Question 6 of 6: Drag of a Plate Immersed in a Turbulent Boundary Layer
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format: National Exams – May 2017, 16-Mec-A6 Advanced Fluid Mechanics. Open book, 3 hours. Six questions of equal value (20 marks); any five constitute a complete paper. All six are solved here as a study resource.
Reference texts: Fox, Pritchard & McDonald, Introduction to Fluid Mechanics, 10th ed.; F. M. White, Fluid Mechanics, 8th ed.; J. D. Anderson, Modern Compressible Flow, 3rd ed. (Q1); I. G. Currie, Fundamental Mechanics of Fluids (Q2); Munson, Young & Okiishi, Fundamentals of Fluid Mechanics (Q5).
Note on the subject. The 16-Mec-A6 sittings (2017–2019) are the Advanced Fluid Mechanics syllabus — compressible flow, potential flow, integral momentum, lubrication theory, dimensional analysis and boundary layers — a different exam from the 07-Mec-A6 pump/turbine papers.
Question 6: Drag of a Plate Immersed in a Turbulent Boundary Layer (20 marks)
Given. A two-sided plate of streamwise length $L$ and height $\delta$ standing in a turbulent boundary layer whose approach velocity varies with height as $u(y)=U_\infty(y/\delta)^{1/7}$; the plate height equals the boundary-layer thickness $\delta$.
Find. (a) the plate drag coefficient; (b) the ratio of this drag to the uniform-stream ($U_\infty$) drag.
Figure 6: Splitter plate ($L\times\delta$) aligned with the flow, immersed in a $1/7$-power-law turbulent boundary layer; each height $y$ sees local free-stream $u(y)$.
Approach. Treat each horizontal strip $dy$ at height $y$ as an independent turbulent flat-plate boundary layer developing over length $L$ at the local free-stream speed $u(y)$, use the standard turbulent friction law $C_{D}=0.074\,Re_L^{-1/5}$ per side, and integrate over $0\le y\le\delta$.
Strip drag. For a strip of height $dy$ at local speed $U(y)$, both sides wetted, the turbulent flat-plate law gives
$$dF=2\left[0.074\left(\frac{U(y)L}{\nu}\right)^{-1/5}\right]\tfrac12\rho\,U(y)^2\,L\,dy=0.074\,\rho L\left(\frac{L}{\nu}\right)^{-1/5}U(y)^{9/5}dy.$$
Integrate over the profile. With $U(y)=U_\infty(y/\delta)^{1/7}$, $U(y)^{9/5}=U_\infty^{9/5}(y/\delta)^{9/35}$, and
$$\int_0^{\delta}\!\Big(\tfrac{y}{\delta}\Big)^{9/35}dy=\delta\int_0^1\xi^{9/35}d\xi=\frac{35}{44}\,\delta.$$
Hence the total (two-sided) drag is
$$F=0.074\left(\frac{35}{44}\right)\rho\,\delta L\,U_\infty^{2}\,Re_L^{-1/5},\qquad Re_L=\frac{U_\infty L}{\nu}.$$
Drag coefficient. Referencing the one-side planform area $A=L\delta$ and dynamic pressure $\tfrac12\rho U_\infty^2$ (with both sides included in $F$),
$$C_D=\frac{F}{\tfrac12\rho U_\infty^2\,L\delta}=2(0.074)\frac{35}{44}Re_L^{-1/5},$$
$$\boxed{C_D=0.118\,Re_L^{-1/5}.}$$
(b) Compare with a uniform stream. In a uniform stream $U_\infty$ the same plate (two sides) has $F_{\text{unif}}=0.074\,\rho\,\delta L\,U_\infty^2\,Re_L^{-1/5}$. The ratio is exactly the profile shape factor,
$$\boxed{\frac{F_{\text{shear}}}{F_{\text{unif}}}=\frac{35}{44}\approx0.795.}$$
The sheared boundary-layer flow produces about 20% less drag, because the slow near-wall fluid carries less momentum than a uniform $U_\infty$ would.