Sensitivity of global energy confinement to the boundary condition due to coupling of MHD and transport processes

1994 ◽  
Vol 51 (2) ◽  
pp. 201-210 ◽  
Author(s):  
X. H. Deng ◽  
C. Zhang ◽  
Y. P. Huo ◽  
J. F. Wang ◽  
Shui Wang

MHD instabilities are governed by the transport-determined plasma profiles, and the transport process is affected in turn by the instabilities. Using a one-dimensional code, we have investigated the inter-relationship between instabilities, transport and plasma profile in a tokamak discharge. The results show that the global energy confinement becomes strongly dependent on the boundary transport condition owing to strong coupling between them, and a higher edge temperature would ensure a higher core temperature and hence greater global energy confinement.

1970 ◽  
Vol 25 (8-9) ◽  
pp. 1207-1212
Author(s):  
J.U. Keller

Abstract In a paper 1 published recently a one-dimensional random walk-model for transport-processes with bounded velocity of propagation like heat conduction, diffusion and Brownian-motion has been given. Now this model is generalized to processes in 3 dimensions. We consider the transport process as a random-walk process in a primitive cubic lattice without boundaries and without external forces. The jump-probabilities of the random-walk-particle generally depend on the history of the particle. The resulting transport-equation contains terms which are due to the structure of the lattice not invariant under rotation. Further on this equation always describes transport-processes with bounded velocity of propagation.


1995 ◽  
Vol 2 (7) ◽  
pp. 2753-2759
Author(s):  
X. H. Deng ◽  
Y. P. Huo ◽  
C. Zhang ◽  
J. F. Wang ◽  
S. Wang

2001 ◽  
Vol 22 (5) ◽  
pp. 35-40 ◽  
Author(s):  
D. C. Look Jr ◽  
Arvind Krishnan

2009 ◽  
Vol 50 (3) ◽  
pp. 407-420
Author(s):  
ROGER YOUNG

AbstractAn analytic solution is developed for the one-dimensional dissipational slip gradient equation first described by Gurtin [“On the plasticity of single crystals: free energy, microforces, plastic strain-gradients”, J. Mech. Phys. Solids48 (2000) 989–1036] and then investigated numerically by Anand et al. [“A one-dimensional theory of strain-gradient plasticity: formulation, analysis, numerical results”, J. Mech. Phys. Solids53 (2005) 1798–1826]. However we find that the analytic solution is incompatible with the zero-sliprate boundary condition (“clamped boundary condition”) postulated by these authors, and is in fact excluded by the theory. As a consequence the analytic solution agrees with the numerical results except near the boundary. The equation also admits a series of higher mode solutions where the numerical result corresponds to (a particular case of) the fundamental mode. Anand et al. also established that the one-dimensional dissipational gradients strengthen the material, but this proposition only holds if zero-sliprate boundary conditions can be imposed, which we have shown cannot be done. Hence the possibility remains open that dissipational gradient weakening may also occur.


2010 ◽  
Vol 50 (6-7) ◽  
pp. 594-599 ◽  
Author(s):  
E. Ascasíbar ◽  
T. Estrada ◽  
M. Liniers ◽  
M. A. Ochando ◽  
F. L. Tabarés ◽  
...  

2010 ◽  
Vol 58 (1) ◽  
pp. 29-37 ◽  
Author(s):  
J. Miyazawa ◽  
H. Yamada ◽  
R. Sakamoto ◽  
H. Funaba ◽  
K. Y. Watanabe ◽  
...  

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