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CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

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Page 1: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

CE 401Climate Change Science and Engineering

solar input, mean energy budget, orbital variations, radiative forcing

17-19 January 2012

Page 2: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

any questions from last time?

we did the entire science section of 401 in a flash

Page 3: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

homework 3 [Stefan-Boltzmann] on website: due Tuesday 24 January 2012• read MacKay Chapter 2• do some computations

HW 2 [Mauna Loa data] due on Thursday, 19 January = next class period

Page 4: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012
Page 5: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

what causes natural variations in the climate system

Page 6: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

natural variations in Earth energy balance are caused by (at least):

• changes in the radiation balance of the Earth-Sun system• intrinsic changes in solar flux

• long term - must be modeled using sunspot numbers• solar cycle - only two cycles measured + 0.05%

• changes in Earth orbital parameters - Milankovitch cycles• periods of 20k - 100k years• explain all the major ice ages – dramatic changes in temperature

• changing aerosol concentrations (e.g. volcanic activity)

Page 7: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

the solar energy input to the Earth system

Page 8: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

1000 nm = 1 µm

Page 9: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

solar and earth spectra

1000 nm = 1 µm

Page 10: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

1000 nm = 1 µm

Page 11: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

why would solar energy output vary?

Page 12: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

the sun is a dynamicobject

Page 13: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

Sun radiation varies in output on an 11 yr and 22 yr cycle, but also over longerperiods that are not understood

number of sunspots vs time

Page 14: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

satellite measurements of solar brightness

0.1% variation

individual instruments vary in calibration – so bring them to a normalization, usually 1368 w/m2

Page 15: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

Stefan-Boltzmann law:

Let S = rate at which the Sun produces energy as measured at the Earth’s orbital distance = solar constant = 1368 w m-2

then

rate at which solar energy strikes the Earth = S R2 (watts)

where R is the radius of the Earth (6370 km)

energy reflected back into space by Earth = S R2

where is the Earth’s average albedo (reflectivity) ~ 0.31 on average

energy absorbed by Earth system = SR2 (1-)

Page 16: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

the Earth cannot get rid of energy by conduction or convection to space, so must radiate its energy to space thermally

energy radiated to space is = 4R2 Te4 [the Stefan-Boltzmann law]

where

= Stefan-Boltzmann constant = 5.67 x 10-8 [w m-2 K-4]

Earth in equilibrium (temp not changing with time), rate of absorption = rate of emission

S R2 (1-) = 4R2 Te4

solving for Te using = 0.31 gives

Te = 255K = -18°C

this is the equilibrium temperature of the Earth in the absence of the atmosphere and it is much lower than observed

Page 17: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

distributed over the entire surface of the Earth, average incoming solar radiation is:

[incoming solar/surface area of Earth] = S R2 /4R2 = 1368/4 = 342 w m-2

since albedo is 0.31, amount of incoming radiation reflected back to spaceis:

[solar energy reflected/surface area of Earth] = S R2 / 4R2 = 107 w m-2

absorbed energy:

[solar energy absorbed/surface area of Earth] = S R2 (1-) / 4R2 = 235 w m-2

Page 18: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

global energy balance – bold numbers are W/m2

Page 19: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

no atmosphere Te = 255K = -18°C

Earth radiates 235 w m-2 at this temperature and this radiation is in theinfrared spectral region where many atmosphere gases absorb radiation

Thus, energy balance is NOT achieved at -18°C, and the Earth temp must increase to get rid of the energy and achieve a balanced equilibrium

Measured average Earth temperature is 288K = +15°C. Using Stefan-Boltzmann, we compute the radiated energy is Te

4 = 390 w m-2

of the 390 w m-2 , only 40 passes directly through (gases do not absorb ALL radiation) 350 w m-2 is absorbed by atmospheric gases, and 324 w m-2 is radiated back to the surface

Page 20: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

checks on our numbers: rate of gain = rate of loss

at Earth surface: 168 + 324 + 30 = 78 + 24 + 30 + 390 OK

Atmosphere: 67 + 78 + 24 + 350 + 40 = 165 + 30 + 324 + 40 OK

Space: 107 + 165 + 30 + 40 = 342 OK

Page 21: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

Earth ~33°C (60°F) warmer than without GHG

Page 22: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

what physical parameters affect the ability of an atmospheric gas tobe a greenhouse gas?

see

http://www.ciesin.columbia.edu/docs/003-074/003-074.html

for GH effect: science and policy

Page 23: CE 401 Climate Change Science and Engineering solar input, mean energy budget, orbital variations, radiative forcing 17-19 January 2012

energy radiated to space is = 4R2 Te4 [the Stefan-Boltzmann law]

where = Stefan-Boltzmann constant = 5.67 x 10-8 [w m-2 K-4]

342 w m-2 is the average energy input to the Earth system

235 w m-2 is the average radiated energy from the Earth system, all radiated in the infrared part of the spectrum