The subsonic compressible flow over a cosine-shaped (wavy) wall is illustrated in Fig- ure 2.17. The wavelength and amplitude of the wall are I and h, respectively, as shown in Figure 2.17. The streamlines exhibit the same qualitative shape as the wall, but with diminishing amplitude as distance above the wall increases. Finally, as y → 0, the Streamline at V , M. 2h Figure 2.17 Subsonic compressible flow over a wavy wall; the streamline pattern. streamline becomes straight. Along this straight streamline, the freestream velocity and Mach number are Vo and Mo, respectively. The velocity field in cartesian coordinates is given by h 2n u = Voo 1+ 2лх -2т Ву/е cos (2.35) ве v =-Voh 2л sin and e-27By/e (2.36) B = VT- M where Consider the particular flow that exists for the case where l = 1.0 m, h = 0.01 m, V = 240 m/s, and Mo = 0.7. Also, consider a fluid element of fixed mass moving along a streamline in the flow field. The fluid element passes through the point (x/E, y/€) = (4, 1). At this point, calculate the time rate of change of the volume of the fluid element, per unit volume.
The subsonic compressible flow over a cosine-shaped (wavy) wall is illustrated in Fig- ure 2.17. The wavelength and amplitude of the wall are I and h, respectively, as shown in Figure 2.17. The streamlines exhibit the same qualitative shape as the wall, but with diminishing amplitude as distance above the wall increases. Finally, as y → 0, the Streamline at V , M. 2h Figure 2.17 Subsonic compressible flow over a wavy wall; the streamline pattern. streamline becomes straight. Along this straight streamline, the freestream velocity and Mach number are Vo and Mo, respectively. The velocity field in cartesian coordinates is given by h 2n u = Voo 1+ 2лх -2т Ву/е cos (2.35) ве v =-Voh 2л sin and e-27By/e (2.36) B = VT- M where Consider the particular flow that exists for the case where l = 1.0 m, h = 0.01 m, V = 240 m/s, and Mo = 0.7. Also, consider a fluid element of fixed mass moving along a streamline in the flow field. The fluid element passes through the point (x/E, y/€) = (4, 1). At this point, calculate the time rate of change of the volume of the fluid element, per unit volume.
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
Section: Chapter Questions
Problem 1.1MA
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Assume an inviscid, incompressible flow. Also, standard sea level density and pressure are 1.23 kg/m3 (0.002377 slug/ft3) and 1.01 × 105 N/m2(2116 lb/ft2), respectively.
Prove that the flow field specified is not incompressible;
i.e., it is a compressible flow as stated without proof .
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