HW10 Solution

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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‘š
1𝑠
𝑑𝑒
Ns
π‘šπ‘š
𝐹𝑑 = 𝜏𝐴 = (πœ‡ ) 𝐴 = (1.79E − 5 2 ) (
) (1000
) ( 1π‘š2 ) = 0.0179 𝑁
𝑑𝑦
m
1 π‘šπ‘š
π‘š
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 1.23π‘˜π‘” 1π‘š 2
𝐹𝑛 = 𝑃𝐴 = ( πœŒπ‘‰ 2 ) 𝐴 = ( (
) ( ) ) (1π‘š2 ) = 0.615 𝑁
2
2
π‘š3
𝑠
Problem 3 (5 points)
The ratio of normal to tangential force is presented bellow.
1
1 2
1
πœŒπ‘‰ (2 𝐿)
𝐹𝑛 2 πœŒπ‘‰ 𝐴 2 πœŒπ‘‰πΏ
=
=
=
= 𝑅𝑒1
𝐿
𝑉
𝐹𝑑
πœ‡
πœ‡
2
πœ‡πΏ 𝐴
Problem 4 (10 points)
The force balance will yield the equation shown bellow. Note that positive forces were in negative x
direction.
(𝑃2)𝑑𝑦𝑑𝑧 − (𝑃1)𝑑𝑦𝑑𝑧 = (𝜏2 )𝑑π‘₯ 𝑑𝑧 − (𝜏1 )𝑑π‘₯ 𝑑𝑧
Next note the following:
𝜏2 = πœ‡
𝜏1 = πœ‡
𝑑𝑒
| 𝑦 = 𝑦2
𝑑𝑦
𝑑𝑒
| 𝑦 = 𝑦1 = 𝑦2 + 𝑑𝑦
𝑑𝑦
𝜏1 = πœ‡ (
𝑑𝑒 𝑑 2 𝑒
+
𝑑𝑦)
𝑑𝑦 𝑑𝑦 2
(P2-P1) =dP
Substituting these equations into the force balance and canceling dz will yield
𝑑𝑃 𝑑𝑦 = −πœ‡
𝑑2 𝑒
𝑑𝑦 𝑑π‘₯
𝑑𝑦 2
𝑑2 𝑒
1 𝑑𝑃
= −
2
𝑑𝑦
πœ‡ 𝑑π‘₯
𝑑𝑒
−1 𝑑𝑃
=
𝑦 + 𝐢1
𝑑𝑦
πœ‡ 𝑑π‘₯
𝑒=
−1 𝑑𝑃 2
𝑦 + 𝐢1𝑦 + 𝐢2
2πœ‡ 𝑑π‘₯
C1 and C2 could be obtained from the boundary conditions:
1) No slip at lower wall  U(y=0) = 0  C2 = 0
1 1 𝑑𝑃
2) No Slip at top wall  U (y = l) = 0  C1 = 2 πœ‡ 𝑑π‘₯ 𝑙
Therefore:
𝑒=
−1 𝑑𝑃 2
1 𝑑𝑃
𝑦 +
𝑙𝑦
2πœ‡ 𝑑π‘₯
2πœ‡ 𝑑π‘₯
Maximum velocity occurs in the center at y = l/2
𝑙
−1 𝑑𝑃 2 −1
1
−0.06π‘ƒπ‘Ž
1π‘š 2
𝑒 (𝑦 = ) =
𝑙 =
(
)(
) (1π‘π‘š)2 (
) = 0.00067π‘š/𝑠
2
8πœ‡ 𝑑π‘₯
8 1.12E − 3Pa ∗ s
1π‘š
100π‘π‘š
Problem 5 (10 points)
Drag on a flat plat could be found from Eq 18.22
𝐢𝑓 =
1.328
√𝑅𝑒
1.328
=
√(1.23 ∗ 1 ∗
1
)
1.79E − 5
= 0.005
1
π·π‘Ÿπ‘Žπ‘” = 𝐢𝑓 πœŒπ‘‰ 2 𝐴 = 0.015𝑁
2
Since the plate has 2 faces
𝑁𝑒𝑑 π·π‘Ÿπ‘Žπ‘” = 2 ∗ π‘ƒπ‘™π‘Žπ‘‘π‘’ π·π‘Ÿπ‘Žπ‘” = 0.03 𝑁
Boundary layer thickness could be calculated using Eq. 18.23
𝛿=
5π‘₯
√𝑅𝑒
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:
𝐢𝑓 = 0.0014
π·π‘Ÿπ‘Žπ‘” = 3.5 𝑁
𝑁𝑒𝑑 π·π‘Ÿπ‘Žπ‘” = 7.03𝑁
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
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