Fluid mechanics and hydraulics miscellaneous
- A circular sewer 2m diameter has to carry a discharge of 2m³ /s when flowing nearly full. What is the minimum required slope to initiate the flow? Assume Manning’s N = 0.015.
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Manning’s equation
V = 1 m2/3C.1/2 n ⇒ Q = 1 m2/3C.1/2 A n m = R = A = (π/4)D² m2/3C.1/2 P πD = (1/4) × 2² 2 = 1 2
N = 0.015
G = 2 m³ /sA = π × 2² = π 4 ⇒ 2 = 1 − 1 2/3 (i)1/2 π 0.015 2
∴ i = 0.00023Correct Option: A
Manning’s equation
V = 1 m2/3C.1/2 n ⇒ Q = 1 m2/3C.1/2 A n m = R = A = (π/4)D² m2/3C.1/2 P πD = (1/4) × 2² 2 = 1 2
N = 0.015
G = 2 m³ /sA = π × 2² = π 4 ⇒ 2 = 1 − 1 2/3 (i)1/2 π 0.015 2
∴ i = 0.00023
- A trapezoidal channel with bottom width of 3m and side slope of 1V I.5H carries a discharge of 8.0m³ /sec with the flow depth of 1.5m. The Froude number of the flow is
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Fr = V √gD
A = [B + My]y
= (3 + 1.5 × 1.5) 1.5
= 7.87 m²
T = B + 2 my
= 3 + (2 × 1.5 × 1.5)
= 7.5 mD = A = 7.87 = 1.05 m T 7.5 V = Q = 8 = 1.016 m/s A 7.87 Fr = V √gD = 1.016 = 0.316 (none is correct) √9.8 × 1.05
If we take D ≈ y ,Fr = 1.016 = 0.0265 √9.81 × 1.5 Correct Option: C
Fr = V √gD
A = [B + My]y
= (3 + 1.5 × 1.5) 1.5
= 7.87 m²
T = B + 2 my
= 3 + (2 × 1.5 × 1.5)
= 7.5 mD = A = 7.87 = 1.05 m T 7.5 V = Q = 8 = 1.016 m/s A 7.87 Fr = V √gD = 1.016 = 0.316 (none is correct) √9.8 × 1.05
If we take D ≈ y ,Fr = 1.016 = 0.0265 √9.81 × 1.5
- The force ‘F’ required at equilibrium on the semi-cylindrical gate shown below is
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Taking horizontal & vertical components of hydrostatic forces
FH = ρ.g.h Aprojected= 1000 × 9.81 × H × (H × 1) 2 = 1000 × 9.81 × 2 × (2 × 1) 2
= 19.62 kN/m width.
Fv = weight of water displaced
= Mg
= ρvg = ρg. v= ρ.g π R² × 1 2a = 1000 × 9.81 × π(1)² × 1 2
= 15.41 kN/m widthLocation of centre of pressure, h' = 2 H 3 = 2 × 2 = 1.33 m 3
= 0.424 m
Moment about hinge,
⇒ –FH × (h' - h) + Fv × x + F × 2/2 = 0
= – 19.62 × (1.33 – 1) + 15.41 × 0.424 + F × 1 = 0
∴ F = 0 kNCorrect Option: B
Taking horizontal & vertical components of hydrostatic forces
FH = ρ.g.h Aprojected= 1000 × 9.81 × H × (H × 1) 2 = 1000 × 9.81 × 2 × (2 × 1) 2
= 19.62 kN/m width.
Fv = weight of water displaced
= Mg
= ρvg = ρg. v= ρ.g π R² × 1 2a = 1000 × 9.81 × π(1)² × 1 2
= 15.41 kN/m widthLocation of centre of pressure, h' = 2 H 3 = 2 × 2 = 1.33 m 3
= 0.424 m
Moment about hinge,
⇒ –FH × (h' - h) + Fv × x + F × 2/2 = 0
= – 19.62 × (1.33 – 1) + 15.41 × 0.424 + F × 1 = 0
∴ F = 0 kN
- The circular water pipes shown in the sketch are flowing full. The velocity of flow (in m/s) in the branch pipe ‘R’ is
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Qp = Qq + Qr
ApVp= AqVq + ArVrπ × 4² × 6 = π × 4² × 5 + π × 2² × V 4 4 4
∴ r = 4 m/s.Correct Option: B
Qp = Qq + Qr
ApVp= AqVq + ArVrπ × 4² × 6 = π × 4² × 5 + π × 2² × V 4 4 4
∴ r = 4 m/s.
- The top width and the depth of flow in a triangular channel were measured as 4 m and 1 m, respectively. The measured velocities on the centre line at the water surface, 0.2 m and 0.8 m below the surface are 0.7 m/s, 0.6 m/s and 0.4 m/s, respectively. Using two-point method of velocity measurement, the discharge (in m³ /s) in the channel is
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Vavg = V.2y + V.8y 2 = 0.6 + 0.4 = 0.5 m/s 2 A = 1 × T × y 2 A = 1 × 4 × 1 = 2 m² 2
Q = Av = 2 × 0.5 = 1 m³ /s.Correct Option: C
Vavg = V.2y + V.8y 2 = 0.6 + 0.4 = 0.5 m/s 2 A = 1 × T × y 2 A = 1 × 4 × 1 = 2 m² 2
Q = Av = 2 × 0.5 = 1 m³ /s.