black body radiation physics 113 goderya chapter(s): 7 learning outcomes:

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Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

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Page 1: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Black Body RadiationPhysics 113 Goderya

Chapter(s): 7Learning Outcomes:

Page 2: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

The Amazing Power of Starlight

Just by analyzing the light received from a star, astronomers can retrieve information about a star’s

1. Total energy output

2. Mass

3. Surface temperature

4. Radius

5. Chemical composition

6. Velocity relative to Earth

7. Rotation period

Page 3: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Temperature Scales

• o F = 9/5(o K) -459.4

• o F = 9/5(o C) + 32

• o K = 273 + o C

o Co K o F

0 32273

100 212373

-100173 -148

Page 4: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Brightness and Luminosity

• Luminosity (L): The total amount of energy a star radiates in 1 second per square meter.

• Brightness (B): Energy received from the source at different distances.

• Inverse square Law:B ≈ 1/(distance)2

• B = L / 4πR2

• Sun 5 x 1026 watts

4 /12 = 4

4 / 22 = 1

Light rays

Page 5: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Star as a Black Body

• Black Body Radiator. A hypothetical object that emits Electromagnetic radiation and whose spectrum is continuous with a peak in the wavelength that corresponds to the temperature of the object.

Wavelength

Ene

rgy

Peak wavelength

Page 6: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Black Body Radiation (1)The light from a star is usually concentrated in a rather narrow range of wavelengths.

The spectrum of a star’s light is approximately a thermal spectrum called a black body spectrum.

A perfect black body emitter would not reflect any radiation. Thus the name “black body”.

Page 7: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Two Laws of Black Body Radiation

2. The peak of the black body spectrum shifts towards shorter wavelengths when the temperature increases. Wien’s displacement law:

max ≈ 3,000,000 nm / TK

(where TK is the temperature in Kelvin).

1. The hotter an object is, the more luminous it is:

L = A**T4

where = Stefan-Boltzmann constant A = surface area;

Page 8: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Sun’s Temperature• The sun =500

nm

• T = 3 x 10 6/500 = 6000 K

• 10,000 F

• Wein’s Law gives the surface temperature

Page 9: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Sun’s Luminosity• The sun: T=

6000 K , R=7 x 108 meters. What is its Luminosity?

• L = 4x 3.14 x (7 x 10 8)2 x 6 x 10-8 (6000)4 = 5 x 1026 Watts

• Compare with 40 watts light bulb

Page 10: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

Color and Temperature

Orion

Betelgeuse

Rigel

Stars appear in different colors,

from blue (like Rigel)

via green / yellow (like our sun)

to red (like Betelgeuse).

These colors tell us about the star’s

temperature.

Page 11: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

The Color Index (1)

B bandV band

The color of a star is measured by comparing its brightness in two different wavelength bands:

The blue (B) band and the visual (V) band.

We define B-band and V-band magnitudes just as we did before for total magnitudes (remember: a larger number indicates a fainter star).

Page 12: Black Body Radiation Physics 113 Goderya Chapter(s): 7 Learning Outcomes:

The Color Index (2)

We define the Color Index

B – V(i.e., B magnitude – V magnitude).

The bluer a star appears, the smaller the color index B – V.

The hotter a star is, the smaller its color index B – V.