Development of a novel spiral antenna system for low loop voltage current start-up at the Steady State Superconducting Tokamak (SST-1)
In general, superconducting tokamaks require low loop voltage current start-up for the safety purpose of their poloidal field coils. The loop voltage inside the vacuum vessel of Steady State Superconducting Tokamak (SST-1) is low in nature since its central solenoid is located outside the cryostat....
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creator | Basu, Debjyoti Raju, Daniel Singh, Raj Mukherjee, Aparajita Patel, Manoj Rathi, Dharmendra Trivedi, R G Vasava, Kirit Jadeja, K A Jayaswal, Sneha P Patel, Vijaykumar N Patnaik, S K Vasava, Paresh Subbarao, Ajesh Kadia, Bhavesh Parmar, Kirit George, Siju Paravastu, Yuvakiran R Dhanani, Kalpesh Bhavsar, Chirag Sharma, Sudhir Gopalakrishna, M V Bandyopadhyay, Mainak Shah, Minsha Gautam, Pramila Nimavat, Hiren D Thankey, Prashant L Khan, Ziauddin Raval, Dilip |
description | In general, superconducting tokamaks require low loop voltage current start-up for the safety purpose of their poloidal field coils. The loop voltage inside the vacuum vessel of Steady State Superconducting Tokamak (SST-1) is low in nature since its central solenoid is located outside the cryostat. The low loop voltage current start-up of the SST-1 is routinely performed by using the electron cyclotron resonance (ECR) method at the toroidal magnetic field
B
t
= 1.5 T (first harmonic) and 0.75 T (second harmonic). Recently, an alternative RF-based plasma current start-up system has been planned for operating the machine, especially for a higher toroidal magnetic field regime
1.5
T
⩽
B
t
⩽
3
T
. The system was already developed based on an antenna system, made of a series of combinations of two flat spiral antennas, to assist plasma current start-up at a lower inductive electric field. It has already been tested and installed in the SST-1 chamber. The system testing was performed without a background magnetic field within the frequency regime of 35 MHz–60 MHz at present. The test results show that it can produce an electron density of
n
e
≃
10
16
m
−
3
measured by the Langmuir probe at the expense of 500 W RF power. The spectroscopy results indicate its capability of producing plasma density greater than
10
13
m
−
3
and an electron temperature of
T
e
=
2
–6 eV. In addition, the results also show the presence of a turbulent electric field of the order of 10
6
V m
−1
at the antenna center and a finite anomalous temperature of neutral particles. Calculations show that the obtained density is sufficient for SST-1 low loop voltage plasma breakdown. The antenna system is also capable of producing plasma at higher frequencies. This article will discuss the development of the prototype and the installed antenna system along with their test results in detail. |
doi_str_mv | 10.1088/1361-6587/ac3498 |
format | Article |
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B
t
= 1.5 T (first harmonic) and 0.75 T (second harmonic). Recently, an alternative RF-based plasma current start-up system has been planned for operating the machine, especially for a higher toroidal magnetic field regime
1.5
T
⩽
B
t
⩽
3
T
. The system was already developed based on an antenna system, made of a series of combinations of two flat spiral antennas, to assist plasma current start-up at a lower inductive electric field. It has already been tested and installed in the SST-1 chamber. The system testing was performed without a background magnetic field within the frequency regime of 35 MHz–60 MHz at present. The test results show that it can produce an electron density of
n
e
≃
10
16
m
−
3
measured by the Langmuir probe at the expense of 500 W RF power. The spectroscopy results indicate its capability of producing plasma density greater than
10
13
m
−
3
and an electron temperature of
T
e
=
2
–6 eV. In addition, the results also show the presence of a turbulent electric field of the order of 10
6
V m
−1
at the antenna center and a finite anomalous temperature of neutral particles. Calculations show that the obtained density is sufficient for SST-1 low loop voltage plasma breakdown. The antenna system is also capable of producing plasma at higher frequencies. This article will discuss the development of the prototype and the installed antenna system along with their test results in detail.</description><identifier>ISSN: 0741-3335</identifier><identifier>EISSN: 1361-6587</identifier><identifier>DOI: 10.1088/1361-6587/ac3498</identifier><identifier>CODEN: PLPHBZ</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>antenna ; development ; spiral ; superconducting tokamak low loop voltage current start up</subject><ispartof>Plasma physics and controlled fusion, 2022-01, Vol.64 (1), p.15004</ispartof><rights>2021 IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c233t-b612e5eda2b798264ca55652dbadd3535319f536f86399fd7820ea663fd3f22f3</cites><orcidid>0000-0002-6489-9284 ; 0000-0002-0677-0079</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1361-6587/ac3498/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,776,780,27901,27902,53821,53868</link.rule.ids></links><search><creatorcontrib>Basu, Debjyoti</creatorcontrib><creatorcontrib>Raju, Daniel</creatorcontrib><creatorcontrib>Singh, Raj</creatorcontrib><creatorcontrib>Mukherjee, Aparajita</creatorcontrib><creatorcontrib>Patel, Manoj</creatorcontrib><creatorcontrib>Rathi, Dharmendra</creatorcontrib><creatorcontrib>Trivedi, R G</creatorcontrib><creatorcontrib>Vasava, Kirit</creatorcontrib><creatorcontrib>Jadeja, K A</creatorcontrib><creatorcontrib>Jayaswal, Sneha P</creatorcontrib><creatorcontrib>Patel, Vijaykumar N</creatorcontrib><creatorcontrib>Patnaik, S K</creatorcontrib><creatorcontrib>Vasava, Paresh</creatorcontrib><creatorcontrib>Subbarao, Ajesh</creatorcontrib><creatorcontrib>Kadia, Bhavesh</creatorcontrib><creatorcontrib>Parmar, Kirit</creatorcontrib><creatorcontrib>George, Siju</creatorcontrib><creatorcontrib>Paravastu, Yuvakiran</creatorcontrib><creatorcontrib>R Dhanani, Kalpesh</creatorcontrib><creatorcontrib>Bhavsar, Chirag</creatorcontrib><creatorcontrib>Sharma, Sudhir</creatorcontrib><creatorcontrib>Gopalakrishna, M V</creatorcontrib><creatorcontrib>Bandyopadhyay, Mainak</creatorcontrib><creatorcontrib>Shah, Minsha</creatorcontrib><creatorcontrib>Gautam, Pramila</creatorcontrib><creatorcontrib>Nimavat, Hiren D</creatorcontrib><creatorcontrib>Thankey, Prashant L</creatorcontrib><creatorcontrib>Khan, Ziauddin</creatorcontrib><creatorcontrib>Raval, Dilip</creatorcontrib><title>Development of a novel spiral antenna system for low loop voltage current start-up at the Steady State Superconducting Tokamak (SST-1)</title><title>Plasma physics and controlled fusion</title><addtitle>PPCF</addtitle><addtitle>Plasma Phys. Control. Fusion</addtitle><description>In general, superconducting tokamaks require low loop voltage current start-up for the safety purpose of their poloidal field coils. The loop voltage inside the vacuum vessel of Steady State Superconducting Tokamak (SST-1) is low in nature since its central solenoid is located outside the cryostat. The low loop voltage current start-up of the SST-1 is routinely performed by using the electron cyclotron resonance (ECR) method at the toroidal magnetic field
B
t
= 1.5 T (first harmonic) and 0.75 T (second harmonic). Recently, an alternative RF-based plasma current start-up system has been planned for operating the machine, especially for a higher toroidal magnetic field regime
1.5
T
⩽
B
t
⩽
3
T
. The system was already developed based on an antenna system, made of a series of combinations of two flat spiral antennas, to assist plasma current start-up at a lower inductive electric field. It has already been tested and installed in the SST-1 chamber. The system testing was performed without a background magnetic field within the frequency regime of 35 MHz–60 MHz at present. The test results show that it can produce an electron density of
n
e
≃
10
16
m
−
3
measured by the Langmuir probe at the expense of 500 W RF power. The spectroscopy results indicate its capability of producing plasma density greater than
10
13
m
−
3
and an electron temperature of
T
e
=
2
–6 eV. In addition, the results also show the presence of a turbulent electric field of the order of 10
6
V m
−1
at the antenna center and a finite anomalous temperature of neutral particles. Calculations show that the obtained density is sufficient for SST-1 low loop voltage plasma breakdown. The antenna system is also capable of producing plasma at higher frequencies. This article will discuss the development of the prototype and the installed antenna system along with their test results in detail.</description><subject>antenna</subject><subject>development</subject><subject>spiral</subject><subject>superconducting tokamak low loop voltage current start up</subject><issn>0741-3335</issn><issn>1361-6587</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp1kE1LAzEQhoMoWKt3jzkquDYfTXb3KPUTCh5az8t0k9Rtt8mSZCv9A_5us1S8yTAM8zLv8PIgdE3JPSVFMaFc0kyKIp9AzadlcYJGf9IpGpF8SjPOuThHFyFsCKG0YHKEvh_1Xreu22kbsTMYsHVJwKFrPLQYbNTWAg6HEPUOG-dx675Suw7vXRthrXHdez-4QwQfs77DEHH81HgRNahDGhDT0nfa186qvo6NXeOl28IOtvhmsVhm9PYSnRlog776nWP08fy0nL1m8_eXt9nDPKsZ5zFbScq00ArYKi9T_mkNQkjB1AqU4iIVLY3g0hSSl6VRecGIBim5UdwwZvgYkePf2rsQvDZV55sd-ENFSTVwrAZo1QCtOnJMlrujpXFdtXG9tyng_-c_WsR1Yg</recordid><startdate>20220101</startdate><enddate>20220101</enddate><creator>Basu, Debjyoti</creator><creator>Raju, Daniel</creator><creator>Singh, Raj</creator><creator>Mukherjee, Aparajita</creator><creator>Patel, Manoj</creator><creator>Rathi, Dharmendra</creator><creator>Trivedi, R G</creator><creator>Vasava, Kirit</creator><creator>Jadeja, K A</creator><creator>Jayaswal, Sneha P</creator><creator>Patel, Vijaykumar N</creator><creator>Patnaik, S K</creator><creator>Vasava, Paresh</creator><creator>Subbarao, Ajesh</creator><creator>Kadia, Bhavesh</creator><creator>Parmar, Kirit</creator><creator>George, Siju</creator><creator>Paravastu, Yuvakiran</creator><creator>R Dhanani, Kalpesh</creator><creator>Bhavsar, Chirag</creator><creator>Sharma, Sudhir</creator><creator>Gopalakrishna, M V</creator><creator>Bandyopadhyay, Mainak</creator><creator>Shah, Minsha</creator><creator>Gautam, Pramila</creator><creator>Nimavat, Hiren D</creator><creator>Thankey, Prashant L</creator><creator>Khan, Ziauddin</creator><creator>Raval, Dilip</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-6489-9284</orcidid><orcidid>https://orcid.org/0000-0002-0677-0079</orcidid></search><sort><creationdate>20220101</creationdate><title>Development of a novel spiral antenna system for low loop voltage current start-up at the Steady State Superconducting Tokamak (SST-1)</title><author>Basu, Debjyoti ; Raju, Daniel ; Singh, Raj ; Mukherjee, Aparajita ; Patel, Manoj ; Rathi, Dharmendra ; Trivedi, R G ; Vasava, Kirit ; Jadeja, K A ; Jayaswal, Sneha P ; Patel, Vijaykumar N ; Patnaik, S K ; Vasava, Paresh ; Subbarao, Ajesh ; Kadia, Bhavesh ; Parmar, Kirit ; George, Siju ; Paravastu, Yuvakiran ; R Dhanani, Kalpesh ; Bhavsar, Chirag ; Sharma, Sudhir ; Gopalakrishna, M V ; Bandyopadhyay, Mainak ; Shah, Minsha ; Gautam, Pramila ; Nimavat, Hiren D ; Thankey, Prashant L ; Khan, Ziauddin ; Raval, Dilip</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c233t-b612e5eda2b798264ca55652dbadd3535319f536f86399fd7820ea663fd3f22f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>antenna</topic><topic>development</topic><topic>spiral</topic><topic>superconducting tokamak low loop voltage current start up</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Basu, Debjyoti</creatorcontrib><creatorcontrib>Raju, Daniel</creatorcontrib><creatorcontrib>Singh, Raj</creatorcontrib><creatorcontrib>Mukherjee, Aparajita</creatorcontrib><creatorcontrib>Patel, Manoj</creatorcontrib><creatorcontrib>Rathi, Dharmendra</creatorcontrib><creatorcontrib>Trivedi, R G</creatorcontrib><creatorcontrib>Vasava, Kirit</creatorcontrib><creatorcontrib>Jadeja, K A</creatorcontrib><creatorcontrib>Jayaswal, Sneha P</creatorcontrib><creatorcontrib>Patel, Vijaykumar N</creatorcontrib><creatorcontrib>Patnaik, S K</creatorcontrib><creatorcontrib>Vasava, Paresh</creatorcontrib><creatorcontrib>Subbarao, Ajesh</creatorcontrib><creatorcontrib>Kadia, Bhavesh</creatorcontrib><creatorcontrib>Parmar, Kirit</creatorcontrib><creatorcontrib>George, Siju</creatorcontrib><creatorcontrib>Paravastu, Yuvakiran</creatorcontrib><creatorcontrib>R Dhanani, Kalpesh</creatorcontrib><creatorcontrib>Bhavsar, Chirag</creatorcontrib><creatorcontrib>Sharma, Sudhir</creatorcontrib><creatorcontrib>Gopalakrishna, M V</creatorcontrib><creatorcontrib>Bandyopadhyay, Mainak</creatorcontrib><creatorcontrib>Shah, Minsha</creatorcontrib><creatorcontrib>Gautam, Pramila</creatorcontrib><creatorcontrib>Nimavat, Hiren D</creatorcontrib><creatorcontrib>Thankey, Prashant L</creatorcontrib><creatorcontrib>Khan, Ziauddin</creatorcontrib><creatorcontrib>Raval, Dilip</creatorcontrib><collection>CrossRef</collection><jtitle>Plasma physics and controlled fusion</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Basu, Debjyoti</au><au>Raju, Daniel</au><au>Singh, Raj</au><au>Mukherjee, Aparajita</au><au>Patel, Manoj</au><au>Rathi, Dharmendra</au><au>Trivedi, R G</au><au>Vasava, Kirit</au><au>Jadeja, K A</au><au>Jayaswal, Sneha P</au><au>Patel, Vijaykumar N</au><au>Patnaik, S K</au><au>Vasava, Paresh</au><au>Subbarao, Ajesh</au><au>Kadia, Bhavesh</au><au>Parmar, Kirit</au><au>George, Siju</au><au>Paravastu, Yuvakiran</au><au>R Dhanani, Kalpesh</au><au>Bhavsar, Chirag</au><au>Sharma, Sudhir</au><au>Gopalakrishna, M V</au><au>Bandyopadhyay, Mainak</au><au>Shah, Minsha</au><au>Gautam, Pramila</au><au>Nimavat, Hiren D</au><au>Thankey, Prashant L</au><au>Khan, Ziauddin</au><au>Raval, Dilip</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Development of a novel spiral antenna system for low loop voltage current start-up at the Steady State Superconducting Tokamak (SST-1)</atitle><jtitle>Plasma physics and controlled fusion</jtitle><stitle>PPCF</stitle><addtitle>Plasma Phys. Control. Fusion</addtitle><date>2022-01-01</date><risdate>2022</risdate><volume>64</volume><issue>1</issue><spage>15004</spage><pages>15004-</pages><issn>0741-3335</issn><eissn>1361-6587</eissn><coden>PLPHBZ</coden><abstract>In general, superconducting tokamaks require low loop voltage current start-up for the safety purpose of their poloidal field coils. The loop voltage inside the vacuum vessel of Steady State Superconducting Tokamak (SST-1) is low in nature since its central solenoid is located outside the cryostat. The low loop voltage current start-up of the SST-1 is routinely performed by using the electron cyclotron resonance (ECR) method at the toroidal magnetic field
B
t
= 1.5 T (first harmonic) and 0.75 T (second harmonic). Recently, an alternative RF-based plasma current start-up system has been planned for operating the machine, especially for a higher toroidal magnetic field regime
1.5
T
⩽
B
t
⩽
3
T
. The system was already developed based on an antenna system, made of a series of combinations of two flat spiral antennas, to assist plasma current start-up at a lower inductive electric field. It has already been tested and installed in the SST-1 chamber. The system testing was performed without a background magnetic field within the frequency regime of 35 MHz–60 MHz at present. The test results show that it can produce an electron density of
n
e
≃
10
16
m
−
3
measured by the Langmuir probe at the expense of 500 W RF power. The spectroscopy results indicate its capability of producing plasma density greater than
10
13
m
−
3
and an electron temperature of
T
e
=
2
–6 eV. In addition, the results also show the presence of a turbulent electric field of the order of 10
6
V m
−1
at the antenna center and a finite anomalous temperature of neutral particles. Calculations show that the obtained density is sufficient for SST-1 low loop voltage plasma breakdown. The antenna system is also capable of producing plasma at higher frequencies. This article will discuss the development of the prototype and the installed antenna system along with their test results in detail.</abstract><pub>IOP Publishing</pub><doi>10.1088/1361-6587/ac3498</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0002-6489-9284</orcidid><orcidid>https://orcid.org/0000-0002-0677-0079</orcidid></addata></record> |
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source | IOP Publishing Journals; Institute of Physics (IOP) Journals - HEAL-Link |
subjects | antenna development spiral superconducting tokamak low loop voltage current start up |
title | Development of a novel spiral antenna system for low loop voltage current start-up at the Steady State Superconducting Tokamak (SST-1) |
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