Abstract
The plane laminar boundary layer equations with a power-law velocity distribution U(x) = cx m at the outer edge admit in the region m < 0 two families of similar solutions [1]. In contrast with the known Falkner-Skan solution [2], the second family of velocity profiles is characterized by reverse flow near the wall. The integral properties of this family of profiles are used widely in approximate methods for calculating the plane boundary layer to describe
Full Text 
Sign-in/Register to access full text options
Sign-in/Register to access full text options 
Published version (
Free)
Free) 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a call
