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212 J. L. Renner<br />

temperature with depth is complex. The change in heat generation and, hence,<br />

heat flow with depth can be ignored for most general heat flow studies in conductive<br />

areas.<br />

Temperature ( T ) at depth ( D ) is given by T � T surface � D Γ , where Γ (temperature<br />

gradient) is related to heat flow ( q ) and rock conductivity ( K ) by Q � K Γ .<br />

Diment et al. [2] provide a general review of temperatures and heat flow, with<br />

particular emphasis on heat content in the USA. Temperature at a given depth<br />

can then be calculated using the relationship, T � T surface � D Γ , where T surface is<br />

the average surface temperature. Tester et al. [3] , Wisian et al. [4] , and Blackwell<br />

and Richards [5] provide detailed discussions of the relationship between rock<br />

conductivity and heat flow. Tester et al. [3, Chapter 2] also provide insight into<br />

projecting temperature gradients to depths beyond those reached by drilling<br />

when heat flow and subsurface geology are reasonably well known.<br />

In older areas of continents, such as much of North America east of the Rocky<br />

Mountains, heat flow is generally 40–60 mW � m � 2 . This heat flow, coupled with<br />

the thermal conductivity of average rocks in the upper 4 km of the crust, yields<br />

a gradient of 20°C� km � 1 and subsurface temperatures of 90–110°C at 4 km depth<br />

if the average surface temperature is 20°C. Heat flow within younger areas is<br />

generally 70–90 mW� m � 2 and temperatures are about 150°C at 4 km. Although<br />

direct-use applications of geothermal energy can utilize temperatures as low as<br />

about 35°C, the minimum temperature suitable for electrical generation in most<br />

instances is about 150°C. Therefore, areas of somewhat above average temperature<br />

with depth require wells about 4 km deep for production of electricity and<br />

geothermal explorationists must seek areas of much higher than average temperatures<br />

for economic electrical production. As will be discussed later, where<br />

energy prices are high and environmental constraints limit greenhouse gas<br />

emissions, deeper drilling can be economic.<br />

The previous discussion assumes that heat transfer in the earth is conductive.<br />

Fortunately for geothermal developers, spatial variations of the thermal energy<br />

within the mantle of the earth can drive convective transfer of mass and energy<br />

within the mantle and crust of the earth. This convective transfer gives rise to<br />

concentrations of thermal energy near the surface of the earth that can provide<br />

an energy resource.<br />

2 .<br />

Tectonic Controls<br />

The unifying geologic concept of plate tectonics provides a generalized view of<br />

geologic processes that move concentrations of heat from deep within the earth<br />

to drillable depths. The reader is directed to Kearey and Vine [6] , for example, for<br />

a discussion of global tectonics. The heat can be related to movement of magma<br />

within the crust, particularly when associated with recent volcanism, or deep circulation<br />

of water in active zones of faulting. Much of the geothermal exploration<br />

occurring worldwide is focused on major plate boundaries ( Figure 12.1 ), since<br />

most of the current volcanic activity of the earth is located near plate boundaries<br />

associated with spreading centers and subduction zones.

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