Loading…
Measured Noise Temperature Versus Theoretical Electron Temperature for Gas Discharge Noise Sources
In the past, measured noise temperatures T/sub n/ of a few commercially available gas discharge noise sources were indicated as agreeing with the predicted electron temperature T/sub e/ of the positive column based on the von Engel and Steenbeck relationship. Data were taken over the past 2 years on...
Saved in:
Published in: | IEEE transactions on microwave theory and techniques 1968-09, Vol.16 (9), p.640-645 |
---|---|
Main Author: | |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | cdi_FETCH-LOGICAL-c362t-cbf8cc633e6874e7a472ff234c6c2b65daf584214df5114aacedb355830aff8b3 |
---|---|
cites | cdi_FETCH-LOGICAL-c362t-cbf8cc633e6874e7a472ff234c6c2b65daf584214df5114aacedb355830aff8b3 |
container_end_page | 645 |
container_issue | 9 |
container_start_page | 640 |
container_title | IEEE transactions on microwave theory and techniques |
container_volume | 16 |
creator | Olson, K.W. |
description | In the past, measured noise temperatures T/sub n/ of a few commercially available gas discharge noise sources were indicated as agreeing with the predicted electron temperature T/sub e/ of the positive column based on the von Engel and Steenbeck relationship. Data were taken over the past 2 years on argon tubes over a pressure range of 5 to 40 mm and on neon tubes at 20 mm, with current variations from 100 to 300 mAdc. These data were compared against predicted electron temperatures. For the argon tubes at pressure-radius products greater than 20 mm/spl dot/cm there appeared to be reasonable correlation between the measured noise temperature and the predicted electron temperature although it is suggested that this correlation was fortuitous. For argon pressure-radius products less than 20 mm/spl dot/cm the measured noise temperature was as much as 15 percent lower than the predicted electron temperature. For neon tubes at 20-mm pressure, with the same variation in tube radius, and for pressure-radius products less than 24.0 mm/spl dot/cm, the measured noise temperature differed even more than for argon from the predicted electron temperature. A difference of as much as 30 percent at a pressure-radius product of 3.0 mm/spl dot/cm was observed. A qualitative explanation for argon is presented based mainly on the fact that these discharges do not have a Maxwellian distribution of electron velocities nor a velocity independent electron collision frequency. For neon the wide variation was not understood. |
doi_str_mv | 10.1109/TMTT.1968.1126766 |
format | article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_28411825</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><ieee_id>1126766</ieee_id><sourcerecordid>28411825</sourcerecordid><originalsourceid>FETCH-LOGICAL-c362t-cbf8cc633e6874e7a472ff234c6c2b65daf584214df5114aacedb355830aff8b3</originalsourceid><addsrcrecordid>eNpVkM1OwzAQhC0EEqXwAIiLT9xS_B_niEopSC0cCFwtx1nToLQudnLg7UnVSIjTana_Ga0GoWtKZpSS4q5cl-WMFkoPkqlcqRM0oVLmWaFycoomhFCdFUKTc3SR0tcghSR6gqo12NRHqPFLaBLgErZ7iLYbVvgDYuoTLjcQInSNsy1etOC6GHb_OB8iXtqEH5rkNjZ-wpj1FvroIF2iM2_bBFfjnKL3x0U5f8pWr8vn-f0qc1yxLnOV184pzkHpXEBuRc68Z1w45VilZG291IJRUXtJqbDWQV1xKTUn1ntd8Sm6PebuY_juIXVmOzwEbWt3EPpkmBaUaiYHkB5BF0NKEbzZx2Zr44-hxBzaNIc2zaFNM7Y5eG6OngYA_vjx-gvS_3MD</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>28411825</pqid></control><display><type>article</type><title>Measured Noise Temperature Versus Theoretical Electron Temperature for Gas Discharge Noise Sources</title><source>IEEE Electronic Library (IEL) Journals</source><creator>Olson, K.W.</creator><creatorcontrib>Olson, K.W.</creatorcontrib><description>In the past, measured noise temperatures T/sub n/ of a few commercially available gas discharge noise sources were indicated as agreeing with the predicted electron temperature T/sub e/ of the positive column based on the von Engel and Steenbeck relationship. Data were taken over the past 2 years on argon tubes over a pressure range of 5 to 40 mm and on neon tubes at 20 mm, with current variations from 100 to 300 mAdc. These data were compared against predicted electron temperatures. For the argon tubes at pressure-radius products greater than 20 mm/spl dot/cm there appeared to be reasonable correlation between the measured noise temperature and the predicted electron temperature although it is suggested that this correlation was fortuitous. For argon pressure-radius products less than 20 mm/spl dot/cm the measured noise temperature was as much as 15 percent lower than the predicted electron temperature. For neon tubes at 20-mm pressure, with the same variation in tube radius, and for pressure-radius products less than 24.0 mm/spl dot/cm, the measured noise temperature differed even more than for argon from the predicted electron temperature. A difference of as much as 30 percent at a pressure-radius product of 3.0 mm/spl dot/cm was observed. A qualitative explanation for argon is presented based mainly on the fact that these discharges do not have a Maxwellian distribution of electron velocities nor a velocity independent electron collision frequency. For neon the wide variation was not understood.</description><identifier>ISSN: 0018-9480</identifier><identifier>EISSN: 1557-9670</identifier><identifier>DOI: 10.1109/TMTT.1968.1126766</identifier><identifier>CODEN: IETMAB</identifier><language>eng</language><publisher>IEEE</publisher><subject>Argon ; Current measurement ; Discharges ; Electron tubes ; Insertion loss ; Microwave measurements ; NIST ; Noise measurement ; Signal to noise ratio ; Temperature measurement</subject><ispartof>IEEE transactions on microwave theory and techniques, 1968-09, Vol.16 (9), p.640-645</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c362t-cbf8cc633e6874e7a472ff234c6c2b65daf584214df5114aacedb355830aff8b3</citedby><cites>FETCH-LOGICAL-c362t-cbf8cc633e6874e7a472ff234c6c2b65daf584214df5114aacedb355830aff8b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1126766$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,27923,27924,54795</link.rule.ids></links><search><creatorcontrib>Olson, K.W.</creatorcontrib><title>Measured Noise Temperature Versus Theoretical Electron Temperature for Gas Discharge Noise Sources</title><title>IEEE transactions on microwave theory and techniques</title><addtitle>TMTT</addtitle><description>In the past, measured noise temperatures T/sub n/ of a few commercially available gas discharge noise sources were indicated as agreeing with the predicted electron temperature T/sub e/ of the positive column based on the von Engel and Steenbeck relationship. Data were taken over the past 2 years on argon tubes over a pressure range of 5 to 40 mm and on neon tubes at 20 mm, with current variations from 100 to 300 mAdc. These data were compared against predicted electron temperatures. For the argon tubes at pressure-radius products greater than 20 mm/spl dot/cm there appeared to be reasonable correlation between the measured noise temperature and the predicted electron temperature although it is suggested that this correlation was fortuitous. For argon pressure-radius products less than 20 mm/spl dot/cm the measured noise temperature was as much as 15 percent lower than the predicted electron temperature. For neon tubes at 20-mm pressure, with the same variation in tube radius, and for pressure-radius products less than 24.0 mm/spl dot/cm, the measured noise temperature differed even more than for argon from the predicted electron temperature. A difference of as much as 30 percent at a pressure-radius product of 3.0 mm/spl dot/cm was observed. A qualitative explanation for argon is presented based mainly on the fact that these discharges do not have a Maxwellian distribution of electron velocities nor a velocity independent electron collision frequency. For neon the wide variation was not understood.</description><subject>Argon</subject><subject>Current measurement</subject><subject>Discharges</subject><subject>Electron tubes</subject><subject>Insertion loss</subject><subject>Microwave measurements</subject><subject>NIST</subject><subject>Noise measurement</subject><subject>Signal to noise ratio</subject><subject>Temperature measurement</subject><issn>0018-9480</issn><issn>1557-9670</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1968</creationdate><recordtype>article</recordtype><recordid>eNpVkM1OwzAQhC0EEqXwAIiLT9xS_B_niEopSC0cCFwtx1nToLQudnLg7UnVSIjTana_Ga0GoWtKZpSS4q5cl-WMFkoPkqlcqRM0oVLmWaFycoomhFCdFUKTc3SR0tcghSR6gqo12NRHqPFLaBLgErZ7iLYbVvgDYuoTLjcQInSNsy1etOC6GHb_OB8iXtqEH5rkNjZ-wpj1FvroIF2iM2_bBFfjnKL3x0U5f8pWr8vn-f0qc1yxLnOV184pzkHpXEBuRc68Z1w45VilZG291IJRUXtJqbDWQV1xKTUn1ntd8Sm6PebuY_juIXVmOzwEbWt3EPpkmBaUaiYHkB5BF0NKEbzZx2Zr44-hxBzaNIc2zaFNM7Y5eG6OngYA_vjx-gvS_3MD</recordid><startdate>19680901</startdate><enddate>19680901</enddate><creator>Olson, K.W.</creator><general>IEEE</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>19680901</creationdate><title>Measured Noise Temperature Versus Theoretical Electron Temperature for Gas Discharge Noise Sources</title><author>Olson, K.W.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c362t-cbf8cc633e6874e7a472ff234c6c2b65daf584214df5114aacedb355830aff8b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1968</creationdate><topic>Argon</topic><topic>Current measurement</topic><topic>Discharges</topic><topic>Electron tubes</topic><topic>Insertion loss</topic><topic>Microwave measurements</topic><topic>NIST</topic><topic>Noise measurement</topic><topic>Signal to noise ratio</topic><topic>Temperature measurement</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Olson, K.W.</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>IEEE transactions on microwave theory and techniques</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Olson, K.W.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Measured Noise Temperature Versus Theoretical Electron Temperature for Gas Discharge Noise Sources</atitle><jtitle>IEEE transactions on microwave theory and techniques</jtitle><stitle>TMTT</stitle><date>1968-09-01</date><risdate>1968</risdate><volume>16</volume><issue>9</issue><spage>640</spage><epage>645</epage><pages>640-645</pages><issn>0018-9480</issn><eissn>1557-9670</eissn><coden>IETMAB</coden><abstract>In the past, measured noise temperatures T/sub n/ of a few commercially available gas discharge noise sources were indicated as agreeing with the predicted electron temperature T/sub e/ of the positive column based on the von Engel and Steenbeck relationship. Data were taken over the past 2 years on argon tubes over a pressure range of 5 to 40 mm and on neon tubes at 20 mm, with current variations from 100 to 300 mAdc. These data were compared against predicted electron temperatures. For the argon tubes at pressure-radius products greater than 20 mm/spl dot/cm there appeared to be reasonable correlation between the measured noise temperature and the predicted electron temperature although it is suggested that this correlation was fortuitous. For argon pressure-radius products less than 20 mm/spl dot/cm the measured noise temperature was as much as 15 percent lower than the predicted electron temperature. For neon tubes at 20-mm pressure, with the same variation in tube radius, and for pressure-radius products less than 24.0 mm/spl dot/cm, the measured noise temperature differed even more than for argon from the predicted electron temperature. A difference of as much as 30 percent at a pressure-radius product of 3.0 mm/spl dot/cm was observed. A qualitative explanation for argon is presented based mainly on the fact that these discharges do not have a Maxwellian distribution of electron velocities nor a velocity independent electron collision frequency. For neon the wide variation was not understood.</abstract><pub>IEEE</pub><doi>10.1109/TMTT.1968.1126766</doi><tpages>6</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0018-9480 |
ispartof | IEEE transactions on microwave theory and techniques, 1968-09, Vol.16 (9), p.640-645 |
issn | 0018-9480 1557-9670 |
language | eng |
recordid | cdi_proquest_miscellaneous_28411825 |
source | IEEE Electronic Library (IEL) Journals |
subjects | Argon Current measurement Discharges Electron tubes Insertion loss Microwave measurements NIST Noise measurement Signal to noise ratio Temperature measurement |
title | Measured Noise Temperature Versus Theoretical Electron Temperature for Gas Discharge Noise Sources |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-08T15%3A01%3A43IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Measured%20Noise%20Temperature%20Versus%20Theoretical%20Electron%20Temperature%20for%20Gas%20Discharge%20Noise%20Sources&rft.jtitle=IEEE%20transactions%20on%20microwave%20theory%20and%20techniques&rft.au=Olson,%20K.W.&rft.date=1968-09-01&rft.volume=16&rft.issue=9&rft.spage=640&rft.epage=645&rft.pages=640-645&rft.issn=0018-9480&rft.eissn=1557-9670&rft.coden=IETMAB&rft_id=info:doi/10.1109/TMTT.1968.1126766&rft_dat=%3Cproquest_cross%3E28411825%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c362t-cbf8cc633e6874e7a472ff234c6c2b65daf584214df5114aacedb355830aff8b3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=28411825&rft_id=info:pmid/&rft_ieee_id=1126766&rfr_iscdi=true |