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Principles of terrestrial ecosystem ecology.pdf

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74 4. Terrestrial Water and Energy Balance<br />

example, have a lower albedo than deciduous<br />

forests, and grasslands with large amounts<br />

<strong>of</strong> standing dead leaves have relatively high<br />

albedo. The albedo <strong>of</strong> a complex canopy is less<br />

than that <strong>of</strong> individual leaves, because much <strong>of</strong><br />

the light reflected or transmitted by one leaf is<br />

absorbed by other leaves and stems. For this<br />

reason, deep, uneven canopies <strong>of</strong> conifer<br />

forests have a low albedo. Changes in <strong>ecosystem</strong><br />

albedo explain in part why high-latitude<br />

regions are projected to warm more rapidly<br />

than low latitudes. As climate warms, snow and<br />

sea ice will melt earlier in the spring, replacing<br />

a reflective snow-covered surface with a dark<br />

absorptive surface. This process, together with<br />

the resulting change in temperature, is referred<br />

to as the snow (or ice) albedo feedback. Over<br />

longer time scales, the northward movement <strong>of</strong><br />

trees into tundra causes an additional reduction<br />

in regional albedo in winter because the dark<br />

forest canopy masks the underlying snowcovered<br />

surface.With the low sun angles typical<br />

<strong>of</strong> high latitudes, this effect is significant even<br />

with sparse canopies. As the treeline moves<br />

north, the land surface absorbs more energy,<br />

which is then transferred to the atmosphere,<br />

causing a positive feedback to regional<br />

warming (Foley et al. 1994). Albedo also varies<br />

diurnally; it is about twice as high in early<br />

morning and evening as at midday. The diurnal<br />

changes in absorbed radiation are therefore<br />

greater than one would expect from diurnal<br />

variations in incoming radiation.<br />

Ecosystem Radiation Budget<br />

The amount <strong>of</strong> longwave radiation emitted<br />

by an object depends on its temperature and<br />

its emissivity, a coefficient that describes the<br />

capacity <strong>of</strong> a body to emit radiation. Most<br />

absorbed radiation is emitted (emissivity<br />

about 0.98in vegetated <strong>ecosystem</strong>s), so differences<br />

among <strong>ecosystem</strong>s in longwave radiation<br />

balance depend primarily on the temperature<br />

<strong>of</strong> the sky, which determines Lin, and the surface<br />

temperature <strong>of</strong> the <strong>ecosystem</strong>, which determines<br />

Lout.<br />

Rnet = ( Kin -Kout)+<br />

( Lin -Lout)<br />

= ( 1 -a)<br />

K + s e T -e<br />

T<br />

( )<br />

4 4<br />

in sky sky surf surf<br />

(4.2)<br />

where a is the surface albedo, s is the Stefan-<br />

Boltzman constant (5.67 ¥ 10 -8 Wm -2 K -4 ), T is<br />

absolute temperature (K), and e is emissivity.<br />

Clouds are warmer than space and effectively<br />

trap longwave emissions from the surface, so<br />

<strong>ecosystem</strong>s receive more longwave radiation<br />

under cloudy than under clear conditions. This<br />

explains why cloudy nights are warmer than<br />

clear ones and why deserts are generally cold<br />

at night, despite the high inputs <strong>of</strong> solar energy<br />

during the day.<br />

Longwave radiation emitted by the <strong>ecosystem</strong><br />

depends on surface temperature, which,<br />

in turn, depends on the quantity <strong>of</strong> radiation<br />

received by the surface and the efficiency with<br />

which this energy is transmitted into the air and<br />

soil. Surfaces that absorb a large amount <strong>of</strong><br />

radiation, due to high solar inputs and/or low<br />

albedo tend to be warmer and therefore emit<br />

more longwave radiation. Dry surfaces and<br />

leaves with low transpiration rates also tend to<br />

be warm because they are not cooled by the<br />

evaporation <strong>of</strong> water. Desert sands, recent burn<br />

scars, and city pavements, for example, are<br />

generally hot. Similarly, a well-watered lawn is<br />

much cooler than an <strong>ecosystem</strong> that is dry or is<br />

dominated by plants with low transpiration<br />

rates. Because L out is a function <strong>of</strong> temperature<br />

raised to the fourth power (Eq. 4.2), surface<br />

temperature has a powerful multiplying effect<br />

on L out.<br />

Canopy structure also influences surface<br />

temperature and surface energy exchange<br />

through its effect on the efficiency <strong>of</strong> energy<br />

dissipation. The irregular surface <strong>of</strong> vegetation<br />

slows down airflow unevenly, creating mechanical<br />

turbulence. Tall uneven canopies such as<br />

conifer forests are aerodynamically more rough<br />

than are short smooth canopies. The mechanical<br />

turbulence generated by airflow across the<br />

vegetation surface creates eddies, which sweep<br />

down into the canopy, transporting bulk air<br />

inward and canopy air out. These eddies transfer<br />

energy away from the surface and mix it<br />

with the atmosphere (Jarvis and McNaughton<br />

1986). Air flowing across short, smooth<br />

canopies such as grasslands or crops tends to be<br />

less turbulent, so these canopies are less efficient<br />

in shedding the energy that they absorb—<br />

that is, they are less tightly coupled to the bulk

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