Energy Efficiency Metal roofs have high solar reflectance and
thermal emissivity, which means that they can efficiently reflect solar heat right back to the atmosphere.
This innovative process produces a heater with tremendous output and high
thermal emissivity.
This study used variations in
the thermal emissivity of the surface observed by the Visible and Infrared Thermal Imaging Spectrometer on the European Space Agency's Venus Express spacecraft to identify compositional differences in lava flows at three hotspots.
Not exact matches
Investigating the thermophysical properties of materials in concentrated sunlight, including
thermal expansion,
thermal conductivity and diffusivity, specific heat, mechanical properties, and spectral
emissivity and absorptivity
This is because the fundamentals of
thermal radiation from an isolated slab:
emissivity, absorptivity, transmissivity, are related by
emissivity = absorptivity = (1 — transmissivity) where transmissivity = exp -LRB-- TAU)(neglecting directionality).
For an arbitrary body emitting and absorbing
thermal radiation in thermodynamic equilibrium, the
emissivity is equal to the absorptivity.
If the radiaitve
thermal equilibrium is both with the sun (a blackbody) and space (a blackbody), then no matter what kind of non-blackbody the earth is, absorptivity must still equal
emissivity at every wavelength, unless someone is arguing that Kirchoff's law no longer holds.
The main point is that for a spherical body in radiative
thermal equilibrium with the sun, where absorptivity =
emissivity, then the temperature is independent of albedo and
emissivity, because they cancel out of the equation.
There is a fundamental relationship (Gustav Kirchhoff's 1859 law of
thermal radiation) that equates the
emissivity of a surface with its absorption of incident light (the «absorptivity» of a surface).
Black soot absorbs
thermal radiation very well; it has an
emissivity as large as 0.97, and hence soot is a fair approximation to an ideal black body.
«Quantitatively,
emissivity is the ratio of the
thermal radiation from a surface to the radiation from an ideal black surface at the same temperature as given by the Stefan — Boltzmann law.»
Oke et al 1991 is a companion study that is much more informative about UHI, with interesting discussions of the contributions to UHI of canyon view,
thermal storage, anthropogenic heat emissions, an urban greenhouse effect from additional pollution and moisture, surface
emissivity etc..
The real GHE is the reduction of surface
emissivity, also possibly coupled convection as atmospheric GHG
thermal - emission Poynting Vectors annihilate the UP PVs in that wavelength interval.
the GHG
thermal radiation from the atmosphere reduces surface
emissivity so the impedance to heat transport from all sources rises.
Nope: the GHG
thermal radiation from the atmosphere reduces surface
emissivity so the impedance to heat transport from all sources rises.
For example, road tar surfaces receive radiation (solar spectrum) from incident «sunlight»; some of which is absorbed and some reflected, so the surface warms, and re-radiates in a completely different
thermal spectrum that depends on the surface temperature and its spectral
emissivity.
If we talk about
thermal modeling it might be the
emissivity of the surface for example.
You get the real GHE from correct radiation physics, which is that
thermal IR from the lower atmosphere blocks surface IR emission in GHG band centres, reducing total
emissivity.
If you want more detail, here are some «standard equations» that specifically deal with
thermal radiation from one object of arbitrary size, shape,
emissivity, and temperature to a second object of arbitrary size, shape,
emissivity, and temperature:
As I understand it Kirchoff's Law states αλ = ελ, but only at
thermal equilibrium and does not require that the absorbtivity and
emissivity of the surroundings be the same as that of the emitting object, otherwise what you are suggesting is that everything has the same absortivity and
emissivity and αλ = ελ = a constant.
As early as 1859, Gustav Kirchhoff proposed that «At
thermal equilibrium, the
emissivity of a body (or surface) equals its absorptivity» and as far as I can understand, nobody objected and his proposition was accepted as part of «Kirchhoff's Law», and, to me, it seems logical and should be unavoidable as it is based on «energy conservation».
There is nothing in the phase transition from solid ice, or liquid water, to H2O vapor by sublimation or evaporation; that suddenly turns off the ability of those molecules to emit a BB like
thermal continuum radiation spectrum according to Planck formula and other applicable laws (don't forget the
emissivity).
But the same slab of silicon can readily radiate a continuous
thermal spectrum, that depends only on the Temperature of the material, and generally follows the Planck formula, with perhaps some spectral
emissivity function.
At
thermal equilibrium, the
emissivity of a body (or surface) equals its absorptivity.
And «
thermal radiation» is produced within an envelope that is the Planckian Black Body Spectral distribution; modified by some spectral
emissivity, that may be very much less than 1.0 specially for gases (any gases, including monoatomic, homo - diatomic molecules, or even GHG molecules.
For the most energy - efficient glass, look at low
emissivity thermal glass options.