Chapter 9: Problem 118
Commercial airliners normally cruise at relatively high altitudes \((30,000 \text { to } 35,000 \mathrm{ft}) .\) Discuss how flying at this high altitude (rather than \(10,000 \mathrm{ft}\), for example) can save fuel costs.
Chapter 9: Problem 118
Commercial airliners normally cruise at relatively high altitudes \((30,000 \text { to } 35,000 \mathrm{ft}) .\) Discuss how flying at this high altitude (rather than \(10,000 \mathrm{ft}\), for example) can save fuel costs.
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Get started for freeAn airplane flies at a speed of \(400 \mathrm{mph}\) at an altitude of \(10,000 \mathrm{ft}\). If the boundary layers on the wing surfaces behave as those on a flat plate, estimate the extent of laminar boundary layer flow along the wing. Assume a transitional Reynelds number of \(\mathrm{Re}_{\mathrm{xcr}}=5 \times 10^{5} .\) If the airplane maintains its 400 -nph speed but descends to sea- level elevation, will the portion of the wing covered by a laminar boundary layer increase or decrease compared with its value at \(10,000 \mathrm{ft}\) ? Explain.
A laminar boundary layer velocity profile is approximated by \(u / U=[2-(y / \delta)](y / \delta)\) for \(y \leq \delta,\) and \(u=U\) for \(y>\delta\) (a) Show that this parabolic profile satisfies the appropriate boundary conditions. (b) Use the momentum integral equation to determine the boundary layer thickness, \(\delta=\delta(x)\). Compare the result with the exact Blasius solution.
An airplane flies at \(150 \mathrm{km} / \mathrm{hr}\). (a) The airplane is towing a banner that is \(b=0.8 \mathrm{m}\) tall and \(\ell=25 \mathrm{m}\) long. If the drag coefficient based on area \(b \ell\) is \(C_{D}=0.06,\) estimate the power required to tow the banner. (b) For comparison, determine the power required if the airplane was instead able to tow a rigid flat plate of the same size. (c) Explain why one had a larger power requirement (and larger drag) than the other. (d) Finally, determine the power required if the airplane was towing a smooth spherical balloon with a diameter of \(2 \mathrm{m}\)
Approximately how fast can the wind blow past a 0.25 -in. diameter twig if viscous effects are to be of importance throughout the entire flow field (i.e., \(\operatorname{Re}<1\) )? Explain. Repeat for a 0.004 -in. diameter tair and a 6 -fi-diameter smokestack.
Compare the rise velocity of an \(\frac{1}{8}\) -in.-diameter air bubble in water to the fall velocity of an \(\frac{1}{8}\) -in.- -diameter water drop in air. Assume each to behave as a solid sphere.
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