Schmucker-Weidelt Lecture Notes, Aarhus, 1975 - MTNet
Schmucker-Weidelt Lecture Notes, Aarhus, 1975 - MTNet Schmucker-Weidelt Lecture Notes, Aarhus, 1975 - MTNet
Very rapid oscillations with frequencies between 1 and, say, 100 cps (=Hz) are called - from the radio enginieers point of view - "very - - low - frequency emissions: VLF. Their ampl.itudes lie well below ly. They occur usually intermittendly in "bursts" and are controlled .in their intensity by the general magnetic activity. In exposed shield areas they may penetrate downward a few kilometers, but everywhere else they w i l l be totally attenuated within the very surface layers. - Sudden storm -- commencements and sclar flare effects: The begin of a magnetic storm is usually marked by strong deflections in H and Z up to 100y within one or two minutes.. This so--called "sudden - - storm - commencemen-t" SSC, signals. the inward :notion of the magnetopause (separating the magnetosphere from the interplanetary space) under the impact of a suddenly increased solar wind intensity. SSC's are a world wide, s imultaneous1.y occuring phenornenon. They are, however, too rarely occuring events (1 per month) for induction studies. The momen-tarily increased solar wave radiation, caused by sun spot e: eruptions, produces a shortlived (5 minutes) in'tensificatrion of the Sq-system, its magnetic effect is called a "sol.ar flare event". It: measures a few gammas and like the ssc is a rarely observed varia- tion type.
Overall - depth - distribution -. Denth of penetation of resistivity . . & ~ n ] (0) : oceans (s) : sedimentary basins (c) : exposed crys-talline EEJ: PEJ: mid-latitude obs erva-t ions equatorj.al. e1.ec'tr.c polar electz~ojet
- Page 51 and 52: and y can again be so adjusted that
- Page 53 and 54: 4.2. In3ral - --- equation method L
- Page 55 and 56: The element GZx is needed for all z
- Page 57 and 58: With this knowledge of the behaviou
- Page 59 and 60: After having determined Qzr VJ,; @,
- Page 61 and 62: 4.3. The surface inteyral approach
- Page 63 and 64: F At the vertical boundaries the co
- Page 65 and 66: The four equations A A A A H = i sg
- Page 68 and 69: 6. Approaches to the inverse proble
- Page 70 and 71: to minimize the quantity a s = 12 /
- Page 72 and 73: It remains to show a way to minimiz
- Page 74 and 75: Agai-n, from a finite erroneous dat
- Page 76 and 77: Here lJ - is a N x P matrix contain
- Page 78 and 79: small eigenvalues. The parameter ve
- Page 80 and 81: Then - 77 - A(E2 - E ) = iwu U (E -
- Page 82 and 83: whence 2k d -2k d where a = CA:(A;)
- Page 84 and 85: . 7. Basic concepts of geomagnetic
- Page 86 and 87: orders of magnitude smaller' than t
- Page 88 and 89: Elimination of - E or .,. H yields
- Page 90 and 91: Observing that rot pot rot g = - ro
- Page 92 and 93: Two special types of such anomalies
- Page 94 and 95: Model : wo+ Solution for uniform ha
- Page 96 and 97: parameter u and that the pressure d
- Page 98 and 99: (=disturbed)-variations: After magn
- Page 100 and 101: with 4 as geographic latitude. From
- Page 104 and 105: ! 8. Data Collection - and Analysis
- Page 106 and 107: A horizontal electric -- field comp
- Page 108 and 109: For a data reducti.on in the fr3equ
- Page 110 and 111: Let q be the tranfer function betwe
- Page 112 and 113: . A as transfer function between A
- Page 114 and 115: -- Structural soundi~z with station
- Page 116 and 117: Since it follows that - E 1 = - T E
- Page 118 and 119: - - . the same or from different si
- Page 120 and 121: The Fourier integral - +- -io t T -
- Page 122 and 123: The weigh-t . function W is then fo
- Page 124 and 125: Two convenient filters are 3 sinx I
- Page 126 and 127: (e.g. X), their realizations by obs
- Page 128 and 129: Observe that the residual, of which
- Page 130 and 131: Example: n = 12 and @ = 95%: 1 n =
- Page 132 and 133: - As a consequence, the real and im
- Page 134 and 135: This relati-on implies .that .the l
- Page 136 and 137: 9. --- Data 5.nterpretatj.on on the
- Page 138 and 139: The "modified apparent - - resistiv
- Page 140 and 141: Exercise Geomagne-tic varj.ations.
- Page 142 and 143: 9.2 Layered Sphere - The sphericity
- Page 144 and 145: The field within the conducting sph
- Page 146 and 147: and An algorithm for the direct pro
- Page 148 and 149: with I - and- a = gn g-n I 1 6-n-1
- Page 150 and 151: with ~ = - T E + as sheet current d
Very rapid oscillations with frequencies between 1 and, say, 100 cps<br />
(=Hz) are called - from the radio enginieers point of view -<br />
"very - - low - frequency emissions: VLF. Their ampl.itudes lie well below<br />
ly. They occur usually intermittendly in "bursts" and are controlled<br />
.in their intensity by the general magnetic activity. In exposed<br />
shield areas they may penetrate downward a few kilometers, but<br />
everywhere else they w i l l be totally attenuated within the very<br />
surface layers.<br />
- Sudden storm -- commencements and sclar flare effects: The begin of a<br />
magnetic storm is usually marked by strong deflections in H and Z<br />
up to 100y within one or two minutes.. This so--called "sudden - - storm<br />
-<br />
commencemen-t" SSC, signals. the inward :notion of the magnetopause<br />
(separating the magnetosphere from the interplanetary space) under<br />
the impact of a suddenly increased solar wind intensity. SSC's<br />
are a world wide, s imultaneous1.y occuring phenornenon. They are,<br />
however, too rarely occuring events (1 per month) for induction<br />
studies.<br />
The momen-tarily increased solar wave radiation, caused by sun spot<br />
e: eruptions, produces a shortlived (5 minutes) in'tensificatrion of the<br />
Sq-system, its magnetic effect is called a "sol.ar flare event". It:<br />
measures a few gammas and like the ssc is a rarely observed varia-<br />
tion type.