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10-15 May 2021
Nice, France
Europe/Vienna timezone
The Conference will be held virtually from 10-15 May 2021

Novel Concept for Disruption Mitigation in the ADITYA - U tokamak by Fast Time Response Electromagnetic Driven Pellet Impurity Injector

12 May 2021, 14:00
4h 45m
Nice, France

Nice, France

Regular Poster Magnetic Fusion Experiments P4 Posters 4


Joydeep Ghosh (Institute for Plasma Research)


Implementation of suitable disruption mitigation technique remains the topmost priority for larger tokamaks including the ITER. The spontaneous disruption in ITER may probably be an unavoidable part, while operated with high performance D-T fuel [1]. Disruptions in ITER could produce very large heat loads on divertor targets and other Plasma Facing Components (PFC), and large electromagnetic forces on the Vacuum Vessel (VV) can lead to structural damages [2]. In order to avoid these detrimental consequences, disruption mitigation is an essential part of tokamak research. The disruption mitigation system (DMS) in ITER is based on massive gas injection (MGI) of impurities, in order to radiate the plasma stored energy and mitigate the potentially damaging effects of disruptions [3]. Although, MGI based technique is suitable for most disruption mitigation, there will be issues in case of having warning time less than 10 ms as may be the case for the onset of some disruptions in ITER [4]. This is due to the slow thermal velocity of the heavier impurity gas molecules, which limits the time needed to travel the distances before it reaches the plasma edge. At present, none of the currently planned disruption mitigations systems for ITER can respond on this time scale. The radiative dissipation of the plasma stored energy during major disruption in ITER by fast injection of massive pellets of low Z impurities, such as Li and Be pellet injection has been numerically modelled by Lukash et al. [5].

A novel concept of electromagnetically driven particle Injector (EPI) having fast time response has been developed and installed on the ADITYA-U tokamak. For the first time, ADITYA-U has experimentally demonstrated the use of electromagnetic pellet injection for firing the pellets into the tokamak plasmas for disruption mitigation studies. This is a significant development towards disruption control that can accomplish the critical need of disruption mitigation in future tokamaks including ITER. The experiments are conducted in ADITYA Upgrade (ADITYA-U), which is a medium sized (R0 = 75 cm, a= 25 cm) heated air core toroidal limiter tokamak, capable of producing circular as well as shaped plasma with single and double null open divertor configuration [6].

In these experiments, a projectile containing a radiative payload, weighing ~ 50 - 200 mg, is accelerated towards the core of the plasma with velocities of ~ 200-220 m/s using a linear coil gun accelerator, which can deposit micron-sized dust deep into the plasma core and radiate whole the plasma stored energy within few milliseconds. Lithium titanate (Li2TiO3) and Lithium carbonate (Li2CO3) particles of 50 – 80 micron are used in the experiments. Before performing the disruption mitigation experiment in ADITYA-U, the machine has been prepared for this experiment. The standard reference discharges of IP ~120 kA of 100 -120 ms duration have been established. Later, lithium titanate (Li2TiO3) impurity particles pellet has been injected into the ADITYA-U plasma during the plasma current flat-top at ~ 51.6 ms. The impurity particles reached the ADITYA-U core plasma within ~ 1.25 ms and causes fast termination of plasma current. The time evolution of two consecutive discharges of ADITYA-U, black curve (#33317) with particle injection and red curve (#33318) without pellet injection are shown in Figure 1, representing the radiative dissipation of the plasma stored energy in the discharge in which particles are injected. The spectroscopy measurements of Li line at 670.8 nm as shown in Fig. 2, confirms the signature of Li2TiO3 injection into the plasma. The chord averaged electron density and electron temperature, terminates very rapidly (Fig. 1(b) and 1(c) respectively), due to the increased of plasma radiation (Fig. 1(d)) after the impurity particles injections. The time evolution of relative intensity of visible radiation at 536 nm with and without particle injection for similar discharges during the disruption phase is shown in Figure 3. The Figure shows significant increase in the radiation level during disruption for the shot having particle injection.

During the experiment, fast visible imaging, high resolution video cameras on two different radial ports were installed on the ADITYA-U machine, to obtain the plasma images at high spatial and temporal resolution. One of the camera was kept for 2D tangential viewing, covers the entire cross-section of the limiter and the other camera covers the entire poloidal cross-section of the port, from where the impurity particles were injected into the plasma. The images clearly showed that the injected impurities radiate the energy from the core plasma and disrupted the whole plasma column within ~ < 2 ms. Furthermore, the disruptions triggered with particle injection using electromagnetically payload and disruptions triggered by massive gas-puff have been compared. Significantly different current quench characteristics have been observed in the disruptions triggered by particle injection, which occurred on faster time-scales as compared to those triggered by massive gas-injection. First results on disruptions in the ADITYA - U by electromagnetically driven fast injection of particles in to the plasma will be discussed in this paper.


[1] Strait E.J. et al 2019 Progress in disruption prevention for ITER Nucl. Fusion 59 112012.
[2] Lehnen M. et al 2015 Disruptions in ITER and strategies for their control and mitigation J. Nucl. Mater. 463 39-48.
[3] Hollmann E. et al 2015 Status of research toward the ITER disruption mitigation system Phys. Plasmas 22 021802.
[4] Raman R. et al 2015 Fast Time Response Electromagnetic Disruption Mitigation Concept Fusion Sci. and Tech. 68:4 797-805.
[5] Lukash V.E. et al 2014 Modeling of Major Disruption Mitigation by Fast Injection of Massive Li Pellets in ITER Like Tokamak-Reactor IAEA (2010) 91.htm#41805 (current as of Nov. 19, 2014).
[6] Tanna R. et al 2019 Overview of operation and experiments in the ADITYA-U tokamak Nucl. Fusion 59 112006.

Affiliation Institute for Plasma Research, Bhat, Gandhinagar, India.
Country or International Organization India

Primary author

Joydeep Ghosh (Institute for Plasma Research)


Dr Sambaran Pahari (Bhabha Atomic Research Center, Computational Analysis Division) bharatkumar doshi (Institute for plasma research) RAKESH TANNA (Institute for Plasma Research) Kumarpalsinh Jadeja (Institute for plasma Research) Kaushal Patel (Institute for Plasma Research) ROHIT KUMAR (Institute For Plasma Research) Tanmay Macwan (Institute for Plasma Research) Suman Aich (Institute for Plasma Research) Devilal Kumawat (Institute for plasma Research Bhat Gandhinagar) Mr M.N. Makwana (Institute for Plasma Research) Mr Kunal S. Shah (Institute for Plasma Research) Mr Shivam Gupta (Institute for Plasma Research) Dr Balakrishnan V. Nair (Institute for Plasma Research) Mr Chet Narayan Gupta (Institute for Plasma Research) Mr Vipul K. Panchal (Institute for Plasma Research) Mr Praveenlal Edappala (Institute for Plasma Research) Mrs Minsha Shah (Institute for Plasma Research) Mr Savita Aditya Nandan (Bhabha Atomic Research Center, Computational Analysis Division) Mr Rahulnath P.P. (Bhabha Atomic Research Center, Computational Analysis Division) Mr Pradeep Kumar Maurya (Bhabha Atomic Research Center, Computational Analysis Division.) Mr Saroj Kumar Jha (Bhabha Atomic Research Center, Computational Analysis Division) Mr Mohan Kumar Raghavendra (Bhabha Atomic Research Center, Computational Analysis Division.) Mr Neeraj Shiv (Bhabha Atomic Research Center, Computational Analysis Division) Mr Nagaraju Belli (Bhabha Atomic Research Center, Computational Analysis Division) Mr Sukanta Mahar (Bhabha Atomic Research Center, Computational Analysis Division) Mr Suryaprasad V.V Illa (Bhabha Atomic Research Center, Computational Analysis Division) Mr Harsh Hemani (Bhabha Atomic Research Center, Computational Analysis Division) Mr Bhavesh Kadia (Institute for Plasma Research) Nandini Yadava (Gujarat University) Malay Bikas Chowdhuri (Institute for Plasma Research) RANJANA MANCHANDA (INSTITUTE FOR PLASMA RESEARCH) Gaurav Shukla (Pandit Deendayal Petroleum University) Mrs Nilam Ramaiya (Institute for Plasma Research) Jayesh Raval (Institute for Plasma Research (IPR), Bhat, Gandhinagar, India) Manoj Kumar (Institute for Plasma Research) Umesh Kumar Nagora (Institute for Plasma Research) Dr Surya Kumar Pathak (Institute for Plasma Research) Kumudni Tahiliani (Institute for Plasma Research, India) Prof. P.K. Chattopadhyay (Institute for Plasma Research) Paritosh Chaudhuri (Institute for Plasma Research) Maya Padivattathumana (ITER-India, Institute for Plasma Research) Dr Rajiv Goswami (Institute for Plasma Research) Abhijit Sen (Institute for Plasma Research) Prof. Rabindranath Pal (Saha Institute of Nuclear Physics, Kolkata, India.) Dr Shashank Chaturvedi (Institute for Plasma Research)

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