Astronomy Semester Exam-Things to know: Exam will consist of Chapters 3, 4, 5, 6, 7, 8, 9, 10, 11, 12 and 13. What to know for Chapters 3, 4 and 5 (Radiation, Spectroscopy & Telescopes): Light, Electromagnetic Radiation, Spectroscopy Wavelength Spectrum (long wavelength -> short) ............(low energy -> high energy) Radio (greater than 100 microns- or 100 x 10-6meters) Infrared (between 100 microns and 0.7 micron) Visible (between about 0.7 microns and 0.4 microns) . . . (or between about 700 nanometers(nm) and about 400 nm) Ultraviolet (between about 400 nm and about 10 nm) X-ray (between about 10 nm and about 0.01 nm) Gamma-ray (below 0.01 nm) All electromagnetic radiation travels at the speed of light . . . . . . . (300,000 kilometers/second) Radiation is composed of "photons" (packets of electromagnetic radiation) the "photons" behave as particles sometimes, and as waves at other times wave-particle duality the "photons" have energies related to the "color" or wavelength short wavelengths -> higher energies like gamma rays long wavelengths -> lower energies like radio waves E=hf where E is energy (in Joules) -h is Planck's constant (h = 6.63 x 10 -34Joule seconds) -and f is frequency in 1/sec, or Hz. Photon energies are very small For example, for visible light (0.5 μ m), f = 6 x 1014 /sec wavelength x frequency = velocity = 300,000 km/sec So, E = 4 x 10-19 Joules "Windows" in the atmosphere visible radio Atmosphere is mostly opaque outside these two "windows". Generation of Electromagnetic Radiation o Electromagnetic Radiation is generated by the movement of charged particles Electrons (negative charge) are most important Blackbody Radiation Peak wavelength decreases with temperature (Wien's Law) Total energy output increases with temperature ...........(increases as T4 - Stefan's Law) Surface temperature of the Sun is 6000 K ...........--> peak of spectrum in the visible light Inverse Square Law o o The apparent brightness of a star is inversely proportional to the square of its distance. o o Doppler Effect Wavelength of light from moving object is shifted Moving away -> Red shift Moving toward -> Blue shift Absorption and Emission Lines Absorption lines (dark lines on continuous spectrum) Emission lines (bright lines) o o o Kirchhoff's Laws Continuous spectrum produced by luminous, dense object Absorption-line spectrum produced by cloud of cool gas on a continuous spectrum Emission-line spectrum produced by a low-density, hot gas Atoms and Molecules Bohr Model of the Atom Nucleus Electrons Orbits Energy levels Ionization molecules Photons The particle nature of electromagnetic radiation represents wave-particle duality photons can be absorbed or emitted by an atom, boosting the electron to an excited state (on absorption) or bringing the electron to a lower energy state (on emission) Since only certain energy states of the atom are allowed, only certain wavelengths of photons are emitted or absorbed, explaining the spectral lines. Spectral Analysis Spectroscope o primitive: prism modern: based on diffraction grating Each element has a characteristic spectrum Comparison of absorption and emission lines of sodium Basic Optics Refraction The bending of light as it crosses the boundary from one transparent material to another Red (long wavelength) bends less than blue (short wavelength) o Line Broadening Line broadening is caused by the environment in which the emission or absorption occurs Example of the broadened line Thermal broadening Rotational broadening Collisional broadening Broadening by magnetic fields (Zeeman effect) Telescopes o o Refracting telescope First used by Galileo in early 17th century Uses lenses Limited by weight Chromatic aberration Reflecting telescope Invented around 1660 Optimal mirror is parabolic shape limited by turbulence in the atmosphere best resolution about 1 arc-second Types: Newtonian Cassegrain Telescope Size Light gathering power scales as the area or diameter-squared Resolution scales as the inverse of the diameter . . . . large diameter resolves most finely also scales as the wavelength . . . . radio telescope inherently worse than optical Hubble Space Telescope Launched from the Space Shuttle in 1990 repaired during a Space Shuttle flight in 1993 above the atmosphere CCDs Charge-coupled Devices (CCDs) finely segmented wafer of silicon "electronic" photographic film Active and adaptive optics active telescopes environment and focus are carefully monitored and controlled adaptive optics blurring effects of the atmospheric turbulence are corrected in real time o o o o achieves 0.1 arc-second resolution Radio Telescopes o First work by Jansky (circa 1930) . . . . -->Center of the Milky Way Galaxy Single dish has pretty poor resolution . . . . Since resolution scales with wavelength Interferometry (sharpens image) . . . . --> VLA (Very Large Array in New Mexico) Value of radio astronomy observe objects obscurred by dust in space (PRIMARY VALUE) observe objects that emit strong radio waves but faint visible waves like cool objects newly formed stars observe at all hours of the day and night Infrared Astronomy Can penetrate dust in space Infrared light absorbed by water vapor in atmosphere Aircraft or Space vehicle (or very high, dry location) Ultraviolet, X-ray, and gamma-ray Astronomy Must be done from outer space due to the "opacity" of the atmosphere. o o