Outgoing Long-wave Radiation (OLR) is electromagnetic radiation of wavelengths between 3.0 and 100 μm emitted from Earth and its atmosphere out to space in the form of thermal radiation. It is also referred to as up-welling long-wave radiation and terrestrial long-wave flux, among others. The flux of energy transported by outgoing long-wave radiation is measured in W/m2.
In the Earth's climate system, long-wave radiation involves processes
of absorption, scattering, and emissions from atmospheric gases,
aerosols, clouds and the surface.
Over 99% of outgoing long-wave radiation has wavelengths between 4 μm and 100 μm, in the thermal infrared part of the electromagnetic spectrum.
Contributions with wavelengths larger than 40 μm are small, therefore
often only wavelengths up to 50 μm are considered . In the wavelength
range between 4 μm and 10 μm the spectrum of outgoing long-wave
radiation overlaps that of solar radiation, and for various applications different cut-off wavelengths between the two may be chosen.
Radiative cooling
by outgoing long-wave radiation is the primary way the Earth System
loses energy. The balance between this loss and the energy gained by
radiative heating from incoming solar shortwave radiation determines global heating or cooling of the Earth system. Local differences between radiative heating and cooling provide the energy that drives atmospheric dynamics.
Atmospheric energy balance
OLR is a critical component of the Earth's energy budget, and represents the total radiation going to space emitted by the atmosphere.
OLR contributes to the net all-wave radiation for a surface which is
equal to the sum of shortwave and long-wave down-welling radiation minus
the sum of shortwave and long-wave up-welling radiation.
The net all-wave radiation balance is dominated by long-wave radiation
during the night and during most times of the year in the polar regions.
Earth's radiation balance is quite closely achieved since the OLR very
nearly equals the Shortwave Absorbed Radiation received at high energy
from the sun. Thus, the Earth's average temperature is very nearly
stable. The OLR balance is affected by clouds and dust in the
atmosphere. Clouds tend to block penetration of long-wave radiation
through the cloud and increases cloud albedo, causing a lower flux of long-wave radiation into the atmosphere.
This is done by absorption and scattering of the wavelengths
representing long-wave radiation since absorption will cause the
radiation to stay in the cloud and scattering will reflect the radiation
back to earth. the atmosphere generally absorbs long-wave radiation
well due to absorption by water vapour, carbon dioxide, and ozone. Assuming no cloud cover, most long-wave up-welling radiation travels to space through the atmospheric window
occurring in the electromagnetic wavelength region between 8 and 11 μm
where the atmosphere does not absorb long-wave radiation except for in
the small region within this between 9.6 and 9.8 μm.
The interaction between up-welling long wave radiation and the
atmosphere is complicated due to absorption occurring at all levels of
the atmosphere and this absorption depends on the absorptivities of the
constituents of the atmosphere at a particular point in time.
Role in greenhouse effect
The reduction of the surface long-wave radiative flux drives the greenhouse effect. Greenhouse gases, such as methane (CH4), nitrous oxide (N2O), water vapor (H2O) and carbon dioxide (CO2),
absorb certain wavelengths of OLR, preventing the thermal radiation
from reaching space, adding heat to the atmosphere. Some of this thermal
radiation is directed back towards the Earth by scattering, increasing
the average temperature of the Earth's surface. Therefore, an increase
in the concentration of a greenhouse gas may contribute to global warming
by increasing the amount of radiation that is absorbed and emitted by
these atmospheric constituents. If the absorptivity of the gas is high
and the gas is present in a high enough concentration, the absorption
bandwidth becomes saturated. In this case, there is enough gas present
to completely absorb the radiated energy in the absorption bandwidth
before the upper atmosphere is reached, and adding a higher
concentration of this gas will have no additional effect on the energy
budget of the atmosphere.
The OLR is dependent on the temperature of the radiating body.
It is affected by the Earth's skin temperature, skin surface emissivity,
atmospheric temperature, water vapor profile, and cloud cover.
OLR measurements
Two
popular remote sensing methods used to estimate up-welling long-wave
radiation are to estimate values using surface temperature and
emissivity, and to estimate directly from satellite top-of-atmosphere
radiance or brightness temperature.
Measuring outgoing long-wave radiation at the top of atmosphere and
down-welling long-wave radiation at the surface is important for
understanding how much radiative energy is kept in our climate system,
how much reaches and warms the surface, and how the energy in the
atmosphere is distributed to affect developments of clouds. Calculating
the long-wave radiative flux from a surface is also a useful an easy way
to assess surface temperature.
Outgoing long-wave radiation (OLR) has been monitored globally
since 1975 by a number of successful and valuable satellite missions.
These missions include broadband measurements from the Earth Radiation
Balance (ERB) instrument on the Nimbus-6 and Nimbus-7 satellites; Earth Radiation Budget Experiment (ERBE) scanner and the ERBE non scanner on NOAA-9, NOAA-10 and NASA Earth Radiation Budget Satellite (ERBS); The Clouds and the Earth's Radiant Energy System (CERES) instrument aboard NASA's Aqua and Terra satellites; and Geostationary Earth Radiation Budget instrument (GERB) instrument on the Meteosat Second Generation (MSG) satellite.
Down-welling long-wave radiation at the surface is mainly measured by Pyrgeometer. A most notable ground-based network for monitoring surface long-wave radiation is Baseline Surface Radiation Network (BSRN), which provides crucial well-calibrated measurements for studying global dimming and brightening.
OLR calculation and simulation
Many applications call for calculation of long-wave radiation
quantities: the balance of global incoming shortwave to outgoing
long-wave radiative flux determines the Energy budget of Earth's climate; local radiative cooling
by outgoing long-wave radiation (and heating by shortwave radiation)
drive the temperature and dynamics of different parts of the atmosphere;
from the radiance from a particular direction measured by an instrument, atmospheric properties (like temperature or humidity) can be retrieved.
Calculations of these quantities solve the radiative transfer equations that describe radiation in the atmosphere. Usually the solution is done numerically by an Atmospheric radiative transfer code adapted to the specific problem.