Fluid Mechanics and Hydraulic Machinery Miscellaneous
- Consider a laminar flow at zero incidence over a flat plate, The shear stress at the wall is denoted by τW, The axial position x1 and x2 on the plate are measured from the leading edge in the direction of flow. If x2 > x1, then
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From Blausius equation,
Cfx = 0.664 √Rex & Cfx = τw 1/2δU²∞ 0.664 = τw √Rex 1/2δU²∞ τw ∝ 1 √x
& we know x2 > x1
τw/w1 = τw/w2Correct Option: C
From Blausius equation,
Cfx = 0.664 √Rex & Cfx = τw 1/2δU²∞ 0.664 = τw √Rex 1/2δU²∞ τw ∝ 1 √x
& we know x2 > x1
τw/w1 = τw/w2
- The arrangement shown in the figure measures the velocity V of a gas of density 1 kg/m³ flowing through a pipe. The acceleration due to gravity is 9.81 m/s². If the manometric fluid is water (density 1000 kg/m³) and the velocity V is 20 m/ s, the differential head h(in mm) between the two arms of the manometer is _________.
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Dynamic pressure of gas = (δgh)water
1 δgasv2 = δm × 9.81 × h 2 1 × 1 × (20)² = 1000 × 9.81 × h 2
h = 0.02038 m of water
h = 20.38 mm of waterCorrect Option: D
Dynamic pressure of gas = (δgh)water
1 δgasv2 = δm × 9.81 × h 2 1 × 1 × (20)² = 1000 × 9.81 × h 2
h = 0.02038 m of water
h = 20.38 mm of water
- A Prandtl tube (Pitot-static tube with C = 1) is used to measure the velocity of water. The differential manometer reading is 10 mm of liquid coiumn with a relative density of 10. Assuming g = 9.8 m/s², the velocity of water (in m/s) is _____ .
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Velocity as water = Cv √2gh
Cv = 1 (Given)h = x sg - 1 s0
= 0.01 (10 – 1) = 0.09 m
∴ velocity of flow = √2 × 9.8 × 0.09 = 1.328 m/ sCorrect Option: C
Velocity as water = Cv √2gh
Cv = 1 (Given)h = x sg - 1 s0
= 0.01 (10 – 1) = 0.09 m
∴ velocity of flow = √2 × 9.8 × 0.09 = 1.328 m/ s
- A streamline and an equipotential line in a flow field
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dy × dy = - 1 dx φ dx ψ
Slope of equipotential Line × slope of stream function = – 1
They are orthogonal to each other.Correct Option: B
dy × dy = - 1 dx φ dx ψ
Slope of equipotential Line × slope of stream function = – 1
They are orthogonal to each other.
- Velocity vector of a flow field is given as = 2xyî - x²zĵ. The vorticity vector at (1, 1, 1) is
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v = 2xyi – x 2zj
Velocity of a vector = ∇ × v= î 0 - δ ( - x²z) - î 0 - δ (2xy) - k̂ 0 - δ (-x²z) - δ (2xy) δz δz δx δy
= î(-x²) + k̂(-2 × z - 2X)
At(1 , 1 , 1),
∇ × v = î + k̂ (-2 -2) = i - 4kCorrect Option: D
v = 2xyi – x 2zj
Velocity of a vector = ∇ × v= î 0 - δ ( - x²z) - î 0 - δ (2xy) - k̂ 0 - δ (-x²z) - δ (2xy) δz δz δx δy
= î(-x²) + k̂(-2 × z - 2X)
At(1 , 1 , 1),
∇ × v = î + k̂ (-2 -2) = i - 4k