Chapter 9 Cuffey & Paterson ©2010 Elsevier, Inc..

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Presentation transcript:

Chapter 9 Cuffey & Paterson ©2010 Elsevier, Inc.

FIGURE 9.1 Variation of temperature over 10 months at South Pole, at six depths in the near-surface firn. At the end of the experiment, the depths of the six thermistors (called T1 through T6) were about 0.2, 0.4, 0.6, 0.8, 1.0, and 1.2 meters. Due to snowfall, the depths increased by about 0.4 m over the year, beginning around hour 3500. Temperature variability decreases with depth. Adapted from Brandt and Warren (1997). ©2010 Elsevier, Inc.

Theoretical seasonal cycle of firn temperatures in central Greenland. Information from: Harold C. Relyea, Congressional Research Service, National Emergencies Powers, 98-505 GOV, CRS-13 -- CRS-16 (2007), http://www.fas.org/sgp/crs/natsec/98-505.pdf FIGURE 9.2 Theoretical seasonal cycle of firn temperatures in central Greenland. ©2010 Elsevier, Inc.

FIGURE 9.3 Warming of firn by latent heat of refreezing meltwater, at 1600m elevation on the Greenland Ice Sheet. Data courtesy of N. Humphrey and T. Pfeffer. ©2010 Elsevier, Inc.

FIGURE 9.4 Variation of temperature with depth in the temperate Blue Glacier (solid line) and variation expected for pure ice in equilibrium with (a) pure water and (b) air-saturated water. Impurities depress the melting point in the glacier. Redrawn from Harrison (1975). ©2010 Elsevier, Inc.

FIGURE 9.5 Dimensionless steady temperature profiles for various values of the advection parameter (γ). Negative value for γ indicates upward velocity; positive values indicate downward velocity. Equations 9.19–9.21 define the variables; θ refers to scaled temperature and ξ to scaled height above the bed. Adapted from Clarke et al. (1977) and used with permission of the American Geophysical Union, Reviews of Geophysics and Space Physics. ©2010 Elsevier, Inc.

strengthen in this case; the basal zone warms, upper layers cool. FIGURE 9.6 Theoretical influence of horizontal advection on the profile of temperature with depth. This example corresponds to the accumulation zone of a 500-m-thick glacier, with 0.4myr−1 of accumulation and surface velocity of 20myr−1. (At depth, the velocity decreases according to the theoretical profile for flow by internal deformation.) Case A: Horizontal flow cools the ice because of an along-glacier temperature gradient of 0.12 ◦Ckm−1, but also warms basal layers by frictional heating. Increasing the along-glacier temperature gradient to twice the value in A gives Case B. Temperatures are reduced at all depths, and a “negative temperature gradient” forms in the upper layers. Increasing the ice velocity to 40myr−1, but leaving the temperature gradient as in A, gives Case C. Advective cooling and frictional heating both strengthen in this case; the basal zone warms, upper layers cool. ©2010 Elsevier, Inc.

FIGURE 9.7 Measured temperature profiles in accumulation zones of polar ice sheets and ice caps. For sites with negligible horizontal advection, the number in parentheses gives the advection parameter defined by Eq. 9.21. Data sources are given in the text. ©2010 Elsevier, Inc.

FIGURE 9.8 Theoretical temperature profiles along an ice sheet flow line. The number on each curve is the distance as a fraction of the flow-line length. The equilibrium line is at 0.91. (b) Closer view of profiles near the margin. A temperate layer develops at the bottoms of profiles 0.83 through 0.98. Adapted from Dahl-Jensen (1989) and used with permission of the American Geophysical Union, Journal of Geophysical Research. ©2010 Elsevier, Inc.

FIGURE 9.9 Temperature profiles in White Glacier, at various distances along the flow line. Depth to bed is indicated in each case. Note change in temperature scale between 9.9 and 12 km. Data from Blatter (1985). ©2010 Elsevier, Inc.

FIGURE 9.10 Propagation of a temperature wave following a 15 °C step increase of surface temperature at time zero. The initial curve (solid line in all panels) is a steady-state profile for an accumulation rate of 0.07myr−1. In all three panels, Case A assumes no change in the vertical ice velocity from the initial state. In Case B, the vertical velocity increases to 0.3myr−1 at time zero. ©2010 Elsevier, Inc.

FIGURE 9.11 Temperature profiles in ice shelves. Broken lines indicate extrapolations. Data sources are given in the text. ©2010 Elsevier, Inc.