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

Author:

Pahari SambaranORCID,P.P. Rahulnath,Savita Aditya Nandan,Maurya Pradeep Kumar,Jha Saroj Kumar,Shiv Neeraj,K. Raghavendra,Hemani Harsh,Nagaraju Belli,Mahar Sukantam,Rao Manmadha,Suryaprasad I.V.V.,Malshe U.D.,Ghosh J.,Doshi B.R.,Chattopadhyay Prabal Kumar,Tanna R.L.ORCID,Jadeja K.A.ORCID,Patel K.M.,Kumar RohitORCID,Macwan TanmayORCID,Raj Harshita,Aich S.ORCID,Singh Kaushlender,Dolui Suman,Kumawat D.,Makwana M.N.,Shah K.S.,Gupta Shivam,Balakrishnan V.,Gupta C.N.,Patnaik Swadesh Kumar,Edappala Praveenlal,Shah Minsha,Kadia Bhavesh,Yadava NandiniORCID,Shah Kajal,Shukla G.,Chowdhuri M.B.ORCID,Manchanda R.ORCID,Ramaiya Nilam,Kumar Manoj,Nagora Umesh,S. Varsha,Pathak S.K.,Asudani Kumudni,Chaudhuri ParitoshORCID,Maya P.N.ORCID,Goswami Rajiv,Sen A.ORCID,Saxena Y.C.ORCID,Pal R.,Chaturvedi S.

Abstract

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 (Li2TiO3/Li2CO3) 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 Li2TiO3 injection causing a faster current quench than Li2CO3 injection, as more power is radiated in the case of Li2TiO3. 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.

Publisher

IOP Publishing

Reference32 articles.

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