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  <channel rdf:about="http://nopr.niscpr.res.in/handle/123456789/25555">
    <title>NOPR Collection:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/25555</link>
    <description />
    <items>
      <rdf:Seq>
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/25662" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/25661" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/25660" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/25659" />
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    <dc:date>2026-10-09T06:10:22Z</dc:date>
  </channel>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/25662">
    <title>FTFN based dual inputs current-mode allpass inverse filters</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/25662</link>
    <description>Title: FTFN based dual inputs current-mode allpass inverse filters
Authors: Shah, N A; Malik, M A
Abstract: In this study,&#xD;
four new configurations implementing first-order current-mode allpass inverse&#xD;
filter signals are presented. The proposed generic circuit with two inputs and&#xD;
a single output employs a single FTFN,&#xD;
three resistors&#xD;
and a capacitor with both the inputs supporting the first-order allpass inverse&#xD;
responses separately. The topologies offer high output impedance,&#xD;
&#xD;
which enable&#xD;
easy cascading in current-mode. The realizability condition is simple and&#xD;
temperature invariant, being in the ratio of two grounded resistors. The&#xD;
additional advantage of the circuit is that the phase can be controlled by&#xD;
adjusting the values of passive components without disturbing the realizability&#xD;
condition. The tracking error performance for the filters has also been&#xD;
studied. The simulation results are also included.
Page(s): 206-209</description>
    <dc:date>2005-06-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/25661">
    <title>Potential and field distribution in a cylindrical tube filled with a dielectric material with a centre hole</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/25661</link>
    <description>Title: Potential and field distribution in a cylindrical tube filled with a dielectric material with a centre hole
Authors: Das, B N; Gayen, Arun; Poddar, D R
Abstract: The paper presents&#xD;
a method of analysis of potential and field distribution in a cylindrical tube (metallic),&#xD;
covered at both ends with metallic plates, and containing a dielectric&#xD;
cylindrical shell whose axis coincides with the axis of the cylinder. The cylindrical&#xD;
surface and lower end are maintained at ground potential and the top plate is insulated&#xD;
and maintained at high potential. The resulting Laplace's equation is solved using&#xD;
the method of separation of variables. The constants appear in the resulting equation&#xD;
are found from the boundary conditions followed by representation of the functions&#xD;
satisfying orthogonality condition in cylindrical co-ordinates. If the field&#xD;
intensity exceeds the breakdown limit,&#xD;
&#xD;
&lt;span style="font-size:12.0pt;line-height:115%;font-family:" times="" new="" roman","serif";="" mso-fareast-font-family:"times="" roman";mso-ansi-language:en-in;mso-fareast-language:="" en-in;mso-bidi-language:hi"="" lang="EN-IN"&gt;the resulting breakdown of the gas leads to plasma generation&#xD;
inside the structure, which can provide a convenient method of generation of laser&#xD;
beam.&lt;/span&gt;
Page(s): 197-205</description>
    <dc:date>2005-06-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/25660">
    <title>&lt;span style="font-size:12.0pt;line-height: 115%;font-family:"Times New Roman","serif";mso-fareast-font-family:"Times New Roman"; mso-ansi-language:EN-IN;mso-fareast-language:EN-IN;mso-bidi-language:HI" lang="EN-IN"&gt;Theoretical &lt;i&gt;Z-R &lt;/i&gt;relationship for precipitating systems using Mie scattering approach&lt;/span&gt;</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/25660</link>
    <description>Title: &lt;span style="font-size:12.0pt;line-height: 115%;font-family:"Times New Roman","serif";mso-fareast-font-family:"Times New Roman"; mso-ansi-language:EN-IN;mso-fareast-language:EN-IN;mso-bidi-language:HI" lang="EN-IN"&gt;Theoretical &lt;i&gt;Z-R &lt;/i&gt;relationship for precipitating systems using Mie scattering approach&lt;/span&gt;
Authors: Rao, Usha N; Sarkar, Abhijit; Mohan, M
Abstract: Making use of Mie&#xD;
scattering formulation from the classical electromagnetic theory, backscattering&#xD;
efficiency and radar reflectivity have been derived for a wide range of rain rates.&#xD;
The coefficients of &lt;i&gt;Z-R &lt;/i&gt;(Z = radar reflectivity factor, &lt;i&gt;R &lt;/i&gt;= rain rate,&#xD;
mm/h) relationships have been theoretically computed for 2.84 GHz (used in coastal&#xD;
Doppler radars), 13.8 GHz&#xD;
&#xD;
(used in the space-borne&#xD;
precipitation radar on-board TRMM satellite) and also 35.5 GHz (to be used in&#xD;
the forthcoming Global Precipitation Mission Radar). The Mie scattering results&#xD;
were compared with those obtained in the Rayleigh approximation. In the present&#xD;
work, analyses have been carried out for the well known Marshall-Palmer and Log-normal&#xD;
&#xD;
dropsize distributions.&#xD;
The theoretical approach described here however allows for any other dropsize distribution&#xD;
of precipitating system and operating radar frequency.
Page(s): 191-196</description>
    <dc:date>2005-06-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/25659">
    <title>TEC derived from incoherent scatter measurements during solar maximum and their comparison with IRI-2001 model</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/25659</link>
    <description>Title: TEC derived from incoherent scatter measurements during solar maximum and their comparison with IRI-2001 model
Authors: Sethi, N K; Pandey, V K
Abstract: The diurnal and&#xD;
seasonal variations of the total electron content (TEC), derived from high&#xD;
resolution electron density profiles measured with the Arecibo (18.4°N, 66.7°W,&#xD;
dip 50&lt;sup&gt;o&lt;/sup&gt;N) incoherent scatter radar, are examined during high sunspot&#xD;
activity period (1989-90). Median values of TEC are then obtained at each hour&#xD;
during different seasons and compared with those obtained from the latest&#xD;
available International Reference Ionosphere (IRI-2001) model. The diurnal&#xD;
variations of TEC show more or less similar trend during all the seasons (i.e.&#xD;
maximum around daytime and minimum around midnight) with the largest values of&#xD;
TEC during equinox. The variability of TEC is larger at night than by day during&#xD;
all the seasons. Comparison of the diurnal variation of the observed median&#xD;
values of TEC with those predicted by the IRI model reveals, in general,&#xD;
similar trend during all the seasons and at all local times except during&#xD;
winter, when the IRI exhibits diurnal peak of TEC at around 0900 hrs LT, and&#xD;
the observed median peak occurs at around 1400 hrs LT. Discrepancies between&#xD;
the IRI and the median values exceed 40% during nighttime for winter and&#xD;
equinox. However, during daytime, they are less than 20% for all the seasons,&#xD;
except w inter morning hours. The TEC peak content increases by a factor of&#xD;
around 4 from solar minimum (1975-1 976) to solar maximum (1989-1990).
Page(s): 184-190</description>
    <dc:date>2005-06-01T00:00:00Z</dc:date>
  </item>
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