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Micro-particle injection experiments in ADITYA-U tokamak using an inductively driven pellet injector

Authors :
Sambaran Pahari
Rahulnath P.P.
Aditya Nandan Savita
Pradeep Kumar Maurya
Saroj Kumar Jha
Neeraj Shiv
Raghavendra K.
Harsh Hemani
Belli Nagaraju
Sukantam Mahar
Manmadha Rao
I.V.V. Suryaprasad
U.D. Malshe
J. Ghosh
B.R. Doshi
Prabal Kumar Chattopadhyay
R.L. Tanna
K.A. Jadeja
K.M. Patel
Rohit Kumar
Tanmay Macwan
Harshita Raj
S. Aich
Kaushlender Singh
Suman Dolui
D. Kumawat
M.N. Makwana
K.S. Shah
Shivam Gupta
V. Balakrishnan
C.N. Gupta
Swadesh Kumar Patnaik
Praveenlal Edappala
Minsha Shah
Bhavesh Kadia
Nandini Yadava
Kajal Shah
G. Shukla
M.B. Chowdhuri
R. Manchanda
Nilam Ramaiya
Manoj Kumar
Umesh Nagora
Varsha S.
S.K. Pathak
Kumudni Asudani
Paritosh Chaudhuri
P.N. Maya
Rajiv Goswami
A. Sen
Y.C. Saxena
R. Pal
S. Chaturvedi
Source :
Nuclear Fusion, Vol 64, Iss 5, p 056007 (2024)
Publication Year :
2024
Publisher :
IOP Publishing, 2024.

Abstract

A first-of-its-kind, inductively driven micro-particle (Pellet) accelerator and injector have been developed and operated successfully in ADITYA-U circular plasma operations, which may ably address the critical need for a suitable disruption control mechanism in ITER and future tokamak. The device combines the principles of electromagnetic induction, pulse power technology, impact, and fracture dynamics. It is designed to operate in a variety of environments, including atmospheric pressure and ultra-high vacuum. It can also accommodate a wide range of pellet quantities, sizes, and materials and can adjust the pellets’ velocities over a coarse and fine range. The device has a modular design such that the maximum velocity can be increased by increasing the number of modules. A cluster of lithium titanate/carbonate (Li _2 TiO _3 /Li _2 CO _3 ) impurity particles with variable particle sizes, weighing ∼50–200 mg are injected with velocities of the order of ∼200 m s ^−1 during the current plateau in ADITYA-U tokamak. This leads to a complete collapse of the plasma current within ∼5–6 ms of triggering the injector. The current quench time is dependent on the amount of impurity injected as well as the compound, with Li _2 TiO _3 injection causing a faster current quench than Li _2 CO _3 injection, as more power is radiated in the case of Li _2 TiO _3 . The increase in radiation due to the macro-particle injection starts in the plasma core, while the soft x-ray emission indicates that the entire plasma core collapses at once.

Details

Language :
English
ISSN :
17414326 and 00295515
Volume :
64
Issue :
5
Database :
Directory of Open Access Journals
Journal :
Nuclear Fusion
Publication Type :
Academic Journal
Accession number :
edsdoj.b4fbf6aa91dc4b888321d7f60c0fcdf1
Document Type :
article
Full Text :
https://doi.org/10.1088/1741-4326/ad2b5f