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PROBLEM 8.2
This is an order-of-magnitude, scalar analysis.
PROBLEM 8.5
This problem is restricted to Cartesian coordinates.
PROBLEM 8.6
This problem is restricted to Cartesian coordinates.
PROBLEM 8.7
This problem is restricted to Cartesian coordinates.
PROBLEM 8.8
This problem is restricted to flow over a flat plate, presumably turbulent flow.
PROBLEM 8.10
This analysis applies to turbulent flow over a flat plate.
PROBLEM 8.11
This problem applies to turbulent flow over a flat plate. The lower limit is 1, instead of zero, to
avoid a singularity when plotting in logarithmic coordinates.
PROBLEM 8.12
This problem is application of the momentum integral method to turbulent flow over a flat plate.
The analysis is essentially the same as the Prandtl-von Kármán solution presented in Section
8.4.3.
PROBLEM 8.13
This problem is application of the momentum integral method to turbulent flow over a flat plate.
The analysis is similar to the Prandtl-von Kármán solution presented in Section 8.4.3.
PROBLEM 8.14
This problem is application of the momentum-heat transfer analogy method to turbulent flow
over a flat plate.
PROBLEM 8.16
This problem is restricted to turbulent flow over a flat plate.
PROBLEM 8.17
This problem is pertains to mixed (laminar and turbulent) flow over a flat plate.
PROBLEM 8.18
This problem is an application of a momentum-heat transfer analogy to flow over a flat plate.
PROBLEM 8.19
This problem applies to mixed (laminar and turbulent) flow over a flat plate.