Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>

This report evaluates the pulsed breakdown performance of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi...

Full description

Saved in:
Bibliographic Details
Main Authors: Luke Silvestre, Jakob Matthies, Luke Boswell, Jacob Stephens, James Dickens, Andrew Young, Andreas Neuber
Format: Article
Language:English
Published: MDPI AG 2024-12-01
Series:Applied Sciences
Subjects:
Online Access:https://www.mdpi.com/2076-3417/14/23/11268
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1850107432617902080
author Luke Silvestre
Jakob Matthies
Luke Boswell
Jacob Stephens
James Dickens
Andrew Young
Andreas Neuber
author_facet Luke Silvestre
Jakob Matthies
Luke Boswell
Jacob Stephens
James Dickens
Andrew Young
Andreas Neuber
author_sort Luke Silvestre
collection DOAJ
description This report evaluates the pulsed breakdown performance of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> under a 6.8 kV/ns voltage excitation. The pulsed dielectric strength of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> is compared to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>S</mi><msub><mi>F</mi><mn>6</mn></msub></mrow></semantics></math></inline-formula> in the same experimental setup, and it is found that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> concentrations of 50% or greater are required to achieve a dielectric strength greater than or equal to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>S</mi><msub><mi>F</mi><mn>6</mn></msub></mrow></semantics></math></inline-formula>. Pure <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> demonstrated higher electric field hold-off for longer time periods and less statistical variance under pulsed conditions when compared to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>S</mi><msub><mi>F</mi><mn>6</mn></msub></mrow></semantics></math></inline-formula>. Mixtures of 50%<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>N</mi><mn>2</mn></msub></semantics></math></inline-formula> or <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>C</mi><msub><mi>O</mi><mn>2</mn></msub></mrow></semantics></math></inline-formula> as buffer gases showed no appreciable difference in pulsed dielectric strength.
format Article
id doaj-art-29eb9983a46f459ba644886ed2d5dd07
institution OA Journals
issn 2076-3417
language English
publishDate 2024-12-01
publisher MDPI AG
record_format Article
series Applied Sciences
spelling doaj-art-29eb9983a46f459ba644886ed2d5dd072025-08-20T02:38:35ZengMDPI AGApplied Sciences2076-34172024-12-0114231126810.3390/app142311268Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>Luke Silvestre0Jakob Matthies1Luke Boswell2Jacob Stephens3James Dickens4Andrew Young5Andreas Neuber6Center for Pulsed Power and Power Electronics Research, Department of Electrical and Computer Engineering, Texas Tech University, Lubbock, TX 79409, USACenter for Pulsed Power and Power Electronics Research, Department of Electrical and Computer Engineering, Texas Tech University, Lubbock, TX 79409, USACenter for Pulsed Power and Power Electronics Research, Department of Electrical and Computer Engineering, Texas Tech University, Lubbock, TX 79409, USACenter for Pulsed Power and Power Electronics Research, Department of Electrical and Computer Engineering, Texas Tech University, Lubbock, TX 79409, USACenter for Pulsed Power and Power Electronics Research, Department of Electrical and Computer Engineering, Texas Tech University, Lubbock, TX 79409, USALawrence Livermore National Laboratory, Livermore, CA 94550, USACenter for Pulsed Power and Power Electronics Research, Department of Electrical and Computer Engineering, Texas Tech University, Lubbock, TX 79409, USAThis report evaluates the pulsed breakdown performance of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> under a 6.8 kV/ns voltage excitation. The pulsed dielectric strength of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> is compared to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>S</mi><msub><mi>F</mi><mn>6</mn></msub></mrow></semantics></math></inline-formula> in the same experimental setup, and it is found that <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> concentrations of 50% or greater are required to achieve a dielectric strength greater than or equal to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>S</mi><msub><mi>F</mi><mn>6</mn></msub></mrow></semantics></math></inline-formula>. Pure <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> demonstrated higher electric field hold-off for longer time periods and less statistical variance under pulsed conditions when compared to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>S</mi><msub><mi>F</mi><mn>6</mn></msub></mrow></semantics></math></inline-formula>. Mixtures of 50%<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mn>4</mn></msub><msub><mi>F</mi><mn>7</mn></msub><mi>N</mi></mrow></semantics></math></inline-formula> with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>N</mi><mn>2</mn></msub></semantics></math></inline-formula> or <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>C</mi><msub><mi>O</mi><mn>2</mn></msub></mrow></semantics></math></inline-formula> as buffer gases showed no appreciable difference in pulsed dielectric strength.https://www.mdpi.com/2076-3417/14/23/11268<i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i><i>SF</i><sub>6</sub>Novec<sup><i>TM</i></sup> 4710pulsed breakdowndielectric strengthelectrical breakdown
spellingShingle Luke Silvestre
Jakob Matthies
Luke Boswell
Jacob Stephens
James Dickens
Andrew Young
Andreas Neuber
Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>
Applied Sciences
<i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i>
<i>SF</i><sub>6</sub>
Novec<sup><i>TM</i></sup> 4710
pulsed breakdown
dielectric strength
electrical breakdown
title Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>
title_full Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>
title_fullStr Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>
title_full_unstemmed Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>
title_short Nanosecond Breakdown Characteristics of <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i> and Various Mixtures at Pressures Above 1 Atmosphere in Comparison with <i>SF</i><sub>6</sub>
title_sort nanosecond breakdown characteristics of i c i sub 4 sub i f i sub 7 sub i n i and various mixtures at pressures above 1 atmosphere in comparison with i sf i sub 6 sub
topic <i>C</i><sub>4</sub><i>F</i><sub>7</sub><i>N</i>
<i>SF</i><sub>6</sub>
Novec<sup><i>TM</i></sup> 4710
pulsed breakdown
dielectric strength
electrical breakdown
url https://www.mdpi.com/2076-3417/14/23/11268
work_keys_str_mv AT lukesilvestre nanosecondbreakdowncharacteristicsoficisub4subifisub7subiniandvariousmixturesatpressuresabove1atmosphereincomparisonwithisfisub6sub
AT jakobmatthies nanosecondbreakdowncharacteristicsoficisub4subifisub7subiniandvariousmixturesatpressuresabove1atmosphereincomparisonwithisfisub6sub
AT lukeboswell nanosecondbreakdowncharacteristicsoficisub4subifisub7subiniandvariousmixturesatpressuresabove1atmosphereincomparisonwithisfisub6sub
AT jacobstephens nanosecondbreakdowncharacteristicsoficisub4subifisub7subiniandvariousmixturesatpressuresabove1atmosphereincomparisonwithisfisub6sub
AT jamesdickens nanosecondbreakdowncharacteristicsoficisub4subifisub7subiniandvariousmixturesatpressuresabove1atmosphereincomparisonwithisfisub6sub
AT andrewyoung nanosecondbreakdowncharacteristicsoficisub4subifisub7subiniandvariousmixturesatpressuresabove1atmosphereincomparisonwithisfisub6sub
AT andreasneuber nanosecondbreakdowncharacteristicsoficisub4subifisub7subiniandvariousmixturesatpressuresabove1atmosphereincomparisonwithisfisub6sub