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UAG-93: Chapters 1 to 5 - URSI

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FIGURE 20.<br />

F]GURE 21.<br />

FIGURE 22.<br />

FIGURE 23.<br />

Results from 2-parameter valley ca)culations, at dip angles from 0 <strong>to</strong> 90'. 59<br />

Results at two djfferent valley depths, for dip angles from 0 <strong>to</strong> 9Oo. 59<br />

Changes in real height and fitting error as the assumed val1ey depth varies. 60<br />

The virtual-height fitting error as a function of assumed va1ley depth. 61<br />

SECTION IO - THE USE OF POLAN<br />

FIGURE 24. Scal ing points for a typical daytime ionogram.<br />

FIGURE 25. Regions where the 0-ray trace should not be scaled.<br />

7I<br />

71<br />

SECTION 11 - THE PROGRAIiI SCION FOR DIGITISING DATA<br />

FIGURE 26. Ionogram layout for digitising, with "off-scale" areas.<br />

76<br />

APPET{DIX A - THE ACCURACY OF N(h) CALCULATIONS<br />

TABLE A1. Real-height errors for a Chapman 1ayer, with modes 1<br />

TABLE A2. Real-height errors for a parabol ic 1ayer, for modes 1<br />

FIGURE AL. The real height profile used <strong>to</strong> produce a large cusp.<br />

TABLE A3. Irrors produced by a large cusp, for modes 1 <strong>to</strong> 6 of<br />

TABLE A4. Cusp errors obtained with different scaled frequency<br />

'i ntervals.<br />

FIGURE A2. Changes in real height caused by changes in the starting<br />

<strong>to</strong> 7 of POLAN.<br />

<strong>to</strong> 7.<br />

POLAN.<br />

correct i on .<br />

B1<br />

B2<br />

B3<br />

B4<br />

B5<br />

B7<br />

APPENDIX B - DIP ANGLE VARIATIOI{S<br />

FIGURE B1. Relat.ive group delays of the extraord.inary and ordinary rays.<br />

FIGURE 82. The group delay ratio Rx.o as a function of dip ang1e.<br />

FIGURE 83. Polynomial f.its <strong>to</strong> the 0- and X-ray group refractive jndices.<br />

B9<br />

B9<br />

90<br />

TABLE ts1.<br />

Enrors in the calculated real-height profile<br />

92<br />

FIGURE 84. The effect of random errors in a slab start analysis.<br />

FIGURE 85. Division of the group-index integration range, at high dip angles.<br />

FIGURE 86. Errors obtained with accurate virtual-height data at different dip angles.<br />

<strong>93</strong><br />

94<br />

95<br />

APPENOIX C - FH HEIGHT VARIATION<br />

FIGURE Ci.<br />

Measured values of gyrofrequency in the .ionosphere.<br />

96<br />

TABLE Cl.<br />

Changes in real and virtual height of a reflecting 1ayer.<br />

9B<br />

FIGURE C2. Changes in the X-ray virtual height due <strong>to</strong> a decrease in FH.<br />

TABLE C2. The relative group retardation of 0 and X rays.<br />

FIGURE C3. The equivalent mono<strong>to</strong>nic distr.ibution for an underlying 1ayer.<br />

FIGURE C4. Virtual heights for a low layer and its equivalent mono<strong>to</strong>nic djstributjon.<br />

TABLE C4. Errors in the slab start calculation, using fixed values of FH.<br />

FIGURE C5. Night E-region profiles used in developing rules for start calculations.<br />

FIGURE C6. Slab start calculatjons using a fixed value of gyrofrequency.<br />

FIGURE C7. Errors obtained from a model ionogram using different values of FH.<br />

FIGURE CB. The separation of "underlying" and "reflectjon" regions for FH.<br />

99<br />

100<br />

101<br />

101<br />

r02<br />

103<br />

105<br />

105<br />

106

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