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  <channel rdf:about="http://nopr.niscpr.res.in/handle/123456789/29681">
    <title>NOPR Collection:</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/29681</link>
    <description />
    <items>
      <rdf:Seq>
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/29713" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/29709" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/29704" />
        <rdf:li rdf:resource="http://nopr.niscpr.res.in/handle/123456789/29698" />
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    </items>
    <dc:date>2026-10-10T09:33:48Z</dc:date>
  </channel>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/29713">
    <title>Synthesis and characterisation of microcrystalline cellulose powder</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/29713</link>
    <description>Title: Synthesis and characterisation of microcrystalline cellulose powder
Authors: Jeevananda, T; Siddaramaiah
Abstract: The influence of the&#xD;
reaction parameters like concentration of hydrolyzing agent (hydrochloric&#xD;
acid), duration of hydrolysis, and temperature of reaction on the bulk density&#xD;
and particle size of the microcrystalline cellulose powder (MCCP) has been&#xD;
investigated. Linear variation of bulk density of MCCP with respect&#xD;
&#xD;
to hydrochloric acid&#xD;
concentration, duration of hydrolysis and temperature have been observed. The highest&#xD;
bulk density of 0.3918 has been obtained for &lt;span style="mso-bidi-font-style:italic"&gt;4&lt;i&gt;&#xD;
N &lt;/i&gt;HCl, 2 h reaction and 60 ± 2°C temperature. The&#xD;
&#xD;
&lt;span style="font-size:12.0pt;font-family:" times="" new="" roman","serif";mso-fareast-font-family:="" "times="" roman";mso-fareast-theme-font:minor-fareast;color:black;mso-ansi-language:="" en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;bulk density values&#xD;
lie in the range of 0.1265-0.3918 g&lt;span style="font-size:12.0pt;&#xD;
font-family:" times="" new="" roman","serif";mso-fareast-font-family:"times="" roman";="" mso-fareast-theme-font:minor-fareast;color:#242424;mso-ansi-language:en-us;="" mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;/&lt;span style="font-size:12.0pt;font-family:" times="" new="" roman","serif";mso-fareast-font-family:="" "times="" roman";mso-fareast-theme-font:minor-fareast;color:black;mso-ansi-language:="" en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;cm&lt;sup&gt;3&lt;/sup&gt;.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 38-40</description>
    <dc:date>1997-02-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/29709">
    <title>&lt;span style="font-size:11.0pt;line-height:115%; font-family:"Calibri","sans-serif";mso-ascii-theme-font:minor-latin;mso-fareast-font-family: "Times New Roman";mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font: minor-latin;mso-bidi-font-family:"Times New Roman";mso-ansi-language:EN-US; mso-fareast-language:EN-US;mso-bidi-language:AR-SA"&gt;Transport properties of amorphous CuO-Bi&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt; semiconducting pellets&lt;/span&gt;</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/29709</link>
    <description>Title: &lt;span style="font-size:11.0pt;line-height:115%; font-family:"Calibri","sans-serif";mso-ascii-theme-font:minor-latin;mso-fareast-font-family: "Times New Roman";mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font: minor-latin;mso-bidi-font-family:"Times New Roman";mso-ansi-language:EN-US; mso-fareast-language:EN-US;mso-bidi-language:AR-SA"&gt;Transport properties of amorphous CuO-Bi&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt; semiconducting pellets&lt;/span&gt;
Authors: Gawande, W J; Pakade, S V; Yawale, S P; Burghate, D K; Motke, S G
Abstract: &lt;span style="font-size:11.0pt;line-height:115%;&#xD;
font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;mso-fareast-font-family:="" "times="" new="" roman";mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:="" minor-latin;mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;="" mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;The results of measurement&#xD;
of de-electrical conductivity and activation energy have been reported for four&#xD;
different composition of CuO-Bi&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt; glass powder pellets&#xD;
pressed at 50°C in the temperature range of 300 - 493 K. A plot of -log &lt;i&gt;&lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-theme-font:minor-latin;mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;σ&lt;span style="font-size:11.0pt;&#xD;
line-height:115%;font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;="" mso-fareast-font-family:"times="" new="" roman";mso-fareast-theme-font:minor-fareast;="" mso-hansi-theme-font:minor-latin;mso-bidi-font-family:arial;mso-ansi-language:="" en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt; &lt;/span&gt;&lt;/span&gt;&lt;/i&gt;&lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;versus 1/&lt;i&gt;T &lt;/i&gt;shows two different regions of&#xD;
conduction suggesting two types of conduction mechanisms switching from one&#xD;
type to another occurring at Rnee temperature. The de-conductivity increases&#xD;
with increase in temperature of the sample and also with increase of mol% of&#xD;
CuO. Activation energy calculated for both regions (LTR and HTR) is below 1 eV,&#xD;
thus the electrical conduction is electronic. Activation energy decreases with&#xD;
increase of mol% of CuO. Non-adiabatic hopping conduction was observed in the&#xD;
sample. A plot of dielectric constant versus log of frequency shows zig-zag&#xD;
nature. Dielectric constant decreases with increase in mol% of CuO.&lt;/span&gt;&lt;/span&gt;
Page(s): 33-37</description>
    <dc:date>1997-02-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/29704">
    <title>Transport properties of zinc-bismuth oxide glasses</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/29704</link>
    <description>Title: Transport properties of zinc-bismuth oxide glasses
Authors: Dhote, D S; Pakade, S V; Yawale, S P
Abstract: &lt;span style="font-size:11.0pt;line-height:115%;&#xD;
font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;mso-fareast-font-family:="" "times="" new="" roman";mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:="" minor-latin;mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;="" mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;Zinc-bismuth oxide glasses&#xD;
of 10-25 mol% of zinc oxide are prepared having thickness between 0.35-0.42 cm&#xD;
and diameter 0.60-0.95 cm. Physical properties such as density &lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:arial;mso-ansi-language:en-us;mso-fareast-language:en-us;="" mso-bidi-language:ar-sa;mso-bidi-font-style:italic"=""&gt;(&lt;i&gt;d&lt;/i&gt;)&lt;i&gt;, &lt;/i&gt;&lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;molar volume &lt;span style="font-size:11.0pt;&#xD;
line-height:115%;font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;="" mso-fareast-font-family:"times="" new="" roman";mso-fareast-theme-font:minor-fareast;="" mso-hansi-theme-font:minor-latin;mso-bidi-font-family:arial;mso-ansi-language:="" en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa;mso-bidi-font-style:="" italic"=""&gt;(&lt;i&gt;V&lt;/i&gt;)&lt;i&gt;,&lt;/i&gt;&lt;span style="font-size:11.0pt;line-height:&#xD;
115%;font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;="" mso-fareast-font-family:"times="" new="" roman";mso-fareast-theme-font:minor-fareast;="" mso-hansi-theme-font:minor-latin;mso-bidi-font-family:"times="" roman";="" mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt; hopping&#xD;
distance &lt;span style="font-size:11.0pt;line-height:115%;font-family:&#xD;
" calibri","sans-serif";mso-ascii-theme-font:minor-latin;mso-fareast-font-family:="" "times="" new="" roman";mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:="" minor-latin;mso-bidi-font-family:arial;mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa;mso-bidi-font-style:italic"=""&gt;(&lt;i&gt;R&lt;/i&gt;)&lt;i&gt;, &lt;/i&gt;&lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;number of ions per cc &lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:arial;mso-ansi-language:en-us;mso-fareast-language:en-us;="" mso-bidi-language:ar-sa;mso-bidi-font-style:italic"=""&gt;(&lt;i&gt;N&lt;/i&gt;)&lt;i&gt; &lt;/i&gt;&lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;and polaron radius &lt;span style="mso-bidi-font-style:&#xD;
italic"&gt;(&lt;i&gt;r&lt;sub&gt;p&lt;/sub&gt;&lt;/i&gt;)&lt;i&gt; &lt;/i&gt;are also reported. Polaron radius&#xD;
is found around 1.85 &lt;span style="font-size:11.0pt;line-height:115%;&#xD;
font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;mso-fareast-font-family:="" "times="" new="" roman";mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:="" minor-latin;mso-bidi-theme-font:minor-latin;mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;Å&lt;span style="font-size:11.0pt;&#xD;
line-height:115%;font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;="" mso-fareast-font-family:"times="" new="" roman";mso-fareast-theme-font:minor-fareast;="" mso-hansi-theme-font:minor-latin;mso-bidi-font-family:"times="" roman";="" mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;&#xD;
which shows formation of small polarons. Measurements of de electrical conductivity&#xD;
are reported in the temperature range 443-573K. - Log &lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-theme-font:minor-latin;mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;σ&lt;span style="font-size:11.0pt;&#xD;
line-height:115%;font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;="" mso-fareast-font-family:"times="" new="" roman";mso-fareast-theme-font:minor-fareast;="" mso-hansi-theme-font:minor-latin;mso-bidi-font-family:"times="" roman";="" mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;&#xD;
versus &lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:arial;mso-ansi-language:en-us;mso-fareast-language:en-us;="" mso-bidi-language:ar-sa;mso-bidi-font-style:italic"=""&gt;1&lt;i&gt;/T &lt;/i&gt;&lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;and –log µ versus 1/&lt;i&gt;T &lt;/i&gt;plots exhibited&#xD;
linearity. Hopping condition given by Holstein was applied. Polaron band-width &lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:arial;mso-ansi-language:en-us;mso-fareast-language:en-us;="" mso-bidi-language:ar-sa;mso-bidi-font-style:italic"=""&gt;(&lt;i&gt;J&lt;/i&gt;)&lt;i&gt; &lt;/i&gt;&lt;span style="font-size:11.0pt;line-height:115%;font-family:" calibri","sans-serif";="" mso-ascii-theme-font:minor-latin;mso-fareast-font-family:"times="" new="" roman";="" mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:minor-latin;="" mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;satisfies the inequality which shows adiabatic&#xD;
hopping conduction. The density of Fermi level and the density of localized&#xD;
states are found to be close to each other.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 28-32</description>
    <dc:date>1997-02-01T00:00:00Z</dc:date>
  </item>
  <item rdf:about="http://nopr.niscpr.res.in/handle/123456789/29698">
    <title>Software reliability modeling and decision making: An approach*</title>
    <link>http://nopr.niscpr.res.in/handle/123456789/29698</link>
    <description>Title: Software reliability modeling and decision making: An approach*
Authors: Goyal, Rajesh
Abstract: &lt;span style="font-size:11.0pt;line-height:115%;&#xD;
font-family:" calibri","sans-serif";mso-ascii-theme-font:minor-latin;mso-fareast-font-family:="" "times="" new="" roman";mso-fareast-theme-font:minor-fareast;mso-hansi-theme-font:="" minor-latin;mso-bidi-font-family:"times="" roman";mso-ansi-language:en-us;="" mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;The aim of this paper is to&#xD;
briefly discuss, the available models for evaluating the reliability of software,&#xD;
along with their assumptions/limitations. This assessment shall finally give a&#xD;
step-by-step procedure for fitting a model to software failure data in order to&#xD;
obtain estimates of performance measures like undetected errors, mean time&#xD;
between failures and software reliability. This approach will help in deciding,&#xD;
whether the system is ready for release, or how much more testing still needs to&#xD;
be done?&lt;/span&gt;
Page(s): 21-27</description>
    <dc:date>1997-02-01T00:00:00Z</dc:date>
  </item>
</rdf:RDF>

