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Wave Interference and Diffraction Part 3: Telescopes and ...

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PHY 2049: Chapter 36 1 Paul Avery University of Florida http://www.phys.ufl.edu/~avery/ [email protected] Wave Interference and Diffraction Part 3: Telescopes and Interferometry PHY 2049 Physics 2 with Calculus
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Page 1: Wave Interference and Diffraction Part 3: Telescopes and ...

PHY 2049: Chapter 36 1

Paul AveryUniversity of Florida

http://www.phys.ufl.edu/~avery/[email protected]

Wave Interference and Diffraction

Part 3: Telescopes and Interferometry

PHY 2049Physics 2 with Calculus

Page 2: Wave Interference and Diffraction Part 3: Telescopes and ...

PHY 2049: Chapter 36 2

Telescopes: Purpose is Light CollectionPupil of eye D ≈ 8mm (in very dim light)

Largest telescope (Keck) has D = 10m

Ratio of areas = (10/0.008)2 = 1.5 × 106

Can collect light for hours rather than 0.1 secMore sensitive light collectors (CCD arrays)Thus telescopes are several billion times more sensitive

Can see near the end of the known universe

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PHY 2049: Chapter 36 3

Telescope ConstructionAll large telescopes are reflectors: Why?

Mirror only needs single high quality surface(lens needs perfect volume since light passes through it)No chromatic aberration (no lens for refracting)Full support for mirror, no distortion from moving

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PHY 2049: Chapter 36 4

Main Limitation on Earth: AtmosphereAir cells in atmosphere

Air cells above telescope mirror cause distortion of lightBest performance is ≈ 0.25 – 0.5″ resolution on the groundThis is why telescopes are sited on high mountains

“Adaptive optics” just beginning to offset this distortion

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PHY 2049: Chapter 36 5

Diffraction Through Circular Opening

Intensity of light after passingthrough a circular opening.Spreading caused by diffraction.

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PHY 2049: Chapter 36 6

Theoretical Performance Limit: DiffractionLight rays hitting mirror spread due to diffraction

These rays interfere, just like for single slitCalculation a little different because of circular shapeAngle of spread Δθ = 1.22λ/D (D = diameter)

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PHY 2049: Chapter 36 7

Example: Optical TelescopesKeck telescope: D = 10m, λ = 550nm

Δθ = 1.22 × 550 × 10-9 / 10 = 6.7 × 10-8 rad = 0.014”Compare this to 0.25” – 0.5” from atmosphere

Hubble space telescope: D = 2.4m, λ = 550nmΔθ = 1.22 × 550 × 10-9 / 2.4 = 2.8 × 10-7 rad = 0.058”But actually can achieve this resolution!

Rayleigh criterionTwo objects separated by Δθ < 1.22λ/D cannot be distinguishedAn approximate rule, shows roughly what is possible

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PHY 2049: Chapter 36 8

Single Star

Units in multiples of λ/D

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PHY 2049: Chapter 36 9

Two Stars: Separation = 2.0

Units in multiples of λ/D

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PHY 2049: Chapter 36 10

Two Stars: Separation = 1.5

Units in multiples of λ/D

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PHY 2049: Chapter 36 11

Two Stars: Separation = 1.22

Units in multiples of λ/D

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PHY 2049: Chapter 36 12

Two Stars: Separation = 1.0

Units in multiples of λ/D

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PHY 2049: Chapter 36 13

Two Stars: Separation = 0.8

Units in multiples of λ/D

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PHY 2049: Chapter 36 14

Two Stars: Separation = 0.6

Units in multiples of λ/D

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PHY 2049: Chapter 36 15

Two Stars: Separation = 0.4

Units in multiples of λ/D

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PHY 2049: Chapter 36 16

Single Star

Units in multiples of λ/D

Page 17: Wave Interference and Diffraction Part 3: Telescopes and ...

PHY 2049: Chapter 36 17

Gemini Telescope w/ Adaptive Optics

Gemini = “twins”D = 8.1 mHawaii, ChileBoth outfitted with

adaptive optics

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PHY 2049: Chapter 36 18

Adaptive Optics in Infrared (936 nm)

9× better!

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PHY 2049: Chapter 36 19

Pluto and Its Moon

Pluto and its moon Charon (0.083″ resolution)

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PHY 2049: Chapter 36 20

Gemini North Images (7x Improvement)

Resolution = 0.6” Resolution = 0.09”

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PHY 2049: Chapter 36 21

Interferometry: Multiple RadiotelescopesCombine information from multiple radiotelescopes

Atomic clocks to keep time information (time = phase)Each telescope records signals on tape with time stampTapes brought to “correlator” to build synthetic image

Single telescope resolutionΔθ = 1.22λ/D (D = diameter of dish or mirror)

Two telescope resolutionΔθ ~ λ/D (D = distance between telescopes)

Spectacular improvement in resolutionDiameter of dish ~ 20 – 50mDistance between two dishes ~ 12,000 km (diameter of earth)Improvement is factor of ~ 200,000 – 500,000

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PHY 2049: Chapter 36 22

Example of InterferometryTwo radiotelescopes

D = 50mSeparated by diameter of earth = 12,700 km6 GHz radio waves, λ = 5 cm

Single telescope resolutionΔθ = 1.22λ/D = 1.22 × 0.05 / 50 = 0.0012 rad = 200”

Two telescope resolutionΔθ ~ λ/D = 0.05 / 1.27 × 107 = 4 × 10-9 rad = 0.0004”Compare to 0.25” for best earthbound telescope, 0.06” for Hubble

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PHY 2049: Chapter 36 23

Radiotelescope (Mauna Kea)

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PHY 2049: Chapter 36 24

Spaced Based Interferometry: Japan

VSOP (VLBI Space Observatory Programme)http://www.vsop.isas.ac.jp/

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PHY 2049: Chapter 36 25

VLBI Using Satellite (λ = 6cm)

Quasar: VLBI ground only Quasar: VLBI ground plus space

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PHY 2049: Chapter 36 26

VLBI Using Satellite (λ = 17cm)

Quasar: VLBI ground only Quasar: VLBI ground plus space

Space based ~ 30,000 km baseline


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