Surface Radiation Budget (SRB) Explanation

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Earth's Radiation Budget

The MY NASA DATA Live Access Server contains a number of parameters of the Earth's Radiation Budget. The schematic below shows where these parameters fit into the bigger picture of the Earth system. The information below further explains these various parameters, which are marked in bold in the text on these explanation pages.

See a NASA Fact Sheet on this topic.
View Earth's Energy Budget (graphic courtesy Loeb et al., 2009).
Click here for a print quality PDF version of the radiation parameters diagram
radiation budget diagram

Earth's Radiation Budget

Location

There are two main locations where we measure the radiation budget:

  • at the surface (SFC; using surface instrumentation or satellite techniques)
  • at the top of the atmosphere (TOA; using satellites).
In theory one could also measure the radiation flow at any level between those two, but it's not so easy to do in practice. Also, the meaning of TOA depends on what you are measuring. For Earth radiation, the best value for the TOA is 20 km, which corresponds to the absorption cross-section of the Earth-atmosphere system (i.e., sunlight that is captured by the Earth and its atmosphere).

Direction

There are two important directions when dealing with the Earth's radiation budget. Energy can either be

  • incoming (Down)
  • or outgoing (Up).
Of course energy goes sideways as well, but that has no effect on the Earth's radiation budget since it does not change the amount of energy in the Earth system.

The NET energy added to the Earth system is simply: NET = incoming - outgoing = Down - Up.

radiation budget diagram
See a NASA Fact Sheet on this topic.
View Earth's Energy Budget (graphic courtesy Loeb et al., 2009).
Click here for a print quality PDF version of the radiation parameters diagram

Earth's Radiation Budget

energy emission from bodies at different temperatures.

Basics

Everything emits electromagnetic radiation, according to its temperature. The graph shows examples for three objects with widely different temperatures (given in degrees Kelvin [K = C + 273.15]). Note that hotter objects emit more energy than cooler objects at every wavelength, and that the hotter objects emit most of their energy at shorter wavelengths than do cooler objects. The peak of the Sun's energy emission is in the wavelengths of visible light (denoted by the rainbow colors in the graph), although it emits other types of energy (like ultraviolet [UV] and infrared [IR]) also. In comparison, the Earth emits orders of magnitude less radiation, and that radiation peaks in the infrared.

A Bit About Units

The units for this energy emission start with the familiar unit Watts, which is used to identify the brightness of light bulbs. However, the units here are more complicated, as they identify Watts PER square meter, PER micron, PER steradian (sr). Decoding this, it means the number of Watts reaching a square meter of area (m2), which depends on the wavelength (measured in microns), schematic showing how the Sun's energy is spread through space. and is spread over a solid angle (measured in steradians). A solid angle is an angle measured in 3D space. The Sun emits in all directions, which means its energy is spread over 4π steradians. Only a small amount of the Sun's energy emission reaches the Earth. Most of it goes off into space in other directions.

The Sun is also very far from the Earth (about 150 million km). So, by the time the Sun's emitted energy reaches the Earth, it is spread over a very large area (a sphere with a radius 216 times larger than the radius of the Sun itself), thus reducing the intensity of energy that Earth receives.

Earth's Radiation Budget

comparing Sun's and Earth's energy AT the Earth.

Energy at the Earth

The figure at right compares the emission from the Earth with the amount of solar energy that reaches the top of the Earth's atmosphere. (The amount of energy from the Sun that actually reaches the Earth's surface is smaller still, and has some very definite spectral features due to absorption and scattering that occur at specific wavelengths in the atmosphere. See a picture. In particular, most of the UV radiation is absorbed in the ozone layer, protecting living things from these harmful rays.) Notice that now, the emission from the Earth is larger than the energy received from the Sun, for wavelengths longer than about 5 microns (a micron is 1.e-6 meters, or one thousandth of a meter). The exact cross-over point depends on the Earth's emission temperature. The average surface temperature is a bit warmer than the emission temperature shown in this graph, so the cross-over point for surface emission occurs at a shorter wavelength. This slightly fuzzy cross-over point is used to define two principal wavelength ranges:

  • shortwave (SW) radiation and
  • longwave (LW) radiation.
Photosynthetically active radiation (PAR) (wavelengths between 0.4 and 0.7 microns) is a subset of the solar radiation that is important for photosynthetic activity in plants.

The combination of SW and LW radiation covers the whole spectrum and is sometimes called the total (TOT) radiation.

Earth's Radiation Budget

Time Interval

The components of the radiation budget change with time. It is not really practical to keep an infinitely detailed, second by second, record. We typically have information averaged over time periods such as
  • hourly,
  • daily,
  • monthly,
  • seasonal,
  • annual averages or
  • climatology: an average over several years.
The numbers in the radiation budget diagram at the top of the page are climatological values.
Most of the parameters in the LAS are for monthly or longer time periods, with a few parameters available at a daily time scale. Given monthly information, you can create seasonal, annual or longer averages.

Sky Condition

The Earth's radiation budget is determined by the amount of energy that actually enters and leaves the Earth, under the sky conditions that actually exist. Clouds have the most influence on what the upward and downward energy actually is. In the shortwave, clouds reflect sunlight. In the longwave, clouds effectively trap infrared energy. To help study and understand how clouds affect the radiation budget, we therefore look at radiation budget parameters under two different sky conditions:
  • All-sky is the term for the actual observed conditions, including clear or cloudy skies wherever they occur.
  • Clear-sky parameters are obtained by taking all observations for a month, discarding any where clouds were present, and computing average conditions for cases of clear sky.
Clear-sky parameters therefore allow you to see more clearly the effects of the Sun's location, and of the Earth's surface (i.e., land vs ocean).

See a NASA Fact Sheet on this topic.

Earth's Radiation Budget

Parameters

Important parameters of the Earth's radiation budget include: