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Summary Chapter 2

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Summary of Chapter 2 of FW Taylor's Elementary Climate Physics book

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  • H2
  • September 19, 2017
  • 3
  • 2017/2018
  • Summary
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H2 Solar radiation and the energy budget of the Earth
2.1 Sun and climate
 99,97% of the energy arrives from the Sun in the form of electromagnetic radiation
 The remainder are negligible for most purposes:
o Interior of the Earth
o Space: energetic particles
o Cosmic rays
o Human power production: fossil and radioactive fuels
 The Sun does behave like a hot, solid sphere emitting radiation at a constant
temperature of about 6000K (5780K precise)
 Sun is a ball of hot, ionized gas or plasma
 The radiation it emits into space originates from different depths in the outermost
layers, which are at different temperatures

2.2 Solar physics
 The Sun is a star of the spectral class G2 on the main sequence of the Hertzsprung-Russel
diagram: it is a scatter plot of stars showing the relationship between the stars’ absolute
magnitudes or luminosities versus their stellar classifications or effective temperatures.
Simple: it plots each star on a graph measuring the star’s brightness against its
temperature (color).
 The Sun is larger than the average star; top 10%
 Radius: 696000 km (100X radius of Earth)
 Mass: 2x1030kg
 Density at centreL 160000 kg m-3
 Consist mostly of hydrogen (91.2%) en helium (8.7%)
 4.5 billion years old  middle aged
 Most mass concentrated in core; T: 15000000K pressure: 10 Mbar
 Rotates with a 25-day period at the solar equator, slowing around 35 days near the poles
 Photosphere: visible surface
 Sunspots: lower T of 4000K; the number fluctuates randomly

2.3 Source of the Sun’s energy
 Gravitational collapse: last stadium of a star, if everything is fused to iron, the inherent
gravity is greater than the force outward  implode

2.4 The radiation laws
 Planck’s radiation law: describes the radiant energy (radiance) emitted from a perfectly
black object as a function of wavelength for a given temperature
 A ‘black’ object: perfect absorber with zero reflectivity
2ℎ𝑐 2 1
 𝑅(𝜆, 𝑇) = 𝜆5 ℎ𝑐 W-3 sr-1
𝑒 𝜆𝑘𝑇 −1
 Radiance is the amount of energy per unit time, per unit area, per unit spectral interval,
and per unit solid angle, passing through a point.
 Stefan-Boltzmann law: total power leaving as radiation at all wavelengths from unit area
of a surface at temperature T
 𝐹 = 𝜎 𝑇 4 𝑊𝑚−2
 𝜎 = 𝑆𝑡𝑒𝑓𝑎𝑛′ 𝑠 𝑐𝑜𝑛𝑠𝑡𝑎𝑛𝑡
 Wiens law: wavelength of the maximum rate of emission at a given temperature
2897
 𝜆𝑚𝑎𝑥 = 𝑇 𝜇𝑚

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