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Astonomy 62 Lecture #9
Liouville's TheoremBlackbody Radiation
Plank FunctionWien's Displacement LawStefan-Boltzmann Law
Plank Function
I T=B T =2 hc2/ 5
eh c/ kT −1
I T =B T =2 h 3 / c2
eh / kT−1
Stefan-Boltzmann Law
L=4 R2T 4
Wien's Displacement Law
peak=0.29 cm
T
Astonomy 62 Lecture #9
Applications of Stefan-Boltzmann LawColor MagnitudeColor Index
Reading for today: 3.6
Reading for next lecture: 5.1-5.4
Topics for TodayTopics for TodayAstonomy 62 Lecture #9
Problem: Problem: Estimate the effective temperature of the Solar surface if L = 3.8x10
26 J/s R = 7.0x10
8 m
Astonomy 62 Lecture #9
T = 5740 KT = 5740 K
Astonomy 62 Lecture #9
Sirius B:Sirius B:T = 27,000 KT = 27,000 KR = 5400 kmR = 5400 km
Earth:Earth:RR++ == 6400 km 6400 km
A
B
Sirius B
Earth
Problem: Sirius BProblem: Sirius BEstimate the radius of Sirius B if its luminosity is L = 0.03 L = 1.1 x 1025 J/s and its spectrum peaks at 107nm.
Astonomy 62 Lecture #9
T c=T∗ R∗
Rc=260 K
Problem: Embedded Star Problem: Embedded Star A young star with surface temperature T* = 10,000K
and radius R* = 1010m is hidden inside a completely
opaque cloud of radius Rc = 100AU. What is the equilibrium temperature of the cloud?
Albedo = percentage of incident radiation Albedo = percentage of incident radiation that is refected. that is refected.
Kirchhoff's RuleKirchhoff's Rule
Good absorbers (low albedo) are also good emitters and vice versa.
Astonomy 62 Lecture #9
Color Magnitudes
Color Magnitude is measured the same way as a regular (bolometric) magnitude, but through a flter which restricts photon detection to a certain wavelength range.
Astonomy 62 Lecture #9
U B V R I � x(A) 3650 4400 5500 7000 9000
Wx(A) 680 980 890 2200 2400
1 Å=0.1nm=10−10 m
Fx=∫0
∞F Sx d
F x≃F xW x
mx ,1−m x ,2=2.5 logFx ,2F x ,1
mx ,1−mx ,2≃2.5 logF , 2 x
F ,1 x
Flux through filter X:
Apparent Color Magnitude:
T
From C&O (Fig. 3.10)
Astonomy 62 Lecture #9
Color–Color Diagram for Normal Stars Color–Color Diagram for Normal Stars