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RELATIVISTIC POSITIONING AND NAVIGATION

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Presentation on theme: "RELATIVISTIC POSITIONING AND NAVIGATION"— Presentation transcript:

1 RELATIVISTIC POSITIONING AND NAVIGATION
Angelo Tartaglia RELGRAV

2 How could the Enterprise starship find her way in the universe?
2011 March 03 RELGRAV A. Tartaglia 2

3 How to use a pulsar to find Starbucks
More practical… How to use a pulsar to find Starbucks Cosmic GPS would employ pulsing stars, not satellites, as celestial beacons 2011 March 03 RELGRAV A. Tartaglia 3

4 Coordinates and positioning
Space-time is a 4-dimensional generally curved metric manifold Gaussian coordinates may be used to localize events. 2011 March 03 RELGRAV

5 Emission coordinates time Signals Light cone Clocks 2011 March 03
RELGRAV

6 Null or light coordinates
Cartesian grid Light rays grid 2011 March 03 RELGRAV

7 Null vectors and waves The wave vector:  is a null vector
2011 March 03 RELGRAV

8 The null basis time space 2011 March 03 RELGRAV

9 Positioning in space-time
event light coordinates r space 2011 March 03 RELGRAV

10 Wave fronts hyperplane 2011 March 03 RELGRAV

11 time a b a b space 2011 March 03 RELGRAV

12 Uncertainty volume Tb Td 2011 March 03 RELGRAV

13 Locally uniform motion
Proper time t time Tb Ta space 2011 March 03 RELGRAV

14 Light coordinates of an event
integer From simple linear equations 2011 March 03 RELGRAV

15 2011 March 03 RELGRAV

16 Uncertainty depends on clock
As big as allowed by the linearity of the worldline 2011 March 03 RELGRAV

17 Accelerated motion Four-velocity Four-acceleration
Maximum integration time 2011 March 03 RELGRAV

18 A gravitational field The gravitational field shows up when:
Gravitational potential 2011 March 03 RELGRAV

19 Pulsars as clocks 2011 March 03 RELGRAV

20 Two options X-ray pulsars Radio-pulsars Our choice is radio-pulsars
~ 1800 “clocks” “Fixed” positions in the sky Very stable clocks Periods ≥ 1 ms 2011 March 03 RELGRAV

21 2011 March 03 RELGRAV

22 Parkes observatory (Australia)
2011 March 03 RELGRAV A. Tartaglia 22

23 Four real pulsars 2011 March 03 RELGRAV A. Tartaglia 23

24 Static observer 2011 March 03 RELGRAV A. Tartaglia 24

25 Uncertainties 2011 March 03 RELGRAV A. Tartaglia 25

26 Eppur si muove 2011 March 03 RELGRAV

27 Extension to moving sources
The method can be extended to nearby moving sources as clocks on satellites or on celestial bodies of the Solar system, provided one has the time dependence of the direction cosines of the null basis vectors 2011 March 03 RELGRAV

28 Conclusion The problem of obtaining the local coordinates from the arrival times of pulses from remote sources has been solved The method naturally includes all relativistic effects The method can be applied both to pulsars and to clocks onboard satellites or celestial bodies 2011 March 03 RELGRAV

29 ML. Ruggiero, E. Capolongo, A
ML. Ruggiero, E. Capolongo, A. Tartaglia, Pulsars as celestial beacons to detect the motion of the Earth, IJMPD, in stampa (2011). A. Tartaglia, ML. Ruggiero, E. Capolongo A null frame for spacetime positioning by means of pulsating sources, Advances in Space Research, 47, , 2011. A. Tartaglia , Emission Coordinates for the Navigation in Space, Acta Astronautica, 67, , 2010 D. Bini, A. Geralico, ML. Ruggiero, A. Tartaglia, Emission vs Fermi coordinates: applications to relativistic positioning systems, Classical and Quantum Gravity, 25, 1-11, 2008. ML. Ruggiero, A. Tartaglia, Mapping Cartesian Coordinates into Emission Coordinates: some Toy Models, IJMPD, 17, , 2008. 2011 March 03 RELGRAV


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