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Published byMitchell Phelps Modified over 9 years ago
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Signal Propagation Electro-Magnetic Signal Geometric Approximation ~ Fast Particle Approximation Speed of Light in Vacuum
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1-Way Propagation Linear Motion of Photon Fast Motion + Non-Relativistic Source Observer t = t 0 t = t 1 photon
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Passive Observables Arrival Time Incoming Direction Received Wavelength
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Equation of Light Time within Solar System Departure Time Arrival Time Light Time = Travel Time Obtain Light Time S O
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Derivation of Eq. of Light Time Beginning/End of Photon Motion Taking the norm Assumption: Body Motions are known
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Derivation (contd.) Velocity Expression (Newtonian) Velocity Expression (Special Relativity)
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Solving Eq. of Light Time Newton Method
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Approximate Solution Initial Guess: Infinite c = Zero Solution First Newton Corrector Further Correction: General Relativity
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Light Direction Aberration: Observer’s Velocity Parallax: Offset of Observer’s Position Periodic: Annual, Diurnal, Monthly, … Correction for Light Time: within Solar System
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Aberration Finiteness of Speed of Light Bradley (1727) Track of Raindrops on Car’s Side Window
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Annual Aberration Order of Magnitude = Aberration Constant Angle Expression S E0E0 q’q’ E1E1 q vEvE
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Annual Aberration (contd.) Adopting Ecliptic Coordinates Approximate Formula Mean Longitude of Sun: L Aberration Ellipse
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Diurnal Aberration Adopting Equatorial Coordinates Approximate Formula Sidereal Rotation Angle: Q Geocentric Latitude: f
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Parallax Offset of Observer’s Position Bessel (1838): 81 Cyg Direction Difference between L&R Eyes
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Annual Parallax Order of Magnitude = Parallax Angle Expression Sun E S q0q0 q
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Annual Parallax (contd.) Ecliptic Coordinates Approximate Formula 90°Phase Shift from Aberration Parallactic Ellipse
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Diurnal (Geocentric) Parallax Very close objects only: Moon Adopting Equatorial Coordinates Approximate Formula Geocentric Parallax
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Doppler Shift Newtonian Approximation Outgoing = Red shift Incoming = Blue shift
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Approximate Doppler Shift Order of Magnitude = Aberration Constant Annual Doppler Diurnal Doppler
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Propagation Delay/Diffractions Vacuum (= Gravitational) – Wavelength independent Non-Vacuum – Eminent in Radio wavelength – Intrergalactic, Interstellar, Solar corona – Ionospheric, Tropospheric – Atmospheric
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Wavelength-Dependent Delay Cancellation by 2 waves measurements – Geodetic VLBI: S-, X-bands – GPS: L1-, L2-bands – Artificial Satellites: Up- and Down-links Empirical Model – Solar corona, Ionospheric, Tropospheric
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Delay Models Solar Corona (Muhleman and Anderson 1981) Tropospheric (Chao 1970)
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Atmospheric Refraction Variation of Zenith Distance Saastamoinen (1972) P: Pressure in hP, P W : Water Vapor Press. T: Temperature in K z
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Multi-Way Propagation Variation of 1-Way Propagation Series of Light-Time Eq. Ex.: t 3, t 2, t 1, t 0 Transponder Delay – Optical: 0 – Radio: Constant Source Observer Transponder 1 Transponder 2 t0t0 t1t1 t2t2 t3t3
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Round Trip Propagation Typical Active Observation Emission/Arrival Times No Need of Target Motion Info Sum of 1-Way Propagations Cancellation of 1-st Order Effects Observer Target t2t2 t0t0 t1t1
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Round Trip Light Time Approximate Mid-Time Approximate Distance at Mid-Time
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Simultaneous Propagation t2t2 Almost Simultaneous Arrivals Summed Light Time Eq. Light Time of Mid-Point Baseline Vector b Mid-Direction k t1t1 t0t0 Observer 1 Observer 2 Source b k
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Summed Light Time Eq. Approximate Equation
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Simult. Propagation (contd.) t2t2 Differenced Light Time Eq. Arrival Time Delay Baseline Vector b Mid-Direction k t1t1 t0t0 Observer 1 Observer 2 Source b k
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Eq. of Interferometric Obs. Approximate Equation = Equation of VLBI Observation
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