Skip to main content

Abrupt Climate Change Modeling

  • Reference work entry

Definition of the Subject

The occurrence of abrupt change of climate at various time scales has attracted a great deal of interest for its theoretical and practical significance [2,3,9]. To some extent, a definition of what constitutes an abrupt climatic change depends on the sampling interval of the data being examined [28]. For the instrumental period covering approximately the last 100 years of annually or seasonally sampled data, an abrupt change in a particular climate variable will be taken to mean a statistically highly significant difference between adjacent 10‐year sample means. In the paleoclimate context (i. e. on long time scales), an abrupt climate change can be in the order of decades to thousands of years. Since the climate dynamics can be often projected onto a limited number of modes or patterns of climate variability (e. g., [21,22]), the definition of abrupt climate change is also related to spatio‐temporal patterns.

The concept of abrupt change of climate is...

This is a preview of subscription content, log in via an institution.

Buying options

Chapter
USD   29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD   3,499.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Hardcover Book
USD   549.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Learn about institutional subscriptions

Abbreviations

Atmosphere:

The atmosphere is involved in many processes of abrupt climate change, providing a strong non‐linearity in the climate system and propagating the influence of any climate forcing from one part of the globe to another. Atmospheric temperature, composition, humidity, cloudiness, and wind determine the Earth's energy fluxes. Wind affects the ocean's surface circulation and upwelling patterns. Atmospheric moisture transport determines the freshwater balance for the oceans, overall water circulation, and the dynamics of glaciers.

Oceans:

Because water has enormous heat capacity, oceans typically store 10–100 times more heat than equivalent land surfaces. The oceans exert a profound influence on climate through their ability to transport heat from one location to another. Changes in ocean circulation have been implicated in abrupt climate change of the past. Deglacial meltwater has freshened the North Atlantic and reduced the ability of the water to sink, inducing long‐term coolings.

Land surface:

The reflective capacity of the land can change greatly, with snow or ice sheets reflecting up to 90% of the sunlight while dense forests absorb more than 90%. Changes in surface characteristics can also affect solar heating, cloud formation, rainfall, and surface‐water flow to the oceans, thus feeding back strongly on climate.

Cryosphere:

The portion of the Earth covered with ice and snow, the cryosphere, greatly affects temperature. When sea ice forms, it increases the planetary reflective capacity, thereby enhancing cooling. Sea ice also insulates the atmosphere from the relatively warm ocean, allowing winter air temperatures to steeply decline and reduce the supply of moisture to the atmosphere. Glaciers and snow cover on land can also provide abrupt‐change mechanisms. The water frozen in a glacier can melt if warmed sufficiently, leading to possibly rapid discharge, with consequent effects on sea level and ocean circulation. Meanwhile, snow‐covered lands of all types maintain cold conditions because of their high reflectivity and because surface temperatures cannot rise above freezing until the snow completely melts.

External factors:

Phenomena external to the climate system can also be agents of abrupt climate change. For example, the orbital parameters of the Earth vary over time, affecting the latitudinal distribution of solar energy. Furthermore, fluctuations in solar output, prompted by sunspot activity or the effects of solar wind, as well as volcanoes may cause climate fluctuations.

Climate time scales :

The climate system is a composite system consisting of five major interactive components: the atmosphere, the hydrosphere, including the oceans, the cryosphere, the lithosphere, and the biosphere. All subsystems are open and non‐isolated, as the atmosphere, hydrosphere, cryosphere and biosphere act as cascading systems linked by complex feedback processes. Climate refers to the average conditions in the Earth system that generally occur over periods of time, usually several decades or longer. This time scale is longer than the typical response time of the atmosphere. Parts of the other components of the Earth system (ice, ocean, continents) have much slower response times (decadal to millennial).

Climate variables and forcing:

State variables are temperature, rainfall, wind, ocean currents, and many other variables in the Earth system. In our notation, the variables are described by a finite set of real variables in a vector \( { x(t)\in\mathbb{R}^n } \). The climate system is subject to two main external forcings \( { F(x,t) } \) that condition its behavior, solar radiation and the action of gravity. Since \( { F(x,t) } \) has usually a spatial dependence, F is also a vector \( { \in\mathbb{R}^n } \). Solar radiation must be regarded as the primary forcing mechanism, as it provides almost all the energy that drives the climate system. The whole climate system can be regarded as continuously evolving, as solar radiation changes on diurnal, seasonal and longer time scales, with parts of the system leading or lagging in time. Therefore, the subsystems of the climate system are not always in equilibrium with each other. Indeed, the climate system is a dissipative, highly non‐linear system, with many instabilities.

Climate models:

are based on balances of energy, momentum, and mass, as well as radiation laws. There are several model categories, full circulation models, low‐order models, and models of intermediate complexity. Climate models simulate the interactions of the atmosphere, oceans, land surface, and ice. They are used for a variety of purposes from study of the dynamics of the weather and climate system, past climate to projections of future climate.

Global climate models or General circulation models :

(GCMs) The balances of energy, momentum, and mass are formulated in the framework of fluid dynamics on the rotating Earth. GCMs discretize the equations for fluid motion and energy transfer and integrate these forward in time. They also contain parametrization for processes – such as convection – that occur on scales too small to be resolved directly. The dimension of the state vector is in the order of \( { n \sim 10^5 - 10^8 } \) depending on the resolution and complexity of the model.

Model categories:

In addition to complex numerical climate models, it can be of great utility to reduce the system to low‐order, box, and conceptual models. This complementary approach has been successfully applied to a number of questions regarding feedback mechanisms and the basic dynamical behavior, e. g. [48,84]. In some cases, e. g. the stochastic climate model of Hasselmann [32], such models can provide a null hypothesis for the complex system. The transition from highly complex dynamical equations to a low‐order description of climate is an important topic of research. In his book “Dynamical Paleoclimatology”, Saltzman [77] formulated a dynamical system approach in order to differentiate between fast‐response and slow‐response variables. As an alternative to this method, one can try to derive phenomenologically based concepts of climate variability, e. g. [21,43]. In between the comprehensive models and conceptual models, a wide class of “models of intermediate complexity” were defined [12].

Earth‐system models of intermediate complexity:

(EMICs) Depending on the nature of questions asked and the pertinent time scales, different types of models are used. There are, on the one extreme, conceptual models, and, on the other extreme, comprehensive models (GCMs) operating at a high spatial and temporal resolution. Models of intermediate complexity bridge the gap [12]. These models are successful in describing the Earth system dynamics including a large number of Earth system components. This approach is especially useful when considering long time scales where the complex models are computationally too expensive, e. g. [47]. Improvements in the development of coupled models of intermediate complexity have led to a situation where modeling a glacial cycle, even with prognostic atmospheric CO2 is becoming possible.

Climate simulation :

A climate simulation is the output of a computer program that attempts to simulate the climate evolution under appropriate boundary conditions. Simulations have become a useful part of climate science to gain insight into the sensitivity of the system.

Climate variability pattern:

Climate variability is defined as changes in integral properties of the climate system. True understanding of climate dynamics and prediction of future changes will come only with an understanding of the Earth system as a whole, and over past and present climate. Such understanding requires identification of the patterns of climate variability and their relationships to known forcing. Examples for climate variability patterns are the North Atlantic Oscillation (NAO) or the El Niño‐Southern Oscillation (ENSO).

Abrupt climate change:

One can define abrupt climate change in the time and frequency domain. (a) Time domain: Abrupt climate change refers to a large shift in climate that persists for years or longer, such as marked changes in average temperature, or altered patterns of storms, floods, or droughts, over a widespread area that takes place so rapidly that the natural system has difficulty adapting to it. In the context of past abrupt climate change, “rapidly” typically means on the order of a decade. (b) Frequency domain: An abrupt change means that the characteristic periodicity changes. Also the phase relation between certain climate variables may change in a relatively short time. For both types of changes examples will be provided.

Regime shifts :

are defined as rapid transitions from one state to another. In the marine environment, regimes may last for several decades, and shifts often appear to be associated with changes in the climate system. If the shifts occur regularly, they are often referred to as an oscillation (e. g., Atlantic Multi‐decadal Oscillation, Pacific Decadal Oscillation). Similarly, one can define a regime shift in the frequency domain.

Anthropogenic climate change:

Beginning with the industrial revolution in the 1850s and accelerating ever since, the human consumption of fossil fuels has elevated CO2 levels from a concentration of \( { \sim 280 } \) ppm to more than 380 ppm today. These increases are projected to reach more than 560 ppm before the end of the 21st century. As an example, a concomitant shift of ocean circulation would have serious consequences for both agriculture and fishing.

Multiple equilibria :

Fossil evidence and computer models demonstrate that the Earth's complex and dynamic climate system has more than one mode of operation. Each mode produces different climate patterns. The evidence of models and data analysis shows that the Earth's climate system has sensitive thresholds. Pushed past a threshold, the system can jump from one stable operating mode to a completely different one.

Long‐term climate statistics :

Starting with a given initial state, the solutions \( { x(t) } \) of the equations that govern the dynamics of a non‐linear system, such as the atmosphere, result in a set of long‐term statistics. If all initial states ultimately lead to the same set of statistical properties, the system is ergodic or transitive. If, instead, there are two or more different sets of statistical properties, where some initial states lead to one set, while the other initial states lead to another, the system is called intransitive (one may call the different states regimes). If there are different sets of statistics that a system may assume in its evolution from different initial states through a long, but finite, period of time, the system is called almost intransitive [50,51,53]. In the transitive case, the equilibrium climate statistics are both stable and unique. Long‐term climate statistics will give a good description of the climate. In the almost intransitive case, the system in the course of its evolution will show finite periods during which distinctly different climatic regimes prevail. The almost intransitive case arises because of internal feedbacks, or instabilities involving the different components of the climatic system. The climatic record can show rapid step‐like shifts in climate variability that occur over decades or less, including climatic extremes (e. g. drought) that persist for decades.

Feedbacks:

A perturbation in a system with a negative feedback mechanism will be reduced whereas in a system with positive feedback mechanisms, the perturbation will grow. Quite often, the system dynamics can be reduced to a low‐order description. Then, the growth or decay of perturbations can be classified by the systems' eigenvalues or the pseudospectrum. Consider the stochastic dynamical system

$$ \frac{\text{d}} {\text{d} t} x(t) = f(x) + g(x) \xi + F(x,t) \:, $$
(1)

where ξ is a stochastic process. The functions \( { f, g } \) describe the climate dynamics, in this case without explicit time dependence. The external forcing \( { F(x,t) } \) is generally time‐, variable‐, and space‐dependent. In his theoretical approach, Hasselmann [32] formulated a linear stochastic climate model

$$ \frac{\text{d}} {\text{d} t} x(t) = A x+ \sigma \xi + F(t) \:, $$
(2)

with system matrix \( { A\in\mathbb{R}^{n\times n} } \), constant noise term σ, and stochastic process ξ. Interestingly, many features of the climate system can be well described by (2), which is analogous to the Ornstein–Uhlenbeck process in statistical physics [89]. In the climate system, linear and non‐linear feedbacks are essential for abrupt climate changes.

Paleoclimate :

Abrupt climate change is evident in model results and in instrumental records of the climate system. Much interest in the subject is motivated by the evidence in archives of extreme changes. Proxy records of paleoclimate are central to the subject of abrupt climate change. Available paleoclimate records provide information on many environmental variables, such as temperature, moisture, wind, currents, and isotopic compositions.

Thermohaline circulation :

stems from the Greek words “thermos” (heat) and “halos” (salt). The ocean is driven to a large extent by surface heat and freshwater fluxes. As the ocean is non‐linear, it cannot be strictly separated from the wind‐driven circulation. The expressions thermohaline circulation (THC) and meridional overturning circulation (MOC) in the ocean are quite often used as synonyms although the latter includes all effects (wind, thermal, haline forcing) and describes the ocean transport in meridional direction. Another related expression is the ocean conveyor belt. This metaphor is motivated by the fact that the North Atlantic is the source of the deep limb of a global ocean circulation system [10]. If North Atlantic surface waters did not sink, the global ocean circulation would cease, currents would weaken or be redirected. The resulting reorganization would reconfigure climate patterns, especially in the Atlantic Ocean. One fundamental aspect of this circulation is the balance of two processes: cooling of the deep ocean at high latitudes, and heating of deeper levels from the surface through vertical mixing.

Bibliography

PrimaryLiterature

  1. Alley RB, Anandakrishnan S, Jung P (2001) Stochastic resonance in the North Atlantic. Paleoceanogr 16:190–198

    ADS  Google Scholar 

  2. Alley RB, Marotzke J, Nordhaus W, Overpeck J, Peteet D, Pielke R Jr, Pierrehumbert R, Rhines P, Stocker T, Talley L, Wallace JM (2002) Abrupt Climate Change: Inevitable Surprises. US National Academy of Sciences, National Research Council Committee on Abrupt Climate Change, National Academy Press, Washington

    Google Scholar 

  3. Alverson K, Oldfield F (2000) Abrupt Climate Change. In: Joint Newsletter of the Past Global Changes Project (PAGES) and the Climate Variability and Predictability Project (CLIVAR), vol 8, no 1. Bern, pp 7–10

    Google Scholar 

  4. Barber DC, Dyke A, Hillaire‐Marcel C, Jennings AE, Andrews JT, Kerwin MW, Bilodeau G, McNeely R, Southon J, Morehead MD, Gagnonk JM (1999) Forcing of the cold event of 8,200 years ago by catastrophic drainage of Laurentide lakes. Nature 400:344–348

    Google Scholar 

  5. Bartoli G, Sarnthein M, Weinelt M, Erlenkeuser H, Garbe-Schönberg D, Lea DW (2005) Final closure of Panama and the onset of northern hemisphere glaciation. Earth Planet Sci Lett 237:33–44

    Google Scholar 

  6. Bender M, Malaize B, Orchardo J, Sowers T, Jouzel J (1999) Mechanisms of Global Climate Change. Clark P et al (eds) AGU 112:149–164

    Google Scholar 

  7. Benzi R, Parisi G, Sutera A, Vulpiani A (1982) Stochastic resonance in climatic change. Tellus 34:10

    ADS  Google Scholar 

  8. Berger A, Loutre MF (1991) Insolation values for the climate of the last 10 million years. Quat Sci Rev 10:297–317

    ADS  Google Scholar 

  9. Berger WH, Labeyrie LD (1987) Abrupt Climatic Change, Evidence and Implications. NATO ASI Series, Series C, Mathematical and Physical Sciences, vol 216. D Reidel, Dordrecht, pp 425

    Google Scholar 

  10. Broecker WS et al (1985) Does the Ocean‐atmosphere System Have More than One Stable Mode of Operation? Nature 315:21–26

    ADS  Google Scholar 

  11. Bryan F (1986) High Latitude Salinity Effects and Inter‐hemispheric Thermohaline Circulations. Nature 323:301–304

    ADS  Google Scholar 

  12. Claussen M, Mysak LA, Weaver AJ, Crucifix M, Fichefet T, Loutre M-F, Weber SL, Alcamo J, Alexeev VA, Berger A, Calov R, Ganopolski A, Goosse H, Lohmann G, Lunkeit F, Mokhov II, Petoukhov V, Stone P, Wang Z (2002) Earth System Models of Intermediate Complexity: Closing the Gap in the Spectrum of Climate System Models. Clim Dyn 18:579–586

    Google Scholar 

  13. CLIMAP project members (1976) The surface of the ice age Earth. Science 191:1131–1137

    ADS  Google Scholar 

  14. Coxall HK, Wilson PA, Pälike H, Lear CH, Backman J (2005) Rapid stepwise onset of Antarctic glaciation and deeper calcite compensation in the Pacific Ocean. Nature 433:53–57. doi:10.1038/nature03135

  15. Crowley TJ (1992) North Atlantic deep water cools the southern hemisphere. Paleoceanogr 7:489–497

    ADS  Google Scholar 

  16. Daubechies I (1992) Ten Lectures on Wavelets. Society for Industrial and Applied Mathematics (SIAM). CBMS-NSF Regional Conference Series in Applied Mathematics, vol 61, Philadelphia

    Google Scholar 

  17. DeConto RM, Pollard D (2003) Rapid Cenozoic glaciation of Antarctica induced by declining atmospheric CO2. Nature 421:245–249. doi:10.1038/nature01290

    ADS  Google Scholar 

  18. DeMenocal et al (2000) Abrupt onset and termination of the African Humid Period: Rapid climate response to gradual insolation forcing. Quat Sci Rev 19:347–361

    ADS  Google Scholar 

  19. Diaz HF, Quayle RG (1980) The climate of the United States since 1895: spatial and temporal changes. Mon Wea Rev 108:149–226

    Google Scholar 

  20. Dijkstra HA, Te Raa L, Weijer W (2004) A systematic approach to determine thresholds of the ocean's thermohaline circulation. Tellus 56A(4):362

    ADS  Google Scholar 

  21. Dima M, Lohmann G (2002) Fundamental and derived modes of climate variability. Application to biennial and interannual timescale. Tellus 56A:229–249

    ADS  Google Scholar 

  22. Dima M, Lohmann G (2007) A hemispheric mechanism for the Atlantic Multidecadal Oscillation. J Clim 20:2706–2719

    ADS  Google Scholar 

  23. EPICA Community Members (2006) One‐to‐one coupling of glacial climate variability in Greenland and Antarctica. Nature 444:195–198. doi:10.1038/nature05301

    ADS  Google Scholar 

  24. Fairbanks RG (1989) A 17,000‐year glacio‐eustatic sea level record: influence of glacial melting rates on the Younger Dryas event and deep‐ocean circulation. Nature 342:637–642

    ADS  Google Scholar 

  25. Flohn H (1986) Singular events and catastrophes now and in climatic history. Naturwissenschaften 73:136–149

    ADS  Google Scholar 

  26. Fraedrich K, Kirk E, Lunkeit F (1998) Portable University Model of the Atmosphere. DKRZ Report 16, Hamburg

    Google Scholar 

  27. Frisius T, Lunkeit F, Fraedrich K, James IN (1998) Storm‐track organization and variability in a simplified atmospheric global circulation model. Q J R Meteorol Soc 124:1019–1043

    ADS  Google Scholar 

  28. Fu C, Diaz HF, Dong D, Fletcher JO (1999) Changes in atmospheric circulation over northern hemisphere oceans associated with the rapid warming of the 1920s. Int J Climatol 19(6):581–606

    Google Scholar 

  29. Ganopolski A, Rahmstorf S (2001) Rapid changes of glacial climate simulated in a coupled climate model. Nature 409:153–158

    Google Scholar 

  30. Ganopolski A, Rahmstorf S (2002) Abrupt glacial climate changes due to stochastic resonance. Phys Rev Let 88(3):038501

    ADS  Google Scholar 

  31. Ganopolski A, Kubatzki C, Claussen M, Brovkin V, Petoukhov V (1998) The influence of vegetation‐atmosphere‐ocean interaction on climate during the mid‐Holocene. Science 280:1916

    ADS  Google Scholar 

  32. Hasselmann K (1976) Stochastic climate models, Part 1, Theory. Tellus 28:289–485

    Google Scholar 

  33. Hays JD, Imbrie J, Shackleton NJ (1976) Variations in the Earth's Orbit: Pacemaker of the Ice Ages. Science 194:1121–1132

    ADS  Google Scholar 

  34. Henderson GM, Slowey NC (2000) Evidence from U‐Th dating against Northern Hemisphere forcing of the penultimate deglaciation. Nature 404:61–66

    ADS  Google Scholar 

  35. Hoskins BJ, Simmons AJ (1975) A multi‐layer spectral model and the semi‐implicit method. Q J R Meteorol Soc 101:1231–1250

    Google Scholar 

  36. Huybers P, Wunsch C (2005) Obliquity pacing of the late Pleistocene glacial terminations. Nature 434:491–494. doi:10.1038/nature03401

    ADS  Google Scholar 

  37. Imbrie J, Imbrie JZ (1980) Modeling the climatic response to orbital variations. Science 207:943–953

    ADS  Google Scholar 

  38. IPCC (2007) Summary for Policymakers. In: Climate change 2007: The Physical Science Basis. Contribution of Working Group I to the Fourth Assessment Report of the Intergrovernmental Panel on Climate Change. Cambridge University Press, Cambridge and New York

    Google Scholar 

  39. Iwashima T, Yamamoto R (1986) Time‐space spectral model of low order barotropic system with periodic forcing. J Meterol Soc Jpn 64:183–196

    Google Scholar 

  40. Kennett JP, Houtz RE, Andrews PB, Edwards AE, Gostin VA, Hajos M, Hampton M, Jenkins DG, Margolis SV, Ovenshine AT, Perch-Nielsen K (1974) Development of the circum‐Antarctic current. Science 186:144–147

    ADS  Google Scholar 

  41. Knorr G, Lohmann G (2003) Southern Ocean Origin for the resumption of Atlantic thermohaline circulation during deglaciation. Nature 424:532–536

    ADS  Google Scholar 

  42. Knorr G, Lohmann G (2007) Rapid transitions in the Atlantic thermohaline circulation triggered by global warming and meltwater during the last deglaciation. Geochem Geophys Geosyst 8(12), Q12006:1–22. doi:10.1029/2007GC001604

  43. Kwasniok F, Lohmann G (2008) Underlying Dynamics of Glacial Millennial‐Scale Climate Transitions Derived from Ice‐Core Data. Phys Rev E (accepted)

    Google Scholar 

  44. Lawver LA, Gahagan LM (2003) Evolution of Cenozoic seaways in the circum‐Antarctic region. Palaeogeography, Palaeoclimatology, Palaeoecology 198:11–37. doi:10.1016/S0031-0182(03)00392-4

  45. Lisiecki LE, Raymo ME (2005) A Pliocene‐Pleistocene stack of 57 globally distributed benthic O-18 records. Paleoceanography 20:PA1003. doi:10.1029/2004PA001071

  46. Lohmann G (2003) Atmospheric and oceanic freshwater transport during weak Atlantic overturning circulation. Tellus 55A:438–449

    ADS  Google Scholar 

  47. Lohmann G, Gerdes R (1998) Sea ice effects on the Sensitivity of the Thermohaline Circulation in simplified atmosphere‐ocean‐sea ice models. J Climate 11:2789–2803

    ADS  Google Scholar 

  48. Lohmann G, Schneider J (1999) Dynamics and predictability of Stommel's box model: A phase space perspective with implications for decadal climate variability. Tellus 51A:326–336

    ADS  Google Scholar 

  49. Lohmann G, Schulz M (2000) Reconciling Boelling warmth with peak deglacial meltwater discharge. Paleoceanography 15:537–540

    ADS  Google Scholar 

  50. Lorenz EN (1963) Deterministic nonperiodic flow. J Atmos Sci 20:130–141

    ADS  Google Scholar 

  51. Lorenz EN (1976) Nondeterministic theories of climatic change. Quat Res 6:495–506

    Google Scholar 

  52. Lorenz EN (1982) Atmospheric predictability experiments with a large numerical model. Tellus 34:505–513

    ADS  Google Scholar 

  53. Lorenz EN (1990) Can chaos and intransitivity lead to interannual variability? Tellus 42A:378–389

    ADS  Google Scholar 

  54. Lorenz S, Lohmann G (2004) Acceleration technique for Milankovitch type forcing in a coupled atmosphere‐ocean circulation model: method and application for the Holocene. Climate Dyn 23(7–8):727–743. doi:10.1007/s00382-004-0469-y

    ADS  Google Scholar 

  55. Lund R, Reeves J (2002) Detection of undocumented changepoints: A revision of the two-phase regression model. J Climate 15:2547–2554

    ADS  Google Scholar 

  56. Lunkeit F, Bauer SE, Fraedrich K (1998) Storm tracks in a warmer climate: Sensitivity studies with a simplified global circulation model. Clim Dyn 14:813–826

    Google Scholar 

  57. Manabe S, Stouffer RJ (1993) Century‐scale effects of increased atmospheric CO2 on the ocean‐atmosphere system. Nature 364:215–218

    ADS  Google Scholar 

  58. Maraun D, Kurths J (2004) Cross wavelet analysis. Significance testing and pitfalls. Nonlin Proc Geoph 11:505–514

    ADS  Google Scholar 

  59. Maraun D, Kurths J (2005) Epochs of phase coherence between El Niño/Southern Oscillation and Indian monsoon. Geophys Res Lett 32:L15709. doi:10.1029/2005GL023225

    ADS  Google Scholar 

  60. Maslin MA, Li XS, Loutre MF, Berger A (1998) The contribution of orbital forcing to the progressive intensification of Northern Hemisphere Glaciation. Quat Sci Rev 17:411–426

    ADS  Google Scholar 

  61. Maslin MA, Ridgewell A (2005) Mid‐Pleistocene Revolution and the eccentricity myth. Special Publication of the Geological Society of London 247:19–34

    Google Scholar 

  62. Milankovitch M (1941) Kanon der Erdbestrahlung. Royal Serb Acad Spec Publ, Belgrad, 132, Sect. Math Nat Sci 33:484

    MathSciNet  Google Scholar 

  63. Mori H (1965) A Continued‐Fraction Representation of the Time‐Correlation Functions Prog Theor Phys 33:423–455. doi:10.1143/PTP.34.399

  64. North Greenland Ice Core Project members (2004) High‐resolution record of Northern Hemisphere climate extending into the last interglacial period. Nature 431:147–151

    Google Scholar 

  65. Paillard D (1998) The timing of Pleistocene glaciations from a simple multiple‐state climate model. Nature 391:378–381

    ADS  Google Scholar 

  66. Palmer TN (1996) Predictability of the atmosphere and oceans: From days to decades. In: Anderson DTA, Willebrand J (eds) Large‐scale transport processes in oceans and atmosphere. NATO ASI Series 44. Springer, Berlin, pp 83–155

    Google Scholar 

  67. Parker DE, Jones PD, Folland CK, Bevan A (1994) Interdecadal changes of surface temperature since the late nineteenth century. J Geophys Res 99:14,373-14,399

    ADS  Google Scholar 

  68. Peixoto JP, Oort AH (1992) Physics of Climate. American Institute of Physics, New York, p 520

    Google Scholar 

  69. Petit JR, Jouzel J, Raynaud D, Barkov NI, Barnola JM, Basile I, Bender M, Chappellaz J, Davis M, Delaygue G, Delmotte M, Kotlyakov VM, Legrand M, Lipenkov VY, Lorius C, Pepin L, Ritz C, Saltzman E, Stievenard M (1999) Climate and atmospheric history of the past 420,000 years from the Vostok ice core, Antarctica. Nature 399:429–436

    ADS  Google Scholar 

  70. Raymo M, Ganley K, Carter S, Oppo DW, McManus J (1998) Millennial‐scale climate instability during the early Pleistocene epoch. Nature 392:699–701

    ADS  Google Scholar 

  71. Reddy SC, Schmidt P, Henningson D (1993) Pseudospectra of the Orr‐Sommerfeld operator. SIAM J Appl Math 53:15–47

    MathSciNet  MATH  Google Scholar 

  72. Rial JA (1999) Pacemaking the Ice Ages by Frequency Modulation of Earth's Orbital Eccentricity. Science 285:564–568

    Google Scholar 

  73. Rial JA (2004) Abrupt Climate Change: Chaos and Order at Orbital and Millennial Scales. Glob Plan Change 41:95–109

    ADS  Google Scholar 

  74. Ridgwell AJ, Watson AJ, Raymo ME (1999) Is the spectral signature of the 100 Kyr glacial cycle consistent with a Milankovitch origin? Paleoceanography 14:437–440

    ADS  Google Scholar 

  75. Rogers JC (1985) Atmospheric circulation changes associated with the warming over the northern North Atlantic in the 1920s. J Climate Appl Meteorol 24:1303–1310

    ADS  Google Scholar 

  76. Romanova V, Lohmann G, Grosfeld K, Butzin M (2006) The relative role of oceanic heat transport and orography on glacial climate. Quat Sci Rev 25:832–845. doi:10.1016/j.quascirev.2005.07.007

    ADS  Google Scholar 

  77. Saltzman (2002) Dynamical Paleoclimatology. Generalized Theory of Global Climate Change. In: International Geophysics Series, vol 80. Harcourt‐Academic Press (Elsevier Science), San Diego, p 354

    Google Scholar 

  78. Schulz M, Paul A, Timmermann A (2004) Glacial‐Interglacial Contrast in Climate Variability at Centennial-to‐Millennial Timescales: Observations and Conceptual Model. Quat Sci Rev 23:2219

    ADS  Google Scholar 

  79. Seidel DJ, Lanzante JR (2004) An assessment of three alternatives to linear trends for characterizing global atmospheric temperature changes. J Geophy Res 109:D14108. doi:10.1029/2003JD004414

    ADS  Google Scholar 

  80. Stocker TF (1998) The seesaw effect. Science 282:61–62

    Google Scholar 

  81. Stocker TF, Johnsen SJ (2003) A minimum thermodynamic model for the bipolar seesaw. Paleoceanography 18(4):1087

    ADS  Google Scholar 

  82. Stommel H (1961) Thermohaline Convection with Two Stable Regimes of Flow. Tellus 13:224–230

    ADS  Google Scholar 

  83. Tiedemann R, Sarnthein M, Shackleton NJ (1994) Astronomic time scale for the Pliocene Atlantic \( { \delta^{18} } \)O and dust flux records of Ocean Drilling Program site 659. Paleoceanography 9:19–638

    Google Scholar 

  84. Timmermann A, Lohmann G (2000) Noise-Induced Transitions in a simplified model of the thermohaline circulation. J Phys Oceanogr 30(8):1891–1900

    ADS  Google Scholar 

  85. Timmermann A, Oberhuber J, Bracher A, Esch M, Latif M, Roeckner E (1999) Increased El Niño frequency in a climate model forced by future greenhouse warming. Nature 398:694–696

    Google Scholar 

  86. Torrence C, Compo G (1998) A practical guide to wavelet analysis. Bull Amer Meteor Soc 79:61–78

    Google Scholar 

  87. Trefethen LN, Trefethen AE, Reddy SC, Driscoll TA (1993) Hydrodynamic stability without eigenvalues. Science 261:578–584

    MathSciNet  ADS  MATH  Google Scholar 

  88. Trenberth KE (1990) Recent observed interdecadal climate changes in the Northern Hemisphere. Bull Am Meteorol Soc 71:988–993

    Google Scholar 

  89. Uhlenbeck GE, Ornstein LS (1930) On the theory of Brownian Motion. Phys Rev 36:823–841

    ADS  MATH  Google Scholar 

  90. Wunsch C (1999) The interpretation of short climate records, with comments on the North Atlantic and Southern Oscillation. Bull Amer Meteor Soc 80:245–255

    Google Scholar 

  91. Wunsch C (2004) Quantitative estimate of the Milankovitch‐forced contribution to observed Quaternary climate change. Quat Sci Rev 23(9–10):1001–1012

    ADS  Google Scholar 

  92. Yamamoto R, Iwashima T, Sanga NK (1985) Climatic jump: a hypothesis in climate diagnosis. J Meteorol Soc Jpn 63:1157–1160

    Google Scholar 

  93. Zachos J, Pagani M, Sloan L, Thomas E, Billups K (2001) Trends, Rhythms, and Aberrations in Global Climate 65 Ma to Present. Science 292(5517):686–693

    ADS  Google Scholar 

  94. Zwanzig R (1980) Thermodynamic modeling of systems far from equilibrium. In: Garrido L (ed) Lecture Notes in Physics 132, in Systems Far From Equilibrium. Springer, Berlin

    Google Scholar 

Books and Reviews

  1. Dijkstra HA (2005) Nonlinear Physical Oceanography, 2nd revised and extended edition. Springer, New York, pp 537

    Google Scholar 

  2. Hansen J, Sato M, Kharecha P (2007) Climate change and trace gases. Phil Trans R Soc A 365:1925–1954. doi:10.1098/rsta.2007.2052

    ADS  Google Scholar 

  3. Lockwood JG (2001) Abrupt and sudden climate transitions and fluctuations: a review. Int J Climat 21:1153–1179

    Google Scholar 

  4. Rial JA, Pielke RA Sr, Beniston M, Claussen M, Canadell J, Cox P, Held H, N deNoblet‐Ducudre, Prinn R, Reynolds J, Salas JD (2004) Nonlinearities, Feedbacks and Critical Thresholds Within the Earth's Climate System. Clim Chang 65:11–38

    Google Scholar 

  5. Ruddiman WF (2001) Earth's Climate. Past and Future. WH Freeman, New York, p 465

    Google Scholar 

  6. Stocker TF (1999) Abrupt climate changes from the past to the future-a review. Int J Earth Sci 88:365–374

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Editor information

Editors and Affiliations

Rights and permissions

Reprints and permissions

Copyright information

© 2009 Springer-Verlag

About this entry

Cite this entry

Lohmann, G. (2009). Abrupt Climate Change Modeling. In: Meyers, R. (eds) Encyclopedia of Complexity and Systems Science. Springer, New York, NY. https://doi.org/10.1007/978-0-387-30440-3_1

Download citation

Publish with us

Policies and ethics