InfoDotInc / archive systemEstablished online record · rebuilding deliberately
InfoDotInc

Technical documents, historic paths, and source-backed reference material.

Archive / FAA Aviation Weather Handbook / FAA Aviation Weather Handbook: Chapter 7 — Earth-Atmosphere Heat Imbalances

Chapter 7 — Earth-Atmosphere Heat Imbalances

Chapter 7 — Earth-Atmosphere Heat Imbalances

FAA-H-8083-28B (2026)

Chapter 7, Earth-Atmosphere Heat Imbalances 7-1

7 Earth-Atmosphere Heat Imbalances

7.1 Introduction

Weather is not a capricious act of nature but , rather, the atmosphere ’s response to unequal rates of

radiational heating and cooling across the surface of the Earth and within its atmosphere. The absorption of

incoming solar radiation causes heating, while the emission of outgoing terrestrial radiation causes cooling.

However, imbalances in the rate of heating and cooling create temperature gradients. 2 Atmospheric

circulations and weather are the atmosphere ’s never-ending attempt to redistribute this heat and achieve

equilibrium. This chapter provides a background on the interaction between the Earth and the atmosphere

for a better understanding of the weather that will affect flight operations.

2 A gradient describes the rate of change of a feature (in this case, temperature) per unit of distance.

Chapter 7, Earth-Atmosphere Heat Imbalances 7-2

7.2 The Earth-Atmosphere Energy Balance

The Earth -atmosphere energy balance is the balance between incoming energy from the Sun (solar

radiation) and outgoing energy from the Earth (terrestrial radiation), as seen in Figure 7-1. When solar

radiation reaches the Earth, some is re flected back to space by air (eight percent), clouds (17 percent), or

the surface ( six percent). Some is absorbed by water v apor/dust/ozone (19 percent) or by clouds

(four percent). The remainder is absorbed by the Earth’s surface (46 percent).

Figure 7-1. Earth-Atmosphere Energy Balance

In Figure 7-1, 100 units of incoming radiation from the Sun is balanced by 100 units of outgoing radiation

from the Earth.

However, since the Earth is much cooler than the Sun, its radiating energy is much weaker (long

wavelength) infrared energy. Indirectly, this energy can be seen radiating into the atmosphere as heat

(e.g., rising from a hot road, creating shimmers on hot sunny days). The Earth -atmosphere energy balance

is achieved as the energy received from the Sun (solar radiation) balances the energy lost back into space

by the Earth (terrestrial radiation). In this way, the Earth maintains a stable average temperature.

The absorption of infrared radiation trying to escape from the Earth back to space is particularly important

to the global energy balance. Energy absorption by the atmosphere stores more energy near its surface than

it would if there was no atmosphere. The average surface temperature of the Moon, which has no

atmosphere, is -18 °C (0 °F). By contrast, the average surface temperature of the Earth is 15 °C (59 °F).

This heating effect is called the greenhouse effect.

Chapter 7, Earth-Atmosphere Heat Imbalances 7-3

Greenhouse warming is enhanced during nights when the sky is overcast (see Figure 7-2). Heat energy from

the Earth can be trapped by clouds, le ading to higher temperatures as compared to nights with clear skies.

The air is not allowed to cool as much with overcast skies. Under partly cloudy skies, some heat is allowed

to escape, and some remains trapped. Clear skies allow for the most cooling to take place.

Figure 7-2. Greenhouse Effect on Nighttime Radiational Cooling

7.3 Heat Imbalances Between Earth’s Surface and the Atmosphere

The Earth-atmosphere energy balance numbers (see Figure 7-1) indicate that both sensible heat ( seven

percent) and latent heat (24 percent) processes transfer heat from the Earth ’s surface into its atmosphere.

Both processes are necessary to prevent the Earth’s surface from continually heating up and the atmosphere

from continually cooling down.

7.3.1 Sensible Heating

Sensible heating involves both conduction and convection. It occurs due to differences in air density. Warm

air is less dense than cool air.

On warm sunny days, the Earth’s surface is heated by incoming solar radiation or insolation. However, the

heating is somewhat uneven because certain areas of the Earth ’s surface absorb more heat from the Sun

than others. Heat is conducted from the relatively warm ground to the cooler overlying air, which warms a

shallow layer of air near the ground. The heated air expands, becomes less dense than the surrounding

cooler air, and rises. Through this process, a large bubble of warm air called a thermal rises a nd transfers

heat energy upwards (see Figure 7-3). Cooler, denser air sinks toward the ground to replace the rising air.

This cooler air becomes heated in turn, rises, and repeats the cycle.

Chapter 7, Earth-Atmosphere Heat Imbalances 7-4

Figure 7-3. Development of a Thermal

In this manner, convection transports heat from the Earth ’s surface into the atmosphere. Because air is a

poor conductor of heat (see Table 5-3), convection is much more important than conduction as a heat

transport mechanism within the atmosphere.

Figure 7-4. Example of Convection in the Atmosphere

7.3.2 Latent Heat

The phase transition of water and associated latent heat exchanges are largely responsible for transferring

the excess heat from the surface of the Earth into its atmosphere. As the Earth ’s surface absorbs radiation,

some of the heat produced is used to evaporate (vaporize) water from oceans, lakes, rivers, soil, and

vegetation. The water absorbs heat energy due to the latent heat of vaporization. Some of this water vapor

Chapter 7, Earth-Atmosphere Heat Imbalances 7-5

condenses to microscopic water droplets or deposits as ice crystals that are visible as clouds. During cloud

formation, the water vapor changes state, and latent heat is released into the atmosphere. During this

process, the excess heat is transferred from the Earth’s surface into its atmosphere.

7.4 Heat Imbalance Variations with Latitude

Global imbalances in radiational heating and cooling occur not only vertically between the Earth’s surface

and its atmosphere but also horizontally with latitude. Since the Earth is essentially spherical, parallel beams

of incoming solar radiation strike lower latitudes more directly than higher lat itudes (see Figure 7-5); that

is, the solar zenith angle is lower, and the Sun is more directly overhead in equatorial regions than at the

poles. At higher latitudes, solar radiation is spread over a larger area and is less intense per unit surface area

than at lower latitudes. Thus, the Earth absorbs more solar radiation at lower latitudes than higher latitudes,

which creates heat imbalances and temperature gradients between the Equator and the poles.

Figure 7-5. Solar Zenith Angle Variations with Latitude

The emission of terrestrial radiation also varies by latitude, but less so than the absorption of solar radiation.

Terrestrial radiation emission decreases with increasing latitude due to a drop in temperature with latitude.

Thus, at higher latitudes, the annual rate of cooling exceeds the rate of warming, while the reverse is true

at lower latitudes.

Averaged over all latitudes, incoming solar radiation must equal outgoing terrestrial radiation. Otherwise,

the Earth would be unable to maintain a constant average temperature. About 35° latitude in both

hemispheres is where incoming and outgoing radiation is equal. This implies there is annual net cooling at

higher latitudes and net warming at lower latitudes ; however, this is untrue. The excess heat in the tropics

Chapter 7, Earth-Atmosphere Heat Imbalances 7-6

must be transported polar by some mechanism(s). This poleward heat transport is accomplished by

atmospheric circulations, weather, and ocean currents.

7.5 Seasons

Seasons are caused by the tilt of the Earth’s rotational axis as the Earth orbits the Sun (see Figure 7-6). The

Earth’s rotational axis is tilted by 23½° from the perpendicular drawn to the plane of the Earth’s orbit about

the Sun and points the same direction in space all year long. The North Pole is tilted most directly toward

the Sun during the summer solstice. Thus, in the Northern Hemisphere, the longest day of the year (lowest

solar zenith angle) occurs on the summer solstice (approximately June 22), while the shortest day of the

year (highest solar zenith angle) occurs on the winter solstice (approximately December 22). Day and night

are of equal length (12 hours) worldwide on the vernal equinox (approximately March 21) and the autumnal

equinox (approximately September 23).

Figure 7-6. Solar Zenith Angle Variations with Northern Hemisphere Seasons

Figure 7-7 illustrates the average seasonal temperature variation in the Northern Hemisphere. Note that the

warmest (coldest days) of the year occur after the summer (winter) solstice. This is due to the time lag

necessary for heat flow processes to fully heat (cool) the surface of the Earth.

Chapter 7, Earth-Atmosphere Heat Imbalances 7-7

Figure 7-7. Average Seasonal Temperature Variation in the Northern Hemisphere

7.6 Diurnal Temperature Variation

Diurnal temperature variation is the daytime maximum and nighttime minimum of air temperature due to

variations of insolation caused by the rising and setting of the Sun (i.e., variations of solar zenith angle) as

the Earth rotates around its axis. Figure 7-8 depicts the typical diurnal temperature and radiation variations

over land when the sky is clear.

Figure 7-8. Clear Sky Diurnal Temperature and Radiation Variations Over Land

Chapter 7, Earth-Atmosphere Heat Imbalances 7-8

Warming and cooling of the Earth depend on an imbalance between solar and terrestrial radiation. The

Earth receives heat during the day through incoming solar radiation. It loses heat to space by outgoing

terrestrial radiation both day and night.

Shortly after sunrise, incoming solar radiation received at the Earth ’s surface (insolation) becomes greater

than outgoing terrestrial radiation and the Earth ’s surface warms. Peak insolation occurs around noon, but

maximum surface air temperature usually occurs during the midafternoon. This lag is necessary for the air

near the ground to heat up due to conduction and convection with the surface. The Earth begins to cool

once the rate of outgoing terrestrial radiation exceeds the rate of insolation.

At night, insolation is absent but outgoing terrestrial radiation continues, and the Earth’s surface continues

to cool. Cooling continues until shortly after sunrise, when incoming solar radiation once again exceeds

outgoing terrestrial radiation. Minimum surface air temperature usually occurs shortly after sunrise.

The magnitude of diurnal temperature variation is primarily influenced by surface type, latitude, sky cover

(e.g., clouds or pollutants), water vapor content of the air, and wind speed. Temperature variation is

maximized over land, at low latitudes, with a clear sky, dry air, and light wind. Conversely, temperature

variation is minimized over water, at high latitudes, with a cloudy sky, moist air, and strong wind.

Original source PDFPublished from pages 87–94 of the recorded source chapter.
Open source PDF ↗