Branching of the Falkner-Skan solutions for λ
✍ Scribed by B. Oskam; A. E. P. Veldman
- Publisher
- Springer
- Year
- 1982
- Tongue
- English
- Weight
- 499 KB
- Volume
- 16
- Category
- Article
- ISSN
- 0022-0833
No coin nor oath required. For personal study only.
✦ Synopsis
The Falkner-Skan equation f'" + ff" + h(1 _f,2) = 0,f(0) =if(0) = 0, is discussed for h < 0. Two types of problems, one with f'(**) = 1 and another with f'(**) = --1, are considered. For h = 0-a close relation between these two types is found. For h < --1 both types of problem allow multiple solutions which may be distinguished by an integer N denoting the number of zeros of f ' --1. The numerical results indicate that the solution branches with f'(*~) = 1 and those with f'(**) = --1 tend towards a common limit curve as N increases indefinitely. Finally a periodic solution, existing for ~. < --1, is presented.
📜 SIMILAR VOLUMES
The Falkner-Skan equation f '" + if" + h(1 -f,2) = 0 is discussed for X > 0. Two types of solutions have been pursued: those satisfying f(0) = f'(0) = 0, f'(oe) = 1 and those being periodic. In both cases, numerical evidence is given for a rich structure of multiple solutions. Branching occurs for X
s transformation a b s t r a c t In this work, an analysis is performed to find the series solution of the boundary layer Falkner-Skan equation for wedge. The boundary layer similarity equation takes into account a special form of the chosen magnetic field. The results are obtained by solving the n