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Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

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Page 1: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Unit 3 Presentation 1July 10, 2015

Solar radiationEnergyGlobal radiation balance Sun in local sky

Page 2: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

SOLAR RADIATION

The Earth intercepts 1.5 quadrillion megawatt-hours per year or 28,000 times the power consumed by the entire population of the planet each year.

Page 3: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Strahler & Strahler 2003

i.e., low frequencies

i.e., high frequencies

Shortwave vs. longwave radiation

Ruddiman 2001

Page 4: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

• Important principles regarding emission of electromagnetic radiation.

(1) There is an inverse relationship between wavelength l and the temperature T of the object emitting it (e.g. the Sun emits very short wavelength energy because it is so hot).

Planck’s Law: E = (2c2h /) e[hc/kT - 1]

where the speed of light c = 3x108 m/s, Boltzmann's constant k = 1.38 x 10-23 J/oK, and Planck's constant h = 6.64 x 10-34 J s.

Radiation and Temperature

NOTE: l is reported in length units: mm = 10-6 m (micrometers) nm = 10-9 m (nanometers) Å = 10-10 m (Ångstroms)

Page 5: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

• Important principles regarding emission of electromagnetic radiation.

(2) Integrating E over all wavelengths gives the total energy flux emanating from the surface of the radiating body: Stefan’s Law: E = T4

where = emissivity of the radiator (= 1 for a blackbody radiator), s = the Stefan-Boltzmann constant (= 5.673 x 10-8 W/(m2 oK4)), and T is the absolute temperature of the radiator's surface in oK.

(3) The Wien Displacement Law explains wavelength shift of peak E with change in T:

max = b/T

With b=2.8977685×10−3m ºK (Wien displacement constant) and T in oK.

Radiation and Temperature

used in all Earth systemand climate models

Page 6: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Shortwave Radiation• Ultraviolet

– short wavelength (0.2 to 0.4 micrometers), high energy. Does not penetrate atmosphere easily.

• Visible light– shorter wavelengths are perceived as violet, longer wavelengths as

red (0.4 to 0.7 micrometers); penetrates atmosphere easily.• Near-infrared radiation

– in the wavelengths from 0.7 to 1.2 micrometers.• Shortwave infrared radiation

– wavelengths from 1.2 to 3 micrometers, invisible to the eye. Penetrates atmosphere easily.

THE SUN

~0.5 mm

E = 2c2h / e[hc/kT - 1]

withT=5800 oK

Page 7: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Longwave radiation

• Thermal infrared radiation– Wavelengths greater than 3 micrometers– This form of radiation is emitted by cooler bodies. – It is perceived as heat.

THE EARTH

~10 mm

E = 2c2h / e[hc/kT - 1]

withT=288oK

Page 8: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Wavelengths of Sun and Earth Radiation

• Earth Energy– Earth’s output peaks

in the thermal infrared

portion of the electro-

magnetic spectrum

Strahler & Strahler 2003

• Solar Energy – Sun’s output peaks

in the visible light

portion of the electro-

magnetic spectrum.

Page 9: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Effects of solar radiation on the ecosystem:

Page 10: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky
Page 11: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

The Sun's surface has an energy flux density of 70 x 106 W/m2. (Note: W/m2 = J/s m2, where J = kg m2/s2). As this radiates out into space, the density diminishes as a function of distance2; by the time it reaches the Earth the density is only on the order of 1370 W/m2.

Path of Radiation from Sun to Earth (or other planet)

Page 12: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

From Ruddiman 2001

At top-of-atmosphere (TOA),solar radiation is I=1368 W/m2.

I affects an area equivalent toa disk of dimension pr2.

Averaging I over a 24-hourperiod gives pr2I/4pr2=I/4=342 W/m2.

Incoming solar radiation on Earth

2

2

Page 13: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

The Global Radiation Balance• The Sun transmits shortwave radiation into space where it is intercepted byEarth.

• The absorbed radiation is ultimately emitted by Earth as longwave radiation to space

Page 14: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

TEarth = ( (1- ) 343 W m-2 / 5.67 x 10-8 W m-2 K-4)1/4

= 279 K (+6 ºC)

Earth blackbody radiator model

But we know Tearth = 288K!

TEarth = ( ( 0.7) 343 W m-2 / 5.67 x 10-8 W m-2 K-4)1/4

= 255 K (-18 ºC)

No albedo (=0):

With albedo ( =0.3):

Input = output

(1-)E=T4

T=[(1-) E/()]1/4 , where =1

Page 15: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

TBR = +6ºC

TBR = -47ºC

TBR = +55ºC

Page 16: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

The Seasonal Cycle

Summer

Page 17: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Sun in the local sky

EquatorC

elestial Equator

Baltimore

Olin Hall

Page 18: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Northern Summer Solstice

At 40ºN solar altitude A=73.5º

At 40ºN sunrise in NE

At 40ºN sunset in NW

Note:Zenith angle z =90º-A

Page 19: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Path of the Sun in the sky at selected

latitudes for summer, winter

solstices and equinox

From Strahler & Strahler 2003

Note: “8” = “ º ”

Page 20: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

EARTH ALBEDO

Albedo (Latin for “white”) is the average reflection coefficient of an object (1=white; 0=black). “Bond albedo” is the total radiation reflected from an object compared to the total incident radiation from the Sun. “Geometric albedo” is the amount of radiation relative to that of a flat Lambertian surface which is an ideal reflector at all wavelengths.

De Pater & Lissauer 2010

Page 21: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Trees and grasses

Page 22: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Rocks and Soils

Page 23: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

Water and Snow

Page 24: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

http://www-surf.larc.nasa.gov/surf/pages/bbalb.html

Broadband Albedo (Oct. 1986)

Page 25: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

http://snowdog.larc.nasa.gov/surf/pages/lat_lon.html

Baltimore MD Oct. 1986

Page 26: Unit 3 Presentation 1 July 10, 2015 Solar radiation Energy Global radiation balance Sun in local sky

END OF PRESENTATION