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6. Optics and Telescopes Refracting telescopes Reflecting telescopes Image degradation Imaging systems Spectrographs Non-optical telescopes Orbiting telescopes

6. Optics and Telescopes

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6. Optics and Telescopes. Refractingtelescopes Reflectingtelescopes Image degradation Imaging systems Spectrographs Non-opticaltelescopes Orbitingtelescopes. Parallel Rays From Distant Objects. Refracting Telescopes. A lens is the primary image-forming tool - PowerPoint PPT Presentation

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Page 1: 6. Optics and Telescopes

6. Optics and Telescopes• Refracting telescopes• Reflecting telescopes• Image degradation• Imaging systems• Spectrographs• Non-optical telescopes• Orbiting telescopes

Page 2: 6. Optics and Telescopes

Parallel Rays From Distant Objects

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Refracting Telescopes• A lens is the primary image-forming tool

– Other lenses and/or mirrors may also be used• Basic physical process

– Refraction• EMR bends due to speed differences in different media

• Basic benefits– Very high contrast of resulting image

• Basic problems– Severe practical limits on the size of the primary

• Lenses cannot be mechanically supported from behind– Chromatic aberration

• Different wavelengths refract by different amounts• Basic solution

– Achromatic lenses

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Reflection By a Planar (Flat) Mirror

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Refracting Telescope Designs• Convex primary lens & convex eyepiece lens

– Inverted image Astronomicaltelescopes

• Convex primary lens & concave eyepiece lens– Upright image Terrestrial

telescopes

Page 6: 6. Optics and Telescopes

Chromatic Aberration In Lenses

Simple lens Achromatic lensOnly one lens Two or more lenses

1 1 2

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Reflecting Telescopes• A mirror is the primary image-forming tool

– Other mirrors and/or lenses may also be used• Basic physical process

– Reflection• Re-direction of incoming light rays

– No practical limits on the size of the primary• Mirrors can be mechanically supported from behind

• Basic problems– Relatively low contrast of resulting image– Spherical aberration

• Edge incident rays focus too close to the primary mirror• Basic solutions

– Parabolic, not spherical primary mirror surface

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Reflection by a Concave Mirror

(Prime Focus)

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Reflecting Telescope Designs

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Isaac Newton’s Second Telescope

http://upload.wikimedia.org/wikipedia/commons/c/cc/NewtonsTelescopeReplica.jpg

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Corrections for Spherical Aberration

Primefocus

SchmidtCassegrain

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Reflector Telescope Technology• Active optics

– Purpose Keep the primary in ideal optical shape• Gravity distorts the primary as the telescope moves

– Properties• Numerous actuators on the back of the primary mirror• Computer-adjusted tens of times per second

• Adaptive optics– Purpose Minimize thermal current effects

• “Twinkle, twinkle, little star…”– Properties

• A corrector plate is inserted near the focal plane• Computer-adjusted thousands of times per second• Image quality depends on processing computer speed• Data from a real or synthetic “guide star”

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Active Optics Actuators: Slow!

http://upload.wikimedia.org/wikipedia/commons/5/5d/GTC_Active_Optics_Acutators.jpg

Thick telescope mirror

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Adaptive Optics Actuators: Fast!

http://upload.wikimedia.org/wikipedia/commons/b/bc/Prototype_of_part_of_the_adaptive_support_system_of_the_E-ELT.jpg

Thindeformable

mirror

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Adaptive Optics Improve Sharpness

Without With adaptive adaptiveoptics optics

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Two Properties of All Telescopes• Magnification Apparent closeness

– Lens or mirror without eyepiece• Directly proportional to the focal length of the primary

– Lens or mirror with eyepiece• Primary focal length / Eyepiece focal length

– Double the primary focal length Double the magnification

– Halve the eyepiece focal length Double the magnification

• Light-gathering power Apparent brightness– Unobstructed lens or mirror

• Directly proportional to the surface area of the primary– Obstructed lens or mirror

• Surface area of primary – Surface area of obstruction– Lens or mirror arrays

• Combined surface area of all primaries in the array– Very Large Array (VLA) radio telescope

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Two More Properties of Telescopes• Angular resolution Apparent detail

– Single lens or mirror Smaller is better• Directly proportional to wavelength of observed EMR• Inversely proportional to diameter of the primary

– Multiple lenses or mirrors• Directly proportional to observed EMR wavelength• Inversely proportional to distance between primaries

• Field of view Apparent sky area– Angular diameter of visible telescope sky region– Important variables

• Inversely related to the focal length of the primary– Short primary focal lengths produce wide fields of view

• Directly related to the focal length of the eyepiece– Long eyepiece focal lengths produce wide fields of view

– Rich-field ’scopes: Low magnification & wide field

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The 200-Inch Palomar Telescope

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The Observatory on Mauna Kea

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Mauna Kea’s Keck I Telescope

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Mauna Kea’s Gemini North ’scope

http://zuserver2.star.ucl.ac.uk/~idh/apod/image/9906/gemini_pfa_big.jpgInstrument array

http://www.hia-iha.nrc-cnrc.gc.ca/atrgv/altair2_e.html

Secondarymirror

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Multiple Mirror Telescope MakeoverBefore 1998 After 2000

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Atmospheric Effects• Thermal currents

– Basic physical process• Low-density warm air rises & high-density cool air falls• Rapid heat loss from the atmosphere after sunset• [Early] nighttime atmospheric instability

– Solutions Adaptive optics & optimal locations• Light pollution

– Basic physical process• Light scatters from air molecules• Very few areas are far from large cities

– Solutions Fewer & well-screened city lights• Air pollution

– Basic physical process• Light scatters from air pollution molecules• Very few areas are far from pollution sources & plumes

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Image Recording Systems: Film• Film The historic recording medium

– Black & white Most sensitive type of film• Often taken through blue & red filters• Often heated to increase sensitivity• Always problematic

– Non-linear response to EMR– Sensitivity & development variables– Dimensional instability (film expands & shrinks with humidity)

– Color Least sensitive type of film• Normally used only for very bright celestial objects

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Image Recording Systems: CCD’s• CCD’s

The modern recording medium– Technology of Charge-Coupled-Devices

• Light-sensitive computer chip• Major advantages

– Highly linear response to EMR– No sensitivity or development variables– Extreme dimensional stability

– Black & white• The native mode of astronomical CCD’s

– Color• Multiple exposure through colored filters

– Red, green & blue for natural color– Other filter combinations for other color composites

– False-color• Arbitrary colors applied to non-visible wavelengths

– Various thermal infrared wavelengths

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A Charge-Coupled Device (CCD)

http://www.tech-faq.com/wp-content/uploads/Charge-Coupled-Device.jpg

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Astronomical Spectroscopes• Basic physical process

– Spread starlight into a rainbow• Observe & analyze spectral features

• Basic types of astronomical spectroscopes– Refraction spectroscopes

• Benefit– Well-known properties of lenses & prisms

• Drawback– Differential absorption of EMR by glass

– Reflection spectroscopes• Benefits

– Refraction gratings work on many EMR wavelengths– No differential absorption of EMR by glass

• Drawback– Transmission through the reflective aluminum coating

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A Rare Refraction Spectrograph

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A Common Reflection Spectrograph

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Displaying A Spectrum• Photographic

– Color representation• Color films never accurately represent colors• Computers rarely accurately represent colors

– Analog rather than digital• Ambiguity regarding the actual brightness

• Graphic– Color representation

• Data drawn on Cartesian coordinates– X-axis represents EMR wavelength– Y-axis represents EMR intensity

• Representation is as accurate as the original data– Digital rather than analog

• No ambiguity regarding the actual brightness

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Two Representations of a Spectrum

Absorptionline

Absorptionline

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Thermal Infrared Observations• Non-dedicated telescopes

– Limiting factors• Dry air minimizes absorption of TIR wavelengths• Remote enough to minimize thermal pollution effects

– Existing telescopes at Mauna Kea, Hawai‘i• Keck I & Keck II

– Near Infrared Camera for the Keck I Telescope(NIRC)

– Near Infrared Camera for the Keck II Telescope(NIRC2)

– Near Infrared Spectrometer(NIRSPEC)

– Long Wavelength Infrared Camera(LWIRC)

• Gemini North telescope• Dedicated TIR telescopes

– Existing telescopes at Mauna Kea, Hawai‘i• NASA Infrared Telescope Facility (IRTF)• United Kingdom Infrared 3.8-meter Telescope

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Radio Telescopes• Brief history

– First EM l’s used for astronomy after visible• Karl Jansky (Bell Telephone Laboratories)

– Discovered radio emissions from the galactic center

1932• Grote Reber

– Built the first radio telescope in his Illinois back yard

1936– Discovered radio emissions from many galactic locations

• Modern radio telescopes– Arecibo

Puerto Rico– Very Large Array (VLA)

New Mexico• Classic example of radio telescope interferometry• Better spatial resolution than any optical telescope

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Radio Telescopes Are Mostly AirRadio l’s are long enough to reflect from a grating

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More Telescope Technology• Basic physical process of telescope arrays

– Constructive interference between focused rays– A “synthetic aperture” larger than one telescope

• Existing instruments– Radio telescope arrays [interferometers]

• Relatively common & extremely successful– Very Large Array (VLA)

– Optical telescope arrays [interferometers]• “All-in-one” telescopes with segmented mirrors

– Keck I & Keck II individually, each with 36 hexagonal mirrors– Multi-Mirror Telescope (MMT), now a single large mirror ! ! !

• Independent telescopes– Keck I & Keck II working together

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Build a Large Synthetic Aperture

Small telescopes

LargeSyntheticaperture

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The Very Large Array (Radio)

Page 38: 6. Optics and Telescopes

The Arecibo Radio Telescope• World’s largest radio telescope

– Built in a doline (limestone sinkhole)

Arecibo O

bservatory in a James B

ond Movie

Page 39: 6. Optics and Telescopes

Earth’s Atmospheric Transparency

• X-rays Completely opaque• Ultraviolet Completely opaque• Visible Mostly transparent• Infrared Intermittently transparent• Microwaves Part is opaque, part transparent• Radio Part is transparent, part opaque

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Entire Sky at Different Wavelengths

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Orbiting Telescopes• Reasons

– Absorption & scattering by Earth’s atmosphere• Gamma rays Strongly absorbed by air

molecules• X-rays Strongly absorbed by air

molecules• Ultraviolet Strongly scattered by air

molecules• Thermal infrared Absorbed by water

vapor– Atmospheric turbulence

• Rising warm & falling cool air parcels• Corrective measures

– Absorption & scattering Extremely high altitude• Recent NASA balloon missions

– Atmospheric turbulence Adaptive optics• Rapidly increasing computer speed

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Hubble Space Telescope (HST)

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Examples of Orbiting Telescopes• Ultraviolet

– Extreme Ultraviolet Explorer (EUVE)• Mission ended in 2000

– Hopkins Ultraviolet Telescope (HUT)• Far-ultraviolet portion of the EMS

• Infrared– Space Infrared Telescope Facility

(SIRTF)• Launch on 25 August 2003

• X-Ray– Chandra X-Ray Observatory

• Reached its operational orbit on 7 August 1999• Gamma Ray

– Compton Gamma Ray Observatory• Launched 7 April 1991

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Next Generation Space Telescope• Renamed “James Webb Space Telescope”

– NASA’s second Administrator• Largely responsible for NASA’s science programs

– Important facts• Replacement for the Hubble Space Telescope• Launch expected in 2017 or 2018• “Naked” primary mirror ~ 6.5 m (21.3 ft) in diameter

– Hexagonal segments folded at launch• Sun shield the size of a tennis court• Operate in the infrared (0.6 to 28 mm) • Orbit 1.5 million km from Earth at the L2 Point

– L2 is a semi-stable point directly opposite the Sun from the Earth

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The Geometry & Location of L2

http://en.wikipedia.org/wiki/File:L2_rendering.jpg

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James Webb Space Telescope

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Proposed Thirty Meter Telescope

http://en.wikipedia.org/wiki/File:Top_view_of_tmt_complex.jpg

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• Refracting & reflecting telescopes– Refraction systematically bends EMR

• Size limits due to sagging lenses– Reflection systematically rejects EMR

• Theoretically no size limits• Newtonian design is very common

• Active & adaptive optics– Active: Adjust for mirror bending– Adaptive: Adjust for atmosphere

• Angular resolution & field of view– AR: Amount of detail in the image– FoV: Size of visible patch of sky

• Magnification & light gathering power– Mag: Apparent closeness of objects– GP: Brightness of objects

• Atmospheric effects– Thermal currents– Air & light pollution

• Image recording systems– Camera & film– CCD’s

• Astronomical spectroscopes– Yield temperature & energy flux– Represented as graphs, not pictures

• Non-optical telescopes– Thermal infrared & radio from Earth– UV, X-ray & gamma ray from space

• Interferometer technology• Orbiting telescopes

– Benefits & costs

Important Concepts