584 research outputs found

    Real-time control of a Tokamak plasma using neural networks

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    This paper presents results from the first use of neural networks for the real-time feedback control of high temperature plasmas in a Tokamak fusion experiment. The Tokamak is currently the principal experimental device for research into the magnetic confinement approach to controlled fusion. In the Tokamak, hydrogen plasmas, at temperatures of up to 100 Million K, are confined by strong magnetic fields. Accurate control of the position and shape of the plasma boundary requires real-time feedback control of the magnetic field structure on a time-scale of a few tens of microseconds. Software simulations have demonstrated that a neural network approach can give significantly better performance than the linear technique currently used on most Tokamak experiments. The practical application of the neural network approach requires high-speed hardware, for which a fully parallel implementation of the multi-layer perceptron, using a hybrid of digital and analogue technology, has been developed

    Developement of real time diagnostics and feedback algorithms for JET in view of the next step

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    Real time control of many plasma parameters will be an essential aspect in the development of reliable high performance operation of Next Step Tokamaks. The main prerequisites for any feedback scheme are the precise real-time determination of the quantities to be controlled, requiring top quality and highly reliable diagnostics, and the availability of robust control algorithms. A new set of real time diagnostics was recently implemented on JET to prove the feasibility of determining, with high accuracy and time resolution, the most important plasma quantities. With regard to feedback algorithms, new model–based controllers were developed to allow a more robust control of several plasma parameters. Both diagnostics and algorithms were successfully used in several experiments, ranging from H-mode plasmas to configuration with ITBs. Since elaboration of computationally heavy measurements is often required, significant attention was devoted to non-algorithmic methods like Digital or Cellular Neural/Nonlinear Networks. The real time hardware and software adopted architectures are also described with particular attention to their relevance to ITER.Comment: 12th International Congress on Plasma Physics, 25-29 October 2004, Nice (France

    Machine Learning and Deep Learning applications for the protection of nuclear fusion devices

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    This Thesis addresses the use of artificial intelligence methods for the protection of nuclear fusion devices with reference to the Joint European Torus (JET) Tokamak and the Wendenstein 7-X (W7-X) Stellarator. JET is currently the world's largest operational Tokamak and the only one operated with the Deuterium-Tritium fuel, while W7-X is the world's largest and most advanced Stellarator. For the work on JET, research focused on the prediction of โ€œdisruptionsโ€, and sudden terminations of plasma confinement. For the development and testing of machine learning classifiers, a total of 198 disrupted discharges and 219 regularly terminated discharges from JET. Convolutional Neural Networks (CNNs) were proposed to extract the spatiotemporal characteristics from plasma temperature, density and radiation profiles. Since the CNN is a supervised algorithm, it is necessary to explicitly assign a label to the time windows of the dataset during training. All segments belonging to regularly terminated discharges were labelled as 'stable'. For each disrupted discharge, the labelling of 'unstable' was performed by automatically identifying the pre-disruption phase using an algorithm developed during the PhD. The CNN performance has been evaluated using disrupted and regularly terminated discharges from a decade of JET experimental campaigns, from 2011 to 2020, showing the robustness of the algorithm. Concerning W7-X, the research involved the real-time measurement of heat fluxes on plasma-facing components. THEODOR is a code currently used at W7-X for computing heat fluxes offline. However, for heat load control, fast heat flux estimation in real-time is required. Part of the PhD work was dedicated to refactoring and optimizing the THEODOR code, with the aim of speeding up calculation times and making it compatible with real-time use. In addition, a Physics Informed Neural Network (PINN) model was proposed to bring thermal flow computation to GPUs for real-time implementation

    A machine-learning-based tool for last closed magnetic flux surface reconstruction on tokamak

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    Nuclear fusion power created by tokamak devices holds one of the most promising ways as a sustainable source of clean energy. One main challenge research field of tokamak is to predict the last closed magnetic flux surface (LCFS) determined by the interaction of the actuator coils and the internal tokamak plasma. This work requires high-dimensional, high-frequency, high-fidelity, real-time tools, further complicated by the wide range of actuator coils input interact with internal tokamak plasma states. In this work, we present a new machine learning model for reconstructing the LCFS from the Experimental Advanced Superconducting Tokamak (EAST) that learns automatically from the experimental data of EAST. This architecture can check the control strategy design and integrate it with the tokamak control system for real-time magnetic prediction. In the real-time modeling test, our approach achieves over 99% average similarity in LCFS reconstruction of the entire discharge process. In the offline magnetic reconstruction, our approach reaches over 93% average similarity

    ๊ฐ•ํ™”ํ•™์Šต์„ ์ด์šฉํ•œ KSTAR ํ† ์นด๋ง‰ ์šด์ „ ๊ถค์  ์„ค๊ณ„

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์—๋„ˆ์ง€์‹œ์Šคํ…œ๊ณตํ•™๋ถ€, 2022. 8. ๋‚˜์šฉ์ˆ˜.ํ† ์นด๋ง‰์—์„œ ์ •๋ฐ€ํ•œ ๋ฌผ๋ฆฌ ์‹คํ—˜์„ ํ•˜๊ธฐ ์œ„ํ•ด์„œ๋Š” ๋จผ์ € ํŠน์ •ํ•œ ๋‚ด๋ถ€ ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ๋‹ฌ์„ฑํ•˜๊ณ  ์œ ์ง€ํ•˜๋Š” ๊ฒƒ์ด ํ•„์š”ํ•˜๋‹ค. ํŠนํžˆ ์ƒ์šฉ ํ•ต์œตํ•ฉ๋กœ ์šด์ „์„ ์œ„ํ•ด์„œ๋Š” ์ž๊ธฐ์œ ์ฒด์—ญํ•™์ ์œผ๋กœ ์•ˆ์ •์ ์ธ ํ”Œ๋ผ์ฆˆ๋งˆ ์˜์—ญ ๋‚ด์—์„œ์˜ ์ œ์–ด๊ฐ€ ํ•„์ˆ˜์ ์ด๋ฉฐ, ๊ณ ์ถœ๋ ฅ์˜ ํ•ต์œตํ•ฉ ๋ฐ˜์‘์„ ์ผ์œผํ‚ฌ ์ˆ˜ ์žˆ๋Š” ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ์œ ์ง€ํ•  ์ˆ˜ ์žˆ์–ด์•ผ ํ•œ๋‹ค. ๊ธฐ์กด์—๋Š” ์‹คํ—˜์—์„œ ๋ชฉํ‘œ๋กœ ํ•˜๋Š” ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•ด, ๋‹ค์–‘ํ•œ ํ† ์นด๋ง‰ ์šด์ „ ์กฐ๊ฑด์—์„œ์˜ ์‚ฌ์ „ ์‹œ๋ฎฌ๋ ˆ์ด์…˜๊ณผ ์‹คํ—˜์—์„œ์˜ ์ถ”๊ฐ€์ ์ธ ์‹œํ–‰์ฐฉ์˜ค๊ฐ€ ํ•„์š”ํ•˜์˜€๋‹ค. ์ด ๊ฒฝ์šฐ ๋งŽ์€ ์ธ์  ๋…ธ๋™๋ ฅ๊ณผ ์‹œ๊ฐ„์ด ์†Œ์š”๋˜์—ˆ์œผ๋ฉฐ, ์ƒˆ๋กœ์šด ๋ชฉํ‘œ ์ƒํƒœ๋“ค์— ๋Œ€ํ•ด ๋งค๋ฒˆ ๋™์ผํ•œ ์ˆ˜์ค€์˜ ์‹œํ–‰์ฐฉ์˜ค๊ฐ€ ์š”๊ตฌ๋œ๋‹ค๋Š” ๋ฌธ์ œ๊ฐ€ ์žˆ๋‹ค. ๋ณธ ๋…ผ๋ฌธ์€ ๋ชฉํ‘œ ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•œ ํ† ์นด๋ง‰์˜ ์šด์ „ ๊ฒฝ๋กœ๋ฅผ ์„ค๊ณ„ํ•˜๋Š” ๊ธฐ๊ณ„ํ•™์Šต ๊ธฐ๋ฐ˜์˜ ์•Œ๊ณ ๋ฆฌ์ฆ˜ ๊ฐœ๋ฐœ์„ ๋‹ค๋ฃฌ๋‹ค. ํ•ด๋‹น ์•Œ๊ณ ๋ฆฌ์ฆ˜์€ ๊ธฐ์กด์˜ ์ƒ๋‹นํ•œ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๋ฐ ์‹œํ–‰์ฐฉ์˜ค๋ฅผ ์ˆ˜ํ–‰ํ•˜๋Š” ์ž‘์—…๋“ค์„ ๋Œ€์ฒดํ•  ์ˆ˜ ์žˆ์œผ๋ฉฐ, ์ด๋ฅผ ํ†ตํ•ด ๋ณด๋‹ค ๋น ๋ฅด๊ณ  ํšจ์œจ์ ์œผ๋กœ ๊ฐ€๋Šฅ์„ฑ ๋†’์€ ์šด์ „ ์กฐ๊ฑด์„ ๋„์ถœํ•  ์ˆ˜ ์žˆ๋‹ค. ์ฒซ ๋ฒˆ์งธ๋กœ, ํ† ์นด๋ง‰ ์šด์ „ ์„ค๊ณ„ ์ธ๊ณต์ง€๋Šฅ ๋ชจ๋ธ์˜ ํ›ˆ๋ จ ํ™˜๊ฒฝ์— ํ•ด๋‹นํ•˜๋Š” ํ† ์นด๋ง‰ ์‹œ๋ฎฌ๋ ˆ์ด์…˜ ๊ธฐ์ˆ ์ด ์—ฐ๊ตฌ๋˜์—ˆ๋‹ค. KSTAR ์‹คํ—˜ ๋ฐ์ดํ„ฐ์˜ ํŒจํ„ด์„ ํ•™์Šตํ•˜์—ฌ ์‹œ๊ฐ„์— ๋”ฐ๋ฅธ ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ์ˆœ์ฐจ์ ์œผ๋กœ ์˜ˆ์ธกํ•˜๋Š” LSTM ๊ธฐ๋ฐ˜์˜ ์ธ๊ณต์‹ ๊ฒฝ๋ง ๋ชจ๋ธ์„ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ๋ฐ์ดํ„ฐ ํ•™์Šต ๊ณผ์ •์—์„œ ๊ณผ์ ํ•ฉ ๋ฐ ์˜ค์ฐจ ๋ˆ„์  ๋“ฑ์˜ ๋ฌธ์ œ๋ฅผ ํ•ด๊ฒฐํ•˜๊ธฐ ์œ„ํ•ด ๋‹ค์–‘ํ•œ ์ˆ˜์น˜์  ๊ธฐ๋ฒ•๋“ค์ด ์ ์šฉ๋˜์—ˆ๋‹ค. ํ•™์Šต๋œ ๋ชจ๋ธ์€ KSTAR์˜ ๋‹ค์–‘ํ•œ ์šด์ „ ์‹œ๋‚˜๋ฆฌ์˜ค ๋ฐฉ์ „๋“ค์— ๋Œ€ํ•ด ์šฐ์ˆ˜ํ•œ ์˜ˆ์ธก ์ •ํ™•๋„๋ฅผ ๋ณด์—ฌ์ฃผ์—ˆ์œผ๋ฉฐ, ์‹ ๋ขฐ๋„ ๋ถ„์„์„ ํ†ตํ•ด ๋ชจ๋ธ์ด ๊ณผ์ ํ•ฉ๋˜์ง€ ์•Š์Œ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋˜ํ•œ ํ•ด๋‹น ๋ชจ๋ธ์„ ๊ธฐ๋ฐ˜์œผ๋กœ, ์‹ค์‹œ๊ฐ„ ์ƒํ˜ธ์ž‘์šฉ์„ ํ†ตํ•œ ๊ฐ€์ƒ ํ† ์นด๋ง‰ ์‹คํ—˜์ด ๊ฐ€๋Šฅํ•˜๋„๋ก ๊ทธ๋ž˜ํ”ฝ ์‚ฌ์šฉ์ž ์ธํ„ฐํŽ˜์ด์Šค (GUI)๋ฅผ ๊ฐœ๋ฐœํ•˜์˜€๋‹ค. ํ•ด๋‹น GUI ์ƒ์—์„œ ์‚ฌ์šฉ์ž๊ฐ€ ํ† ์นด๋ง‰ ์šด์ „ ๋ณ€์ˆ˜๋“ค์„ ์กฐ์ •ํ•จ์— ๋”ฐ๋ผ ํ”Œ๋ผ์ฆˆ๋งˆ์˜ ๋ณ€ํ™”๋ฅผ ์‹ค์‹œ๊ฐ„์œผ๋กœ ์‹œ๊ฐ์ ์œผ๋กœ ํ™•์ธํ•  ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์— ๋ฌผ๋ฆฌ ์—ฐ๊ตฌ ๋ฟ ์•„๋‹ˆ๋ผ ์ „๋ฌธ๊ฐ€ ๊ต์œก์šฉ์œผ๋กœ์„œ์˜ ์˜์˜๊ฐ€ ์žˆ๋‹ค. ๋‘ ๋ฒˆ์งธ๋กœ, ๊ฐœ๋ฐœ๋œ ์‹œ๋ฎฌ๋ ˆ์ดํ„ฐ ์ƒ์—์„œ ์Šค์Šค๋กœ ์šด์ „ ๋ณ€์ˆ˜๋“ค์„ ์กฐ์ •ํ•˜์—ฌ ๋ชฉํ‘œ๋กœ ํ•˜๋Š” ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ๋‹ฌ์„ฑํ•˜๋Š” ์ธ๊ณต์ง€๋Šฅ ๋ชจ๋ธ์„ ๊ฐ•ํ™”ํ•™์Šต ๊ธฐ๋ฒ•์„ ์ด์šฉํ•˜์—ฌ ํ›ˆ๋ จํ•˜์˜€๋‹ค. ์ด๋ฅผ ํ†ตํ•ด ๋ชฉํ‘œ ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•œ ์ ์ ˆํ•œ ํ† ์นด๋ง‰ ์šด์ „ ๊ฒฝ๋กœ๋ฅผ ์„ค๊ณ„ํ•˜๋Š” ์•Œ๊ณ ๋ฆฌ์ฆ˜์„ ๊ฐœ๋ฐœํ•  ์ˆ˜ ์žˆ๋‹ค. ๋จผ์ € ๋ชฉํ‘œ ฮฒ_N ๋‹ฌ์„ฑ์„ ์œ„ํ•ด ํ”Œ๋ผ์ฆˆ๋งˆ ์ „๋ฅ˜, ํ”Œ๋ผ์ฆˆ๋งˆ ํ˜•ํƒœ ๋ฐ ๊ฐ€์—ด ํŒŒ์›Œ๋ฅผ ๊ฒฐ์ •ํ•˜๋Š” ๋ชจ๋ธ์„ ํ›ˆ๋ จํ•˜์˜€๋‹ค. ํ›ˆ๋ จ๋œ ๋ชจ๋ธ์ด ์„ค๊ณ„ํ•œ ์šด์ „ ๊ฒฝ๋กœ๋ฅผ ์ด์šฉํ•˜์—ฌ ์‹คํ—˜์„ ์ˆ˜ํ–‰ํ•ด๋ณธ ๊ฒฐ๊ณผ ์˜ค์ฐจ๋ฒ”์œ„ ๋‚ด์—์„œ ๋ชฉํ‘œ ฮฒ_N์ด ๋„์ถœ๋จ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ํŠนํžˆ ํ•œ์ •๋œ ๊ฐ€์—ด ์กฐ๊ฑด์—์„œ ๋†’์€ ์„ฑ๋Šฅ์„ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•ด ํ”Œ๋ผ์ฆˆ๋งˆ ํ˜•ํƒœ๋ฅผ ์ ์ ˆํžˆ ์กฐ์ •ํ•˜์—ฌ ๊ฐ€๋‘  ์„ฑ๋Šฅ์„ ํ–ฅ์ƒ์‹œํ‚ค๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ดํ›„ ๋ณด๋‹ค ๋” ๊ตฌ์ฒด์ ์ธ ํ”Œ๋ผ์ฆˆ๋งˆ ์ƒํƒœ๋ฅผ ๋‹ฌ์„ฑํ•˜๊ธฐ ์œ„ํ•ด, ํ”Œ๋ผ์ฆˆ๋งˆ ์••๋ ฅ (ฮฒ_p) ๋ฟ ์•„๋‹ˆ๋ผ ์ž๊ธฐ์žฅ ๊ตฌ์กฐ (q_95) ๋ฐ ๋‚ด๋ถ€ ์ธ๋•ํ„ด์Šค (l_i)์˜ ๋‹ค์ค‘ ํŒŒ๋ผ๋ฏธํ„ฐ๋“ค์˜ ๋ชฉํ‘œ๊ฐ’์„ ๋™์‹œ์— ๋‹ฌ์„ฑ์ผ€ ํ•˜๋Š” ์ธ๊ณต์ง€๋Šฅ ๋ชจ๋ธ ๋˜ํ•œ ํ›ˆ๋ จํ•˜์˜€๋‹ค. ํ•ด๋‹น ๋ชจ๋ธ์ด ์„ค๊ณ„ํ•œ ์šด์ „ ๊ฒฝ๋กœ๋ฅผ ์‹ค์ œ ์‹คํ—˜์— ์ ์šฉํ•ด๋ณธ ๊ฒฐ๊ณผ, ๋‹ค์ค‘ ํ”Œ๋ผ์ฆˆ๋งˆ ํŒŒ๋ผ๋ฏธํ„ฐ๋“ค์ด ์„ฑ๊ณต์ ์œผ๋กœ ๋ชฉํ‘œ๊ฐ’์œผ๋กœ ์ œ์–ด๋จ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ ๊ฐœ๋ฐœ๋œ ๊ธฐ๊ณ„ํ•™์Šต ๊ธฐ๋ฐ˜ ์•Œ๊ณ ๋ฆฌ์ฆ˜์€ ์ถ”ํ›„ ๊ณ ์„ฑ๋Šฅ ์šด์ „ ์‹œ๋‚˜๋ฆฌ์˜ค ์—ฐ๊ตฌ์— ๋„์›€์„ ์ค„ ์ˆ˜ ์žˆ์œผ๋ฉฐ, ์ •๋ฐ€ํ•œ ๋ฌผ๋ฆฌ ์กฐ๊ฑด์„ ์š”๊ตฌํ•˜๋Š” ์‹คํ—˜์—์„œ ์ดˆ๊ธฐ ์กฐ๊ฑด ๋‹ฌ์„ฑ์„ ์œ„ํ•œ ๊ธฐ์ˆ ๋กœ ์ ์šฉ๋  ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ๊ธฐ๋Œ€๋œ๋‹ค. ์ถ”ํ›„ ์‹ค์‹œ๊ฐ„ ํ”ผ๋“œ๋ฐฑ ์ œ์–ด์— ์ ์šฉ๋จ์œผ๋กœ์จ ๋‹ค์–‘ํ•œ ์ƒํ™ฉ์—์„œ ์ž์œจ์ ์œผ๋กœ ์ œ์–ด๋˜๋Š” ํ•ต์œตํ•ฉ๋กœ ๊ธฐ์ˆ  ๊ฐœ๋ฐœ์„ ์œ„ํ•œ ์ดˆ์„์ด ๋  ์ˆ˜ ์žˆ์„ ๊ฒƒ์œผ๋กœ ์ „๋งํ•œ๋‹ค.In order to conduct a sophisticated physics experiment in a tokamak, it is necessary to achieve and sustain a specific target plasma state first. Especially, the commercial fusion reactor requires controlling plasmas within a stable parametric range and maintaining a favorable plasma state for high fusion power generation. Conventionally, we had to conduct numerous simulations with various tokamak operating conditions and experiment with trials and errors for achieving a target plasma state. This takes lots of labor and time and requires the same level of trial and error for different targets each time. This thesis addresses the development of a reinforcement learning (RL)-based algorithm that designs the tokamak operation trajectory to achieve a given target plasma state. This algorithm replaces the conventional manual tasks of numerous simulative experiments and provides a probable tokamak operation condition faster and more efficiently. First, the tokamak simulator, corresponding to the training environment of the RL agent that designs the operation trajectory, was developed. An LSTM-based neural network was trained that sequentially predicts the plasma state over time by learning the patterns of the KSTAR experimental data. Various numerical techniques were applied to prevent overfitting and error accumulation during the training process. The trained model showed reasonable prediction accuracy for various operation scenarios in KSTAR, and reliability analyses verified that the model was not significantly overfitted. Furthermore, based on the trained model, we developed a graphical user interface (GUI) to enable virtual tokamak experiments through real-time interaction. By adjusting the tokamak operation parameters on the GUI, the user can visually check the plasma evolution in real time, which can be useful not only for physics research but also for expert education. Second, an artificial agent was trained using a reinforcement learning technique, that adjusts the operation parameters to achieve a target plasma state in the developed simulator. This agent can design a plausible tokamak operation trajectory to achieve a given target after training. First, the agent was trained to determine the plasma current, the plasma shape, and the heating power to achieve the target ฮฒ_N. We conducted a KSTAR experiment with the operation trajectory designed by the trained agent, and it was verified that the target performance was achieved within the tolerance range. In particular, it was observed that the confinement enhancement factor was improved by adjusting the plasma shape to achieve high performance under limited heating conditions. Moreover, in order to achieve a more specific plasma state, another RL agent was trained to achieve multiple targets of ฮฒ_p, q_95, and l_i simultaneously. The KSTAR experiment with the RL operation design showed that multiple plasma parameters were successfully controlled to the target values. The RL-based algorithm addressed in this thesis can provide clues for the research of advanced operation scenarios and can be applied to achieve initial plasma states in experiments that require sophisticated physical conditions. By applying this algorithm to real-time feedback control in the future, it will become a basis for developing a self-operating fusion reactor that can be autonomously controlled to achieve high power generation.1. Introduction ๏ผ‘ 1.1. Advanced operation scenario in tokamak ๏ผ“ 1.2. Machine learning in fusion research ๏ผ” 1.2.1. Precedent research ๏ผ” 1.2.2. AI operation trajectory design and control ๏ผ– 1.2.3. Simulation of tokamak plasmas ๏ผ‘๏ผ 1.3. Objective and outline of this dissertation ๏ผ‘๏ผ• 2. Data-driven tokamak simulator ๏ผ‘๏ผ— 2.1. Predictive modeling with DNN ๏ผ‘๏ผ˜ 2.1.1. Construction and training of the LSTM-based model ๏ผ‘๏ผ˜ 2.1.2. Demonstration and validation ๏ผ’๏ผ™ 2.2. Analysis for model reliability ๏ผ“๏ผ’ 2.2.1. Uncertainties in dataset ๏ผ“๏ผ’ 2.2.2. Consistency with prior knowledge ๏ผ“๏ผ” 3. Operation trajectory design algorithm ๏ผ“๏ผ– 3.1. Environment of the RL training ๏ผ“๏ผ— 3.2. Control of normalized beta ๏ผ“๏ผ™ 3.2.1. The action, observation, and reward for RL ๏ผ“๏ผ™ 3.2.2. RL training ๏ผ”๏ผ” 3.3. Simultaneous control of multiple parameters ๏ผ”๏ผ• 3.3.1. The action, observation, and reward for RL ๏ผ”๏ผ• 3.3.2. RL training ๏ผ”๏ผ™ 4. Validation in KSTAR ๏ผ•๏ผ“ 4.1. Control of normalized beta ๏ผ•๏ผ” 4.1.1. Case 1: ฮฒ_N control to 2.4 and 1.8 ๏ผ•๏ผ” 4.1.2. Case 2: ฮฒ_N control to 2.7 ๏ผ•๏ผ— 4.1.3. Case 3: ฮฒ_N control to 3.5 ๏ผ–๏ผ 4.2. Simultaneous control of multiple 0D parameters ๏ผ–๏ผ’ 4.2.1. Experiment with RL-designed trajectory ๏ผ–๏ผ’ 4.2.2. Comparison with other shots in dataset ๏ผ–๏ผ– 5. Conclusion ๏ผ–๏ผ™ Bibliography ๏ผ—๏ผ‘ Abstract in Korean ๏ผ—๏ผ—๋ฐ•

    Using LSTM for the Prediction of Disruption in ADITYA Tokamak

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    Major disruptions in tokamak pose a serious threat to the vessel and its surrounding pieces of equipment. The ability of the systems to detect any behavior that can lead to disruption can help in alerting the system beforehand and prevent its harmful effects. Many machine learning techniques have already been in use at large tokamaks like JET and ASDEX, but are not suitable for ADITYA, which is comparatively small. Through this work, we discuss a new real-time approach to predict the time of disruption in ADITYA tokamak and validate the results on an experimental dataset. The system uses selected diagnostics from the tokamak and after some pre-processing steps, sends them to a time-sequence Long Short-Term Memory (LSTM) network. The model can make the predictions 12 ms in advance at less computation cost that is quick enough to be deployed in real-time applications.Comment: 7 pages, 4 figure
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