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Hydromagnetic waves in Earth's core and their influence on ...

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18 Chapter 2 — Space-time analysisFigure 2.1: Relati<strong>on</strong> of latitude-l<strong>on</strong>gitude maps to time-l<strong>on</strong>gitude(TL) plots.Field values at all gridded l<strong>on</strong>gitudes at a chosen latitude (10 ◦ S here) are taken fromlatitude-l<strong>on</strong>gitude maps at each discrete time <str<strong>on</strong>g>in</str<strong>on</strong>g>terval to c<strong>on</strong>struct time-l<strong>on</strong>gitude plotsat the chosen latitude (the equator <str<strong>on</strong>g>in</str<strong>on</strong>g> this example).of n<strong>on</strong>-axisymmetric field features.Hovmöller (1949) was the first to employ the technique of us<str<strong>on</strong>g>in</str<strong>on</strong>g>g TL plots to studywave moti<strong>on</strong>s <str<strong>on</strong>g>in</str<strong>on</strong>g> a planetary scale rotat<str<strong>on</strong>g>in</str<strong>on</strong>g>g fluid. He c<strong>on</strong>sidered the height of the 500mb pressure level as a tracer field of atmospheric moti<strong>on</strong>s.The result<str<strong>on</strong>g>in</str<strong>on</strong>g>g TL plot isreproduced <str<strong>on</strong>g>in</str<strong>on</strong>g> figure 2.2a. He visually determ<str<strong>on</strong>g>in</str<strong>on</strong>g>ed the azimuthal phase speed of fieldmoti<strong>on</strong>s by follow<str<strong>on</strong>g>in</str<strong>on</strong>g>g the positi<strong>on</strong> of crests <str<strong>on</strong>g>and</str<strong>on</strong>g> troughs 1 (see, for example, the dashedl<str<strong>on</strong>g>in</str<strong>on</strong>g>es <str<strong>on</strong>g>in</str<strong>on</strong>g> figure 2.2a).He <str<strong>on</strong>g>in</str<strong>on</strong>g>ferred an azimuthal group speed by follow<str<strong>on</strong>g>in</str<strong>on</strong>g>g the path oftransmissi<strong>on</strong> of energy (proporti<strong>on</strong>al to squared field amplitude) by identify<str<strong>on</strong>g>in</str<strong>on</strong>g>g pathsal<strong>on</strong>g which field maxima <str<strong>on</strong>g>and</str<strong>on</strong>g> m<str<strong>on</strong>g>in</str<strong>on</strong>g>ima are c<strong>on</strong>sistently observed (see the solid l<str<strong>on</strong>g>in</str<strong>on</strong>g>es <str<strong>on</strong>g>in</str<strong>on</strong>g>figure 2.2a).He used these observati<strong>on</strong>s to test whether the moti<strong>on</strong>s were c<strong>on</strong>sistentwith Rossby’s theory of planetary <str<strong>on</strong>g>waves</str<strong>on</strong>g> 2 <str<strong>on</strong>g>in</str<strong>on</strong>g> the atmosphere (Rossby, 1939), c<strong>on</strong>clud<str<strong>on</strong>g>in</str<strong>on</strong>g>gthis was the case.1 A more sophisticated way to determ<str<strong>on</strong>g>in</str<strong>on</strong>g>e phase speeds, especially useful when energy is present over arange of frequencies <str<strong>on</strong>g>and</str<strong>on</strong>g> wavenumbers, is to filter so that <strong>on</strong>ly a s<str<strong>on</strong>g>in</str<strong>on</strong>g>gle frequency comp<strong>on</strong>ent or wavenumbercomp<strong>on</strong>ent rema<str<strong>on</strong>g>in</str<strong>on</strong>g>s. The azimuthal speed of these features is then the azimuthal phase speed associatedwith that frequency. By perform<str<strong>on</strong>g>in</str<strong>on</strong>g>g this procedure over a range of frequencies or wavenumbers,the dispersi<strong>on</strong> (frequency versus wavenumber) characteristics of the field moti<strong>on</strong> can be determ<str<strong>on</strong>g>in</str<strong>on</strong>g>ed.Azimuthal group speeds associated with the speed of transmissi<strong>on</strong> of energy are often determ<str<strong>on</strong>g>in</str<strong>on</strong>g>ed byfollow<str<strong>on</strong>g>in</str<strong>on</strong>g>g peaks of the square of the field amplitude.2 Planetary (or Rossby) <str<strong>on</strong>g>waves</str<strong>on</strong>g> are large scale, slowly propagat<str<strong>on</strong>g>in</str<strong>on</strong>g>g, <str<strong>on</strong>g>waves</str<strong>on</strong>g> found <str<strong>on</strong>g>in</str<strong>on</strong>g> rotat<str<strong>on</strong>g>in</str<strong>on</strong>g>g fluids.Their existence is a c<strong>on</strong>sequence of the restor<str<strong>on</strong>g>in</str<strong>on</strong>g>g force that arises due to the variati<strong>on</strong> of the Coriolisforce with latitude. Readers unfamiliar with these <str<strong>on</strong>g>waves</str<strong>on</strong>g> should c<strong>on</strong>sult Andrews (2000) for an accessible<str<strong>on</strong>g>in</str<strong>on</strong>g>troductory account.

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