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Solar Radiation Emission and Absorption V1003 - Climate and Society

Solar Radiation Emission and Absorption

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Solar Radiation Emission and Absorption . V1003 - Climate and Society. Take away concepts. Conservation of energy. Black body radiation principle Emission wavelength and temperature (Wein’s Law). Radiation vs. distance relation Black body energy flux (Stefan-Boltzmann Law) - PowerPoint PPT Presentation

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Page 1: Solar Radiation Emission and Absorption

Solar Radiation Emission and Absorption

V1003 - Climate and Society

Page 2: Solar Radiation Emission and Absorption

Take away concepts

1. Conservation of energy. 2. Black body radiation principle3. Emission wavelength and temperature (Wein’s Law). 4. Radiation vs. distance relation 5. Black body energy flux (Stefan-Boltzmann Law) 6. Effective temperature calculation, differences from

actual temperature.

Page 3: Solar Radiation Emission and Absorption

What is Energy?

Energy: “The ability to do work”.Energy measured in Joules (1 J = 0.24

calories). Power measured in Watts (1 J/s)

Energy is always conserved (1st law of TD). Energy can be changed from one form to

another, but it cannot be created or destroyed.

Page 4: Solar Radiation Emission and Absorption

Solar Energy

Nuclear fusion: H to HeEmits Electromagnetic

radiation (radiant E)

EM waves behave like particles and waves

EM travels at c (3 x 108 m/s)

Page 5: Solar Radiation Emission and Absorption

EM Radiation

Since c is constant, frequency of EM wave emission related to electron vibrationWarm things have more energy than cold things, so ….?

Page 6: Solar Radiation Emission and Absorption

Properties of waves

Amplitude (A)Wavelength (µm)Period (sec)Frequency (1/sec)

c is constant

Page 7: Solar Radiation Emission and Absorption

Blackbody Radiation

A “blackbody” absorbs and emits radiation at 100% efficiency (experimentally, they use graphite, or carbon nanotubes)

energy in = energy out

Across all wavelengths

Page 8: Solar Radiation Emission and Absorption

Wein’s Law emission wavelength and temperature

max = a / T

Where:

max is wavelength of emitted

radiation (in µm) a = 2898, constant

T emitter temperature (in K)

Recall that K = T°C + 273.15

Sun’s temperature is 5800KWhat’s its wavelength?

Page 9: Solar Radiation Emission and Absorption

The Sun’s temperature is 5800 K, that is the wavelength of its radiation?

a. 5000 µmb. 50 µmc. 0.5 µmd. 2 µme. 20µm

max = a / T

max is wavelength of emitted

radiation (in µm) a = 2898, constant

T emitter temperature (in K)

Recall that K = T°C + 273.15

Page 10: Solar Radiation Emission and Absorption

What’s your wavelength?

max = a / T(a = 2898)

Your body is 37°Cor 37+273 = 310K

max = ?9.4 µm (far infrared)

Page 11: Solar Radiation Emission and Absorption

Earth as we see it (visible)

Page 12: Solar Radiation Emission and Absorption

Earth’s Infrared “Glow”: 15µm

Page 13: Solar Radiation Emission and Absorption

Electromagnetic spectrum

1 µm = 1000 nm

“hot” “cold”

0.5 µm

9 µm

Page 14: Solar Radiation Emission and Absorption

Visualizing emission temperatures

Blackbody applet: http://qsad.bu.edu/applets/blackbody/applet.html

Sunny day: 6000KSunset: 3200K Candlelight: 1500K

Page 15: Solar Radiation Emission and Absorption

The effect of distance on radiation “the 1 / r2 rule”

Sun emission decreases in proportion to 1 / r2 of the Sun-Planet distance

Page 16: Solar Radiation Emission and Absorption

Mars is 1.52 AU

(1 AU = earth-sun distance =

1.5 x 1011 m)

Using 1/ r2 rule…

1 / (1.5*1.5) = 0.44

Mars receives ~44% of the Earth’s solar radiation.

Page 17: Solar Radiation Emission and Absorption

Jupiter is roughly 5 AU from the Sun, what fraction of Earth’s solar radiation does it get?

a. 1/2b. 1/5 c. 1/10d. 1/25e. 1/125

Page 18: Solar Radiation Emission and Absorption

Summary so far…

Wein’s Law (emission freq. and temperature)

The “1 / r2” law (radiation amt and distance)

Now let’s calculate the total radiative energy flux into or out of a planet using the:

Stefan - Boltzmann Law

Page 19: Solar Radiation Emission and Absorption

Stefan - Boltzmann LawEnergy emitted by a black body is greatly

dependent on its temperature:

I = T4

Where:I = Black body energy radiation = (Constant) 5.67x10-8 Watts/m2/K4

T = temperature in Kelvin

= albedo (“reflectivity”)

Example: Sun surface is 5800K, so I = 6.4 x 107 W/m2

Page 20: Solar Radiation Emission and Absorption

Calculating the Earth’s “Effective Temperature”

Easy as 1-2-3…

1. Calculate solar output.2. Calculate solar energy reaching the Earth.3. Calculate the temperature the Earth should

be with this energy receipt.

Page 21: Solar Radiation Emission and Absorption

1. Calculate solar output.

Calculate Sun temperature assuming it behaves as a blackbody (knowing that sun= 0.5µm).

From S-B law: Isun = 6.4 x 10 7 W/m2

We need surface area of sun:Area = 4r2 = 4(6.96x108 m) = 6.2 x 10 18 m2

Total Sun emission: 3.86 x 1026 Watts (!)SolarEmissionPower

Page 22: Solar Radiation Emission and Absorption

2. Calculate solar energy reaching the Earth.

Simple Geometry.(recall the inverse square law..)

Earth-Sun distance (D): 1.5 x 1011 mArea of sphere = 4 r 2

So, 3.86 x 10 26 Watts / (4 (1.5 x 1011 m)2 )

Earth’s incoming solar radiation: 1365 W/m2

Page 23: Solar Radiation Emission and Absorption

3. Earth energy in = energy out

You have Iearth, solve for Tearth

Stefan - Boltzmann law: Iearth = (1-) Tearth4

Incoming solar radiation: 1365 W/m2

About 30% is reflected away by ice, clouds, etc.: reduced to 955 W/m2

Incoming on dayside only (DISK), but outgoing everywhere (SPHERE), so outgoing is 1/4 of incoming, or 239 W/m2

that is: (0.7)*(0.25)*1365 = energy that reaches Earth surface

Energy in = 239 W/m2 = T4

Page 24: Solar Radiation Emission and Absorption

Solve for Teffective = 255K

Earth Effective temp: 255 K, or -18°CEarth Actual temp: 288K, or +15°C

… the difference of +33°C is due to the natural greenhouse effect.

Page 25: Solar Radiation Emission and Absorption

So what Earth’s radiation wavelength?

max = a / T

Where:

max is wavelength of emitted

radiation (in µm) a = 2898, constant

T emitter temperature (in K)

If Earth effective temperature is 255KWhat’s the wavelength?

Page 26: Solar Radiation Emission and Absorption

Emission Spectra: Sun and Earth

0.5 µm 15 µm9 µm

Page 27: Solar Radiation Emission and Absorption

Radiation and Matter

Also dependent upon the frequency of radiation! (next lecture)

Page 28: Solar Radiation Emission and Absorption

Emission Spectra: Sun and Earth

Page 29: Solar Radiation Emission and Absorption

Blackbody emission curves and absorption bands

Page 30: Solar Radiation Emission and Absorption

Why is the Sky blue?Rayleigh scattering of incoming,

short wavelength radiation (photons with specific energy)

Radiation scattered by O3, O2 in stratosphere (10-50 km)

Page 31: Solar Radiation Emission and Absorption

Why are sunsets red?

Blue wavelengths are scattered/absorbed

Red and orange pass through to surface