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This is a repository copy of On Optimal Control of Plasma Confinement . White Rose Research Online URL for this paper: http://eprints.whiterose.ac.uk/75917/ Monograph: Banks, S.P and Mousavi-Khalkhali, S.A. (1981) On Optimal Control of Plasma Confinement. Research Report. ACSE Report 155 . Department of Control Engineering, University of Sheffield, Mappin Street, Sheffield [email protected] https://eprints.whiterose.ac.uk/ Reuse Unless indicated otherwise, fulltext items are protected by copyright with all rights reserved. The copyright exception in section 29 of the Copyright, Designs and Patents Act 1988 allows the making of a single copy solely for the purpose of non-commercial research or private study within the limits of fair dealing. The publisher or other rights-holder may allow further reproduction and re-use of this version - refer to the White Rose Research Online record for this item. Where records identify the publisher as the copyright holder, users can verify any specific terms of use on the publisher’s website. Takedown If you consider content in White Rose Research Online to be in breach of UK law, please notify us by emailing [email protected] including the URL of the record and the reason for the withdrawal request.

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Page 1: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron

This is a repository copy of On Optimal Control of Plasma Confinement.

White Rose Research Online URL for this paper:http://eprints.whiterose.ac.uk/75917/

Monograph:Banks, S.P and Mousavi-Khalkhali, S.A. (1981) On Optimal Control of Plasma Confinement. Research Report. ACSE Report 155 . Department of Control Engineering, University of Sheffield, Mappin Street, Sheffield

[email protected]://eprints.whiterose.ac.uk/

Reuse Unless indicated otherwise, fulltext items are protected by copyright with all rights reserved. The copyright exception in section 29 of the Copyright, Designs and Patents Act 1988 allows the making of a single copy solely for the purpose of non-commercial research or private study within the limits of fair dealing. The publisher or other rights-holder may allow further reproduction and re-use of this version - refer to the White Rose Research Online record for this item. Where records identify the publisher as the copyright holder, users can verify any specific terms of use on the publisher’s website.

Takedown If you consider content in White Rose Research Online to be in breach of UK law, please notify us by emailing [email protected] including the URL of the record and the reason for the withdrawal request.

Page 2: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 3: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 4: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 5: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 6: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 7: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 8: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 9: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 10: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 11: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 12: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 13: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 14: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 15: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 16: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 17: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 18: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 19: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 20: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 21: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 22: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 23: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 24: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron
Page 25: On Optimal Control of Plasma Confinementeprints.whiterose.ac.uk/75917/1/report 155.pdfVlasov equation for a collision less plasma oj (1.1) are the respective and f = e for electron