Lesson 4 - Telescopes
Reading Assignment
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•Chapter 5.1: Optical Telescopes
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•Chapter 5.3: Images and Detectors
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•Chapter 5.2: Telescope Size
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•Discovery 5-1: The Hubble Space Telescope
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•Chapter 5.4: High-Resolution Astronomy
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•More Precisely 7-1: Why is the Sky Blue?
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•Chapter 5.5: Radio Astronomy
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•Chapter 5.6: Interferometry
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•Chapter 5.7: Space-Based Astronomy
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•Chapter 5.8: Full-Spectrum Coverage
Summary of Major Space Telescopes
Read Discovery 5-1 and Chapter 5.7.
Infrared
Infrared Astronomy Satellite (IRAS)
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•0.6-meter diameter mirror
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•far infrared (FIR)
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•1983 - 95
Infrared Space Observatory (ISO)
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•0.6-meter diameter mirror
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•FIR
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•1995 - 98
Hubble Space Telescope (HST)
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•NASA's 1st "Great Observatory"
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•2.5-meter diameter mirror
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•near infrared (NIR) / optical / near ultraviolet (NUV)
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•1990 - present
Spitzer Space Telescope (SST)
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•NASA's 4th "Great Observatory"
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•0.85-meter diameter mirror
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•FIR
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•2003 - present
Visible
HST
Ultraviolet
International Ultraviolet Explorer (IUE)
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•NUV
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•1978 - 96
HST
Extreme Ultraviolet Explorer (EUVE)
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•far ultraviolet (FUV) / soft X-rays
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•1992 - 2000
Far Ultraviolet Spectrographic Explorer (FUSE)
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•FUV
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•1999 - 2007
Galaxy Evolution Explorer (GALEX)
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•NUV
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•2003 - present
X-rays
Einstein Observatory
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•1978 - 80
Röntgen Satellite (ROSAT)
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•1991 - 99
Chandra X-ray Observatory (CXO)
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•NASA's 3rd "Great Observatory"
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•1999 - present
X-ray Multi-Mirror Newton Satellite (XMM-Newton)
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•European equivalent of a "Great Observatory"
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•1999 - present
Gamma rays
Compton Gamma-Ray Observatory (CGRO)
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•NASA's 2nd "Great Observatory"
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•1991 - 2000
Swift Gamma-Ray Burst Explorer
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•2004 - present
Fermi Gamma-Ray Space Telescope
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•Equivalent of a "Great Observatory"
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•2008 - present
Math Notes
Light-Gathering Power
Read Chapter 5.2.
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•LGP = light gathering power, or the rate at which a telescope collects light
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•A = collecting area, or the area of a telescope's mirror
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•D = diameter of a telescope's mirror
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•LGP is proportional to A.
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•A is proportional to D2.
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•Hence, the following is true.
( 1 )
LGP is proportional to D2- Example: UNC's new 4.1-meter diameter SOAR telescope in the Chilean Andes collects light how many times faster than UNC's old 0.6-meter diameter Morehead Observatory telescope in Chapel Hill?
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Solution: Since LGPSOAR is proportional DSOAR2 and LGPMO is proportional DMO2, then Hence, the SOAR telescope collects light 47 times more quickly than the Morehead Observatory telescope.
=LGPSOAR LGPMO DSOAR DMO
=2 4.1 m 0.6 m
= 47.2
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•LG = light gathered
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•t = integration time, or the total amount of time that a telescope's camera records the collected light
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•LG is also proportional to LGP × t.
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•Hence, the following is true.
( 2 )
LG is proportional to D2 × t- Example: How much more light does one collect with the SOAR telescope in 1 minute than with the Morehead Observatory telescope in 47 minutes?
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Solution: Since LGSOAR is proportional to DSOAR2 × tSOARand LGMO is proportional toDMO2 × tMO,then
=LGPSOAR LGPMO DSOAR DMO
×2 tSOAR tMO
=Hence, the SOAR telescope collects just as much light in 1 minute as the Morehead Observatory telescope collects in 47 minutes.4.1 m 0.6 m
×2 1 min 47 min
= 1.
Resolving Power
Read Chapter 5.2, Chapter 5.4, and Chapter 5.6.
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•θ = resolving power, or the angle over which a telescope smears out a point of light
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•λ = wavelength of observed light
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•D = telescope diameter
( 3 )
θ = 0.25" ×
(λ / 1 µm) |
(D / 1 m) |
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•Note: Without adaptive optics, no ground-based optical telescope can resolve light better than about an arcsecond because of atmospheric blurring effects.
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•For radio telescopes, λ is usually measured in cm and θ in arcminutes. Hence, you might find this, equivalent, form easier to use.
( 4 )
θ = 40' ×
(λ / 1 cm) |
(D / 1 m) |
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•I love radio astronomy. This program can now be taken for Experiential Education credit as ASTR 111L!