Astronomy 2eAstronomyThe birth ofAstronomyChapter Summary2.4 The Birth of Modern AstronomyNicolaus Copernicus introduced the heliocentric cosmology to Renaissance Europe inhis book De Revolutionibus. Although he retained the Aristotelian idea of uniformcircular motion, Copernicus suggested that Earth is a planet and that the planets allcircle about the Sun, dethroning Earth from its position at the center of the universe.Galileo was the father of both modern experimental physics and telescopic astronomy.He studied the acceleration of moving objects and, in 1610, began telescopicobservations, discovering the nature of the Milky Way, the large-scale features of theMoon, the phases of Venus, and four moons of Jupiter, Although he was accused ofheresy for his support of heliocentric cosmology, Galileo is credited with observationsand brilliant writings that convinced most of his scientific contemporaries of the realityof the Copernican theory.2.2 Ancient AstronomyAncient Greeks such as Aristotle recognized that Earth and the Moon are spheres, andunderstood the phases of the Moon, but because of their inability to detect stellarparallax, they rejected the idea that Earth moves. Eratosthenes measured the size ofEarth with surprising precision. Hipparchus carried out many astronomicalobservations, making a star catalog, defining the system of stellar magnitudes, anddiscovering precession from the apparent shift in the position of the north celestialpole. Ptolemy of Alexandria summarized classic astronomy in his Almagest; heexplained planetary motions, including retrograde motion, with remarkably goodaccuracy using a model centered on Earth. This geocentric model, based oncombinations of uniform circular motion using epicycles, was accepted as authority formore than a thousand years.2.3 Astrology and AstronomyThe ancient religion of astrology, with its main contribution to civilization a heightenedinterest in the heavens, began in Babylonia. It reached its peak in the Greco-Romanworld, especially as recorded in the Tetrabiblos of Ptolemy. Natal astrology is based onthe assumption that the positions of the planets at the time of our birth, as describedby a horoscope, determine our future. However, modern test clearly show that there isno evidence for this, even in a broad statistical sense, and there in no verifiable theoryto explain what might cause such an astrological influence.2.1 The Sky AboveThe direct evidence of our senses supports a geocentric perspective, with the celestialsphere pivoting on the celestial poles and rotating about a stationary Earth. We seeonly half of this sphere at one time, limited b the horizon; the point directly overhead isour zenith. The Sun's annual path on the celestial sphere is the ecliptic - a line that runsthrough the center of the zodiac, which is the 18-degree-wide strip of the sky withinwhich we always find the Moon and planets. The celestial sphere is organized into 88constellations, or sectors.3.2 Newton's Great SynthesisIn his Principia, Isaac Newton established the three laws that govern the motion ofobjects: (1) objects continue to be at rest or move with a constant velocity unless actedupon by an outside force; (2) an outside force causes an acceleration (and changes themomentum) for an object; and (3) for every action there is an equal and oppositereaction. Momentum is a measure of the motion of an object and depends on both itsmass and its velocity. Angular momentum is a measure of the motion of a spinning orrevolving object and depends on its mass, velocity and distance from the point aroundwhich it revolves. The density of an object is its mass divided by its volume.Fgravity=GM1 M23.1 The Laws of Planetary MotionTycho Brahe's accurate observations of planetary positions provided the data used byJohannes Kepler to derive his three fundamental laws of planetary motion. Kepler'slaws describe the behavior of planets in their orbits as follows: (1) planetary orbits areellipses with the Sun at one focus; (2) in equal intervals, a planet's orbit sweeps outequal areas; and (3) the relationship between the orbital period (P) and the semimajoraxis (a) of an orbit is given by P² = a³ (when a is units of AU and P is in units of Earthyears).3.6 Gravity with More Than Two BodiesCalculating the gravitational interaction of more than two objects is complicated andrequires large computers. If one object (like the Sun in our solar system) dominatesgravitationally, it is possible to calculate the effects of a second object in terms of smallperturbations. This approach was used by John Couch Adams and Urbain Le Verrier topredict the position of Neptune from its perturbations of the orbit of Uranus and thusdiscover a new planet mathematically.3.5 Motions of Satellites and SpacecraftThe orbit of an artificial satellite depends on the circumstances of its launch. Thecircular satellite velocity needed to orbit Earth's surface is 8 kilometers per second, andthe escape speed from our planet is 11 kilometers per second. There are many possibleinterplanetary trajectories, including those that use gravity-assisted flybys of one objectto redirect the spacecraft toward its next.3.4 Orbits in the Solar SystemThe closes point in a satellite orbit around Earth is its perigee, and the farthest point isits apogee (corresponding to perihelion and aphelion for an orbit around the Sun). Theplanets follow orbits around the Sun that are nearly circular and in the same plane.Most asteroids are found between Mars and Jupiter in the asteroid belt, whereascomets generally follow orbits of high eccentricity.3.3 Newton's Universal Law of GravitationGravity, the attractive force between all masses, is what keeps the planets in orbit.Newton's universal law of gravitation relates the gravitational force to mass anddistance:The force of gravity is what gives us our sense of weight. Unlike mass, which isconstant, weight can vary depending on the force of gravity (or acceleration) you feel.When Kepler's law are reexamined in the light of Newton's gravitational law, it becomeclear that the masses of both objects are important for the third law, which becomes a³ = (M1 + M2) x P². Mutual gravitational effects permit us to calculate the masses ofastronomical objects, from comets to galaxies.Orbits and GravityEarth, Moon& Sky4.1 Earth & SkyThe terrestrial system of latitude and longitude makes use of the great circles calledmeridians. Longitude is arbitrarily set to 0° at the Royal Observatory at Greenwich,England. An analogous celestial coordinate system is called right ascension (RA) anddeclination, with 0° of declination starting at the vernal equinox. These coordinatesystems help us locate any object on the celestial sphere. The Foucault pendulum is away to demonstrate that Earth is turning.4.2 The SeasonsThe familiar cycle of the seasons results from the 23.5° tilt of Earth’s axis of rotation. Atthe summer solstice, the Sun is higher in the sky and its rays strike Earth more directly.The Sun is in the sky for more than half of the day and can heat Earth longer. At thewinter solstice, the Sun is low in the sky and its rays come in at more of an angle; inaddition, it is up for fewer than 12 hours, so those rays have less time to heat. At thevernal and autumnal equinoxes, the Sun is on the celestial equator and we get about12 hours of day and night. The seasons are different at different latitudes.4.3 Keeping TimeThe basic unit of astronomical time is the day—either the solar day (reckoned by theSun) or the sidereal day (reckoned by the stars). Apparent solar time is based on theposition of the Sun in the sky, and mean solar time is based on the average value of asolar day during the year. By international agreement, we define 24 time zones aroundthe world, each with its own standard time. The convention of the International DateLine is necessary to reconcile times on different parts of Earth.4.4 The CalendarThe fundamental problem of the calendar is to reconcile the incommensurable lengthsof the day, month, and year. Most modern calendars, beginning with the Roman (Julian)calendar of the first century BCE, neglect the problem of the month and concentrate onachieving the correct number of days in a year by using such conventions as the leapyear. Today, most of the world has adopted the Gregorian calendar established in 1582while finding ways to coexist with the older lunar calendars’ system of months.4.5 Phases and Motions of the MoonThe Moon’s monthly cycle of phases results from the changing angle of its illuminationby the Sun. The full moon is visible in the sky only during the night; other phases arevisible during the day as well. Because its period of revolution is the same as its periodof rotation, the Moon always keeps the same face toward Earth.4.6 Ocean Tides and the MoonThe twice-daily ocean tides are primarily the result of the Moon’s differential force onthe material of Earth’s crust and ocean. These tidal forces cause ocean water to flowinto two tidal bulges on opposite sides of Earth; each day, Earth rotates through thesebulges. Actual ocean tides are complicated by the additional effects of the Sun and bythe shape of the coasts and ocean basins.4.7 Eclipses of the Sun and MoonThe Sun and Moon have nearly the same angular size (about 1/2°). A solar eclipseoccurs when the Moon moves between the Sun and Earth, casting its shadow on a partof Earth’s surface. If the eclipse is total, the light from the bright disk of the Sun iscompletely blocked, and the solar atmosphere (the corona) comes into view. Solareclipses take place rarely in any one location, but they are among the most spectacularsights in nature. A lunar eclipse takes place when the Moon moves into Earth’s shadow;it is visible (weather permitting) from the entire night hemisphere of Earth.5.2 The Electromagnetic SpectrumThe electromagnetic spectrum consists of gamma rays, X-rays, ultraviolet radiation,visible light, infrared, and radio radiation. Many of these wavelengths cannot penetratethe layers of Earth’s atmosphere and must be observed from space, whereasothers—such as visible light, FM radio and TV—can penetrate to Earth’s surface. Theemission of electromagnetic radiation is intimately connected to the temperature of thesource. The higher the temperature of an idealized emitter of electromagnetic radiation,the shorter is the wavelength at which the maximum amount of radiation is emitted.The mathematical equation describing this relationship is known as Wien’s law:λmax=(3×10⁶)/T. The total power emitted per square meter increases with increasingtemperature. The relationship between emitted energy flux and temperature is knownas the Stefan-Boltzmann law: F=σT⁴5.1 The Behavior of LightJames Clerk Maxwell showed that whenever charged particles change their motion, asthey do in every atom and molecule, they give off waves of energy. Light is one form ofthis electromagnetic radiation. The wavelength of light determines the color of visibleradiation. Wavelength (λ) is related to frequency (f) and the speed of light (c) by theequation c = λf. Electromagnetic radiation sometimes behaves like waves, but at othertimes, it behaves as if it were a particle—a little packet of energy, called a photon. Theapparent brightness of a source of electromagnetic energy decreases with increasingdistance from that source in proportion to the square of the distance—a relationshipknown as the inverse square law.5.6 The Doppler EffectIf an atom is moving toward us when an electron changes orbits and produces aspectral line, we see that line shifted slightly toward the blue of its normal wavelengthin a spectrum. If the atom is moving away, we see the line shifted toward the red. Thisshift is known as the Doppler effect and can be used to measure the radial velocities ofdistant objects.5.5 Formation of Spectral LinesWhen electrons move from a higher energy level to a lower one, photons are emitted,and an emission line can be seen in the spectrum. Absorption lines are seen whenelectrons absorb photons and move to higher energy levels. Since each atom has itsown characteristic set of energy levels, each is associated with a unique pattern ofspectral lines. This allows astronomers to determine what elements are present in thestars and in the clouds of gas and dust among the stars. An atom in its lowest energylevel is in the ground state. If an electron is in an orbit other than the least energeticone possible, the atom is said to be excited. If an atom has lost one or more electrons, itis called an ion and is said to be ionized. The spectra of different ions look different andcan tell astronomers about the temperatures of the sources they are observing.5.4 The Structure of the AtomAtoms consist of a nucleus containing one or more positively charged protons. Allatoms except hydrogen can also contain one or more neutrons in the nucleus.Negatively charged electrons orbit the nucleus. The number of protons defines anelement (hydrogen has one proton, helium has two, and so on) of the atom. Nuclei withthe same number of protons but different numbers of neutrons are different isotopes ofthe same element. In the Bohr model of the atom, electrons on permitted orbits (orenergy levels) don’t give off any electromagnetic radiation. But when electrons go fromlower levels to higher ones, they must absorb a photon of just the right energy, andwhen they go from higher levels to lower ones, they give off a photon of just the rightenergy. The energy of a photon is connected to the frequency of the electromagneticwave it represents by Planck’s formula, E = hf.5.3 Spectroscopy in AstronomyA spectrometer is a device that forms a spectrum, often utilizing the phenomenon ofdispersion. The light from an astronomical source can consist of a continuous spectrum,an emission (bright line) spectrum, or an absorption (dark line) spectrum. Because eachelement leaves its spectral signature in the pattern of lines we observe, spectralanalyses reveal the composition of the Sun and stars.Radiation& Spectrahttps://www.heavens-above.com/skychart2.aspx
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