form of the resistance coefficient for porous, rigid screens of infinite extent. The second part examines the flow through and around a porous, rigid body of finite extent. This body will be located in an infinite flowfield, and will be rigid and incapable of significant distortion under the aerodynamic loading. Experimental results for tests on porous, circular disks will be given in Part II. Furthermore, it will be argued and demonstrated in Part II that a macroscopic examination of the flowfield neglects an important phenomenon which relates to the microscopic flow structure behind the adjacent small elements within the porous body. References 6-8 and 10 all relate to various macroscopic treatments.
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Bryan W. Robert (1980) studied this question.
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