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Transcript
Planck Curves
Every hot body has its unique distribution of energy which determines the colour that the glowing object appears.
STAR
TEMPERATURE (K)
COLOUR
Betelgeuse
Capella
Sun
Sirius
Rigel
3,000
6,000
6,000
12,000
18,000
Red/Orange
Yellow/White
Yellow/White
White
Blue/White
ENERGY/J
The Planck radiation law assumes that the object
observed is a perfect radiator and absorber of
energy (black body).
Stars, although not perfect black bodies, are close
enough so that Planck curves are useful
descriptions of their radiation.
Short
WAVELENGTH
Long
A. Wien’s Law
This law can be derived from Planck's Law. It states that the radiation peak on the Planck curve varies inversely with the
temperature, so red stars are relatively cool, but blue stars (shorter  are hot.
π‘€π‘Žπ‘₯π‘–π‘šπ‘’π‘š π‘ƒπ‘’π‘Žπ‘˜ π‘Šπ‘Žπ‘£π‘’π‘™π‘’π‘›π‘”π‘‘β„Ž =
or
π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘
𝑇
πœ†π‘šπ‘Žπ‘₯ 𝑇 = π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘ = 2.9 π‘₯10βˆ’3 𝐾 π‘š
B.
Stefan-Boltzmann Law
This law can also be derived from Planck's law, and it states that the total power (luminosity) from a radiating object (like a star)
at all wavelengths is directly proportional to the fourth power of kelvin temperature. Therefore, a small change in temperature
results in a large change in the energy output per second. As previously discussed a doubling of temperature results in a 16 fold
increase in luminosity (are under the E graphs.
𝐿 = πœŽπ΄π‘‡ 4 = 4πœ‹πœŽπ‘…2 𝑇 4 π‘€β„Žπ‘’π‘Ÿπ‘’ 𝑅 𝑖𝑠 π‘‘β„Žπ‘’ π‘Ÿπ‘Žπ‘‘π‘–π‘’π‘  π‘œπ‘“ π‘‘β„Žπ‘’ π‘ π‘‘π‘Žπ‘Ÿ
2. Inverse square law for Brightness
The apparent brightness of a light source varies inversely with the square of the distance.
π΅π‘Ÿπ‘–π‘”β„Žπ‘‘π‘›π‘’π‘ π‘  𝑏 ο‚΅
1
𝑑2
If the distance is doubled, the brightness of the object (star) decreases by four times.