<?xml version="1.0" encoding="UTF-8"?>
<feed xmlns="http://www.w3.org/2005/Atom" xmlns:dc="http://purl.org/dc/elements/1.1/">
  <title>NOPR Collection:</title>
  <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/29689" />
  <subtitle />
  <id>http://nopr.niscpr.res.in/handle/123456789/29689</id>
  <updated>2026-10-10T08:12:03Z</updated>
  <dc:date>2026-10-10T08:12:03Z</dc:date>
  <entry>
    <title>A simple and inexpensive automated pulse programmer for pulsed NMR</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/29783" />
    <author>
      <name>Reddy, V Rajagopal</name>
    </author>
    <author>
      <name>Reddy, P N</name>
    </author>
    <author>
      <name>Reddy, B P N</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/29783</id>
    <updated>2016-07-20T06:37:12Z</updated>
    <published>1996-04-01T00:00:00Z</published>
    <summary type="text">Title: A simple and inexpensive automated pulse programmer for pulsed NMR
Authors: Reddy, V Rajagopal; Reddy, P N; Reddy, B P N
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:arial;mso-ansi-language:en-us;mso-fareast-language:="" en-us;mso-bidi-language:ar-sa"=""&gt;A &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;microcomputer&#xD;
(IBM compatible) controlled flexible pulse programmer has been designed and&#xD;
built for using in pulsed nuclear magnetic resonance (NMR) spectrometer is&#xD;
described. It generates pulse sequences required in NMR to measure spin-lattice&#xD;
relaxation time &lt;i style="mso-bidi-font-style:normal"&gt;T&lt;/i&gt;&lt;sub&gt;1&lt;/sub&gt;,&#xD;
spin-spin relaxation time &lt;i&gt;T&lt;sub&gt;2&lt;/sub&gt; &lt;/i&gt;and spin-lock relaxation time &lt;i&gt;T&lt;/i&gt;&lt;sub&gt;&lt;span style="mso-bidi-font-style:italic"&gt;3&lt;/span&gt;&lt;/sub&gt;&lt;i&gt;. &lt;/i&gt;The pulse sequence&#xD;
parameters like pulse widths, interpulse intervals, repetition times can be&#xD;
programmed with menu driven software. The pulse widths can be varied from 100&#xD;
ns to 6.5 ms in steps of 100 ns. The design and operational features of the&#xD;
pulse programmer are described in this paper. The software, developed in Turbo&#xD;
Basic accepts the pulse sequence parameters from the user and generates the&#xD;
pulse sequences as per the specified values, besides controlling the&#xD;
spectrometer and signal average operations.&lt;/span&gt;&lt;/span&gt;
Page(s): 88-90</summary>
    <dc:date>1996-04-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Characterisation of titania, zirconia and alumina powders for their surface area and pore size distribution</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/29782" />
    <author>
      <name>Seshadri, K S</name>
    </author>
    <author>
      <name>Sumangala, R K</name>
    </author>
    <author>
      <name>Raj, S S</name>
    </author>
    <author>
      <name>Lal, K B</name>
    </author>
    <author>
      <name>Panicker, P K</name>
    </author>
    <author>
      <name>Krishnasamy, V</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/29782</id>
    <updated>2016-07-20T06:37:00Z</updated>
    <published>1996-04-01T00:00:00Z</published>
    <summary type="text">Title: Characterisation of titania, zirconia and alumina powders for their surface area and pore size distribution
Authors: Seshadri, K S; Sumangala, R K; Raj, S S; Lal, K B; Panicker, P K; Krishnasamy, V
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;In order to develop ceramic&#xD;
membranes for treating radioactive liquid effluents titania, zirconia and&#xD;
alumina obtained through hydrolysis of their respective alkoxides, have been&#xD;
characterized for their specific surface area and pore size distribution. The&#xD;
samples are treated over a temperature range of 673-1473 K. In all cases, the&#xD;
specific surface area is found to vary with temperature, with zirconia 234-2 m&lt;sup&gt;2&lt;/sup&gt;/g&#xD;
over temperature range 743-1473K, titania 174-10 and alumina 271-141 m&lt;sup&gt;2&lt;/sup&gt;/g&#xD;
over the temperature 673-1473K. The pore size distribution studies show the&#xD;
peak positions of the pore radius of titania, zirconia and alumina in the range&#xD;
23-45, 19-32 and 18-48 &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;
respectively, in the temperature range studied.&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;
Page(s): 85-87</summary>
    <dc:date>1996-04-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Dielectric permittivity of gall-stones as a function of density</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/29781" />
    <author>
      <name>Singh, Jasvir</name>
    </author>
    <author>
      <name>Bhatti, S S</name>
    </author>
    <author>
      <name>Singh, V R</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/29781</id>
    <updated>2016-07-20T06:36:44Z</updated>
    <published>1996-04-01T00:00:00Z</published>
    <summary type="text">Title: Dielectric permittivity of gall-stones as a function of density
Authors: Singh, Jasvir; Bhatti, S S; Singh, V R
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 dielectric permittivity&#xD;
of different types of gallstones has been determined at 150 kHz frequency at&#xD;
room temperature 28°C. The average values of this parameter for soft, mixed and&#xD;
hard type of gall-stones have been found to be 23.92, 30.31 and 40.03&#xD;
respectively. This has been found to increase as the density of the specimen is&#xD;
increased.&lt;/span&gt;
Page(s): 83-84</summary>
    <dc:date>1996-04-01T00:00:00Z</dc:date>
  </entry>
  <entry>
    <title>Preparation of lanthanum- &lt;i&gt;β&lt;/i&gt;-alumina with high surface area by a homogeneous precipitation method for use as catalyst support</title>
    <link rel="alternate" href="http://nopr.niscpr.res.in/handle/123456789/29780" />
    <author>
      <name>Parida, K M</name>
    </author>
    <author>
      <name>Das, J</name>
    </author>
    <author>
      <name>Rao, S B</name>
    </author>
    <id>http://nopr.niscpr.res.in/handle/123456789/29780</id>
    <updated>2016-07-20T06:29:29Z</updated>
    <published>1996-04-01T00:00:00Z</published>
    <summary type="text">Title: Preparation of lanthanum- &lt;i&gt;β&lt;/i&gt;-alumina with high surface area by a homogeneous precipitation method for use as catalyst support
Authors: Parida, K M; Das, J; Rao, S B
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-bidi-theme-font:minor-bidi;="" mso-ansi-language:en-us;mso-fareast-language:en-us;mso-bidi-language:ar-sa"=""&gt;Samples&#xD;
containing mixtures of 5 mol % La&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt; and 95 mol % Al&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;3&lt;/sub&gt;&#xD;
were prepared by homogeneous precipitation method with or without the presence&#xD;
of various anions, and calcined at different temperatures in the range of&#xD;
873-1473 K. Sample prepared by urea hydrolysis in the absence of anions, and&#xD;
calcined at about 1273 K results in the formation of pure lanthanum-&lt;i style="mso-bidi-font-style:normal"&gt;β&lt;/i&gt;-alumina (LBA) with high surface area.&#xD;
However, in the presence of additive anions, the formation of LBA is retarded.&lt;/span&gt;
Page(s): 79-82</summary>
    <dc:date>1996-04-01T00:00:00Z</dc:date>
  </entry>
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