By Hairer E.
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Additional resources for A- and B-stability for Runge-Kutta methods-characterizations and equivalence
Pure and Applied Mathematics, 7 , 159-93. 7). 14) for the internal energy e . 9). 1 1) reduces to a convection-diffusion balance of the stagnation enthalpy H when the Prandtl number is equal to one and when only the contribution from the work of the shear stresses related to the viscous diffusion of the kinetic energy is taken into account. Hint: Assume constant flow properties, setting k = yce in the absense of external sources, and separate the contributions to the term V ( 7 * U ) according to the following relations, valid for incompressible flows: V(7 - U ) = a,[p(a,v, + ~,u,)v,I= V a [pV(~2/2)1 + V.
1 showsthe sequenceof Mach contours at different times during the third buzz cycleat low mass flow (subcritical) regime for an incident Mach number of two. The oscillations develop as a consequenceof a shear layer instability due to separatedboundary layers, which amplify small pressuredisturbancesin a closedfeedback loop of reflected expansion and compression waves. Strong shockwave interactions and unsteady boundary layer separationsare marked phenomenaof this complex flow pattern. 1 ms) a region of reverse flow extends betweenthe baseof the bow shock and the cowl lip, with a shearlayer dividing thetwo regions.
PW)=O 3 1 - . Iwork of external forces fe- Wr = pfe k
A- and B-stability for Runge-Kutta methods-characterizations and equivalence by Hairer E.