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The outline of the paper is as follows. In the next section, we will define the tensor analysis and introduce the concept of Christoffel symbols. In section 3, we will discuss what part of the tensor analysis play role in the definition of the shell radial stress in the cylinder shell problem. In section 4, we will specify the torque acting on the cylinder shell due to the fluid driven by the centrifugal force. In section 5, we will define the induced membrane flow and the contribution of the surface flow to the shell stress. In section 6, we will discuss why the membrane flow has a significant contribution to the shell stress and how it is related to the thickness of the membrane. Finally, in section 7, we will use the results of the paper to find the critical physical values of the parameters and the corresponding infinite series expansions.
The designation of notation and definitions used in this paper has been as follows. Upper case letters denote manifolds whereas lower case letters stand for the later or intermediate variables. The quantities independent of the coordinate system on Riemannian manifold are called the tensor fields. Let M be a differentiable manifold. A vector field μ on M is called an infinitesimal vector field, or simply a vector. A tensor field T of type (0,q) on M is a function that assigns a vector to each point of M, i.e., T: M>>V = R(M, V), for each vector field V in Vp(M), where the tensor R is of type (q, 0) on M. A tensor field of type (1,1) is a linear mapping (see [1960]):
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