Lecture 2: Thermal Radiation- Nailing the Planck Curve
"It isn't the heat, its the humidity."
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Date:
January 26, 1995
Reading Assignment: pp.
62-78
Description :
overview of the EM spectra, thermal radiation, and the Doppler shift
Objectives
Lecture Outline
Slide # 1: Thermal Radiation
Slide # 2: The Universe- A Quick Inventory
Slide # 3: The Universe - composition
Slide # 4: The Universe - size and age
Slide # 5: TodayÕs Lecture Objectives
Slide # 6: Visible Light (GRAPHICS)
Slide # 7: Cycles of Space and Time (GRAPHICS)
Slide # 8: Cycles of Space and Time (GRAPHICS)
Slide # 9: Wavelengths of Visible Light
Slide # 10: Red Light vs Blue Light
Red has a longer wavelength
Red has a lower frequency
Remember: Longer wavelengths = lower frequencies
Slide # 11: Electromagnetic Waves
wavelengths > 7 x 10-5 cm are invisible to humans
wavelengths < 4 x 10-5 cm are invisible to humans
longer and shorter wavelengths are also electromagnetic radiation
Slide # 12: The Electromagnetic Spectrum
Radio
Infrared
Visible
Ultraviolet
X-ray
Gamma-ray
Slide # 13: Radio
Wavelengths > 1 mm
Frequencies 0 to 300 Giga-Hz (3x1011Hz)
Typical Examples
AM/FM Radios
TV signals
Slide # 14: Infrared
Wavelengths between 1mm and 7 x 10-5 cm
Frequencies between 3 x 1011 Hz and 4 x 1014 Hz
Typical Examples
Heating devices
stove burners
space heaters
TV remote controls
Slide # 15: Visible
Wavelengths between 7 x 10-5 cm and 3 x 10-5 cm
Frequencies between 4 x 1014 Hz and 1 x 1015 Hz
Typical Examples
All that you see
Slide # 16: Ultraviolet
Wavelengths between 3 x 10-5 cm and 3 x 10-7 cm
Frequencies between 1 x 1015 Hz and 1 x 1017 Hz
Typical Examples
Sunlight which causes sunburn and suntan
Slide # 17: X-rays
Wavelength between 3 x 10-7 cm and 3 x 10-10 cm
Frequencies between 1 x 1017 Hz and 1 x 1020 Hz
Typical Example
Medical X-ray Machines
Slide # 18: Gamma-Rays
Wavelengths < than 3 x 10-10 cm
Frequencies > 1 x 1020 Hz
Typical Examples
Nuclear reactions
Nuclear bombs
Slide # 19: Atmospheric Blockage
some wavelengths are blocked by the atmosphere
Slide # 20: Opacity
the extent which a wavelength is blocked
opaque is the opposite of transparent
Slide # 21: Atmospheric Opacity- Why does it happen?
gases absorb and scatter light
the amount of absorption depends on
the type of molecule
the wavelength of light
Slide # 22: Atmospheric Opacity - Some Examples
Water and Oxygen absorb some radio frequencies
Carbon Dioxide absorbs some infrared frequencies
the Ozone layer blocks most Ultraviolet, X-ray and Gamma-rays
Slide # 23: Constellation Corner (GRAPHICS)
The Constellation de Jour
Slide # 24: Ursa Minor (GRAPHICS)
Fairfax - Feb 1 - 10pm - NNE - 6.0
Slide # 25: Ursa Minor (GRAPHICS)
Fairfax - Feb 1 - 10pm - NNE - 6.0
Slide # 26: Ursa Minor (GRAPHICS)
Fairfax - Feb 1 - 10pm - NNE - 5.0
Slide # 27: Ursa Minor (GRAPHICS)
Fairfax - Feb 1 - 10pm - NNE - 4.0
Slide # 28: Ursa Minor (GRAPHICS)
Fairfax - Feb 1 - 10pm - NE
Slide # 29: Intensity
the strength of radiation
how bright something appears
proportional to number of photons per second per unit area seen by an observer
Slide # 30: Temperature
a measure of an objectÕs heat
Kelvin scale = Celsius Scale + 273
Nothing is below zero Kelvin
Slide # 31: Thermal Radiation
Intensity is only related to temperature
Independent of the type of material
Slide # 32: Thermal Radiation Spectra
The Planck Curve is one type of spectra
curve of a perfect thermal emitter
Also known as the Ōblack-body curveĶ
Slide # 33: A Planck Curve (GRAPHICS)
the signature of thermal emission
Slide # 34: The Planck Curve (GRAPHICS)
The Shape of the Curve is Independent of
Temperature
Composition
Slide # 35: The Planck Curve (GRAPHICS)
The position of the peak and the area under the curve depend on Temperature
Slide # 36: The Planck Curve
Two laws describe the Planck Curve
WienÕs Law
StephanÕs Law
Slide # 37: WienÕs Law (GRAPHICS)
Describes the wavelength of the Peak of the Planck Curve
Slide # 38: WienÕs Law
Peak Wavelength in cm
T in Kelvin
Slide # 39: WienÕs Law (GRAPHICS)
changing temperature changes the peak wavelength
Slide # 40: WienÕs Law
If you can measure the Peak Wavelength, you can determine the Temperature
The peak wavelength is determined using spectroscopy
Slide # 41: StephanÕs Law
Describes the flux from a black-body
Flux is the
amount of energy
per second
per square centimeter
A measure of how bright a Surface appears
Slide # 42: StephanÕs Law (GRAPHICS)
energy radiated depends on the fourth power of Temperature
Slide # 43: StephanÕs Law (GRAPHICS)
sigma is
Stephan-Boltzmann constant
5.67 x 10-5 erg/s/cm2/K4
Slide # 44: StephanÕs Law (GRAPHICS)
Slide # 45: Applications of the Planck Curve
The Sun is approximately a black-body
temperature is about 6000K
Planets emit most of their infrared energy as black-bodies
peak of the spectrum tells us the planetÕs average temperature
Slide # 46: Planck Curves
one way to tell the temperature and flux of distant objects
Slide # 47: Units Review
Hertz (Hz) = cycles per second
Angstroms = 10-10 meters = 10-8 cm
Ergs - unit of energy
very small unit
100 watt light bulb = 109 erg/second
Slide # 48: Thermal Radiation vs Photoelectric Effect
StephanÕs and WienÕs laws are for thermal radiators
the Photoelectric effect applies to individual photons
Slide # 49: The Photoelectric Effect
Blue Light
wavelength = 4000 Angstroms
frequency = 7.5 x 1011 Hz
Energy/photon =5.0 x 10-15 ergs
Red Light
wavelength = 7000 Angstroms
frequency = 4.3 x 1011 Hz
Energy/photon = 2.8 x 10-15 ergs
Slide # 50: PlanckÕs Constant - h
6.63 x 10-27 erg seconds
relates frequency in Hz to energy in ergs
only applies to individual photons
Slide # 51: Photoelectric Effect
Discovered by Albert Einstein
Einstein receive Nobel Prize for this work (1921)