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Blackbody Radiation

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Title: Blackbody Radiation


1
Blackbody Radiation
  • Astrophysics Lesson 9

2
Homework
  • None today, module exams?

3
Learning Objectives
  • Define the term blackbody.
  • Sketch and describe how shape of black body
    curves change as temperature is increased.
  • Use Wiens displacement law to estimate
    black-body temperature of sources.
  • Use Stefans law to estimate area needed for
    sources to have same power output as the sun.
  • Recap inverse square law, state assumptions in
    its application.

4
Definition of a Blackbody
  • A body that absorbs all wavelengths of
    electromagnetic radiation and can emit all
    wavelengths of electromagnetic radiation.

Pure black surfaces emit radiation strongly and
in a well-defined way this is called blackbody
radiation. It is a reasonable approximation to
assume that stars behave as black bodies.
5
Black Body Radiation
  • The blackbody radiation of stars produces a
    continuous spectrum.
  • A graph of intensity against wavelength for black
    body radiation is known as a black body curve.
  • The blackbody curve is dependent on the
    temperature.

6
Black Body Curve Shape
7
Note the following for black bodies
  • a hot object emits radiation across a wide range
    of wavelength
  • As the temperature of the object increases-
  • peak of the graph moves towards the shorter
    wavelengths.
  • the peak is higher
  • the area under the graph is the total energy
    radiated per unit time per unit surface area.

8
Wiens Displacement Law
  • The peak wavelength, ?max, is the wavelength at
    which maximum energy is radiated. 
  • This is inversely proportional to the
    temperature, T, in Kelvin.
  • This is called Wien's  Displacement Law (as the
    peak is displaced towards shorter wavelengths)-
  •  
  • Note the units of mK means a metrekelvin.

9
Worked Example
  • What is the peak wavelength of a black body
    emitting radiation at 2000 K?  In what part of
    the electromagnetic spectrum does this lie?
  • ?max 0.0029 mK 2000 K
  • ? max 1.45 x 10-6 m 1450 nm
  • This is in the infra-red region.

10
Question
  • Betelgeuse appears to be red.  If red light has a
    wavelength of about 600 nm, what would the
    surface temperature be?
  • Why no green stars?

11
Answer
  • Betelgeuse appears to be red.  If red light has a
    wavelength of about 600 nm, what would the
    surface temperature be?
  • T 0.0029 mK 600 x 10-9 m 
  • T 4800 K
  • Why no green stars?

12
Why no green stars?
  • You don't get green stars because the light from
    stars is emitted at a range of wavelengths, so
    there is mixing of colours.  So those stars with
    a ?max in the green region will actually appear
    to be white.

13
Luminosity of Stars
  • The luminosity of a star is the total energy
    given out per second, so it's the power. 
  • From the graph the luminosity increases rapidly
    with temperature, which gives rise to Stefan's
    Law. 
  • The total energy per unit time radiated by a
    black body is proportional to the fourth power of
    its absolute temperature.
  •  

14
Stefans Law
  • In other words double the temperature and the
    power goes up sixteen times.  In symbols
  • L Luminosity of the star (W)
  • s Stefan's constant 5.67 x 10-8 W m-2 K-4
  • A surface area (m2)
  • T surface temperature (K)

15
Applied to Stars
  • We can treat a star as a perfect sphere (A
    4pr2) and a perfect black body.  So for any star,
    radius r, we can write
  •  

16
Inverse Square Law
  • From Earth we can measure the intensity of the
    star-
  • Where L is the luminosity of the star
  • d is the distance from the star

17
Question
  • If the Sun has a radius of 6.96 x 108 m and a
    surface temperature of about 6000 K, what is its
    total power output? 
  • What is the power per unit area? 
  • What is the peak wavelength?

18
Answer
  • L 4 p (6.96 x 108 m)2 5.67 10-8 W m-2
    K-4 x (6000 K)4
  • L 4.47 1026 W
  •  
  • The power per unit area 4.47 1026 W 6.09
    1018 m2 7.34 107  W/m2
  • Peak wavelength ?max 0.0029 mK 6000 K 4.82
    10-7 m 482 nm
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