Modelling Pliocene warmth: contribution of atmosphere, oceans and cryosphere

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Abstract

The relative role of the atmosphere, oceans and cryosphere in contributing towards middle Pliocene warmth (ca 3 Ma BP) is investigated using the HadCM3 coupled ocean–atmosphere general circulation model. The model was initialised with boundary conditions from the USGS PRISM2 data set and a Pliocene atmospheric CO2 level of 400 ppmv and run for 300 simulated years. The simulation resulted in a global surface temperature warming of 3°C compared to present-day. In contrast to earlier modelling experiments for the Pliocene, surface temperatures warmed in most areas including the tropics (1–5°C). Compared with present-day, the model predicts a general pattern of ocean warming (1–5°C) in both hemispheres to a depth of 2000 m, below which no significant differences are noted. Sea ice coverage is massively reduced (up to 90%). The flow of the Gulf Stream/North Atlantic Drift is up to 100 mm s−1 greater in the Pliocene case. Analysis of the model-predicted meridional streamfunction suggests a global pattern of reduced outflow of Antarctic bottom water (AABW; up to 5 Sv), a shallower depth for North Atlantic deep water formation and weaker thermohaline circulation (3 Sv). The decrease in AABW occurs mainly in the Pacific rather than Atlantic Ocean. Model diagnostics for heat transports indicate that neither the oceans nor the atmosphere are transporting significantly more heat in the Pliocene scenario. Rather, these results indicate that the major contributing mechanism to global Pliocene warmth was the reduced extent of high-latitude terrestrial ice sheets (50% reduction on Greenland, 33% reduction on Antarctica) and sea ice cover resulting in a strong ice-albedo feedback. These results highlight the need for further studies designed to improve our knowledge regarding Pliocene terrestrial ice configurations.

Introduction

The middle Pliocene (ca 3 Ma BP) represents a recent period in geological history when the climate of the Earth was significantly warmer than present-day. The period has been studied extensively by palaeoenvironmental/climatologists. Geological data supporting the assertion of a warmer than present climate includes sea surface temperatures (SSTs) reconstructed from planktonic foraminifera [1], [2], [3], [4], [5], ostracods [6], [7], siliceous microfossil records [8], diatom records [9], terrestrial vegetation records [10], [11], [12] and numerous records of higher than present sea levels [13], [14], [15].

Numerous modelling studies have been conducted for the period. The first study used the PRISM0 8°×10° digital data set and the GISS (Goddard Institute for Space Studies) atmospheric general circulation model (GCM; 8°×10° model resolution) which focussed on the middle Pliocene climate of the Northern Hemisphere [16]. The second model investigation used a 2°×2° version of the (PRISM1) digital data set to prescribe the boundary conditions for the NCAR (National Centre for Atmospheric Research) GENESIS atmospheric GCM (4.5°×7.5° model resolution) which examined the nature of the middle Pliocene climate on a global scale [17]. A global scale palaeoclimate reconstruction for the middle Pliocene was conducted using the updated PRISM2 digital data set and the UKMO (United Kingdom Meteorological Office) atmospheric GCM, running with an enhanced spatial resolution of 2.5°×3.75° [18]. The same model has been used to carry out detailed data/model comparisons on a regional scale [19], [20] and to conduct ice sheet sensitivity/biome experiments for the period [21], [22], [23].

Despite these modelling studies, the cause of middle Pliocene warmth continuous to be the subject of much debate [16], [17], [24], [25], [26], [27]. A combination of modelling studies and evidence from Pliocene proxy data indicate that CO2 concentrations at 3 Ma BP were greater (absolute value 400 ppmv) compared to mid-19th century levels (∼280 ppmv) [28], [29], [25], [30], [31]. However, an increase in CO2 alone would be expected to raise surface temperatures at all latitudes, and, hence, cannot explain the reconstructed pattern of little or no SST change at the equator [2], [3], [4].

Variations in oceanic circulation and increased heat advection away from the equator to high latitudes have been proposed as a significant causal factor in producing the climate of the middle Pliocene [25], [26], [3]. Such an increase in heat advection could be a response to enhanced thermohaline circulation in the oceans or enhanced surface gyre flow resulting from increased regional atmospheric winds and wind stresses [19]. Thus far, all palaeoclimate modelling studies of the middle Pliocene have been restricted to using atmospheric GCMs utilising prescribed SSTs and/or a simple slab-ocean model [32], [22]. Although slab-ocean models are capable of simulating part of the feedbacks of the oceans on climate, they are incapable of simulating changes to horizontal ocean heat transports, and related changes to ocean currents and thermohaline circulation. These have been recognised as potentially pivotal mechanisms in forcing climate change for the Pliocene and many other time periods [33], [34], [35].

Thus it has not been possible to robustly examine the oceans role in generating and or maintaining mid-Pliocene warmth. This study aims to remedy this situation through the use of a fully coupled atmosphere–ocean model.

Section snippets

The UKMO GCM

The particulars of the version of the UKMO GCM (hereafter referred to as HadCM3) used in this study are well documented [36]. However, some discussion of the model itself and how HadCM3 differs from HadCM2 is necessary. HadCM3 was developed at the Hadley Centre for Climate Prediction and Research, which is a part of the UK Meteorological Office. The model is one of a new breed of coupled ocean–atmosphere GCMs (OAGCM) that requires no flux corrections to be made, even for simulations of a

Surface temperature (°C)

The global average surface temperature for the Pliocene coupled experiment is equal to 18.27°C which represents a positive ΔT of 3.09°C compared to the coupled experiment for present-day. Compared to the Pliocene fixed SST experiment the global annual average surface temperature in the coupled experiment is 1.64°C warmer. Average warming compared to the present-day coupled and fixed SST simulation over land is equal to 4.2 and 2.21°C. Over the oceans this changes to 3.35 and 0.8°C respectively.

Ocean temperatures (°C)

As an annual zonal average, SSTs in the Pliocene coupled experiment are 2.2°C warmer than the present-day case. The spatial difference in annual and seasonal SSTs between the Pliocene coupled, present-day coupled and Pliocene fixed SST experiments are shown in Fig. 1. Compared to present-day, SSTs are warmer in the low and mid-latitudes by an average of 1–5°C. At high latitudes SST warming is predicted to be 5–10°C, which is indicative of a reduced sea ice coverage and depth in the Pliocene

Forcing of oceans, atmosphere and cryosphere on Pliocene warmth

Numerous proposals exist within the literature to account for the relative climatic warmth of the middle Pliocene. These include increased concentrations of CO2 [31], enhanced thermohaline circulation [25], a more vigorous flow of surface ocean gyres [19], [47], alterations in the outflow of Antarctic deep water [27], and changes in the elevations of mountain chains [48]. All of these explanations have weaknesses when examined in detail and there may have been numerous contributing factors to

Conclusions

This paper presents the results from the first-ever coupled OAGCM model experiment for the middle Pliocene using the HadCM3 and the USGS PRISM2 data set. The model was integrated for 300 simulated years and used a Pliocene atmospheric CO2 concentration of 400 ppmv.

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    The simulation resulted in an increase in the global surface temperatures of 3°C compared to present-day.

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    In contrast to earlier Pliocene modelling experiments using fixed SSTs or a slab-ocean, surface temperature warming occurred over

Acknowledgments

Dr Harry Dowsett and the United States Geological Survey’s PRISM Group are noted for their kind support and encouragement. Dr Lisa Sloan is thanked for providing thoughtful comments on results from the Pliocene coupled modelling. Dr Samantha Cook is thanked for her assistance with the data/model comparison. The authors would like to acknowledge the help and kind assistance of Prof. B.W. Sellwood, Dr D. Seidov and an anonymous reviewer for providing useful comments and reviews which greatly

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