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Light and Atoms

Light and Atoms. Arny, 3 rd Edition, Chapter 3. Introduction. Due to the vast distances, with few exceptions, direct measurements of astronomical bodies are not possible We study remote bodies indirectly by analyzing their light Understanding the properties of light is therefore essential

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Light and Atoms

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  1. Light and Atoms Arny, 3rd Edition, Chapter 3

  2. Introduction • Due to the vast distances, with few exceptions, direct measurements of astronomical bodies are not possible • We study remote bodies indirectly by analyzing their light • Understanding the properties of light is therefore essential • Care must be given to distinguish light signatures that belong to the distant body from signatures that do not (e.g., our atmosphere may distort distant light signals)

  3. Properties of Light • Introduction • Light is radiant energy: it does not require a medium for travel • Light travels at 299,792.458 km/s (3.00 X108 m/s) • Speed of light is constant and represented by the letter “c” • However, the speed of light is reduced as it traverses transparent materials and the speed is also dependent on color

  4. Properties of Light • The Nature of Light – Waves or Particles? • One model of light: electromagnetic wave • The wave travels as a result of a fundamental relationship between electricity and magnetism • A changing magnetic field creates an electric field and a changing electric field creates a magnetic field • This changing/creation scheme allows the light to bootstrap its way across a vacuum • Wave picture cannot explain all of light’s properties

  5. Properties of Light • The Nature of Light (continued) • Another model of light: photons • Light thought of as a stream of particles • Each photon particle carries energy • Wave – Particle Duality • In a vacuum, photons travel in straight lines, but behave like waves • Sub-atomic particles also act as waves • Wave-particle duality: All particles of nature behave as both a wave and a particle • Which property of light manifests itself depends on the situation

  6. Properties of Light • Light and Color • Colors to which the human eye is sensitive is referred to as the visible spectrum • In the wave theory, color is determined by the light’s wavelength (symbolized as l) • Nanometer (10-9 m)is the convenient unit • Red = 700 nm (longest visible wavelength), violet = 400 nm (shortest visible wavelength) • Characterizing Electromagnetic Waves by Their Frequency • Frequency (or n) is the number of wave crests that pass a given point in 1 second (measured in Hertz, Hz) • Important relation: nl = c

  7. Properties of Light • Light with no distinguishing color is called white light • White light is a mixture of all colors • A prism demonstrates that white light is a mixture of wavelengths by its creation of a spectrum • Additionally, one can recombine a spectrum of colors and obtain white light

  8. The EM Spectrum: Beyond Visible Light • Introduction • Electromagnetic spectrum is composed of radio waves, microwaves, infrared, visible light, ultraviolet, x rays, and gamma rays • Longest wavelengths are more than 103 km • Shortest wavelengths are less than 10-18 m • Various instruments used to explore the various regions of the spectrum • Infrared Radiation • Sir William Herschel (around 1800) showed heat radiation related to visible light • He measured an elevated temperature just off the red end of a solar spectrum – infrared energy • Our skin feels infrared as heat

  9. The EM Spectrum: Beyond Visible Light • Ultraviolet Light • J. Ritter in 1801 noticed silver chloride blackened when exposed to “light” just beyond the violet end of the visible spectrum • Radio Waves • Predicted by Maxwell in mid-1800s, Hertz produced radio waves in 1888 • Jansky discovered radio waves from cosmic sources in the 1930s, the birth of radio astronomy • Radio waves used to study a wide range of astronomical processes • Radio waves also used for communication, microwave ovens, and search for extraterrestrials

  10. The EM Spectrum: Beyond Visible Light • Other Wavelength Regions • X-rays • Roentgen discovered X rays in 1895 • First detected beyond the Earth in the Sun in late 1940s • Used by doctors to scan bones and organs • Used by astronomers to detect black holes and tenuous gas in distant galaxies • Gamma rays and region between infrared and radio • Relatively unexplored regions • Difficult to measure

  11. The EM Spectrum: Beyond Visible Light • Energy Carried by EM Radiation • Each photon of wavelength l carries an energy E given by: E = hc/l where h is Planck’s constant • Notice that a photon of short wavelength radiation carries more energy than a long wavelength photon

  12. The EM Spectrum: Beyond Visible Light • Wien’s Law: A Wavelength-Temperature Relation • Heated bodies generally radiate across the entire electromagnetic spectrum • There is one particular wavelength, lm, at which the radiation is most intense and is given by Wien’s Law: lm = k/T Where k is some constant and T is the temperature of the body • Note hotter bodies radiate more strongly at shorter wavelengths • As an object heats, it appears to change color from red to white to blue • Measuring lm gives a body’s temperature • Careful: Reflected light does not give the temperature

  13. The EM Spectrum: Beyond Visible Light • Blackbodies and Wien’s Law • A blackbody is an object that absorbs all the radiation falling on it • Since such an object does not reflect any light, it appears black when cold, hence its name • As a blackbody is heated, it radiates more efficiently than any other kind of object • Blackbodies are excellent absorbers and emitters of radiation and follow Wien’s law • Very few real objects are perfect blackbodies, but many objects (e.g., the Sun and Earth) are close approximations • Gases, unless highly compressed, are not blackbodies and can only radiate in narrow wavelength ranges

  14. Formation of a Spectrum • The Spectrum • The key to determining the composition and conditions of an astronomical body • Spectroscopy is the technique to capture and analyze a spectrum • Spectroscopy assumes that every atom or molecule will have a unique spectral signature • How a Spectrum is Formed • Electron orbits are more properly thought of as energy levels with the lowest energy level corresponding to the smallest orbit • Wavelength of emitted (or absorbed) light is calculated from the energy difference of the two levels involved

  15. Formation of a Spectrum • Types of Spectra • Continuous spectrum • Spectra of a blackbody • Typical objects are solids and dense gases • Emission–line spectrum • Produced by hot, tenuous gases • Fluorescent tubes, aurora, and many interstellar clouds are typical examples • Dark-line or absorption–line spectrum • Light from blackbody passes through cooler gas leaving dark absorption lines • Fraunhofer lines of Sun is an example • Spectra may be depicted in a variety of ways

  16. The Doppler Shift • Doppler Shift • If a source of light is set in motion relative to an observer, its spectral lines shift to new wavelengths in a phenomenon known as Doppler shift • The shift in wavelength is given as Dl = l – lo = lov/c where l is the observed (shifted) wavelength, lo is the emitted wavelength, v is the source non-relativistic radial velocity, and c is the speed of light • An observed increase in wavelength is called a redshift • a decrease in observed wavelength is called a blueshift (regardless of whether or not the waves are visible) • Doppler shift is used to determine an object’s velocity

  17. Absorption in the Atmosphere • Gases in the Earth’s atmosphere absorb electromagnetic radiation to the extent that most wavelengths from space do not reach the ground • Visible light, most radio waves, and some infrared penetrate the atmosphere through atmospheric windows, wavelength regions of high transparency • Lack of atmospheric windows at other wavelengths is the reason for astronomers placing telescopes in space

  18. A wave of electromagnetic energy moves through empty space at the speed of light, 299,792.5 kilometers per second. The wave carries itself along by continually changing its electric energy into magnetic energy and vice versa. Back

  19. Photons—particles of energy—stream away from a light source at the speed of light. Back

  20. The distance between crests defines the wavelength, l, for any kind of wave, be it water (top photo) or electromagnetic (bottom illustration). Back

  21. White light is spread into a spectrum by a prism. Back

  22. The electromagnetic spectrum. Back

  23. As a body is heated, the wavelength at which it radiates most strongly, lm, shifts to shorter wavelengths, a relation known as “Wien's Law.” Thus the color of an electric stove burner changes from red to yellow as it heats up. Note also that as the object's temperature rises, the amount of energy radiated increases at all wavelengths. Back

  24. Sketch of an atom's structure, showing electrons orbiting the nucleus. The electrons are held in orbit by the electrical attraction between their negative charge and the positive charge of the protons in the nucleus. “Orbits” are in reality more like clouds. Back

  25. Energy is released when an electron drops from an upper to a lower orbit, causing the atom to emit electromagnetic radiation. Back

  26. An atom can absorb light, using the light's energy to lift an electron from a lower to a higher orbit. To be absorbed, the energy of the light's photons must equal the energy difference between the atom's electron orbits. In this example, the green light's energy matches the energy difference, but the red and blue light's energy does not. Therefore only the green is absorbed. Back

  27. Sketch of a spectroscope and how it forms a spectrum. Either a prism or grating may be used to spread the light into its component colors. Back

  28. Sketch of electron orbits in hydrogen and helium. Back

  29. Emission of light from a hydrogen atom. The energy of an electron dropping from an upper to lower orbit is converted to light. Back

  30. The emission spectra of hydrogen and of helium. Back

  31. Gas between an observer and a source of light that is hotter than the gas creates an absorption-line spectrum. Atoms in the gas absorb only those wavelengths whose energy equals the energy difference between their electron orbits. The absorbed energy lifts the electrons to upper orbits. The lost light makes the spectrum darker at the wavelengths where it is absorbed. Back

  32. Types of spectra: (A) continuous, (B) emission-line, and (C) absorption-line. Back

  33. (A) A radio spectrum of a cold interstellar cloud. (Courtesy Doug McGonagle, FCRAO.) (B) An X-ray spectrum of hot gas from an exploding star. (Courtesy P. F. Winkler, Middlebury College.) Back

  34. (A) The Doppler shift: waves appear to shorten as a source approaches and lengthen as it recedes. (B) Doppler shift of sound waves from a passing car. (C)Doppler shift of radar waves in a speed trap. (D) A Slinky illustrates the shortening of the space between its coils as its ends move toward each other and a lengthening of the space as the ends move apart. Back

  35. Atmospheric absorption. Wavelength regions where the atmosphere is essentially transparent, such as the visible spectrum, are called atmospheric windows. Wavelengths and atmosphere not drawn to scale. Back

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