Page 4 - 83 basic knowledge of astronomy
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2    Various Classifications of Astronomical Ra-
                           dio Sources


                      There are several ways to classify astronomical radio sources. Typical clas-
                      sifications are:

                         •    – Thermal source
                                 Source emitting via a thermal mechanism (e.g. blackbody radia-
                                 tion),
                              – Non-thermal source
                                 Source emitting via a non-thermal mechanism (e.g. synchrotron
                                 radiation, inverse Compton scattering, annihilation radiation, maser
                                 emission, etc.),

                         •    – Continuum source
                                 Source emitting over a broad range of frequencies,

                              – Spectralline source
                                 Source emitting in narrow lines at specific frequencies,
                           and

                         •    – Galactic source
                                 Source inside our Milky Way Galaxy,
                              – Extragalactic source
                                 Source outside our Galaxy.



                      3    Spectra of Typical Continuum Radio Sources


                      Figure 2 shows typical spectra of continuum radio sources.
                      These spectra are characterized by a quantity called ‘spectral index’ α, de-
                      fined by the formula: S ν ∝ ν    −α , where S ν is a quantity called the ‘flux
                                                               −2
                                                                    −1
                      density’ [unit: Jy (Jansky) ≡ 10 −26 Wm Hz ], which is a measure of the
                      strength of the radiation from a source.
                         Thermal and non–thermal sources usually show different spectral indices,
                      namely:
                           ∼
                        α = −2 for thermal sources,
                      and
                        α ≥ 0 for non-thermal sources.





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