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Lecture 1 - basic astronomy

Course: AST 1002, Fall 2009
School: University of Florida
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Introduction An to Radio Astronomy Lecture 1 some basic astronomy Where on earth.? Far out in the uncharted backwaters of the unfashionable end of the western spiral arm of the Galaxy lies a small unregarded yellow sun. Orbiting this at a distance of roughly ninety-two million miles is an utterly insignificant little blue green planet whose apedescended life forms are so amazingly primitive that they still...

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Introduction An to Radio Astronomy Lecture 1 some basic astronomy Where on earth.? Far out in the uncharted backwaters of the unfashionable end of the western spiral arm of the Galaxy lies a small unregarded yellow sun. Orbiting this at a distance of roughly ninety-two million miles is an utterly insignificant little blue green planet whose apedescended life forms are so amazingly primitive that they still think digital watches are a pretty neat idea. D Adams, The Hitch Hikers Guide to the Galaxy, Random House 1979. The solar system sizes to scale, relative distance to sun not. (NASA, Wikipedia). Early history of astronomy Astronomy is a natural science studying celestial objects (stars, planets, comets, galaxies etc) and extraterrestrial phenomena (CMBR). One of the oldest sciences prehistoric cultures left artefacts (Stonehenge). Early civilizations (Babylonians, Greeks, Chinese, Indians, and Maya) made methodical observations of night sky. Invention of telescope (1608) required before the modern science could develop. Our galaxy Spiral galaxy, approximately 100 000 light years diameter. Solar system located approx 30 000 light years from core. Geocentric vs. Heliocentric models Until early 17th century (Kepler, Galilei) geocentricity ruled (although sun-centred models had been proposed in 3rd century BC). Even today, many astronomical concepts (celestial sphere) are essentially geocentric. 1568 illustration of Ptolemaic geocentric system Modern science From 17th century, rapid developments. Newton Principia of 1687 laid foundations of celestial mechanics; also developed reflecting telescope (1668). Lacaille produced extensive star catalogues. Herschel discovered Uranus in 1781. Euler et al worked on three body problem; improved by Lagrange and Laplace; improved predictions of orbital motion. 19th century advances in spectroscopy and photography impacted on astronomy. 20th century Existence of our own galaxy, Milky Way, only proven in 20th century! Other galaxies then found - and expansion of the Universe. Exotic objects discovered: quasars, pulsars. Exotic predictions made: black holes, neutron stars. Cosmology made great strides (Big Bank, CMBR). Observational astronomy added new parts of EM spectrum: Radio IR Optical (traditional) UV X-ray Gamma-ray Some basics of the Earth Located 149.7 million km from sun - 1 AU (by defn). Mean diameter 12 742 km. Orbit around sun in 365.24 sidereal days (leap years every 4 years, unless divisible by 100 and not divisible by 400!) Axis tilted approx 23.5 degrees relative to plane of ecliptic. The Earth, see from Apollo 17 The orbit of the earth Note that the direction of earths rotation (west to east) is in the same direction as its orbit around the sun (a prograde orbit). Solar vs sidereal days Because the Earth rotates both about its own axis, and about the sun, the solar day (between the sun at its highest) and sidereal day (stars ditto) differ (by approx 1 degree - 4 min - per day, or one day in the year). Earth (solar) time The day as we use it is actually the mean solar day, averaged over the year. Because firstly, the earth moves in a slightly elliptical orbit, and secondly, the earths axis is tilted relative to its plane of orbit, the length of the true solar day actually varies (noticeably) during the year. Near the Dec solstice, the day is lengthened by about 30 seconds; near the March (and Sept) equinoxes, shortened by about 18 (21) secs. Result is that local noon is not constant (by our clocks) during the year; for instance, latest sunset in the W Cape occurs well into January (not midsummers day). Sunrise, sunset and length of day in Cape Town The equation of time This equation gives the difference between apparent solar time (i.e. measured with a sundial) and mean solar time. Negative means the sun is slow, i.e. noon is delayed and the sun sets later. Eqn of time (contd) As noted, it is due to two superimposed effects with different periods: The ellipticity of the earths orbit (dark dash-dot; annual period) The inclined axis of rotation of the earth (mauve broken line, biannual period). Rgd former, earths moves fastest at perihelion (closest to earth) and slowest at aphelion around 4 mins of arc per day difference. Eqn of time (contd 2) Even if the earth moved at constant speed, the apparent motion of the sun would still vary. See below and opp, central (1) is vernal equinox, ditto (2) summer solstice (N.H.) Location on earth Lines of latitude and longitude provide location in a variant of essentially spherical coordinates here, (,). Prime meridian runs through Royal Observatory, Greenwhich. (Selected 1884). Determining latitude and longitude (pre-GPS) Latitude can be determined from altitude of celestial pole (=latitude). At sea, this is done by observing the sun's angle at noon (i.e., it when reached its highest point in the sky, or culmination). Longitude is more difficult. On land, can be determined from transit (crossing the meridian) of star with accurately measured coordinates. At sea, needs accurate knowledge of UTC (GMT); combined with measure of local noon, gives longitude. Until mid 18th century, clocks not sufficiently accurate (invention of marine chronometers). The celestial sphere and spherical (positional) astronomy (location in the heavens) The celestial sphere is an imaginary sphere of arbitrarily large radius, concentric with the Earth and rotating upon the same axis. All objects in the sky can be thought of as projected upon the celestial sphere. Projected upward from Earth's equator and poles are the celestial equator and the celestial poles. In geocentric models, celestial sphere was viewed as a physical reality rather than a geometrical projection. Celestial coordinate systems Horizon system of coordinates Equatorial coordinates Ecliptic coordinates Galactic coordinates Horizon system of coordinates Plane through observing point parallel to local horizon is plane of reference. Zenith is point overhead. Nadir is point underfoot. Coordinates given by azimuth (ref: N, clockwise) and altitude (ref: horizon). Meridian circle is great circle passing through celestial poles and zenith. Useful for altazimuth mounting (telescope steerable around vertical and horizontal axes). Equatorial coordinates Right ascension (abbrev. RA; symbol ) and declination, (abbrev. dec; symbol ) are the astronomical terms for the two coordinates of a point on the celestial sphere when using the equatorial coordinate system. Declination Declination in astronomy is comparable to geographic latitude, but projected onto the celestial sphere. Declination is measured in degrees north and south of the celestial equator. Points N of the celestial equator have positive declinations, while those S have negative declinations. Right ascension Right ascension is the celestial equivalent of terrestrial longitude . Both and measure an angle that increases toward the east as measured from a zero point on an equator. For former, the zero point is the Prime Meridian on the geographic equator. For latter, the zero point is known as the first point of Aries (for historical reasons Aries has shifted over the years), which is the place in the sky where the Sun crosses the celestial equator at the March equinox. customarily measured in hours, minutes, and seconds, with 24 hours being equivalent to a full circle (360 degrees). 1 hour of right ascension = 124 of 360, or 15 degrees of arc; 1 of = 15 of arc, etc. Hour angle Another astronomical term is hour angle. The hour angle (HA) of an object is equal to the difference between the current local sidereal time (LST) and the right ascension () of that object: HA = LST Thus, the object's hour angle indicates how much sidereal time has passed (or is still to pass, if negative) since the object was (or will be) on the local meridian. Movement of heavenly bodies For an observer on earth, stars etc appear to move in circular paths. Depending on the latitude of the observer and the declination of the object, it may: rise and set; remain visible continuously (circumpolar); or remain entirely below the horizon. Rising and setting of stars Assume that stars etc are fixed to inner surface of CS. As earth rotates about p1-p2 from W to E, stars appear to move in opposite direction, and in a circular motion. Assuming observers view unobstructed, his horizon is plane X-Y. Rising and setting contd. which when drawn to scale (as CS is at infinity) is great circle NESW (note that this depends on latitude). Star on celestial equator rises in east at E, sets at W, with equal time above and below horizon. Star A1 is visible for shorter time; A2 for more; stars above small circle NT are always visible (to this observer). Celestial horizon depends on observers latitude (sketch is for one in N. Europe). Astronomical distances Astronomical distances are enormous. Common measurements: Astronomical unit (distance earth-sun: 149.7 million km, 500 light seconds) Light years (closest star Alpha Centauri, 4.3 light years) Parsecs (closest star just over 1pc) Parsecs The parsec (parallax of one arcsecond; symbol: pc) is a unit of length, equal to just under 31 trillion (311012) kilometres (about 19 trillion miles), 206265 AU, or about 3.26 light-years. Defined as the length of the adjacent side of an imaginary right triangle in space. The two dimensions that specify this triangle are the parallax angle (defined as 1 arcsecond) and the opposite side (defined as 1 astronomical unit (AU), the distance from the Earth to the Sun). d=1/p, where d is the distance in pc, and p is the parallex angle, in sec of arc. Hyperdrive, worm holes etc
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University of Florida - AST - 1002
University of Florida - AST - 1002
University of Florida - AST - 1002
University of Florida - AST - 1002
University of Florida - AST - 1002
University of Florida - AST - 1002
University of Florida - AST - 1002
University of Florida - MAC - 2234
QUIZ #1A 9a x 4a zB 8a x 6a zQ1: Find the cross product of the vectors A and Ba 9a x 4a z 8a x 6a z 54(a x) 32(a z ) 86a y a xza yayQ2: Find the dot product of the vectors A and B 9a x 4a z 8a x 6a z 72 24 48Q3: Convert the cylindrical coordin
University of Florida - MAC - 2234
= 3y + 8zQUIZ #1 = 5y 2zQ1: Find the dot product of the vectors and . = 3 5 + 8 (2) = 1Q2: Find the cross product of the vectors and .x y z = 0 38 = x (3 (2) 5 8) + y (8 0 (2) 0) + z (0 5 0 3) = 46x0 5 2Q3: Convert the rectangular coordinates o
University of Florida - MAC - 2234
A 5a x 3a yB 4a x 11a yQUIZ #1Q1: Find the cross product of the vectors A and B(5a x 3a y ) ( 4a x 11a y ) 55a z 12( a z ) 67a zQ2: Find the dot product of the vectors A and B(5a x 3a y ) ( 4a x 11a y ) 20 33 13Q3: Convert the cylindrical coordinat
University of Florida - MAC - 2234
QUIZ #2Q1: What is the total charge Q on the following finite surface 2 m, 1.5 , 0.5 z 0.5 mcharged with a uniform density s = 1012 C/m2.Q s 0.5 ( zmax zmin ) 1012 0.5 2 1 1012 CQ2: Find the E field vector (in RCS) at the point P(0,0,0) due toan inf
University of Florida - MAC - 2234
QUIZ #2Q1: What is the total charge Q in the volume0 r 0.1 m, 0 / 2, 0 2if the volume charge density v is constant and equal to 1012 C/m3.2 1512 1 43Q = v v = 10 10 =10 C233r30Q2: Find the flux density vector D (in RCS) at the point P(0,0,0)
University of Florida - MAC - 2234
QUIZ #2Q1: What is the total charge Q in the volume0 0.05 m, 0 / 2, 0.005 z 0.005 mif the volume charge density is v = 1010 C/m3.Q2: Find the E field vector (in RCS) at the point P(0,0,0) due to aninfinite planar charge of density s = 1010 C/m2 distr
University of Florida - MAC - 2234
QUIZ #2Q1: What is the total charge Q in the volume0 0.05 m, 0 / 2, 0.005 z 0.005 mif the volume charge density is uniform and v = 1010 C/m3.25102Q vV 10 ( 0.05 ) 0.01 / 4 1016 19.6 1016 C4Q2: Find the E-field vector (in RCS) at the point P(0,0
University of Florida - MAC - 2234
QUIZ #3Q1: Find the divergence of the following vectorD xa x ya y x 2 ya zDx Dy DzD 1 1 0 0xyzQ2: Find the total flux through a sphere of radius a = 1 m centeredat the origin (0,0,0) due to an infinite uniformly charged line alongthe x axis of
University of Florida - MAC - 2234
QUIZ #3Q1: Find the divergence of the vector D (given below) at the pointP(2, 2, 2). Coordinates are rectangular and in meters.11D = a x za y + 2 a zxy D = 1 / x 2 D P = 1 / 4 = 0.25Q2: An infinite uniformly charged line of density l = 1012 C/mi
University of Florida - MAC - 2234
QUIZ #3Q1: Find the charge density v if the flux density vector is givenin CCS as D ( 1a 2 a za z ) 1012 , C/m2 .11 F FzHelp: F ( F ) zQ2: The point charge Q1 = 1 pC is located at the point (0,0,0) andthe point charge Q2 = 5 pC is located at
University of Florida - MAC - 2234
QUIZ #3Q1: Find the charge density v if the flux density vector is givenin CCS as D ( 1a 2 a za z ) 1012 , C/m2 .11 D Dz v D( D )(001)1012 1 pC/m 3 zQ2: The point charge Q1 = 1 pC is located at the point (0,0,0) andthe point charge Q2 = 5 pC i
University of Florida - MAC - 2234
QUIZ #4Q1: The E-field inside a parallel-plate capacitor has magnitude 1kV/m. Find the voltage applied to the capacitor if the distancebetween the two plates is 1cm.V E D 1000 0.01 10 VQ2: The potential in a region of space is given as V = 0.5x2+2y,
University of Florida - MAC - 2234
QUIZ #4Q1. The voltage applied to a parallel-plate capacitor is 10 V. If thedistance between the two plates is 1 cm, find the E-field 0.2 cmaway from one of the plates.= 10 / 0.01 1000 VE=Q2. The potential in a region of space is given as V = 0.5x3
University of Florida - MAC - 2234
QUIZ #4Q1: Two infinite large metal plates are placed at z = 1 mm, and z= 2 mm. The voltages applied to the two plates are 3 V and 3 V,respectively. Find the E-field at the origin.Q2: The potential in a region of space is given as V = 5x2 + 2y3 + 2zV
University of Florida - MAC - 2234
QUIZ #4Q1: Two infinite large metal plates are placed at z = 1 mm, and z= 2 mm. The voltages applied to the two plates are 3 V and 3 V,respectively. Find the E-field at the origin.V6E is constant: E a z a z a z 2000 V/m3D3 10Q2: The potential i
University of Florida - MAC - 2234
QUIZ #5Q1: An infinite straight wire with current 0.5 A lies along the xaxis. The current flows in the positive x direction. Find themagnetic field vector H and the flux density vector B at the point P(0,0,0.5) m. ( 0 4 107 H/m)I0.51H a y a y a
University of Florida - MAC - 2234
QUIZ #5Q1: Two infinite straight wires parallel to the x axis are located at y =1 m, z = 0 and y = 2 m, z = 0, respectively. They have the samecurrent of 1 A flowing in the positive x direction. Find the magneticfield vector H and the flux density vec
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 1Orthogonal CoordinateSystems and TransformationsSections: 1.3, 1.4, 1.5, 1.8, 1.9 (1.2, 1.6, 1.7 covered in T01)Homework: See homework fileLECTURE 1 slide 1Coordinates and Position Vector in RCSexamplezPzOP0xPxP ( xP , y P , z P )y
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 2Coulombs Law, Charge DensitySections: 2.1, 2.2, 2.3, 2.4, 2.5Homework: See homework fileLECTURE 2slide1Electric Charge 1The electric charge is a fundamental property of matter. It ismeasured in coulombs (C). The electric-current unit amp
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 3Total Charge:Line, Surface and Volume IntegralsSections: 1.8, 1.9, 2.3Homework: See homework fileLECTURE 3slide1Line Elements 1metric increment due to a differential change in position along a line2-D SPACEpolar CSrectangular CSyya
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 4Vector Superposition:The Field of Standard ChargeDistributionsSections: 2.4, 2.5Homework: See homework fileLECTURE 4slide1E-field of Multiple Sources superposition means adding the individual contributions of sources superposition hold
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 5Electric Flux and Flux Density,Gauss Law in Integral FormSections: 3.1, 3.2, 3.3Homework: See homework fileLECTURE 5slide1Faradays Experiment (1837), Flux charge transfer from inner to outer sphere electric induction: charge deposition
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 6Divergence, Gauss Law inDifferential FormSections: 3.4, 3.5, 3.6, 3.7 (7th ed.) [3.4, 3.5, 3.6 (8th ed.)]Homework: See homework fileLECTURE 6slide1Flux 1flux is the net normal flow of the vector field F through a surface F ds F cos ds c
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 7Electrostatic PotentialSections: 4.1, 4.2, 4.3, 4.4Homework: See homework fileLECTURE 7slide1Work: Definitiondifferential workW F L dW F dL FdL cos Ftotal work done from A to BBW F dL, JdLABLFAwork is positive if the applied f
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 8Electrostatic Field and PotentialGradientSections: 4.5, 4.6Homework: See homework fileLECTURE 8slide1Conservative Property of Potential of Point Charge 1 the potential of a single point charge at the origin depends solelyon the radial d
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 9Electrostatic Energy and EnergyDensitySections: 4.8Homework: See homework fileLECTURE 9slide1Energy of System of Point Charges 1 any system of charged bodies held static in relatively closeproximity contains potential energy the potent
University of Florida - PHY - 2049
LECTURE 10 - Examples
University of Florida - PHY - 2049
Lecture 10Current DensityOhms Law in Differential FormSections: 5.1, 5.2, 5.3Homework: See homework fileLECTURE 10slide1Electric Direct Current ReviewDC is the flow of charge under Coulomb (electrostatic) forces inconductorsGeorg Simon Ohm was
University of Florida - PHY - 2049
Homework: Repeat for an infinite uniform line charge along the x-axis at z = 3, y = 0 (above ground plane).
University of Florida - PHY - 2049
Lecture 11Perfect Conductors, BoundaryConditions, Method of ImagesSections: 5.4, 5.5Homework: See homework fileLECTURE 11slide1Perfect Conductors 1 metals such as Cu, Ag, Al are closely approximated by theconcept of a perfect electric conductor
University of Florida - PHY - 2049
There are no hand-writtenexamples for Lecture 12LECTURE 12slide1
University of Florida - PHY - 2049
Lecture 12Dielectrics: Dipole, PolarizationSections: 4.7, 6.1 (in 8th ed.: 4.7, 5.7)Homework: See homework fileLECTURE 12slide1Electric Dipole and its Dipole Momentelectric dipole: two point charges of equal charge but oppositepolarity in close p
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 13Boundary Conditions atDielectric InterfacesSections: 6.2 (in 8th ed.: 5.8)Homework: See homework fileLECTURE 13slide1BCs for the Tangential Field Components 1 we consider interfaces between two perfect ( = 0) dielectric regions use con
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 14CapacitanceSections: 6.3, 6.4, 6.5 (8th ed.: 6.1, 6.2, 6.3, 6.4)Homework: See homework fileLECTURE 14slide1Definition of Capacitancecapacitance is a measure of the ability of the physical structure toaccumulate electrical free charge un
University of Florida - PHY - 2049
University of Florida - PHY - 2049
Lecture 15Magnetostatic Field Forcesand the Biot-Savart LawSections: 8.1, 9.1, 9.2Homework: See homework fileLECTURE 15slide1Magnetic Forces Review 1Ampres force law (motor equation)LFm IL(a I B), Nmagnetic fluxdensity vectorIBFmforce doe
University of Florida - EEL - 3111
238MICROWAVE AND RF DESIGN: A SYSTEMS APPROACH4.14SummaryIn this chapter a classical treatment of transmission lines was presented.Transmission lines are distributed elements and form the basis of microwavecircuits. A distinguishing feature is they
University of Florida - EEL - 3111
280MICROWAVE AND RF DESIGN: A SYSTEMS APPROACHSlow-Wave ModeThe third possible mode of propagation is the slow-wave mode [76, 77], forwhich the sectional equivalent circuit model of Figure 5-21(d) is applicable.This mode occurs when f is not so large
University of Florida - EEL - 3111
366MICROWAVE AND RF DESIGN: A SYSTEMS APPROACHmade in design, partly because of necessary simplications that mustbe made in modeling, but also because many of the material propertiesrequired in a detailed design can only be approximate. An example is
University of Florida - EEL - 3111
408MICROWAVE AND RF DESIGN: A SYSTEMS APPROACH7.16SummaryMany passive microwave elements exploit particular physical phenomena.Many make use of the characteristics of transmission lines. Each year newvariants of microwave elements are developed and
University of Florida - EEL - 3111
454MICROWAVE AND RF DESIGN: A SYSTEMS APPROACH8.10Exercises1. Repeat the analysis in Example 8.1 on Page419 for the case B = 1/L.2. Develop a two-element matching network forthe source/load conguration shown in theFigure below. The matching networ