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    <title>NOPR Community:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/35615</link>
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    <pubDate>Fri, 09 Oct 2026 15:16:14 GMT</pubDate>
    <dc:date>2026-10-09T15:16:14Z</dc:date>
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      <title>Size distribution of radar echoes from convective clouds around Delhi during monsoon season</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/35685</link>
      <description>Title: Size distribution of radar echoes from convective clouds around Delhi during monsoon season
Authors: Chatterjee, R N; Ali, K; Prakash, Prem; Majumdar, S C
Abstract: The size distributions of radar echoes from convective clouds observed in Delhi region during each monsoon season of the 6-year period from 1967 to 1972 have been investigated. It has been found that the size distribution of about 99 per cent of the total echoes in each monsoon season and covering echoes up to diameter 35 km (30 km in 1972) are well represented by the exponential distribution N&lt;sub&gt;D&lt;/sub&gt; = &lt;i&gt;a&lt;/i&gt; exp (-&lt;i&gt;b&lt;/i&gt;&lt;img src='http://www.niscair.res.in/jinfo/dbar1.gif' border=0&gt;), where N&lt;sub&gt;D&lt;/sub&gt; is the number of echoes in the diameter interval &lt;i&gt;D&lt;/i&gt; to &lt;i&gt;D&lt;/i&gt; + &lt;img src='/image/spc_char/delta.gif' border=0&gt;&lt;i&gt;D&lt;/i&gt;, &lt;i&gt;&lt;img src='http://www.niscair.res.in/jinfo/dbar1.gif' border=0&gt;&lt;/i&gt; is the mid-value of the interval, i.e. &lt;i&gt;D&lt;/i&gt; + &lt;img src='/image/spc_char/delta.gif' border=0&gt;&lt;i&gt;D&lt;/i&gt;/2, and &lt;i&gt;a&lt;/i&gt; and &lt;i&gt;b&lt;/i&gt; are the coefficients to describe the exponential distribution. The possibility of using these results in connection with the estimation of rain attenuation for millimeter wave propagation has been discussed.
Page(s): 124-128</description>
      <pubDate>Sat, 01 Jun 1996 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/35685</guid>
      <dc:date>1996-06-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Hall and Pedersen conductivities in the auroral ionosphere of Jupiter</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/35684</link>
      <description>Title: Hall and Pedersen conductivities in the auroral ionosphere of Jupiter
Authors: Singhal, R P
Abstract: Hall and Pedersen conductivities in the auroral ionosphere of Jupiter have been calculated. Conductivity profiles are presented for three characteristic energies 10, 30 and 100 keV of the Maxwellian distribution of precipitating particles (electrons). Calculations are performed for three values of the magnetic fields, i.e. for 6, 10 and 14 G. Height integrated conductivities are tabulated. Results are compared with previous estimates. God qualitative agreement is found. It is found that that the major contribution to the conductivities comes from the heavy hydrocarbon ions and not H+ as assumed in some earlier works.
Page(s): 361-366</description>
      <pubDate>Sun, 01 Dec 1996 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/35684</guid>
      <dc:date>1996-12-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Implication of the ionosphere in low latitude micropulsations</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/35683</link>
      <description>Title: Implication of the ionosphere in low latitude micropulsations
Authors: Roy, Manashi
Abstract: The low frequency hydromagnetic waves in the terrestrial magnetosphere, known as geomagnetic micropulsations, have to propagate through the ionosphere before they are detected on the ground. It is generally argued that the polarization suffers a 90° rotation while it crosses the ionosphere. All ground data are analysed on this premise. The arguments put forward to this theory have been briefly reviewed and it has been shown that this is not always true, certainly not in the low latitude ionosphere. A general expression is then derived for the low latitude ionospheric effects demonstrating that the rotation angle is substantially different from &lt;img src='/image/spc_char/pi.gif' border=0&gt;/2. Moreover, the amount of rotation is a function of the direction of the wave field. Since the transformation matrix is a complex quantity the ionosphere also introduces phase change among the two horizontal components. Thus the nature of polarization also changes as the wave penetrates the ionosphere.
Page(s): 356-360</description>
      <pubDate>Sun, 01 Dec 1996 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/35683</guid>
      <dc:date>1996-12-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Wave-particle interactions and charged particle precipitation</title>
      <link>http://nopr.niscpr.res.in/handle/123456789/35682</link>
      <description>Title: Wave-particle interactions and charged particle precipitation
Authors: Singh, U P; Singh, Ashok K; Singh, D P; Singh, R P; Singh, R N
Abstract: The lightning-generated electric field produces ducted whistler mode waves. These short-duration electric fields penetrate to the equator and alter the dynamics of cyclotron resonant interactions between trapped energetic electrons and whistler mode waves. The electric field also enhances pitch angle diffusion which results into enhanced precipitation of charged particles in the upper atmosphere. Numerical results for the precipitation of electrons into different regions of the magnetosphere are discussed. The enhanced precipitating fluxes produce pimples of different sizes in the ionization density at the bottom of the ionosphere which may result in various changes in radio signals propagating in the earth-ionosphre waveguide.
Page(s): 351-355</description>
      <pubDate>Sun, 01 Dec 1996 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://nopr.niscpr.res.in/handle/123456789/35682</guid>
      <dc:date>1996-12-01T00:00:00Z</dc:date>
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