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Milankovitch cycles/ Chaotic obliquity variations

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Presentation on theme: "Milankovitch cycles/ Chaotic obliquity variations"— Presentation transcript:

1 Milankovitch cycles/ Chaotic obliquity variations
Chapter 14—Part 2 Milankovitch cycles/ Chaotic obliquity variations

2 in carbonate sediments
Marine 18O record in carbonate sediments Remember: High 18O  low T Low 18O  high T (because polar ice is depleted in 18O)

3 Ice Age Cycles: 100,000 years between ice ages Smaller cycles also recorded every 41,000 years*, 19, ,000 years *This cycle dominates prior to 0.9 kA

4 Asymmetric cycles: Slow cooling Rapid warming
after Bassinot et al. 1994

5 Eccentricity (orbit shape) 100,000 yrs 400,000 yrs Obliquity (tilt)
Precession (wobble) 19,000 yrs 23,000 yrs 22o

6 Q: What makes eccentricity vary
Q: What makes eccentricity vary? A: The gravitational pull of the other planets The pull of another planet is strongest when the planets are close together The net result of all the mutual inter- actions between planets is to vary the eccentricities of their orbits

7 Eccentricity Variations
Current value: 0.017 Range: Period(s): ~100,000 yrs ~400,000 yrs

8 Unfiltered Orbital Element Variations 65o N solar insolation Today
800 kA Today Unfiltered Orbital Element Variations 0.06 65o N solar insolation Imbrie et al., Milankovitch and Climate, Part 1, 1984

9 Q: What makes the obliquity and precession vary
Q: What makes the obliquity and precession vary? A: First, consider a better known example… Example: a top Gravity exerts a torque --i.e., a force that acts perpendicular to the spin axis of the top This causes the top to precess and nutate g

10 the Earth is about twice as strong as the Sun’s
Q: What makes the obliquity and precession vary? A: i) The pull of the Sun and the Moon on Earth’s equatorial bulge N g g Equator The Moon’s torque on the Earth is about twice as strong as the Sun’s S

11 Q: What makes the obliquity and precession vary
Q: What makes the obliquity and precession vary? A: ii) Also, the tilting of Earth’s orbital plane N N S Tilting of the orbital plane is like a dinner plate rolling on a table If the Earth was perfectly spherical, its spin axis would always point in the same direction but it would make a different angle with its orbital plane as the plane moved around S

12 Obliquity Variations Current value: 23.5o Range: 22o-24.5o
Period: 41,000 yrs

13 Precession Variations
Range: 0-360o Current value: Perihelion occurs on Jan. 3  North pole is pointed almost directly away from the Sun at perihelion Periods*: ~19,000 yrs ~23,000 yrs Today N S *Actual precession period is 26,000 yrs, but the orienta- tion of Earth’s orbit is varying, too (precession of perihelion)

14 Which star is the North Star today? 11,000 yrs ago Today N S

15  Polaris Which star was the North Star at
the opposite side of the cycle? Polaris 11,000 yrs ago Today N S

16  *Actually, Vega would have been the North Star more Polaris Vega
11,000 yrs ago* Today N S *Actually, Vega would have been the North Star more like 13,000 years ago

17 Unfiltered Orbital Element Variations 65o N solar insolation Today
800 kA Today Unfiltered Orbital Element Variations 0.06 65o N solar insolation Imbrie et al., Milankovitch and Climate, Part 1, 1984

18 Eccentricity Obliquity Precession Filtered Orbital Element Variations
Ref: Imbrie et al., 1984 Eccentricity Obliquity Precession Filtered Orbital Element Variations Today 800 kA

19 Interestingly, Earth’s obliquity variations would
be quite different if the Earth didn’t have a Moon The obliquity would vary chaotically from 0-85o on a time scale of tens of millions of years Chaos: Mathematically, this term is used to describe dynamical systems in which small changes in initial conditions lead to large changes in the solution after some period of time

20 Earth’s obliquity with and without the Moon Daylength (with no moon)
Chaotic region Daylength (with no moon) Laskar and Robutel (1993)

21 Back to the climate story…

22 Milutin Milankovitch, Serbian mathematician
                       Milutin Milankovitch, Serbian mathematician 1924--he suggested solar energy changes and seasonal contrasts varied with small variations in Earth’s orbit He proposed these energy and seasonal changes led to climate variations NOAA

23 Optimal Conditions for Glaciation:
Low obliquity (low seasonal contrast) High eccentricity and NH summers during aphelion (cold summers in the north) Milankovitch’s key insight: Ice and snow are not completely melted during very cold summers. (Most land is in the Northern Hemisphere.)

24 Optimal Conditions for Deglaciation:
High obliquity (high seasonal contrast) High eccentricity and NH summers during perihelion (hot summers in the north) Today 11,000 yrs ago N S N S Optimal for glaciation Optimal for deglaciation

25 NH Insolation vs. Time

26 O isotopes—the last 900,000 yrs
Peak NH summertime insolation after Bassinot et al. 1994

27 Big Mystery of the ice ages:
Why is the eccentricity cycle so prominent? The change in annual average solar insolation is small (~0.5%), but this cycle records by far the largest climate change Two possible explanations: 1) The eccentricity cycle modulates the effects of precession (no change in insolation when e = 0) 2) Some process or processes amplify the temperature change. This could take place by a positive feedback loop

28 What are some possible glacial climate feedbacks?

29 What are some possible glacial climate feedbacks? 1) Ice-Albedo
2) CO2 variations Temperature Planetary albedo Snow and Ice cover


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