Hydraulics 3
Hydraulics 3 - Fluid Flow in Pipes and Reservoirs
Pipes
- Closed conduits for fluid transport; flow can be full or partial.
- Fluids flow full in pipes, while open channels have partial flow.
- Steady Flow Types:
- Laminar Flow: Fluid particles move without intersecting paths.
- Reynold's Number (NR) indicates flow type. Laminar flow occurs when NR \le 2000.
- Turbulent Flow: Fluid particle paths intersect continuously.
- Turbulent flow occurs when N_R \ge 4000.
- Transitional Flow: Occurs when 2000 < N_R < 4000.
- Laminar Flow: Fluid particles move without intersecting paths.
Reynold's Number
- Dimensionless parameter: Ratio of inertia force to viscous force.
- Formula: N_R = \frac{\rho vD}{\mu} = \frac{vD}{\nu}
- Where:
- v = mean velocity
- D = diameter
- \mu = dynamic viscosity
- \rho = density
- \nu = kinematic viscosity
- g = gravitational acceleration
- Where:
- Non-circular Pipes:
- D = 4R, where R is the hydraulic radius.
- Hydraulic Radius, R = \frac{Area, A}{Wetted Perimeter, P}.
Velocity Distribution in Pipes
Laminar Flow
- Velocity distribution follows a parabolic law; zero velocity at the walls.
- Centerline velocity: Vc = 2V{ave}, where V_{ave} is the mean velocity.
- Velocity (u) at distance "r" from the center (pipe radius ro): u = vc(1-\frac{r^2}{r_o^2}).
Turbulent Flow
- Velocity distribution varies with Reynold's Number; zero velocity at the walls, increasing rapidly.
- Centerline velocity: v_c = v(1 + 1.33\sqrt{f})
- Mean velocity related to centerline velocity: v = vc - 3.75\sqrt{\frac{To}{\rho}}
- Where:
- v_c = centerline velocity
- f = friction factor
- T_o = maximum shearing stress in the pipe
- v = mean velocity
- Where:
Shear Stress at Pipe Walls
- Shear Stress: T = \frac{fpv^2}{8}
Head Losses in Pipe Flow
Major Head Losses
- Darcy-Weisbach Formula:
- h_L = f \frac{Lv^2}{2gD}
- For circular pipes: h_L = \frac{0.0826fLQ^2}{D^5}.
- Manning's Formula:
- h_L = \frac{10.29n^2LQ^2}{D^{16/3}}, where n is the roughness coefficient.
- Hazen-Williams Formula:
- h_L = \frac{10.67LQ^{1.85}}{C^{1.85}D^{4.87}}, where C is the Hazen-Williams constant.
Values of Friction Factor, f
- Laminar Flow: f = \frac{64}{N_R}
- Turbulent Flow:
- Smooth Pipe (3000 \le NR \le 10000): f = \frac{0.316}{NR^{0.25}}
- All Pipes: \frac{1}{\sqrt{f}} = -2 \log(\frac{E}{3.7D} + \frac{2.51}{N_R\sqrt{f}})
- (Colebrook and White Formula)
Pipes Connected in Series
- Flow is equal in all pipes: Q = Q1 = Q2 = Q3 = … = Qn
- Total head loss is the sum of individual head losses: HL = h{L1} + h{L2} + h{L3} + … + h_{Ln}
Pipes Connected in Parallel
- Head loss in individual pipes is equal: HL = h{L1} = h{L2} = h{L3} = … = h_{Ln}
- Total discharge is the sum of individual discharges: QT = Q1 + Q2 + Q3 + … + Q_n
Equivalent Pipe
- Must have the same discharge and head loss as the original pipe system.
- Discharge, total head loss, and total length from source to supply point are conserved.
Sample Problems
Situation 1
A 60-mm diameter pipe contains glycerin (\rho = 1250 kg/m^3) flowing at 2.36 L/sec. Viscosity of glycerin is 0.0556 Pa-s. Assume steady laminar flow:
- Reynold's Number:
- N_R = 2002.57
- Direction of Flow:
- A to B
- Head Loss:
- 18.56 m
- Equivalent Friction Factor (L = 1.2 km):
- 0.0378
Situation 2
A cast iron pipe carries a flow of 6.20 cfs, length is 30 ft, and diameter is 6 inches.
- Friction Factor = 0.014:
- Head Loss = 11.70 ft
- Roughness Coefficient = 0.015:
- Head Loss = 48.76 ft
- Hazen-Williams Constant = 110:
- Head Loss = 33.37 ft
Situation 3
Pipes 1, 2, and 4 are in series; pipes 2 and 3 are parallel.
- Pipeline 2 Discharge = 40 liters/sec
| Pipelines | Length (m) | Diameter (mm) | Friction Factor |
|---|---|---|---|
| 1 | 2,800 | 200 | 0.02 |
| 2 | 4,000 | 300 | 0.02 |
| 3 | 2,000 | 200 | 0.02 |
| 4 | 2,600 | 400 | 0.02 |
- Discharge in Pipeline 3:
- 26.4 liters/sec
- Discharge in Pipeline 4:
- 66.4 liters/sec
Situation 4
Two pipes are connected in parallel between two reservoirs.
| Pipelines | Length (m) | Diameter (mm) | C |
|---|---|---|---|
| A | 2,600 | 1,300 | 90 |
| B | 2,400 | 900 | 100 |
- Rate of Flow at Pipe A:
- 0.14652 m^3/s
- Rate of Flow at Pipe B:
- 0.49918 m^3/s
- Equivalent length of 1000mm Diameter Pipe (C=120):
- 627,826 m
Flow in Three Reservoirs
Three Reservoir Problems
Step 1: Identify the Case (One Supplier or Two Suppliers)
- Compare discharges of the highest and lowest reservoirs.
- Place the top of the piezometer at the same elevation as the middle reservoir (hB = 0).
- Get the difference in elevations between the highest and middle reservoir (hA) and between the middle and lowest reservoir (hC).
Step 2: Solve for Head Losses
- Use major head loss equations (Darcy, Manning, Hazen-Williams).
- Express head losses in terms of QA, QB, and Q_C.
Step 3: Solve for QA and QC and Compare
- If QA > QC, CASE I: Reservoir A supplies both B and C.
- If QA < QC, CASE II: Reservoirs A and B supply C.
Case I: Reservoir A Supplies both B and C
- ElevA - ElevB = h{fA} + h{fB}
- ElevA - ElevC = h{fA} + h{fC}
- QA = QB + QC
Calculator Technique: x = \frac{AElev{AB}}{A'} + \frac{AElev_{AC}}{C'}
- Where: A' and C' are pipe properties, x – head loss of reservoir A
Case II: Reservoirs A and B Supply C
- ElevA - ElevC = h{fA} + h{fC}
- ElevB - ElevC = h{fB} + h{fC}
- QA + QB = QC
Calculator Technique: x = \frac{AElev{AC}}{A'} + \frac{AElev_{BC}}{B'}
- Where: A' and B' are pipe properties, x = head loss of reservoir C
Sample Problem: Three Reservoirs
Problem: Determine the flow in each pipe connecting the three reservoirs.
Given:
- Pipe 1:
- Length = 2000 m
- Diameter = 500 mm
- f = 0.02
- Pipe 2:
- Length = 2500 m
- Diameter = 600 mm
- f = 0.02
- Pipe 3:
- Length = 4500 m
- Diameter = 800 mm
- f = 0.02
- Reservoir Elevations:
- A = 110 m
- B = 70 m
- C = 20 m
Solution:
- Headloss Formula: h = \frac{0.0826fLQ^2}{D^5}
Headloss Calculations:
*hA = 105.728 QA^2
*hB = 53.11 QB^2
*hC = 22.69 QC^2
*Case:* QA + QB = QC Discharge:
*QA = 0.4515 m^3/s
*QB = 1.2853 m^3/s *QC = 1.7368 m^3/s
Practice Problems
Problems 1 - 3
Three reservoirs A, B, and C with elevations 346 m, 301 m, and 241 m, respectively. Flow rate at 1 is 200 L/sec.
| PIPE | LENGTH (M) | DIAMETER (MM) | HAZENS, C |
|---|---|---|---|
| 1 | 600 | 450 | 120 |
| 2 | 3600 | 300 | 100 |
| 3 | 1200 | D3 | 110 |
- Head Loss of Pipeline 2:
- 42.73 m
- Discharge of Pipeline 3:
- 94 L/sec
- Diameter of Pipeline 3:
- 180 mm
Problems 4 - 6
Pressure heads at points A and E are 70 m and 46 m, respectively. Assume C = 120 for all pipes.
- Flow Rate of Water Through B:
- 0.103 m^3/s
- Flow Rate of Water Through C:
- 0.039 m^3/s
- Flow Rate of Water Through D:
- 0.07 m^3/s
Problems 7 - 9
A 6-km cast-iron (new) pipeline conveys 320 L/sec of water at 30°C. The pipe diameter is 30 cm.
- Head Loss (m) - Darcy-Weisbach (f = 0.0195):
- 408
- Head Loss (m) - Hazen-Williams (C = 130):
- 314
- Head Loss (m) - Manning Equation (n = 0.011):
- 496
Problem 10
A buried, horizontal concrete pipe (n = 0.012) of unknown length needs replacement. Pressure head drop is 29.9 ft, flow rate is 30.0 cfs.
- Length (ft) of New Pipe Needed:
- 2000