KUNDU Fluid Mechanics 2E Episode 15 doc

... = y/sin0, (1 5.6) where Eq. (15. 4) has been used. We now eliminate 0 between Eqs. (15. 5) and (15. 6). First note from Eq. (15. 6) that cos2e = (2btan fi - y)/2btan p, ... obtain (1 5.4) x2 sinze - y2 cosze = 4b2 sin% cos2e. (15. 5) To understand the shape of the curve represented by Eq. (15. 5) we must express 0 in terms of x, y,...

Ngày tải lên: 13/08/2014, 16:21

Ngày tải lên: 13/08/2014, 16:21

... = 0.85 x 16. R. Mehta, Ann. Rev Fluid Mech. 17 151 -189.1985. Photograph reproduced with permission from theAnnua1 Review of Fluid Mechanics, Vol. 17 @ 1985 Annual Reviews ... momentum, and energy) governing fluid motion. These predictions normally occur under those conditions defined in terms of flow geometry, thc physical properties of a fluid, and the...

Ngày tải lên: 13/08/2014, 16:21

... 12.3508 12.5695 12.79 I6 13.0172 13.2463 13.4789 13. 715 I 13.9549 14.1 984 14.4456 14.6965 14.9513 15. 2099 15. 4724 15. 7388 16.0092 16.2837 16.5622 16.WY 17.1317 17.4228 ... 0.0706 0.0264 Plhl 0.2200 0. 2152 0.2104 0.2058 0.20 I3 0.1968 0.1925 0.1841 0.1800 0.1 760 0.1721 0.1683 0.1646 1.1609 0 .157 4 0 .153 9 0 .150 5 0.1472 0.1439 0.1408 0...

Ngày tải lên: 13/08/2014, 16:21

... half-body, 159 -160 relevance of, 148 -150 sources and sinks, 156 uniqueness of, 175-176 unsteady. 113-1 14 veltrily potential and Laplace equation, 1sn -152 at wall angle, 154 -156 Irmtational ... body moving through a fluid, and is perhaps the greatest single discovery in the history of fluid mechanics. He showed that frictional effects in a slightly viscous flui...

Ngày tải lên: 13/08/2014, 16:21

... Exercises Literam Cited Supplemental Reading Confonnal Mapping 148 150 152 154 156 157 157 159 160 163 166 170 171 173 175 176 181 184 185 187 188 .I 89 190 ... R(!udirig 23 IO. Skilie Equilihhm (fa (,~ompn?ssil)kc I. lluid .Mechanics Fluid mechanics deals with the flow of fluids. Its study is important to physicists, whosc main int...

Ngày tải lên: 14/03/2014, 16:20

... Exercises Literam Cited Supplemental Reading Confonnal Mapping 148 150 152 154 156 157 157 159 160 163 166 170 171 173 175 176 181 184 185 187 188 .I 89 190 ... Asmmechanics, Ncw York Dover Publications. (A clear and simplc discussion of potential and adiibalic temperature gradients is given.) In memory of Pijush Kundu Pijush Kanti Kundu...

Ngày tải lên: 27/06/2014, 18:20

... Exercises Literam Cited Supplemental Reading Confonnal Mapping 148 150 152 154 156 157 157 159 160 163 166 170 171 173 175 176 181 184 185 187 188 .I 89 190 ... Decp Fluids Waves in a Finitc Layer Overlying an Infinitely Deep Fluid Shallow Layer Overlying an Inhitcly Deep Fluid Equations of Motion for a Continuously Stratified Fluid ....

Ngày tải lên: 13/08/2014, 16:21

... called a streamtube (Figure 3.5). No fluid can cross the streamtube because the velocity vector is tangent to this surface. In experimcntal fluid mechanics, the concept of path line ... suspending aluminum or otherreflecting materials on the fluid surfacc, illuminated by a source of light. Suppose that the cntirc fluid is covered wilh such particles, and a brieftim...

Ngày tải lên: 13/08/2014, 16:21

... “memoryy’ effect gives the fluid an clastic property, in addition to its viscous property. Most non-Newtonian fluids are thercfore wiscoelasric. Only Newtonian fluids will be considered ... the rate of strain in a fluid medium is examincd in this section. In a fluid at rest there are only nod components of stress on a surface, and the shss docs not depend on the...

Ngày tải lên: 13/08/2014, 16:21