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    <title>NOPR Collection:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/33800</link>
    <description />
    <items>
      <rdf:Seq>
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/33807" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/33806" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/33805" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/33804" />
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    </items>
    <dc:date>2026-10-10T14:56:12Z</dc:date>
  </channel>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/33807">
    <title>Evaluation of capacitance matrix of artificial orbiting satellites</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/33807</link>
    <description>Title: Evaluation of capacitance matrix of artificial orbiting satellites
Authors: Alad, Rizwan H; Chakrabarty, S B
Abstract: &lt;span style="font-size:11.0pt;mso-bidi-font-size:&#xD;
10.0pt;font-family:" times="" new="" roman","serif";mso-fareast-font-family:"times="" roman";="" mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"="" lang="EN-US"&gt;The&#xD;
paper presents the evaluation of capacitance matrix of an artificial orbiting&#xD;
satellite considering a composite metallic structure of a parabolic reflector&#xD;
antenna with cuboid and plates. Integral equations are formed by relating the&#xD;
unknown charge density on the metallic conductor and are solved using the Method&#xD;
of Moments (MoM) in which the pulse functions are used as basis functions and&#xD;
the delta functions are used as testing functions. The surfaces of the&#xD;
conducting structure are meshed using non-uniform triangular patches. The&#xD;
matrix equations are solved by iterative generalized minimum residual (GMRES)&#xD;
algorithm. The numerical data on the capacitance matrix and charge distribution&#xD;
of these structures have been presented. The capacitance of a metallic cuboid&#xD;
is computed to validate the approach.&lt;/span&gt;
Page(s): 199-204</description>
    <dc:date>2015-12-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/33806">
    <title>Equatorial electrojet in the African sector</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/33806</link>
    <description>Title: Equatorial electrojet in the African sector
Authors: Rastogi, R G; Chandra, H
Abstract: &lt;span style="font-size:11.0pt;mso-bidi-font-size:&#xD;
10.0pt;font-family:" times="" new="" roman","serif";mso-fareast-font-family:"times="" roman";="" mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"="" lang="EN-US"&gt;Hourly&#xD;
values of the deviations in the geomagnetic X and Y field at two equatorial&#xD;
electrojet stations in Africa, viz. Freetown (FTN) on the western part and&#xD;
Addis Ababa (AAE) on the eastern part, are studied for three years 1962-64. The&#xD;
declination is almost along the geographic N-S at AAE and 14° towards west of&#xD;
the geographic N-S at FTN. The annual mean daily range in X is around 80 nT at&#xD;
FTN and 70 nT at AAE with peak around 1100 hrs LT. Deviations in Y at FTN show&#xD;
a broad minimum of about -20 nT around noon while the decrease is much&#xD;
smaller at AAE with a minimum of -5 nT at noon. Seasonal mean variations of the&#xD;
daily range in X show almost equal peaks during December solstice and equinox&#xD;
at FTN but at AAE it is highest during equinoctial months and lowest during&#xD;
June solstice. The seasonal asymmetry at FTN could be due to large declination.&#xD;
The equinoctial peak in March - April is higher than the peak in September -&#xD;
October at both the stations. Another notable feature at FTN is the steady&#xD;
increase in deviation in X from about -10 nT at 1800 hrs LT to 10 nT at 0600&#xD;
hrs LT. The direction of the H vector is aligned almost along the geographic&#xD;
N-S for December solstice and equinox at AAE and along 12° W of north during&#xD;
June solstice. At FTN, it is aligned along about 5° W of north during &#xD;
D and E-months and to about 20° W of north during June solstice.&lt;/span&gt;
Page(s): 187-198</description>
    <dc:date>2015-12-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/33805">
    <title>Spread F at tropical latitude stations in India</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/33805</link>
    <description>Title: Spread F at tropical latitude stations in India
Authors: Rastogi, R G; Chandra, H
Abstract: &lt;span style="font-size:11.0pt;mso-bidi-font-size:&#xD;
10.0pt;font-family:" times="" new="" roman","serif";mso-fareast-font-family:"times="" roman";="" mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"="" lang="EN-US"&gt;Regular&#xD;
radio soundings of the ionosphere over Ahmedabad were started in 1953 and&#xD;
several studies describe the various features of the ionosphere close to the&#xD;
equatorial ionization anomaly crest. Finer characteristics of the spread F&#xD;
echoes could not be studied earlier due to the very wide pulse of the&#xD;
transmitter. The characteristics of the spread F at Ahmedabad are described in&#xD;
the present paper using the recordings of recently installed Digisonde during&#xD;
June - July 2012. The spread F echoes at Ahmedabad are not due to the &lt;i&gt;in&#xD;
situ&lt;/i&gt; produced irregularities as at an equatorial station Thumba. The spread&#xD;
F echoes at Ahmedabad during the June solstices of 2012 are due to reflection&#xD;
(not scattering) from the off-vertical direction that produce multiple traces&#xD;
from off-vertical direction overlapping over the main (vertical) h'-f trace,&#xD;
sometimes giving an appearance of diffuse echoes near the critical frequencies.&#xD;
Presence of medium scale traveling ionospheric disturbances (TIDs) could be a&#xD;
possibility to account for such off-vertical reflections.&lt;/span&gt;
Page(s): 177-186</description>
    <dc:date>2015-12-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/33804">
    <title>&lt;span style="font-size:11.0pt;mso-bidi-font-size: 10.0pt;font-family:"Times New Roman","serif";mso-fareast-font-family:"Times New Roman"; mso-ansi-language:EN-GB;mso-fareast-language:EN-US;mso-bidi-language:AR-SA" lang="EN-GB"&gt;Study of O&lt;sup&gt;+&lt;/sup&gt;(&lt;sup&gt;2&lt;/sup&gt;P-&lt;sup&gt;2&lt;/sup&gt;D) 732.0 nm dayglow emission under geomagnetic storm conditions&lt;/span&gt;</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/33804</link>
    <description>Title: &lt;span style="font-size:11.0pt;mso-bidi-font-size: 10.0pt;font-family:"Times New Roman","serif";mso-fareast-font-family:"Times New Roman"; mso-ansi-language:EN-GB;mso-fareast-language:EN-US;mso-bidi-language:AR-SA" lang="EN-GB"&gt;Study of O&lt;sup&gt;+&lt;/sup&gt;(&lt;sup&gt;2&lt;/sup&gt;P-&lt;sup&gt;2&lt;/sup&gt;D) 732.0 nm dayglow emission under geomagnetic storm conditions&lt;/span&gt;
Authors: Dharwan, Maneesha; Singh, Vir
Abstract: &lt;span style="font-size:11.0pt;mso-bidi-font-size:&#xD;
10.0pt;font-family:" times="" new="" roman","serif";mso-fareast-font-family:"times="" roman";="" letter-spacing:-.1pt;mso-ansi-language:en-gb;mso-fareast-language:en-us;="" mso-bidi-language:ar-sa"="" lang="EN-GB"&gt;The effect of geomagnetic storms on &lt;span style="mso-bidi-font-weight:bold"&gt;O&lt;sup&gt;+&lt;/sup&gt;(&lt;sup&gt;2&lt;/sup&gt;P&lt;span style="mso-bidi-font-weight:bold"&gt;-&lt;sup&gt;2&lt;/sup&gt;D&lt;span style="mso-bidi-font-weight:bold"&gt;)&lt;b&gt; &lt;/b&gt;732.0 nm dayglow emission is&#xD;
studied using recently updated photochemical model of Thirupathaiah &lt;i&gt;et al. &lt;/i&gt;[An&#xD;
updated model of O&lt;sup&gt;+&lt;/sup&gt;(&lt;sup&gt;2&lt;/sup&gt;P) 7320 Å dayglow emission, &lt;i style="mso-bidi-font-style:normal"&gt;Indian J Radio Space Phys&lt;/i&gt;, 44 (2015),&#xD;
7]. Three geomagnetic storms, which occurred on 23-27 August 2005, 13-17 April&#xD;
2006 and 1-5 February 2008 are chosen in the present study. A negative&#xD;
correlation is found between the volume emission rate (VER) and the Dst index&#xD;
for all the three geomagnetic storms. The present study shows that the relative&#xD;
variation of VER with respect to the initial value of VER (before the onset of&#xD;
a geomagnetic storm) during the main phase increases above 260 km. It is also&#xD;
found that the altitude of the peak emission rate does not show any appreciable&#xD;
variation with the activity of geomagnetic storm. A positive correlation is&#xD;
found between the zenith intensity and the atomic oxygen number density. The&#xD;
atomic oxygen number density obtained from NRLMSISE-00 model is compared with&#xD;
the measurements of Earle &lt;i&gt;et al. &lt;/i&gt;[Low latitude thermospheric responses&#xD;
to magnetic storms, &lt;i style="mso-bidi-font-style:normal"&gt;J Geophys Res&lt;/i&gt; &lt;i style="mso-bidi-font-style:normal"&gt;(USA)&lt;/i&gt;, 118 (2013), 3866] during a&#xD;
geomagnetic storm. This comparison shows that the atomic oxygen number density&#xD;
as provided by NRLMSISE-00 model is significantly lower than the measured&#xD;
value. Consequently, the atomic oxygen number density is treated as a variable&#xD;
parameter in the photochemical model and its effect on the VER of 732.0 nm&#xD;
dayglow emission is further studied. The zenith intensity is found to increase&#xD;
about 70% even in the case of weakest storm when the atomic oxygen number&#xD;
density is doubled. &lt;span style="mso-bidi-font-weight:bold"&gt;The latitudinal&#xD;
effect on the VER and zenith intensity of 732.0 nm is also studied. It is found&#xD;
that the VER decreases as the latitude increases. The decrease in VER from low&#xD;
to mid latitudes is due to the decrease in atomic oxygen number density with&#xD;
latitude. The zenith intensity at the maximum geomagnetic activity is about 12%&#xD;
higher than the zenith intensity before the start of the geomagnetic storm in&#xD;
equatorial region. However, no appreciable change in the zenith intensity is&#xD;
found at higher latitudes.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 167-176</description>
    <dc:date>2015-12-01T00:00:00Z</dc:date>
  </item>
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