(in case you missed it yesterday ) Merger of Two Neutron Stars!

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(in case you missed it yesterday ) Merger of Two Neutron Stars! https://cmns.umd.edu/news-events/features/3997 More on this later in the semester

Lecture #14: Plan Light (cont d) Atomic physics Formation of spectra Doppler effect Telescopes

Light: Inverse-Square Law B = L / (4 π d 2 ) B = apparent brightness L = luminosity (= total energy output rate) d = distance from light source (e.g., star)

You see this every day!

The Nature of Matter: Atoms Atomic structure: Nucleus (10-6 10-4 nm) orbiting electrons (0.1 10 nm) Electrons are negatively charged Nucleus (> 99.9% of the mass!): neutrons (no charge) protons (positively charged) Chemical Elements: 1 = Hydrogen 2 = Helium 6 = Carbon 8 = Oxygen

Atoms Electrons are only allowed to move in fixed orbits about nucleus Energy levels are distinct for each element

Conservation of Energy Energy can never be created or destroyed. It can only be changed in form Forms of energy: Motion (mechanical / kinetic) Gravitational Electrical / Magnetic Light

Atomic Energy Levels Energy High State Low State High State Energy Low State

Atoms: Origin of Light Emission of light: Electrons move from higher to lower orbits Absorption of light: Electrons move from lower to higher orbits

Absorption

Emission

Types of Spectra Hot, high density gas, liquid, solid gives a continuous spectrum light at all λ s Hot, low density gas gives an emission line spectrum light only at some λ s Cool gas between observer and continuous light source gives an absorption line spectrum light missing or dimmer at some λ s

Emission Spectra

Absorption Spectra

Types of Spectra? Sun interior, stove burner, carbon filament,? Solar atmosphere, cool interstellar clouds,? Solar corona, aurora, sodium street lamps,?

Spectra of Astronomical Objects

Doppler Shift: Sound (Fire Engine Siren) Higher pitch when approaching, Lower pitch when moving away

Doppler Shift: Light Observer sees wavelength emitted or absorbed by moving source shifted to: Longer λ s if source and observer are moving apart (redshift) Shorter λ s if source and observer are moving toward each other (blueshift) Sound Light

Doppler Shift: Light Velocity of source, V, is given by: V = c (λ λ 0 ) / λ 0 λ = wavelength measured by observer λ 0 = wavelength emitted or absorbed by source (rest wavelength) c = speed of light

Example: Wise-guy speeder vs Smart cop λ = 500 nm (green) [observed color] λ 0 = 700 nm (red) [actual color, seen by cop] V/c = (λ λ 0 ) / λ 0 = (500 700) / 700 = 200 / 700 = 2/7 [approaching] V = (2/7) c = (2/7) (3 x 10 5 km/s) = 86,000 km/s = 2 x 10 8 mph! No ticket for running the red light But a huge speeding ticket! e.g. 1 / mph over 100 mph $ 2,000,000!!!

Telescopes

Types of Telescopes Refracting Telescopes or Refractors Use lenses to collect light Reflecting Telescopes or Reflectors Use mirrors to collect light

Refractors

Refracting Telescopes Disadvantages: Large lenses are expensive Large lenses sag under gravity Many lens materials absorb ultraviolet Chromatic aberration due to wavelength dependence of refraction

Refracting Telescopes

Reflecting Telescopes

Different styles of reflectors

Multiple Mirrors Reflectors can be made very large if multiple mirrors are used as the primary mirror Example: Keck Telescopes (diameter of 10 meters! Made of 36 x 1.8 meter hexagonal segments)

Multiple Mirrors: Future (~20-30-40 meters) GMT ELT

Collecting Area Light bucket : the bigger the area of the telescope s mirror or lens, the more photons it collects Collecting Area ~ (Diameter of telescope) 2

Collecting Area Example: Eye (D = 5 mm) vs Keck (D = 10 m) Collecting power (Keck) / Collecting power (eye) = D(Keck) 2 / D(eye) 2 = [D(Keck) / D(eye)] 2 = [10 / 5 x 10-3 ] 2 = [2 x 10 3 ] 2 = 4 x 10 6 Keck is 4,000,000 x more powerful than our eye!

Resolving Power The bigger the size of the telescope, the better it is at discerning fine details Resolving power ~ (Diameter of telescope) / λ

Radio Telescopes are big! (radio! longer λ, so larger D is needed to get the same resolving power as optical telescopes)

Radio Telescopes: Interferometry (Combine the signal from an array of radio telescopes to increase effective D)