphelion, orbital distance varies by ~1/6, insolation varies by ~1/3, temperature theoretically varies by up to 30 K. Practically, I'd expect something between 10K and 20K from that source. Definitely noticable; the details depend on the magnitude of your axial tilt and how the equinoxes aligns with perihelion and aphelion.
 
  • #25
Yea i should have been more precise with the orbit. It orbits at 1.06 au. So at its nearest it orbits at 0.971 au and at the furthest it orbits at 1.14 au. The only reason the temperature isn't colder is because of the abundance of Co2 and water in the atmosphere. The axis tilt varies from 23-28 degrees because of the moon but its at 25 degrees right now.
 
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  • #26
^ Right, but you still need to decide on the alignment. The axial tilt is larger than Earth's, and so would still be the primary source of the planet's seasons, so let me for the sake of simplicity use Earth's months to describe the progress of the orbit.

If perihelion were to occur in March and aphelion in September, say, then in the Northern hemisphere the result would be pretty much be a two-season year: Summer from March to September, winter from September to March, with little in the way of a gradual spring and autumn. In the Southern hemisphere, the result would be the same, just shifted by a quarter-year: Summer from December to June, winter from June to December.

If, on the other hand, perihelion were to occur in June and Aphelion in December, you get something quite different: In the Northern hemisphere, you get the familiar four-season year, except that the difference between summer and winter is far greater. Spring and autumn still occur from March to June and September to December, and with about the same temperatures as those we get. But as the eccentricity-driven insolation changes now add to the tilt-driven insolation changes, you might get temperatures of 55 rather than 35 Celsius in summer and -25 rather than -5 Celsius in winter, in what we would consider temperature latitudes. In the Southern hemisphere, the two changes cancel out, and you might get temperature differences between "summer" and "winter" of no more than 10 Celsius. Hardly worth being called seasons at all.

Overall, if you want a situation like on Earth, in which the two hemispheres are pretty much mirror images of each other, have perihelion and aphelion near the equinoxes. If you want a situation in which the two hemispheres have weather patterns as different as those equatorial and temperate regions have on Earth, have perihelion and aphelion near the solstices.

See how that works? :smile:
 
  • #27
For Earth's sake perihelion would occur in March and alphelion in September. I am trying to have the planet be familiar to earthlings while at the same time being very different in terms of climate, weather patterns and gravity. I am still trying to figuer where exactly the tropics and cold regions would be.
 
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  • #28
Best guess, your planet would have a single atmospheric circulation cell per hemisphere, instead of the terrestrial three shown below:

AtmosphCirc2.png


It has to be an odd number, and as your planet is significantly smaller than Earth, and as the size of such cells tends to increase with both mean absolute temperature and mean rate of change of temperature with latitudinal distance, one cell seems like the obvious choice.

The result is pretty boring, unfortunately. There'd be a cold Northeasterly everywhere in the Northern hemisphere and a cold Southeasterly everywhere in the Southern hemisphere, without any of the transient high and low pressure systems which give us the unpredictable changes most of us mean when we talk of "weather". The only variations would be seasonal ones, see above, and daily ones due to the day-night cycle. Nothing in-between.

Further, this would constitute a far more efficient mechanism of latitudinal heat transfer than what we have on Earth, so you probably wouldn't get any ice-caps at the poles. If there's land there, it'll be cold desert, if there's water, it'll just be cold. The mid-latitudes should be drier than ours, generally speaking, and should directly give way to the tropics, without an intervening desert belt.

Do you have an idea how your 20% land is distributed, overall?
 
  • #29
The 20% land is divided into 2 different continents and there are 2 main oceans separating the 2 continents along with polar oceans north and south. Both land masses occupy regions in between the tropic of capricorn and tropic of cancer passing through the equater they are on opposite side of the planet from each other. There is a 1,200 mile long mountain range cutting across the northern end of one of the continents. There are dozens of small islands scattered in between the oceans most of them are volcanic. I am curious what if we tweaked the eccentricity from .08 down to .02 and left the axis at 25 degrees Also switch the perihelion to january and the aphelion to june? Just wondering what would change then. Btw planet is still at 1.06 au with the thick atmosphere.
 
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  • #30
I wish i could draw the planet and its oceans and continents to give a better detail of what I am thinking.

Yes please. No need to go to any trouble, even a picture that's the result of a minute's work in MS Paint is often better than a paragraph of text. You can upload it to e.g. tinypic.com.
 
  • #31
I forgot to add the atmospheric composition.
70% nitrogen, 20% oxygen, 5% xenon, 3% carbon dioxide, 1% water vapor and the rest methane carbon monoxide neon argon and trace hydrogen. The xenon is one of the reasons for the denser atmosphere. The oceans also have a salinity of 5-6% idk if that would do anything but I am just trying to be more specific. Sorry i couldn't add a picture my mind is better with a picture in my mind then laying down words, hard to explain its how my mind works haha. Hope this gives a better idea of the planet.
 
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  • #32
20% oxygen means will have life and the CO2 means if you have plants they will grow to potentially huge sizes. Yes xenon will make the atmosphere denser even on its own. I have a website that will show you the atmospheric retention of all the main gases you have.
http://astro.unl.edu/naap/atmosphere/animations/gasRetentionPlot.html
So you can see that xenon, co2, oxygen and nitrogen can be all retained for many billion of years even longer. Water can also be retained but for several billion maybe 5-6 billion years in the atmosphere but there is an ocean to keep supplying, methane will also last because there is life replenishing it just as on earth. Hydrogen will only last a few thousand years and then dissapear. Having 80% water will help absorb the CO2 more than Earth so if your CO2 was reduced to Earth's level it would be a little colder. Plants will supply oxygen. As for humans settling on its surface we can but there are 2 major factors we will have to get used to, 1 the gravity and 2 the extra heat. The less eccentric orbit will help it be more Earth like. Hope this helps better
 
  • #33
So with a denser atmosphere does that mean water boils at a higher temperature or does the gravity affect it as well. Say a person lands there and they want to boil water for tea or something, would the boiling point be higher or lower than 100 c? Also you didnt explain what the weather would be?
 
  • #35
Sorry about bringing this up again but something confuses me. I get that the water vapor would only last several billion years but what about the liquid ocean on the surface? The planet would get about 92% solar luminousity the Earth does and the reason its heated is the greenhouse gases.
The atmosphere is 1.5 bar which would make the boiling point higher. Plus the atmosphere is denser than Earth's so wouldn't the oceans stay until its star becomes a red giant or will the oceans disappear before then? I am just confused how liquid water on the surface can seep, but i fully understand water seeping in the exosphere.
 
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  • #36
Yes your star will reach red giant stage well before all the surface water on your planet seeps into space on its own.
 
  • #37
How long will the red giant take to evaporate all the surface water? Could life survive after that?
 
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  • #38
KTevolved said:
Sorry about bringing this up again but something confuses me. I get that the water vapor would only last several billion years but what about the liquid ocean on the surface? The planet would get about 92% solar luminousity the Earth does and the reason its heated is the greenhouse gases.
The atmosphere is 1.5 bar which would make the boiling point higher. Plus the atmosphere is denser than Earth's so wouldn't the oceans stay until its star becomes a red giant or will the oceans disappear before then? I am just confused how liquid water on the surface can seep, but i fully understand water seeping in the exosphere.
As long as you have liquid water some amount of it would evaporate.

Out of that water that evaporated, some, in upper layers of atmosphere would either be directly lost, or got smashed by UV and some of the hydrogen atoms will be lost. The process would keep an equilibrium by repeating itself. In long run the share of harder to loose deuterium would increase in relation to normal hydrogen.

Actually if the planet was colder with loosing water you might reach an intermediate solution - partially stripped atmosphere -> poor heat transfer -> remaining water mostly frozen in glaciers at the pools.
KTevolved said:
How long will the red giant take to evaporate all the surface water? Could life survive after that?
You have a planet that at the start of your scenario is already at the hotter verge of HZ, right? And it's going to become hotter?

When the conditions are finally right to tip the point the process should be rather fast from geological perspective.

If you include extermofiles that live a few kilometers below the ground I'd give them a chance. As long as the atmosphere is quickly stripped without reaching serious sterilizing everything greenhouse phase, the system might allow some remnants of simple life in some cold oasis.

EDIT:
One factor that I think was missed:

High temperature quickens weathering of silicate materials and helps capturing carbon dioxide.

http://en.wikipedia.org/wiki/Future_of_the_Earth#Climate_impact
 
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  • #39
Yes its in the warmer part of the habitable zone. The temperature over the last hundreds of millions of years have ranged from 285-312 K. Right now its in a warm period. So its only water in the upper part of the atmosphere that gets lost and not water from the surface just reaching escape velocity? There are ups and downs in temperature. Its not in a phasew where the temperature will keep rising up rapidly.
 
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  • #40
KTevolved said:
So its only water in the upper part of the atmosphere that gets lost and not water from the surface just reaching escape velocity?
Right. But in long run this process would remove water from surface anyway, just in less direct method.

If you want to have a semi-livable planet after oceans evaporation I have an idea for you:

http://www.astro.washington.edu/courses/astro557/HZ_DRY_PLANET.pdf

Executive summary: poor heat transfer, dry hell near equator, but at pools liquid water possible
 
  • #41
Adding a few points that seem to have been overlooked:

(1) The oxygen-rich atmosphere on Earth has been created by living things. An oxygen-rich atmosphere is a high chemical energy atmosphere, far from chemical equilibrium with the planetary surface. It is something that can only arise on a planet as the result of insolation of photosynthesizing organisms. The carbon dioxide/oxygen system is a dynamic system that needs to be constantly replenished. On Earth the turnover time is 5000 years.

(2) Water vapour is not lost from the Earth's atmosphere. Water is lost in very small quantities as the result of photochemical reaction with solar radiation at high levels in the atmosphere to make hydrogen which is lost, and atomic oxygen which is not. The very low temperatures at the tropopause (~8-15 km altitude) and the mesopause (~80-95 km altitude) are particularly effective at trapping water in the lower part of the atmosphere and minimizing the escape to the outer regions where this photochemistry can occur. Meteoric inputs of water, the most common compound in the solar system, are also significant as a balancing factor for water loss, though we have no accurate way of quantifying these.

(3) An oxygen content of at least around 2% is necessary to maintain an ozone layer (also a dynamic phenomenon), and an ozone layer is the only factor that allows life to flourish on the land surface of a planet. The ozone layer is also a dynamic phenomenon, dependant on chemical processes to regenerate it as it is destroyed by the UV radiation it is shielding.

(4) The Earth's hemispheric symmetry is not nearly as marked as has been suggested in previous posts. The climates in North and South of the Earth are affected by 3 main differentiating influences:
a) 50/50 land to water in the North as against 10/90 in the South.
b) shallow sea ice at the north pole as against huge and high ice cap at south pole. This is in association with mostly land with a few high mountains in the immediate sub-Arctic, as opposed to 99% ocean in the sub-Antarctic.
c) perihelion occurs at summer solstice in the South, meaning a shorter summer season in the South than in the North.

5) On any planet with a large amount of ocean, the atmospheric content of carbon dioxide cannot be higher than about 2% because of immediate equilibrium with bicarbonate and dissolved carbon dioxide in the oceans, and ultimate equilibrium with formation and weathering of carbonate minerals in surface layers.
 
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