The interaction of a cylindrical element of hot or cold gas (the "entropy s
pot") with a shock wave is considered. An exact solution in the limit of we
ak spot amplitudes is elaborated, using the linear interaction analysis the
ory and the procedure of decomposition proposed by Ribner (Technical Report
No. 1164, NACA, 1953). The method is applied to an entropy spot with a Gau
ssian profile. Results are presented for a wide range of shock Mach numbers
, with a special interest at M-1=2. The resulting vorticity field consists
of a pair of primary counter-rotating vortices, as well as a pair of second
ary vortices of opposite sign and weaker amplitude. An expression for the c
irculation in half a plane is derived and compared to existing results. The
pressure field consists of a cylindrical acoustic wave which propagates aw
ay from the transmitted spot and an evanescent nonpropagative field confine
d behind the shock. For a hot spot, the cylindrical wave is a rarefaction w
ave on its forward front and a compression wave on its upstream propagating
parts, and the nonpropagative field corresponds to a pressure deficit. The
structure of the transmitted spot and the shock deformation are also discu
ssed. The linear solution is compared with numerical simulation results for
M-1=2 and M-1=4. The comparison shows qualitative and quantitative agreeme
nt when linear as well as nonlinear spot amplitudes are considered. Finally
, the method is applied to the case of a constant spot with a tophat profil
e, and the results are compared to the case of a Gaussian spot. This paper
also contains in the Appendix a general formulation of the linear interacti
on problem for the three kinds of plane waves (entropy, vorticity, and pres
sure waves) impinging upon a shock. (C) 2001 American Institute of Physics.