On the (Nonlinear) Causes of Abrupt Climate Change During the Last Ice Age J.A. Rial Wave Propagation Lab, University of North Carolina-Chapel Hill The Astronomical Theory of the Ice Ages • • • Precession Tilt Eccentricity The Milankovitch Periodicities Eccentricity Tilt or Obliquity 41,000years Eccentricity 100,000years Precession of the Equinoxes 21,000years Evidence of Climate's Nonlinear Response to Astronomical Forcing • • • Frequency shifts Frequency (or phase) modulation Fast warming, slow cooling and 'self -similarity' 'self-similarity' Frequency shift at the Mid-Pleistocene Transition Frequency Modulation Tilt Eccentricity Rial,J.A., Science, Science, 285 (1999) Saw-tooth self-similarity: Fast Warming-Slow Cooling DansgaardOeschger oscillations Rial et al., Climatic Change, 2004 A “toy” model to visualize the sawtooth asymmetry and FM Wave Propagation Lab, UNC-Chapel Hill (No external forcing required) Sawtooth waveform Frequency Modulation Ice Volume and Temperature Fitting the long-period records Modeling the Greenland (GRIP) Short-Period Time Series Greenland ice core w w w w w w today 100,000 yrs ago W: Abrupt warming (10oC or more) FREQUENCY DEMODULATION OF GRIP REVEALS A 2.75ky 'CARRIER' Modulating Phase or "Intelligence" Best Fitting Periods 72.1ky and 41ky Modulating Phase (LP filtered) 1/75 ~ 1/41-1/95 1/72.1 = 1/41 - 1/95 (combination tone) 1/35 ~ 1/19-1/41 Heinrich events-> 1 The thermal oscillator has the form of a Van der Pol nonlinear equation Wave Propagation Lab, UNC-Chapel Hill The Van der Pol Equation (Self-exciting oscillations with a limit cycle) d2x/dt2 + v(x2-1)dx/dt + ωo2 x = 0 Is equivalent to dx/dt = y - v (x3/3 -x) dy/dt = - ωo2x Wave Propagation Lab, UNC-Chapel Hill In a simplified climate model An energy balance equation CT dT/dt = -αL -βT + Q(1+ε coswt) Coupled to a logistic growth equation for the sea ice CLdL/dt = T/α - (a L3/3 -bL) Become a Van der Pol equation for the sea ice extent d2L/dt2 + v(L2-1) dL/dt + ωo2 L = G(1+ε coswt) …and with G=0, it gives Saltzman's nonlinear thermal oscillator CT, CL, Q, α, β, a, b are positive constants Saltzman's NONLINEAR THERMAL OSCILLATOR ICE AGE ATMOSPHERE L(t) 0 T(t) SEA ICE OCEAN θ(t) Saltzman's NONLINEAR THERMAL OSCILLATOR ICE AGE ATMOSPHERE L(t) 0 T(t) SEA ICE OCEAN θ(t) Saltzman's NONLINEAR THERMAL OSCILLATOR ICE AGE ATMOSPHERE L(t) 0 T(t) SEA ICE OCEAN θ(t) Saltzman's NONLINEAR THERMAL OSCILLATOR ICE AGE ATMOSPHERE L(t) 0 T(t) SEA ICE OCEAN θ(t) Saltzman's NONLINEAR THERMAL OSCILLATOR ICE AGE ATMOSPHERE L(t) 0 T(t) SEA ICE OCEAN θ(t) The self-sustained, relaxation oscillation of the thermal oscillator Forcing Saltzman's Oscillator with Milankovitch Cycles Linear, forced by cosine QuickTime™ and a Animation decompressor are needed to see this picture. Nonlinear, forced by cosine QuickTime™ and a Animation decompressor are needed to see this picture. Time (arbitrary units) Nonlinear, forced by simulated Insolation QuickTime™ and a Animation decompressor are needed to see this picture. Time (arbitrary units) GRIP vs VdPol Model VdPol Model is Robust GRIP vs VdPol Model GRIP Kyears B.P. Prediction GRIP vs VdPol Model Kyears B.P. Concluding Remarks • A simplified climate model describing the nonlinear oscillations of sea ice driven by deep ocean temperature closely reproduces the GRIP data. A natural free period of 2.75ky retrieved form the data by demodulation appears to be the free period of the sea ice/atmosphere/ocean system. • Frequency modulation of this free oscillation by the insolation (tilt and precession) generates time-series features consistent with many of the puzzling features of the GRIP time series. • The model is deterministic, and it can be chaotic. • Though the origin of the 2.75ky period is not resolved, it is commensurate with predictions made by Saltzman's sea ice oscillator. We shall use GCMs to understand the origin and physics of this period. Research supported by NSF grant ATM-0241274 Wave Propagation Laboratory, University of North Carolina-Chapel Hill Ice core data from Greenland (millennial scale) Dansgaard-Oeschger Oscillations. -16 FM in the D/O Relative Temp (oC) FM in the D/O -6 -12 -16 Carrier: 2.7ky Modulator: 7.5ky The Paleoclimate Time Series A Complex tale of • • • • Fast warming-Slow cooling Frequency Modulation Non-Stationarity Chaos and Order Sawtooth Mid-Pleistocene Transition FM The abrupt warming episodes of the last Ice Age …and the Dow Jones crash of 1987 What does self-similarity mean? The abrupt warming episodes of the last Ice Age …and the Dow Jones crash of 1987 What does self-similarity mean? Fast Warming - Slow Cooling and The Younger Dryas (YD) event Milankovitch Forcing and Ice Core Data ~ 21ky 0 -10 Tilt 41ky -20 QuickTime™ and a Animation decompressor are needed to see this picture. QuickTime™ and a Animation decompressor are needed to see this picture. QuickTime™ and a Animation decompressor are needed to see this picture. Time (arbitrary units) Global temperature over the last Millennium ∆T (oC) 1 0 … and during the last Ice Age Normal abrupt climate change, or CO2 warming? Time series from the Antarctic Ice cap Today 400,000 years ago The self-sustained, relaxation oscillation of the thermal oscillator 1 2 4 3 4 1 3 2 Frequency modulation (FM) in millennial-scale climate series 7.5ky 1/74 ~ 1/41-1/95 1/37 ~ 1/19-1/41 Deep-sea sediment Ice core Sea-surface Temp