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James Croll (1821–1890): ice, ice ages and the Antarctic connection

Published online by Cambridge University Press:  13 November 2014

David E. Sugden*
Affiliation:
School of GeoSciences, University of Edinburgh, Edinburgh EH8 9XP, UK
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Abstract

The thrust of this paper is that James Croll should be more generously lauded for his remarkable contribution to the study of ice ages, glacier flow and the nature of the Antarctic ice sheet. Croll was the first to calculate the link between fluctuations of the Earth’s orbit and glacial/interglacial cycles, and to identify the crucial role of positive feedback processes necessary to transform minor insolation changes into major climatic changes. He studied the mechanisms of glacier flow and explained flow over horizontal land surfaces at a continental scale, including the excavation of rock basins. Croll relied on a quantitatively based deductive approach. One of his most remarkable achievements was his study of the thickness, thermal regime and dynamics of the Antarctic ice sheet (1879). This contains important insights, which are relevant today, and yet the paper was published before anyone had landed on the continent!

Information

Type
Original Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (http://creativecommons.org/licenses/by/3.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© Antarctic Science Ltd 2014
Figure 0

Fig. 1 James Croll signed this photo of himself for his friend James Campbell Irons, who compiled the Autobiographical Sketch of James Croll (1896).

Figure 1

Fig. 2 Prediction of the variation in eccentricity of the Earth’s orbit calculated by Croll using Leverrier’s formula. Lower panel. The vertical line marked zero in the centre represents the year 1880 and the predictions to the right are for the next one million years. Predictions for the past one million years are to the left and show eight cold phases, a reasonable approximation of modern discoveries. Upper panel. Predictions from one million years ago (right) to 3 million years ago (left). Full glaciations occur at periods of high eccentricity, namely 2.6 and 2.5 million years ago and 850 000 years ago, while the next full glaciations are predicted to occur 800 000 and 900 000 years in the future. From Croll (1875, following page 312).

Figure 2

Fig. 3 “Chart showing the general agreement between the system of ocean currents and winds.” (Croll 1875, p. 213). It was this agreement that suggested to Croll that winds played an important role on ocean circulation. Lower temperatures in the polar regions of one hemisphere increase the strength of the trade winds and thereby ocean circulation; this leads to positive feedback since the increased turnover further cools the ocean, thereby enhancing the cooling of the atmosphere.

Figure 3

Fig. 4 Reconstruction of the former ice sheet in north-west Europe compiled by James Croll and used in his paper on the thickness of the Antarctic ice sheet. This reconstruction showed ice could cross basins and explained the transverse ice flow in Shetland and the onshore flow at the tip of Caithness, northern Scotland. The reconstruction is not too different to that now accepted, except that the inhabitants of unglaciated southern England will question whether he has been a little too enthusiastic! After Croll (1879, following page 34).

Figure 4

Fig. 5 The cover page of the impressive paper on the Antarctic ice sheet.

Figure 5

Fig. 6 Page extract from Croll’s 1879 Antarctic paper in which he grapples with the issue of scale and perception. To the right of the text he draws a vertical cross section through the presumed Antarctic ice sheet assuming a thickness of 12 miles in the centre. As he explains in the lively text, it is not an unreasonable thickness if viewed at a continental scale. In a range of possible thickness reconstructions, Croll assumes a constant ice-surface gradient, which explains the high calculated thicknesses.