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Wave Interference and Diffraction Part 3: Telescopes and Interferometry PHY 2049 Physics 2 with Calculus PHY 2049: Chapter 36 1 Telescopes: Purpose is Light Collection ÎPupil of eye D ≈ 8mm (in very dim light) ÎLargest ÎRatio telescope (Keck) has D = 10m of areas = (10/0.008)2 = 1.5 × 106 Can collect light for hours rather than 0.1 sec More sensitive light collectors (CCD arrays) Thus telescopes are several billion times more sensitive ÎCan see near the end of the known universe PHY 2049: Chapter 36 2 Telescope Construction ÎAll 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 PHY 2049: Chapter 36 3 Keck Telescope (D = 10 m) PHY 2049: Chapter 36 4 Keck Hexagonal Mirror (36 Segments) PHY 2049: Chapter 36 5 Keck Primary Mirror (Each segment 1.8 m) Hole PHY 2049: Chapter 36 6 Main Limitation on Earth: Atmosphere ÎAir cells in atmosphere Air cells above telescope mirror cause distortion of light Best performance is ≈ 0.25 – 0.5″ resolution on the ground This is why telescopes are sited on high mountains ΓAdaptive optics” just beginning to offset this distortion PHY 2049: Chapter 36 7 Diffraction Through Circular Opening Intensity of light after passing through a circular opening. Spreading caused by diffraction. PHY 2049: Chapter 36 8 Theoretical Performance Limit: Diffraction ÎLight rays hitting mirror spread due to diffraction These rays interfere, just like for single slit Calculation a little different because of circular shape Angle of spread Δθ = 1.22λ/D (D = diameter) PHY 2049: Chapter 36 9 Example: Optical Telescopes ÎKeck 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 ÎHubble space telescope: D = 2.4m, λ = 550nm Δθ = 1.22 × 550 × 10-9 / 2.4 = 2.8 × 10-7 rad = 0.058” But actually can achieve this resolution! ÎRayleigh criterion objects separated by Δθ < 1.22λ/D cannot be distinguished An approximate rule, shows roughly what is possible Two PHY 2049: Chapter 36 10 Single Star Units in multiples of λ/D PHY 2049: Chapter 36 11 Two Stars: Separation = 2.0 Units in multiples of λ/D PHY 2049: Chapter 36 12 Two Stars: Separation = 1.5 Units in multiples of λ/D PHY 2049: Chapter 36 13 Two Stars: Separation = 1.22 Units in multiples of λ/D PHY 2049: Chapter 36 14 Two Stars: Separation = 1.0 Units in multiples of λ/D PHY 2049: Chapter 36 15 Two Stars: Separation = 0.8 Units in multiples of λ/D PHY 2049: Chapter 36 16 Two Stars: Separation = 0.6 Units in multiples of λ/D PHY 2049: Chapter 36 17 Two Stars: Separation = 0.4 Units in multiples of λ/D PHY 2049: Chapter 36 18 Single Star Units in multiples of λ/D PHY 2049: Chapter 36 19