Light and Telescopes

1. 0 Light and Telescopes Chapter 6

2. 0 Guidepost • In the early chapters of this book, you looked at the sky the way ancient astronomers did, with the unaided eye. In this chapter, you will see how modern astronomers use telescopes and other instruments to gather and focus light and its related forms of radiation. That will lead you to answer five essential questions about the work of astronomers: • What is light? • How do telescopes work, and how are they limited? • How do astronomers record and analyze light? • Why do astronomers use radio telescopes? • Why must some telescopes go into space?

3. 0 Guidepost (continued) • Astronomy is almost entirely an observational science, so astronomers must think carefully about the limitations of their instruments. That will introduce you to an important question about scientific data: • How do we know?What limits the detail you can see in an image? • Fifteen chapters remain, and every one will discuss information gathered by telescopes.

4. 0 Outline I. Radiation(輻射): Information from Space A. Light as a Wave and a Particle B. The Electromagnetic Spectrum(電磁光譜) II. Optical Telescopes A. Two Kinds of Telescopes B. The Powers of a Telescope C. Buying a Telescope D. New-Generation Telescopes E. Interferometry(干涉儀) III. Special Instruments A. Imaging Systems B. The Spectrograph

5. 0 Outline (continued) IV. Radio Telescopes A. Operation of a Radio Telescope B. Limitations of the Radio Telescope C. Advantages of Radio Telescopes V. Astronomy from Space A. The Ends of the Visual Spectrum B. Telescopes in Space C. Cosmic Rays

6. 0 Light and Other Forms of Radiation • The Electromagnetic Spectrum In astronomy, we cannot perform experiments with our objects (stars, galaxies, …). The only way to investigate them, is by analyzing the light (and other radiation) which we observe from them.

7. 0 Light as a Wave (1) l c = 300,000 km/s = 3*108 m/s • Light waves are characterized by a wavelength l and a frequency f. f = c/l • f and l are related through

8. 0 Light as a Wave (2) • Wavelengths of light are measured in units of nanometers (nm) or Ångström (Å): 1 mm = 10-3 m 1 μm = 10-6 m 1 nm = 10-9 m 1 Å = 10-10 m = 0.1 nm Visible light has wavelengths between 4000 Å and 7000 Å (= 400 – 700 nm).

9. 0 Wavelengths and Colors Differentcolors of visible light correspond to different wavelengths.

10. 0 Light as Particles • Light can also appear as particles, called photons (explains, e.g., photoelectric effect). • A photon has a specific energy E, proportional to the frequency f: E = h*f h = 6.626x10-34 J*sis the Planck constant. The energy of a photon does notdepend on the intensity of the light!!! Intensity: 在單位時間 單位面積 單位角度 單位頻率 內 所接收(放出)的能量

11. 0 The Electromagnetic Spectrum Wavelength Frequency High flying air planes or satellites Need satellites to observe

12. 0 The Electromagnetic Spectrum

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14. 0 Optical Telescopes Astronomers use telescopes to gather more light from astronomical objects. The larger the telescope, the more light it gathers.

15. 0 Refracting/Reflecting Telescopes 折射式望遠鏡Refracting Telescope: Lens focuses light onto the focal plane Focal length 反射式望遠鏡Reflecting Telescope: Concave Mirror focuses light onto the focal plane Focal length Almost all modern telescopes are reflecting telescopes.

16. 0 Secondary Optics In reflecting telescopes: Secondary mirror, to re-direct the light path towards the back or side of the incoming light path. Eyepiece: To view and enlarge the small image produced in the focal plane of the primary optics.

17. 0 Disadvantages of Refracting Telescopes • Chromatic aberration(色差): Different wavelengths are focused at different focal lengths (prism effect). Can be corrected, but not eliminated by second lens out of different material • Difficult and expensive to produce: All surfaces must be perfectly shaped; glass must be flawless; lens can only be supported at the edges

18. 0 The Powers of a Telescope:Size Does Matter 1. Light-gathering power(or collecting power): Depends on the surface area A of the primary lens / mirror, proportional to diameter squared: D A = p (D/2)2

19. 0 The Powers of a Telescope (2) 2. Resolving power: Wave nature of light => The telescope aperture produces fringe rings that set a limit to the resolution of the telescope. Resolving power = minimum angular distance amin between two objects that can be separated. amin = 1.22 (l/D) amin For optical wavelengths, this gives amin = 11.6 arcsec / D[cm]

20. 0 Seeing Weather conditions and turbulence in the atmosphere set further limits to the quality of astronomical images. Bad seeing Good seeing

21. 0 The Powers of a Telescope (3) 3. Magnifying Power = ability of the telescope to make the image appear bigger. The magnification depends on the ratio of focal lengths of the primary mirror/lens (Fo) and the eyepiece (Fe): M = Fo/Fe A larger magnification does not improve the resolving power of the telescope!

22. 0 The Best Location for a Telescope Far away from civilization – to avoid light pollution

23. 0 The Best Location for a Telescope (2) Paranal Observatory (ESO), Chile On high mountain-tops – to avoid atmospheric turbulence (seeing) and other weather effects

24. 0 Traditional Telescopes (1) Secondary mirror Traditional primary mirror: sturdy, heavy to avoid distortions

25. 0 Traditional Telescopes (2) 4 m The 4-m Mayall Telescope at Kitt Peak National Observatory (Arizona)

26. 0 Advances in Modern Telescope Design (1) Modern computer technology has made significant advances in telescope design possible: Segmented mirror 1. Lighter mirrors with lighter support structures, to be controlled dynamically by computers Floppy mirror

27. 0 Adaptive Optics Computer-controlled mirror support adjusts the mirror surface (many times per second) to compensate for distortions by atmospheric turbulence

28. 0 Advances in Modern Telescope Design (2) 2. Simpler, stronger mountings (“Alt-azimuth mountings”) to be controlled by computers Equatorial mounting: 赤道儀 Alt-azimuth mounting: 經緯儀

29. 0 Examples of Modern Telescope Design (1) Design of the Large Binocular Telescope (LBT)

30. 0 Examples of Modern Telescope Design (2) The Very Large Telescope (VLT) 8.1-m mirror of the Gemini Telescopes

31. 0 Interferometry Recall: Resolving power of a telescope depends on diameter D: amin = 1.22 l/D. This holds true even if not the entire surface is filled out. • Combine the signals from several smaller telescopes to simulate one big mirror  • Interferometry

32. 0 CCD Imaging CCD = Charge-coupled device • More sensitive than photographic plates • Data can be read directly into computer memory, allowing easy electronic manipulations Negative image to enhance contrasts False-color image to visualize brightness contours

33. 0 The Spectrograph Using a prism (or a grating), light can be split up into different wavelengths (colors!) to produce a spectrum. Spectral lines in a spectrum tell us about the chemical composition and other properties of the observed object

34. 0 Radio Astronomy Recall: Radio waves of l ~ 1 cm – 1 m also penetrate the Earth’s atmosphere and can be observed from the ground.

35. 0 Radio Telescopes Large dish focuses the energy of radio waves onto a small receiver (antenna) Amplified signals are stored in computers and converted into images, spectra, etc.

36. 0 Radio Maps Radio maps are often color coded: Like different colors in a seating chart of a baseball stadium may indicate different seat prices, … colors in a radio map can indicate different intensities of the radio emission from different locations on the sky.

37. 0 Radio Interferometry Just as for optical telescopes, the resolving power of a radio telescope is amin = 1.22 l/D. For radio telescopes, this is a big problem: Radio waves are much longer than visible light. Use interferometry to improve resolution!

38. 0 Radio Interferometry (2) The Very Large Array (VLA): 27 dishes are combined to simulate a large dish of 36 km in diameter. Even larger arrays consist of dishes spread out over the entire U.S. (VLBA = Very Long Baseline Array) or even the whole Earth (VLBI = Very Long Baseline Interferometry)!

39. 0 The Largest Radio Telescopes The 300-m telescope in Arecibo, Puerto Rico The 100-m Green Bank Telescope in Green Bank, WVa.

40. 0 Science of Radio Astronomy Radio astronomy reveals several features, not visible at other wavelengths: • Neutral hydrogen clouds (which don’t emit any visible light), containing ~ 90 % of all the atoms in the Universe • Molecules (often located in dense clouds, where visible light is completely absorbed) • Radio waves penetrate gas and dust clouds, so we can observe regions from which visible light is heavily absorbed.

41. 0 Infrared Astronomy Most infrared radiation is absorbed in the lower atmosphere. NASA infrared telescope on Mauna Kea, Hawaii However, from high mountain tops or high-flying air planes, some infrared radiation can still be observed. Infrared cameras need to be cooled to very low temperatures, usually using liquid nitrogen.

42. 0 NASA’s Space Infrared Telescope Facility (SIRTF) Infrared light with wavelengths much longer than visible light (“Far Infrared”) can only be observed from space.

43. 0 Ultraviolet Astronomy • Ultraviolet radiation with l < 290 nm is completely absorbed in the ozone layer of the atmosphere. • Ultraviolet astronomy has to be done from satellites. • Several successful ultraviolet astronomy satellites: IUE, EUVE, FUSE • Ultraviolet radiation traces hot (tens of thousands of degrees), moderately ionized gas in the Universe.

44. 0 The Hubble Space Telescope • Launched in 1990; maintained and upgraded by several space shuttle service missions throughout the 1990s and early 2000’s • Avoids turbulence in the Earth’s atmosphere • Extends imaging and spectroscopy to (invisible) infrared and ultraviolet

45. 0 Gamma-Ray Astronomy Gamma-rays: most energetic electromagnetic radiation; traces the most violent processes in the Universe The Compton Gamma-Ray Observatory

46. 0 X-Ray Astronomy • X-rays are completely absorbed in the atmosphere. • X-ray astronomy has to be done from satellites. X-rays trace hot (million degrees), highly ionized gas in the Universe. NASA’s Chandra X-ray Observatory

47. 0 Cosmic Rays • Radiation from space does not only come in the form of electromagnetic radiation (radio, …, gamma-rays) • Earth is also constantly bombarded by highly energetic subatomic particles from space: Cosmic Rays • The source if cosmic rays is still not well understood.