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63 Cards in this Set

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Phases of the moon: New moon?
<img src="Phases of the Moon/Moon_phase_0.png"><br />New Moon (Phase 1 of 8)
Phases of the moon: Waxing Crescent?
<img src="Phases of the Moon/Moon_phase_1.png"><br />Waxing Crescent (Phase 2 of 8)
Phases of the moon: First Quarter?
<img src="Phases of the Moon/Moon_phase_2.png"><br />First Quarter (Phase 3 of 8)
Phases of the moon: Waxing Gibbous?
<img src="Phases of the Moon/Moon_phase_3.png"><br />Waxing Gibbous (Phase 4 of 8)
Phases of the moon: Full Moon?
<img src="Phases of the Moon/Moon_phase_4.png"><br />Full Moon (Phase 5 of 8)
Phases of the moon: Waning Gibbous?
<img src="Phases of the Moon/Moon_phase_5.png"><br />Waning Gibbous (Phase 6 of 8)
Phases of the moon: Last quarter?
<img src="Phases of the Moon/Moon_phase_6.png"><br />Last Quarter (Phase 7 of 8)
Phases of the moon: Waning Crescent?
<img src="Phases of the Moon/Moon_phase_7.png"><br />Waning Crescent (Phase 8 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_0.png">
New Moon (Phase 1 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_1.png">
Waxing Crescent (Phase 2 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_2.png">
First Quarter (Phase 3 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_3.png">
Waxing Gibbous (Phase 4 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_4.png">
Full Moon (Phase 5 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_5.png">
Waning Gibbous (Phase 6 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_6.png">
Last Quarter (Phase 7 of 8)
Phases of the moon:<br /><img src="Phases of the Moon/Moon_phase_7.png">
Waning Crescent (Phase 8 of 8)
Spherical aberration
light reflected from the mirror's edge gets focused to a slightly different point than light reflected from the center
light reflected from the mirror's edge gets focused to a slightly different point than light reflected from the center
Spherical aberration
Astigmatism
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
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
Astigmatism
Coma
stars near the edge of the field look elongated, like comets, while those in the center are sharp points of light
stars near the edge of the field look elongated, like comets, while those in the center are sharp points of light
Coma
telescope's apparent field of view
how much of sky in degres is seen edge-to-edge through the eyepiece alone
how much of sky in degres is seen edge-to-edge through the eyepiece alone
telescope's apparent field of view
telescope's true/real field of view
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
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
telescope's true/real field of view
synodic period
time interval between oppositions
time interval between oppositions
synodic period
sideral period
time interval measured relative to background stars
time interval measured relative to background stars
sideral period
equatorial coordinate system
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
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
equatorial coordinate system
local sideral time of an observer
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
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
local sideral time of an observer
vernal equinox
intersection of celestial equator and the ecliptic
intersection of celestial equator and the ecliptic
vernal equinox
proper motion
transverse velocity, appears as slow, angular change in equatorial coordinates<br><br>u = dtheta/dt =transverse velocity/distance to star
transverse velocity, appears as slow, angular change in equatorial coordinates<br><br>u = dtheta/dt =transverse velocity/distance to star
proper motion
radial velocity
line-of-sight component of a star <br><br>receeding star<br><br>
line-of-sight component of a star <br><br>receeding star<br><br>
radial velocity
Planck Radiation formula -> Radiated power: Stefan-Boltzman Law<br><br><img src="Plank.PNG"><br><br><img src="Stefan.PNG">
integrate over wavelength to get total power radiated
integrate over wavelength to get total power radiated
Planck Radiation formula -> Radiated power: Stefan-Boltzman Law<br><br><img src="Plank.PNG"><br><br><img src="Stefan.PNG">
Planck Radiation Formula -> Wien Displacement Law<br><br><$> \lambda_peak = \frac{0.0029}{T}</$>
Take derivative to find the peak of the distribution
Take derivative to find the peak of the distribution
Planck Radiation Formula -> Wien Displacement Law<br><br><$> \lambda_peak = \frac{0.0029}{T}</$>
Planck Radiation Formula -> Energy density in photons<br><br>Energy density = <$>4/c \sigma T^4</$>
Relate radiated power to energy density
Relate radiated power to energy density
Planck Radiation Formula -> Energy density in photons<br><br>Energy density = <$>4/c \sigma T^4</$>
Planck Radiation -> Radiative Cooling Time<br><br>
Relate time to temperature <br><br><$>t_cooling = \frac{Nk}{2\epsilion \sigma A} [1/T^3_final - 1/T^3_hot]</$>
Stefan-Boltzman Law
<$>\frac{P}{A} = e \sigma (T^4 - T^4_c) j/m^2s</$><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
<$>\frac{P}{A} = e \sigma (T^4 - T^4_c) j/m^2s</$><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
Stefan-Boltzman Law
Plank radiation formula
describes EM radiation in a region is at equalibrium w/ surroundings
describes EM radiation in a region is at equalibrium w/ surroundings
Plank radiation formula
Stefan Boltzmann law
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
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
Stefan Boltzmann law
power
rate of doing work<br><br><$>ML^2/T^3</$>
rate of doing work<br><br><$>ML^2/T^3</$>
power
watt
erg/s
erg/s
watt
dyne
Newton
Newton
dyne
dyne cm<br><br>or<br><br>joule
erg
erg
dyne cm<br><br>or<br><br>joule
Units of work/energy
<$>\frac{ML^2}{T^2}</$>
<$>\frac{ML^2}{T^2}</$>
Units of work/energy