lecture 12

60
Lecture 12 ASTR 111 – Section 002

Upload: rigel-mcclain

Post on 30-Dec-2015

12 views

Category:

Documents


0 download

DESCRIPTION

Lecture 12. ASTR 111 – Section 002. Measurements in Astronomy. In astronomy, we need to make remote and indirect measurements Think of an example of a remote and indirect measurement from everyday life. Using Light. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Lecture 12

Lecture 12

ASTR 111 – Section 002

Page 2: Lecture 12

Measurements in Astronomy

• In astronomy, we need to make remote and indirect measurements– Think of an example of a remote and indirect

measurement from everyday life

Page 3: Lecture 12

Using Light

• Light has many properties that we can use to learn about what happens far away

• Light interacts with matter in a special way

Page 4: Lecture 12

• Only photons with special wavelengths will interact with atom

• How will this affect what a person will see at point X?

• When is the atom “hotter”?

X

Page 5: Lecture 12

Why is UV light usually blamed for skin cancer? What is special about it compared to other light sources?

Page 6: Lecture 12
Page 7: Lecture 12

Cloudof

GasA prism bends photons more or less depending on their wavelength

Page 8: Lecture 12

Cloudof

GasA prism bends photons more or less depending on their wavelength

Page 9: Lecture 12

What will the spectrum look like here?

Page 10: Lecture 12

Emission line spectrum

Page 11: Lecture 12

Continuous Spectrum• A blackbody emits

photons with many energies (wavelengths) – a continuous spectrum

Page 12: Lecture 12

What will the spectrum look like here?

Page 13: Lecture 12

Absorption Spectrum

Page 14: Lecture 12

Absorption vs. Emission

Page 15: Lecture 12

• What type of spectrum is produced when the light emitted from a hot, dense object passes through a prism?

• What type of spectrum is produced when the light emitted directly from a cloud of gas passes through a prism?

• Describe the source of light and the path the light must take to produce an absorption spectrum

• There are dark lines in the absorption spectrum that represent missing light. What happened to this light that is missing in the absorption line spectrum?

From Lecture Tutorials for Introductory Astronomy, page 61.

Page 16: Lecture 12

Each chemical element produces its own unique set of spectral lines

Page 17: Lecture 12
Page 18: Lecture 12

• Stars like our Sun have low-density, gaseous atmospheres surrounding their hot, dense cores. If you were looking at the spectra of light coming from the Sun (or any star), which of the three types of spectra would be observed?

• If a star existed that was only a hot dense core and did not have a low-density atmosphere surrounding it, what type of spectrum would you expect this particular star to give off?

• Two students are looking at a brightly lit full Moon, illuminated by reflected light from the Sun. Consider the following discussion between two students about what the spectrum of moonlight would look like:– I think moonlight is just reflected sunlight, so we will see the Sun’s

absorption line spectrum.– I disagree, an absorption spectrum has to come from a hot, dense

object. Since thie Moon is not a hot, dense object, it can’t give off an absorption line spectrum.

Do you agree or disagree with either or both of these students? Explain your reasoning.

Page 19: Lecture 12

• Imagine that your are looking at two different spectra of the Sun. Spectrum #1 is obtained using a telescope that is in a high orbit far above Earth’s atmosphere. Spectrum #2 is obtained using a telescope located on the surface of Earth. Label each spectrum below as either Spectrum #1 or Spectrum #2.

Page 20: Lecture 12

Would this make sense?

This dark line was removed

Page 21: Lecture 12

Energy and electromagnetic radiation Planck’s law relates the

energy of a photon to its frequency or wavelength

E = energy of a photonh = Planck’s constantc = speed of light = wavelength of light

The value of the constant h in this equation, called Planck’s constant, has been shown in laboratory experiments to be

h = 6.625 x 10–34 J s

hc

E

Page 22: Lecture 12

• Which electromagnetic wave has a higher energy: one with f=10 cycles per second or f=1 cycles per second?

Page 23: Lecture 12

Three Temperature Scales

Page 24: Lecture 12

Color and Temperature

Page 25: Lecture 12

An opaque object emits electromagnetic radiationaccording to its temperature

Page 26: Lecture 12

http://www.straightdope.com/mailbag/mhotflame.html

Blue: Hot or Not?

Page 27: Lecture 12
Page 28: Lecture 12

Blackbody Definition• Does not reflect incoming radiation, only

absorbs• Emits radiation, depending on temperature• Temperature and emitted radiation

intensity follow a special relationship

Photon enters

If hole is very small, what is probability that it exits?

One way of creating a blackbody

Page 29: Lecture 12

Wien’s law and the Stefan-Boltzmann law are useful tools for analyzing

glowing objects like stars

• A blackbody is a hypothetical object that is a perfect absorber of electromagnetic radiation at all wavelengths

• Stars closely approximate the behavior of blackbodies, as do other hot, dense objects

Page 30: Lecture 12

• Blackbodies do not always appear black!

–The sun is close to being a “perfect” blackbody

–Blackbodies appear black only if their temperature very low

Page 31: Lecture 12

Special Relationship

Wavelength

Inte

nsity

For Intensity, think photons/second on a small area

Page 32: Lecture 12

Question

• Why is photon/second similar to energy/second? How are they related?

Page 33: Lecture 12

Watt? Energy Flux?

Page 34: Lecture 12

Flux

Flux is a measure of how much “stuff” crosses a small patch in a given amount of time. Can have flux of green photons, red photons, etc.

Page 35: Lecture 12

Blackbodies and Astronomy

Page 36: Lecture 12

Blackbody Laws• Stefan-Boltzmann Law – relates

energy output of a blackbody to its temperature

• Wein’s law – relates peak wavelength output by a blackbody to its temperature

Page 37: Lecture 12

Special Relationship

Wavelength

Ene

rgy

Flu

x In

tens

ity For Intensity, think photons/second on a small area

Page 38: Lecture 12

Stefan-Boltzmann Law

• A blackbody radiates electromagnetic waves with a total energy flux F directly proportional to the fourth power of the Kelvin temperature T of the object:

4~ TF

Page 39: Lecture 12

Special Relationship

Wavelength

Stefan-Boltzmann Law tells us that if we add up the energy from all wavelengths, then the total energy Flux

4~ TF

Ene

rgy

Flu

x In

tens

ity

Page 40: Lecture 12

Special Relationship

Wavelengthmax

Wien’s law tells us that max depends on temperature

Max intensity at max

T

1~max

Ene

rgy

Flu

x In

tens

ity

Page 41: Lecture 12

Special Relationship

Wavelength

Sketch this curve for larger and smaller T

Ene

rgy

Flu

x In

tens

ity

Page 42: Lecture 12
Page 43: Lecture 12

Overall amplitude increases with Temperature

At high wavelengths, intensity goes to zero

As wavelength goes to zero, intensity goes to zero

Wavelength of peak decreases as temperature increases

Page 44: Lecture 12

Color and Temperature

Page 45: Lecture 12

What would this object look like at these three temperatures?

Page 46: Lecture 12

Why does it glow white before blue?

Page 47: Lecture 12

• Can this figure help us explain?

Page 48: Lecture 12

• Can this figure help us explain?

Near this temperature, this special combination of intensities is what we call white. Also, the realcurve is a little flatter near the peak

Page 49: Lecture 12

The Sun does not emit radiation with intensities that exactly follow the blackbody curve

Page 50: Lecture 12

So, what color is the sun in space?

• http://casa.colorado.edu/~ajsh/colour/Tspectrum.html

Right side is (should be) alittle “pinker”

Left side is white

Page 51: Lecture 12

If blue light has higher energy, and energy is proportional to temperature, why are my cold spots blue?

Page 52: Lecture 12

AB

C

Ene

rgy

Flu

x

1

2

3

4

5

0

Page 53: Lecture 12

• Which curve represents an ideal blackbody?– Curve A– Curve B– Curve C

Page 54: Lecture 12

• If the object in Figure 1 were increased in temperature, what would happen to curves A, B, and C?

Page 55: Lecture 12

• Curve C is more jagged. The locations where the curve C is small correspond to– Spectral lines of a blackbody– Spectral lines of atmospheric molecules– Instrumentation error– Diffraction lines– Spectral lines of the lens used to the light into

colors

Page 56: Lecture 12

• What is the intensity of curve B at 550 nm?– Impossible to tell; 550 nm is not shown in this

figure– Nearest 0.2– Nearest 0.1– Nearest 0.05– Nearest 0.0

Page 57: Lecture 12

• Venus has no atmosphere. If you measure the spectrum from its surface, – Curves B and C would not change– Curve C would look more like A– Curve C would look more like B– Curve B would look more like A– Curve B would look more like C

Page 58: Lecture 12

• White light is composed of– Equal intensities of all colors of the rainbow– Unequal intensities of all colors of the rainbow– Equal number of photons of all colors of the

rainbow– Unequal number of photons of all colors of the

rainbow– Equal numbers of red, green, and blue

photons

Page 59: Lecture 12

• Does a blackbody have color?– Yes, and they all appear the color of the sun– No, you cannot see a blackbody– Yes, but its depends on its temperature– Maybe, it depends on if it is an ideal

blackbody

Page 60: Lecture 12

• Why is the best reason for putting a telescope in orbit? – Closer to stars– Better view of celestial sphere– The speed of light is higher in space– Less atmospheric interference– Cost