THE LINEARIZED EQUATIONS OF MOTION \_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_ 3 MOBILITIES \_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_.\_\_\_\_\_.\_.\_\_\_\_\_.\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_\_ 5 A\_ Lowest order multipole; point force approximation \_\_\_\_\_\_\_\_.\
On the non-linear eqlations of the selfsimilar motion of a viscous fluid
β Scribed by V.I. Naidenov
- Publisher
- Elsevier Science
- Year
- 1988
- Weight
- 820 KB
- Volume
- 28
- Category
- Article
- ISSN
- 0041-5553
No coin nor oath required. For personal study only.
π SIMILAR VOLUMES
The non-linear equations of motion of pipes conveying fluid are derived in simple and accessible terms, by energy and Newtonian methods. Different derivations are made for cantilevered pipes, where the centreline is assumed inextensible, and for pipes with both ends fixed; it is shown that the deriv
## Abstract We study the __p__βsystem with viscosity given by __v__~__t__~ β __u__~__x__~ = 0, __u__~__t__~ + __p__(__v__)~__x__~ = (__k__(__v__)__u__~__x__~)~__x__~ + __f__(β« __v__d__x__, __t__), with the initial and the boundary conditions (v(x, 0), u(x,0)) = (__v__~0~, __u__~0~(__x__)), __u__(0,