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Notes
for the lecture on Thursday October 4
Supplementary notes on Daisyworld |
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The lecture
focused on the above diagram which was constructed as described in the
text. It is based on two separate relationships that govern the climate
of Daisyworld.
![]() Effect of daisy coverage on surface temperature The first of these relationships is that the larger the fraction of the surface of the planet that is covered by white daisies, the higher the albedo (albedo = fraction of sunlight which is reflected by the surface), and consequently the cooler the planet. You can see this relationship more clearly if you rotate the diagram counterclockwise 90 degrees so that the DAISY COVERAGE axis is along the bottom. (The DAISY COVERAGE scale will go backwards but that doesn't matter.) The family of diagonal lines describes the equilibrium temperature of the planet for various fractions of daisy coverage ranging from 0% on the right to 100% on the left. Each blue line corresponds to a different luminosity of Daisyworld's sun. The more luminous the sun, the warmer the temperature. If the sun is weak, the temperature of Daisyworld will be cold, even if there are no daisies present to whiten the surface. If the surface is 100% covered by daisies, the planet will reflect all the solar radiation impinging on it back to space without absorbing any of it, so its equilibrium temperature will be absolute zero, regardless of how luminous the sun is. Effect of surface temperature on
daisy coverage
These two relationships were then used
to examine the climate history of Daisyworld in response to the increasing
luminosity of this planet's sun.
Response of Daisyworld to increasing
solar luminosity
As the state approaches the top of the hump Q, the daisy coverage begins to level off and the temperature of the planet begins to increase more rapidly in response to increasing solar luminosity until it reaches point Q, which marks the optimal temperature for the daisies. Any further increase in luminosity will cause daisies to begin to die off, lowering the albedo, making the planet warmer, causing more daisies to die off, etc., etc. until the daisies are all gone (positive feedback between daisy coverage and surface temperature). This catastrophe will happen very rapidly and once the daisies are gone the temperature of the planet will be much hotter than it was when they were present (i.e., the state of the system would jump from Q directly to S in just the time it takes the daisies to wilt). Hence, the daisies are able to maintain the temperature of the planet in the range between their lower limit for survival and their optimal temperature for a remarkably long time just by 'doing their thing', but once the planet reaches their optimal temperature, their population abruptly 'crashes'. Stable equilibrium
Unstable equilibrium
So if we ran the experiment
in reverse and started with a strong sun with a luminosity so strong that
Daisyworld was too hot to support daisies, and if we gradually reduced
the luminosity what would happen? In this case the state of the system
would start near S move from right to left along the x-axis until it encountered
the base of the hump R. Then it would jump abruptly to the top of
the hump Q and
Daisyworld simulation
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Contact
the instructor at: jaegle@atmos.washington.edu
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