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Planetary Engineering 1
Climate Modeling Class Exercise
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Zero-Dimensional GEBM
Global energy balance: Radiative equilibrium (in = out) Recall the energy balance in 0-dimensions and what it means for temperature.
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Goal: Planets’ Temperatures
Important Fact: Sun heats less the farther it is. What factor(s) affect change in S with distance from sun? Important Factor: How does S change with orbit?
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Change in solar flux: sun earth
Recall from Topic 1: Change in solar flux: sun earth At photosphere surface, solar flux ~ W-m-2 Note strong decrease from photosphere to Earth’s orbit. At Earth’s orbit, solar flux ~ 1360 W-m-2
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Two Spheres Surrounding Sun
Total energy flux the same through each sphere R2 = 2 x R1 R2 R1 Consider 2 spheres surrounding the sun. Both intercept all the energy emitted by the sun. The larger sphere covers 4 x the surface area of the innner sphere. Thus the same amount of energy is spread over 4 times greater area. The same area at R2 intercepts only 1/4 of energy it intercepts at R1 Flux decreases as R-2
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Global energy balance: Radiative equilibrium (in = out)
For Earth Global energy balance: Radiative equilibrium (in = out) Recall what we derived for Earth, based on observed S and albedo. Thus, TRAD = 255 K
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What about other planets?
How does Trad change with orbit?
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What about other planets?
How does Trad change with orbit? Planet Distance Albedo Outgoing IR Trad from sun [A.U.] [W-m2] [K] Mercury Venus Earth Mars Jupiter Saturn Uranus Neptune This table can be easily filled in.
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Tsurface ≈ Trad. How warm can we make its surface?
For Mars Tsurface ≈ Trad. How warm can we make its surface? Suppose we can alter the surface of Mars. How can we engineer a warmer surface?
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Tsurface ≈ Trad. How cool can we make its surface?
For Mercury Tsurface ≈ Trad. How cool can we make its surface? Similarly for Mercury.
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Why can’t we adjust Venus the same way?
What is different about Venus? (Hint: Why does Tsurface ≠ Trad for Earth?)
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End Planetary Engineering 1
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