Part 4:
Energy Balance
How much radiation does the earth's surface absorb? What causes the air to
warm during the day? How does the temperature change over the course of a
day? We will try to answer these questions in this section.
As mentioned earlier, almost all the energy we see and feel comes from the
sun. Scientists have determined a standard value for that amount of
energy, which is called the solar constant. It is the average
amount of energy that reaches the top of the atmosphere, on a plane
perpendicular to the sun's rays, at an average distance from the sun. This
value is approximately 1370 watts per square meter (W/m2). We
say approximately because the sun's energy output does change slightly
with time, due to sun spots and other phenomena, which we'll save for the
astronomers. There are two key points, however. First, the sun's energy
output is relatively constant, and there is essentially no interference (obstructions) with that radiation until it enters the atmosphere.
The Earth's average temperature remains fairly constant from year to year.
There are long term trends (like the ice ages), but no evidence of any
dramatic temperature change from one year to the next. Therefore, the
Earth must be releasing into space the same amount of energy that it
receives from the sun. If this did not occur, the atmosphere would
measurably warm or cool, depending on the amount of heat lost to space.
So what happens to solar radiation once it enters the atmosphere, and how
does energy get radiated into space? Well, we can think of the incoming
solar radiation as being broken up into parts. The diagram below shows the
average break down of solar radiation as it enters the atmosphere.
(Click image to view in separate window)
When we combine the break down of incoming radiation with the break down
of outgoing radiation, we have the earth-atmosphere energy balance.
The chart below displays the average break down of energy lost and gained
at the earth's surface. The units used are relative to the amount of
incoming radiation. Notice that the total energy lost at the earth's
surface (lower left hand corner) is equal to the amount gained at the
surface (lower right hand corner).
(Click image to view in separate window)
The net energy at the earth's surface can be thought of as the sum of the
incoming energy minus the energy required to heat the air minus the energy
to evaporate water. This simple equation is known as the energy budget
equation. The energy used to heat the air is directed upward, away
from the surface, and so is considered a subtraction. The same is true for
the energy required to evaporate water. This energy, however, is in the
form of a heat we can't feel. It is known as latent heat.
When you touch a hot stove, the heat you feel is called sensible heat (because your sense of feel is able to react to it). Latent heat is not really heat you can feel, but energy required to break
the molecular bonds that keep molecules in a single phase. For example, it
is latent heat that is used when you boil water and form steam. Latent
heat is absorbed from the surroundings to melt ice and evaporate water.
This makes sense because water molecules vibrate faster than ice molecules
(as any liquid has more energy than its corresponding solid state). Latent
heat is released when you go the other direction: freezing water and condensing vapor. The concept of latent heat is crucial to understanding why
clouds develop. As the water vapor in the air cools, it condenses,
releasing huge amounts of energy that allow the cloud to develop further
by decreasing stability. We will discuss stability in greater depth in
Session 6.
Bowen Ratio
The comparison between the amount of sensible heat and the amount of latent heat is often important when determining energy balance. As a quick method to compare the amount of sensible heat energy to the amount of latent heat energy, the Bowen Ratio was developed. It has the following form:
where B is the Bowen Ratio value, HS is the sensible heat, and HL is the latent heat. In situations where there is little moisture available, the HL value will be small, and the Bowen Ratio will be greater than one. In situations where it is very humid, the HL value will be large, and the Bowen Ratio will be less than one. In situations where the amount of sensible heat energy is near the amount of latent heat energy, the Bowen Ratio will be approximately one.
During the night, there is no incoming solar radiation, so the amount of sensible heat energy becomes minimal or even negative (loss of heat energy) . In these situations, the Bowen Ratio will be very small or even negative, as latent heat is not as dependent on incoming solar radiation.
Let's look at the energy balance in terms of the daily variations in
temperature. Incoming solar energy is a maximum when the sun is highest in
the sky. But the surface of the earth warms continuously from the time the
sun rises to the time it sets. Therefore, the earth radiates its maximum
amount at sunset, and does not begin to slow down until the sun sets (no
more incoming radiation). The earth is releasing the least amount of
energy early in the morning, before the sun rises. The net energy at the
surface is therefore the difference in the incoming radiation (shortwave)
and the radiation emitted from the earth (longwave). The chart
demonstrates further. Here, the energy surplus area means that more energy
is entering the earth than is leaving it. The deficit area is just the
opposite -- more energy is lost by the Earth than gained (due to the
absence of sunlight). Remember, the total amount of net energy gained is
zero -- there is an energy balance. The surplus area on the chart is
showing the daily replenishment of energy into the Earth-atmosphere system
necessary to maintain that balance.
One important item to notice is that the earth's maximum emission of heat
is skewed to the right (toward sunset) of the maximum incoming energy .
Another key observation is that the earth emits and absorbs radiation
much more efficiently than the atmosphere. That is why the late afternoon
is often much warmer than at noon, when the incoming shortwave radiation
is a maximum. That's also why the early morning is the coolest time of
day. The atmosphere warms and cools slowly, but the ground warms and cools
much more quickly. The next time you're outside, feel the ground with your
hand. If it is mid-day, it will feel significantly warmer than the air. If
it is late night, it will feel significantly cooler. Differences in the
rate of radiation absorption and release are a major factor influencing
energy balance. This, and other factors, are discussed in the next section.
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