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63 Cards in this Set
- Front
- Back
Phases of the moon: New moon?
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<img src="Phases of the Moon/Moon_phase_0.png"><br />New Moon (Phase 1 of 8)
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Phases of the moon: Waxing Crescent?
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<img src="Phases of the Moon/Moon_phase_1.png"><br />Waxing Crescent (Phase 2 of 8)
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Phases of the moon: First Quarter?
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<img src="Phases of the Moon/Moon_phase_2.png"><br />First Quarter (Phase 3 of 8)
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Phases of the moon: Waxing Gibbous?
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<img src="Phases of the Moon/Moon_phase_3.png"><br />Waxing Gibbous (Phase 4 of 8)
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Phases of the moon: Full Moon?
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<img src="Phases of the Moon/Moon_phase_4.png"><br />Full Moon (Phase 5 of 8)
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Phases of the moon: Waning Gibbous?
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<img src="Phases of the Moon/Moon_phase_5.png"><br />Waning Gibbous (Phase 6 of 8)
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Phases of the moon: Last quarter?
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<img src="Phases of the Moon/Moon_phase_6.png"><br />Last Quarter (Phase 7 of 8)
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Phases of the moon: Waning Crescent?
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<img src="Phases of the Moon/Moon_phase_7.png"><br />Waning Crescent (Phase 8 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_0.png">
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New Moon (Phase 1 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_1.png">
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Waxing Crescent (Phase 2 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_2.png">
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First Quarter (Phase 3 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_3.png">
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Waxing Gibbous (Phase 4 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_4.png">
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Full Moon (Phase 5 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_5.png">
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Waning Gibbous (Phase 6 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_6.png">
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Last Quarter (Phase 7 of 8)
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Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_7.png">
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Waning Crescent (Phase 8 of 8)
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Spherical aberration
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light reflected from the mirror's edge gets focused to a slightly different point than light reflected from the center
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light reflected from the mirror's edge gets focused to a slightly different point than light reflected from the center
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Spherical aberration
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Astigmatism
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the mirror is not ground symmetrically about its center (it might be slightly egg-shaped, for example); star images focus to crosses rather than to points
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the mirror is not ground symmetrically about its center (it might be slightly egg-shaped, for example); star images focus to crosses rather than to points
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Astigmatism
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Coma
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stars near the edge of the field look elongated, like comets, while those in the center are sharp points of light
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stars near the edge of the field look elongated, like comets, while those in the center are sharp points of light
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Coma
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telescope's apparent field of view
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how much of sky in degres is seen edge-to-edge through the eyepiece alone
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how much of sky in degres is seen edge-to-edge through the eyepiece alone
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telescope's apparent field of view
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telescope's true/real field of view
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how much of the sky in degrees can be seen when the eyepiece is in conjunction with a telescope<br><br>true field = apparent field/magnification
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how much of the sky in degrees can be seen when the eyepiece is in conjunction with a telescope<br><br>true field = apparent field/magnification
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telescope's true/real field of view
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synodic period
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time interval between oppositions
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time interval between oppositions
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synodic period
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sideral period
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time interval measured relative to background stars
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time interval measured relative to background stars
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sideral period
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equatorial coordinate system
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based on latitude-longitude system of Earth but does not participate in the planet's rotation<br><br>Declination -> latitude, measured in degrees N & S of equator<br>Right Ascension -> longitude, measured eastward along celestia equatior from vernal equinox to its intersection with object's hour circle (circle through object and north celestial pole), measured in hours, minutes, and seconds
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based on latitude-longitude system of Earth but does not participate in the planet's rotation<br><br>Declination -> latitude, measured in degrees N & S of equator<br>Right Ascension -> longitude, measured eastward along celestia equatior from vernal equinox to its intersection with object's hour circle (circle through object and north celestial pole), measured in hours, minutes, and seconds
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equatorial coordinate system
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local sideral time of an observer
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amount of time that has elapsed since the vernal equinox last traversed the meridian<br><br>also,<br><br>the hour angle of the vernal equinox: angle between a celestial object and the observer's meridian, measured in the direction of the object's motion around the celestial sphere
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amount of time that has elapsed since the vernal equinox last traversed the meridian<br><br>also,<br><br>the hour angle of the vernal equinox: angle between a celestial object and the observer's meridian, measured in the direction of the object's motion around the celestial sphere
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local sideral time of an observer
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vernal equinox
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intersection of celestial equator and the ecliptic
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intersection of celestial equator and the ecliptic
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vernal equinox
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proper motion
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transverse velocity, appears as slow, angular change in equatorial coordinates<br><br>u = dtheta/dt =transverse velocity/distance to star
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transverse velocity, appears as slow, angular change in equatorial coordinates<br><br>u = dtheta/dt =transverse velocity/distance to star
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proper motion
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radial velocity
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line-of-sight component of a star <br><br>receeding star<br><br>
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line-of-sight component of a star <br><br>receeding star<br><br>
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radial velocity
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Planck Radiation formula -> Radiated power: Stefan-Boltzman Law<br><br><img src="Plank.PNG"><br><br><img src="Stefan.PNG">
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integrate over wavelength to get total power radiated
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integrate over wavelength to get total power radiated
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Planck Radiation formula -> Radiated power: Stefan-Boltzman Law<br><br><img src="Plank.PNG"><br><br><img src="Stefan.PNG">
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Planck Radiation Formula -> Wien Displacement Law<br><br><$> \lambda_peak = \frac{0.0029}{T}</$>
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Take derivative to find the peak of the distribution
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Take derivative to find the peak of the distribution
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Planck Radiation Formula -> Wien Displacement Law<br><br><$> \lambda_peak = \frac{0.0029}{T}</$>
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Planck Radiation Formula -> Energy density in photons<br><br>Energy density = <$>4/c \sigma T^4</$>
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Relate radiated power to energy density
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Relate radiated power to energy density
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Planck Radiation Formula -> Energy density in photons<br><br>Energy density = <$>4/c \sigma T^4</$>
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Planck Radiation -> Radiative Cooling Time<br><br>
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Relate time to temperature <br><br><$>t_cooling = \frac{Nk}{2\epsilion \sigma A} [1/T^3_final - 1/T^3_hot]</$>
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Stefan-Boltzman Law
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<$>\frac{P}{A} = e \sigma (T^4 - T^4_c) j/m^2s</$><br><br>e is emissivity (e = 1 for ideal radiator)<br><br>P is net radiated power<br>A is radiating area<br>sigma is Stefans constant<br>T is temp of radiator<br>Tc is temp of surroundings
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<$>\frac{P}{A} = e \sigma (T^4 - T^4_c) j/m^2s</$><br><br>e is emissivity (e = 1 for ideal radiator)<br><br>P is net radiated power<br>A is radiating area<br>sigma is Stefans constant<br>T is temp of radiator<br>Tc is temp of surroundings
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Stefan-Boltzman Law
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Plank radiation formula
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describes EM radiation in a region is at equalibrium w/ surroundings
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describes EM radiation in a region is at equalibrium w/ surroundings
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Plank radiation formula
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Stefan Boltzmann law
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total energy radiated from an area in a region of space<br>energy density can be related to this law by factor of c/4
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total energy radiated from an area in a region of space<br>energy density can be related to this law by factor of c/4
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Stefan Boltzmann law
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power
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rate of doing work<br><br><$>ML^2/T^3</$>
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rate of doing work<br><br><$>ML^2/T^3</$>
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power
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watt
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erg/s
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erg/s
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watt
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dyne
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Newton
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Newton
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dyne
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dyne cm<br><br>or<br><br>joule
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erg
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erg
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dyne cm<br><br>or<br><br>joule
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Units of work/energy
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<$>\frac{ML^2}{T^2}</$>
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<$>\frac{ML^2}{T^2}</$>
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Units of work/energy
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