-
1
-
-
0018003009
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(1978)
Nucl. Fusion
, vol.18
, pp. 1089
-
-
Tang, W.M.1
-
2
-
-
0020720147
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(1983)
Nucl. Fusion
, vol.23
, pp. 331
-
-
Hugill, J.1
-
3
-
-
0022059957
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(1985)
Nucl. Fusion
, vol.25
, pp. 543
-
-
Liewer, P.C.1
-
4
-
-
13044274473
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(1990)
Phys. Fluids B
, vol.2
, pp. 2879
-
-
Wootlon, A.J.1
Carreras, B.A.2
Matsumoto, H.3
McGuire, K.4
Peebles, W.A.5
Ritz, C.P.6
Terry, P.W.7
Zweben, S.J.8
-
5
-
-
0029404103
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(1995)
Plasma Phys. Controlled Fusion
, vol.37
-
-
Connor, J.W.1
-
6
-
-
0001057458
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(2000)
Plasma Phys. Controlled Fusion
, vol.42
-
-
Hahm, T.S.1
Burrell, K.H.2
Lin, Z.3
Nazikian, R.4
Synakowski, E.J.5
-
7
-
-
0035250107
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(2001)
Plasma Phys. Controlled Fusion
, vol.43
, pp. 155
-
-
Connor, J.W.1
Pogutse, O.P.2
-
8
-
-
0036573413
-
-
For a series of reviews see W. M. Tang, Nucl. Fusion 18, 1089 (1978); J. Hugill, ibid. 23, 331 (1983); P. C. Liewer, ibid. 25, 543 (1985); A. J. Wootlon, B. A. Carreras, H. Matsumoto, K. McGuire, W. A. Peebles, C. P. Ritz, P. W. Terry, and S. J. Zweben, Phys. Fluids B 2, 2879 (1990); J. W. Connor, Plasma Phys. Controlled Fusion 37, A119 (1995); T. S. Hahm, K. H. Burrell, Z. Lin, R. Nazikian, and E. J. Synakowski, ibid. 42, A205 (2000); J. W. Connor and O. P. Pogutse, ibid. 43, 155 (2001); T. S. Hahm, ibid. 44, A87 (2002).
-
(2002)
Plasma Phys. Controlled Fusion
, vol.44
-
-
Hahm, T.S.1
-
20
-
-
0001084316
-
-
P. Rutherford and E. A. Frieman, Phys. Fluids 11, 569 (1968); J. B. Taylor and R. J. Hastie, Plasma Phys. 10, 479 (1968).
-
(1968)
Plasma Phys.
, vol.10
, pp. 479
-
-
Taylor, J.B.1
Hastie, R.J.2
-
21
-
-
0003901895
-
-
G. Knorr, F. R. Hansen, J. P. Lynov, H. L. Pécseli, and J. Juul Rasmussen, Phys. Scr. 38, 829 (1988).
-
(1988)
Phys. Scr.
, vol.38
, pp. 829
-
-
Knorr, G.1
Hansen, F.R.2
Lynov, J.P.3
Pécseli, H.L.4
Juul Rasmussen, J.5
-
26
-
-
4243995387
-
-
B. Scott, Phys. Rev. Lett. 65, 3289 (1990); Phys. Fluids B 4, 2468 (1992).
-
(1990)
Phys. Rev. Lett.
, vol.65
, pp. 3289
-
-
Scott, B.1
-
27
-
-
0001587236
-
-
B. Scott, Phys. Rev. Lett. 65, 3289 (1990); Phys. Fluids B 4, 2468 (1992).
-
(1992)
Phys. Fluids B
, vol.4
, pp. 2468
-
-
-
29
-
-
11844281670
-
GEM - An energy conserving electromagnetic gyrofluid model
-
to be published
-
B. Scott, "GEM - An energy conserving electromagnetic gyrofluid model," Phys. Plasmas (to be published).
-
Phys. Plasmas
-
-
Scott, B.1
-
33
-
-
0003610460
-
-
Kl.235
-
E. Noether, Nachr. Ges. Wiss. Goettingen, Math.-Phys. Kl.235 (1918); [English translation by M. A. Travel.Transp. Theory Stat. Phys. 1, 183 (1971)], see The Classical Theory of Fields, edited by L. D. Landau and E. M. Lifshitz (Pergamon, New York, 1972) for an elementary introduction
-
(1918)
Nachr. Ges. Wiss. Goettingen, Math.-Phys.
-
-
Noether, E.1
-
34
-
-
84863910689
-
-
E. Noether, Nachr. Ges. Wiss. Goettingen, Math.-Phys. Kl.235 (1918); [English translation by M. A. Travel.Transp. Theory Stat. Phys. 1, 183 (1971)], see The Classical Theory of Fields, edited by L. D. Landau and E. M. Lifshitz (Pergamon, New York, 1972) for an elementary introduction
-
(1971)
Transp. Theory Stat. Phys.
, vol.1
, pp. 183
-
-
Travel, M.A.1
-
35
-
-
0003831091
-
-
Pergamon, New York
-
E. Noether, Nachr. Ges. Wiss. Goettingen, Math.-Phys. Kl.235 (1918); [English translation by M. A. Travel.Transp. Theory Stat. Phys. 1, 183 (1971)], see The Classical Theory of Fields, edited by L. D. Landau and E. M. Lifshitz (Pergamon, New York, 1972) for an elementary introduction
-
(1972)
The Classical Theory of Fields
-
-
Landau, L.D.1
Lifshitz, E.M.2
-
42
-
-
11844261638
-
-
note
-
E appears also in the symplectic form; these differ by a simple Lie transform. The version used here results in the appearance of polarization effects solely in the self-consistent field equation for the potential, hence the same mathematical structure as in the gyrokinetic theory, which is desirable for computational reasons.
-
-
-
-
43
-
-
0000019980
-
-
F. Jenko, W. Dorland, M. Kotschenreuther, and B. N. Rogers, Phys. Plasmas 7, 1904 (2000).
-
(2000)
Phys. Plasmas
, vol.7
, pp. 1904
-
-
Jenko, F.1
Dorland, W.2
Kotschenreuther, M.3
Rogers, B.N.4
-
45
-
-
0001367102
-
-
This choice is set to recover the desired pressure equation with two degrees of freedom, so that the factors in gyroaveraging emerge correctly. CGL theory uses s = pnB [cf. G. F. Chew, M. L. Goldberger, and F. E. Low, Proc. R. Soc. London, Ser. A 236, 112 (1956), and later V. Ilgisonis, Phys. Plasmas 3, 4577 (1996)] but also depends on MHD ordering with respect to the velocities (neEΔp). It is possible the CGL forms are superior in the case full temperature anisotropy is treated; we will address this in future work.
-
(1956)
Proc. R. Soc. London, Ser. A
, vol.236
, pp. 112
-
-
Chew, G.F.1
Goldberger, M.L.2
Low, F.E.3
-
46
-
-
0040665563
-
-
This choice is set to recover the desired pressure equation with two degrees of freedom, so that the factors in gyroaveraging emerge correctly. CGL theory uses s = pnB [cf. G. F. Chew, M. L. Goldberger, and F. E. Low, Proc. R. Soc. London, Ser. A 236, 112 (1956), and later V. Ilgisonis, Phys. Plasmas 3, 4577 (1996)] but also depends on MHD ordering with respect to the velocities (neEΔp). It is possible the CGL forms are superior in the case full temperature anisotropy is treated; we will address this in future work.
-
(1996)
Phys. Plasmas
, vol.3
, pp. 4577
-
-
Ilgisonis, V.1
|