Homework 10 Solution Manual Problem 1 (6points) SI (kg /m*s) 1.79E-5 1.12E-3 1 Air Water 10W30 English (lb*s/ft^2) 3.74E-7 2.34E-5 0.02 Munson, Bruce, Donald Young, and Theodore Okiishi. Fundamentals of fluid mechanics. 4. Appendix B. John Wiley & Sons Inc, 2002. Print. Problem 2a (5 points) The sheer force is the only force in the tangential direction. π 1π ππ’ Ns ππ πΉπ‘ = ππ΄ = (π ) π΄ = (1.79E − 5 2 ) ( ) (1000 ) ( 1π2 ) = 0.0179 π ππ¦ m 1 ππ π Problem 2b (5 points) Stagnation pressure creates the normal force on the plate. The stagnation pressure can be calculated using be Bernoulli equation. 1 1 1.23ππ 1π 2 πΉπ = ππ΄ = ( ππ 2 ) π΄ = ( ( ) ( ) ) (1π2 ) = 0.615 π 2 2 π3 π Problem 3 (5 points) The ratio of normal to tangential force is presented bellow. 1 1 2 1 ππ (2 πΏ) πΉπ 2 ππ π΄ 2 πππΏ = = = = π π1 πΏ π πΉπ‘ π π 2 ππΏ π΄ Problem 4 (10 points) The force balance will yield the equation shown bellow. Note that positive forces were in negative x direction. (π2)ππ¦ππ§ − (π1)ππ¦ππ§ = (π2 )ππ₯ ππ§ − (π1 )ππ₯ ππ§ Next note the following: π2 = π π1 = π ππ’ | π¦ = π¦2 ππ¦ ππ’ | π¦ = π¦1 = π¦2 + ππ¦ ππ¦ π1 = π ( ππ’ π 2 π’ + ππ¦) ππ¦ ππ¦ 2 (P2-P1) =dP Substituting these equations into the force balance and canceling dz will yield ππ ππ¦ = −π π2 π’ ππ¦ ππ₯ ππ¦ 2 π2 π’ 1 ππ = − 2 ππ¦ π ππ₯ ππ’ −1 ππ = π¦ + πΆ1 ππ¦ π ππ₯ π’= −1 ππ 2 π¦ + πΆ1π¦ + πΆ2 2π ππ₯ C1 and C2 could be obtained from the boundary conditions: 1) No slip at lower wall ο¨ U(y=0) = 0 ο¨ C2 = 0 1 1 ππ 2) No Slip at top wall ο¨ U (y = l) = 0 ο¨ C1 = 2 π ππ₯ π Therefore: π’= −1 ππ 2 1 ππ π¦ + ππ¦ 2π ππ₯ 2π ππ₯ Maximum velocity occurs in the center at y = l/2 π −1 ππ 2 −1 1 −0.06ππ 1π 2 π’ (π¦ = ) = π = ( )( ) (1ππ)2 ( ) = 0.00067π/π 2 8π ππ₯ 8 1.12E − 3Pa ∗ s 1π 100ππ Problem 5 (10 points) Drag on a flat plat could be found from Eq 18.22 πΆπ = 1.328 √π π 1.328 = √(1.23 ∗ 1 ∗ 1 ) 1.79E − 5 = 0.005 1 π·πππ = πΆπ ππ 2 π΄ = 0.015π 2 Since the plate has 2 faces πππ‘ π·πππ = 2 ∗ ππππ‘π π·πππ = 0.03 π Boundary layer thickness could be calculated using Eq. 18.23 πΏ= 5π₯ √π π Boundary Layer Thickness 0.02 BL Thickness (m) 0.015 0.01 0.005 0 -0.005 0 0.2 0.4 0.6 -0.01 -0.015 -0.02 Length Downstream (m) 0.8 1 Problem 6 (5 points) Following steps in problem 5 yields: πΆπ = 0.0014 π·πππ = 3.5 π πππ‘ π·πππ = 7.03π Boundary Layer Thickness in Water 0.006 BL Thickness (m) 0.004 0.002 0 0 0.2 0.4 0.6 0.8 -0.002 -0.004 -0.006 Length Downstream (m) Boundary Layer thickness Decreases but the drag increase. 1 1.2