ASTR - lec 12

ASTR 1P02 - lec 12

Lecture 12: Starlight

Key Learning Objectives
  • How star brightness is measured.

  • Light and the electromagnetic spectrum.

  • The meaning of the colors of stars.

  • Information derived from analyzing starlight.


Introduction to Star Brightness
  • Measurement Units:

    • Standard unit of energy: Joule (J)

    • Definition: 1 J is the energy required to accelerate a 1 kg mass at 1 m/s² over a distance of 1 m.

    • Power: Energy per unit time (measured in watts (W))

    • Definition: 1 W = 1 J/s.

    • Example: A 100 W lightbulb consumes 100 J every second.


Luminosity of Stars
  • Luminosity: Total energy emitted per second in light.

    • Measured in watts (W).

    • Sun's luminosity: L=3.828×1026 WL_\odot = 3.828 \times 10^{26} \text{ W}

    • Symbol \odot represents the Sun.

    • Sun's mass M2.0×1030 kgM_\odot ≈ 2.0 \times 10^{30} \text{ kg}.

    • Sun's radius R7.0×108 mR_\odot ≈ 7.0 \times 10^{8} \text{ m}.

    • Example star: BAT99-98 in the Large Magellanic Cloud has a luminosity of approximately 5,000,000 LL_\odot.

    • Faint star 2MASS J0523-1403 has a luminosity of approximately 0.0001 LL_\odot .


Apparent Magnitude of Stars
  • Definition: Measures how bright a star appears from Earth.

    • Depends on three factors:

    1. Luminosity of the star.

    2. Distance from Earth (light dims with distance).

    3. Interstellar dust on the line of sight (blocks light).

    • Distinction made:

    • Luminosity is an objective property.

    • Apparent magnitude is subjective, varying with the observer's location.


Understanding Light Emission
  • Stars emit light in all directions; we only see a portion directed toward Earth.

  • As distance increases, light spreads over a larger area, decomposing intensity.


Inverse Square Law of Brightness
  • Brightness diminishes with distance:(A=L4πr2)(A = \frac{L}{4\pi r^2})

    • Light is spread out as a sphere, increasing surface area with radius rr.

    • Surface area of a sphere: A=4πr2A = 4\pi r^2

    • Brightness is inversely proportional to the square of distance:

    • extBrightness1r2ext{Brightness} \propto \frac{1}{r^2}.

  • Example Calculation:

    • Distance from Sun to Earth: 1 AU 150,000,000extkm≈ 150,000,000 ext{ km}.

    • Distance from Sun to Neptune: ~30 AU; light is 900 times less bright on Neptune than on Earth: 302=90030^2 = 900.

    • Distance from Sun to Mercury: ~0.4 AU; light is 6.25 times brighter on Mercury than Earth: 2.52=6.252.5^2 = 6.25.


Apparent Magnitude Scale
  • Apparent magnitude indicates visibility:

    • Under -25: Painfully bright.

    • Under -4: Visible during the day.

    • Under +6.5: Visible to the naked eye under ideal conditions.

    • Under +27.7: Visible through the Subaru Telescope.

    • Under +31.5: Visible to the Hubble Space Telescope.

  • Examples of objects and their magnitudes:

    • Sun: -26.8, Full Moon: -12.7, Sirius: -1.5, Proxima Centauri: +11, Charon: +15.6.


Absolute Magnitude
  • Definition: Apparent magnitude if viewed from a distance of 32.6 light-years without obstructions.

    • Example:

    • Betelgeuse: Apparent Magnitude +0.5; Absolute Magnitude -5.85.

    • Vega: Apparent Magnitude +0.03; Absolute Magnitude +0.58.


Properties of Light as a Wave
  • Light characterized as both:

    1. Electromagnetic wave: Made of electric and magnetic fields.

    2. Particles (photons): Massless elementary particles.

  • This phenomenon is known as wave-particle duality in quantum mechanics.

  • Wave}: Regular disturbance in a medium; characterized by:

    • Amplitude (A): Maximum displacement from equilibrium (e.g., loudness in sound).

    • Wavelength (λ): Distance between two crests.

    • Frequency (f): Number of wavelengths per second (measured in Hz).

    • Speed (c): Speed of wave propagation.


Wave Relationships
  • Relationship: c=λfc = \lambda f

    • Wavelength λ\lambda and frequency ff are inversely proportional:

    • High frequency = Short wavelength.

  • Speed of light in vacuum: c3×108extm/sc ≈ 3 \times 10^8 ext{ m/s}.


Color and Temperature of Stars
  • Photon energy relation: E=hf=hcλE = hf = \frac{hc}{\lambda} (Planck’s Equation)

    • h4.1×1015exteV/Hzh ≈ 4.1 \times 10^{-15} ext{ eV/Hz}.

  • Color spectrum ranges visible to the human eye:

    • Unique wavelength ~380-750 nm; frequency ~400-790 THz.

    • Monochromatic light: Single wavelength.

    • Non-spectral colors: Combinations of wavelengths (e.g., magenta).


Electromagnetic Spectrum Overview
  • Spectrum from lowest to highest frequency:

    • Radio waves, Microwaves, Infrared, Visible light, Ultraviolet, X-rays, Gamma rays.

  • Wavelength examples:

    • Visible light ~0.5 × 10⁻⁶ m, Ultraviolet ~1 × 10⁻⁸ m.


Black Body Radiation
  • Black body: Ideal body absorbing all incident electromagnetic radiation.

  • Emission characteristic: According to Wien’s Displacement Law:

    • Peak wavelength: λpeak=bT\lambda_{peak} = \frac{b}{T} where b2.9×103extmKb ≈ 2.9 \times 10^{-3} ext{ m⋅K}.


Stellar Temperatures and Colors
  • Temperature affects star color and therefore its emitted spectrum.

    • Red stars: lower temperatures (~3,000 K).

    • Blue stars: higher temperatures (~25,000 K).

    • Planckian locus illustrates black-body spectrum transitions (red to blue).


Light Interaction within Atmosphere
  • Rayleigh scattering effects on sunlight through the atmosphere.

    • Shorter wavelengths (blue) scatter more, leading to a blue sky and yellow/red appearance of the Sun.


Spectroscopy
  • Absorption of specific light frequencies based on gas composition yields dark lines in the spectrum.

    • Example: Fraunhofer lines in the Sun’s spectrum indicate chemical composition.

  • Heating a gas causes emission lines reflecting the same frequencies as absorption lines.


Bohr Model of the Atom
  • Electrons in discrete orbits defined by quantum numbers.

  • Energy emitted upon transition: E=R<em>hc(1n</em>f21ni2)E = R<em>hc \left( \frac{1}{n</em>f^2} - \frac{1}{n_i^2} \right) with RR as Rydberg constant.