flow through pipes part1.ppt - civil engineering explore

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8/18/2012 1 Dr. Sanghamitra Kundu Assistant Professor Civil Engineering Department BITS Pilani Types of flow Darcy-Weisbachequation Hydraulic Grade Line and Energy Grade Line Flow through long pipes Pipes in series or compound pipe Equivalent pipe Pipes in parallel Branched pipes Transmission of power through pipes Flow through nozzle at the end of a pipe Water hammer in pipes Pipe networks Laminar: highly ordered fluid motion with smooth streamlines. Turbulent: highly disordered fluid motion characterized by velocity fluctuations and eddies. Transitional: a flow that contains both laminar and turbulent regions Reynolds number, is the key parameter in determining whether flow is laminar or turbulent. Given: L1, L2, L3 D1, D2, D3 f1, f2, f3 Assumptions Flow steady Minor losses small; hence neglected Reservoirs are large enough; so their water surface levels are constant Basic equations used to solve Continuity equation Bernoulli’s equation Darcy- Weisbach Equation

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Page 1: Flow through pipes PART1.ppt - Civil Engineering Explore

8/18/2012

1

Dr. Sanghamitra Kundu

Assistant Professor

Civil Engineering Department

BITS Pilani

� Types of flow

� Darcy-Weisbach equation

� Hydraulic Grade Line and Energy Grade Line

� Flow through long pipes

� Pipes in series or compound pipe

� Equivalent pipe

� Pipes in parallel

� Branched pipes

� Transmission of power through pipes

� Flow through nozzle at the end of a pipe

� Water hammer in pipes

� Pipe networks

Laminar: highly ordered fluid motion

with smooth streamlines.

Turbulent: highly disordered fluid motion characterized by velocity fluctuations and eddies.

Transitional: a flow that contains both

laminar and turbulent regions

Reynolds number, is the key parameter in determining whether flow is laminar or turbulent.

� Given:� L1, L2, L3

� D1, D2, D3

� f1, f2, f3

� Assumptions� Flow steady

� Minor losses small; hence neglected

� Reservoirs are large enough; so their water surface levels are constant

� Basic equations used to solve� Continuity equation

� Bernoulli’s equation

� Darcy- Weisbach Equation

Page 2: Flow through pipes PART1.ppt - Civil Engineering Explore

8/18/2012

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� Type 1� Given:

� D, f, L for all

� Q1, ZA, ZB

� To determine:� Q2, Q3, ZC

� Type 2� Given:

� D, f, L for all

� ZA, ZC, Q2

� To determine:� ZB, Q1, Q3

� Type 3� Given:

� D, f, L for all

� ZA, ZB, ZC

� To determine:� Q1, Q2, Q3

� Water flows from a reservoir A through a pipe of diameter D1 = 120 mm andlength L1 = 120 m to a junction at D, from which a pipe of diameter D2 = 75 mmand length L2 = 60 m leads to reservoir B in which the water level is 16m belowthat in reservoir A. A third pipe, of diameter D3 = 60 mm and length L3 = 40 m,leads from D to reservoir C, in which the water level is 24 m below that inreservoir A. Taking f = 0.01 for all the pipes and neglecting all losses other thanthose due to friction, determine the volume rates of flow in each pipe.

� L1 = 1500 m, D1 = 90 cm; L2 = 450 m; D2 = 60 cm; L3 = 1200 m; D3 = 45 cm; ZA =90 m; ZB = 75 m; Q1 = 1.42 m3/s; ZC = ?? [f = 0.02 for all pipes]

� A pipe having a length of 6000 m and dia. 70 cm connects tworeservoirs A and B, the difference between their water levels is 30m. Halfway along the pipe there is a branch through which watercan be supplied to a third reservoir C. Taking f = 0.024,determine the rate of flow of reservoir when (a) no water isdischarged to reservoir C; (b) the quantity of water discharged toreservoir C is 0.15 m3/s. Neglect minor losses.

� The water levels in the two reservoirs A and B are respectively 66m and 61.5 m above datum. A pipe joins each to a common pointD where the pressure is 103 KN/m2 gauge and height is 45 mabove datum. Another pipe connects D to another tank C. Whatwill be the height of water level in assuming the same value offriction factor for all pipes?� LAD = 2400 m; DAD = 0.30 m� LBD = 2700 m; DBD = 0.45 m� LCD = 3000 m; DCD = 0.60 m

� Software: Pipe flow expert (Demo) for 3-reservoir problem� http://www.youtube.com/watch?v=RFH0E1wC-qI

� Pipes carrying water under pressure from one point to another may be used to transmit hydraulic power.

� Used for functioning of several hydraulic machines

� P = f (Q, H)

� The power (or energy per sec) available at the outlet of the pipe is� P = wt. of water/sec × head available

� P = wQ(H-hf)

� Max. power transmitted when H = 3hf

� A nozzle is a gradually converging short tube which isfitted at the outlet end of a pipe for the purpose ofconverting the total energy of flowing water intovelocity energy

� E.g. fire extinguishers, impulse turbines

� Conditions for:� Maximum power available from a nozzle

� H = 3hf

� Dia. Of the Nozzle for transmitting maximum power

2A fL

a D=

Page 3: Flow through pipes PART1.ppt - Civil Engineering Explore

8/18/2012

3

� A turbine operating under a total fall of 36 m issupplied water through 90 m long, 0.2 m dia. pipe. Ifthe flow rate is such that 9.5 m of head is lost infriction in the pipe, what will be the power delivered tothe turbine? Take f = 0.022.

� An interconnected system of pipes is called a pipe network

� Water distribution systems for municipalities

� Multiple sources and multiple sinks connected with aninterconnected network of pipes.

� The main problem in a pipe flow network is to determinethe distribution of flow through the various pipes of thenetwork such that all conditions of flow are satisfied andall the circuits are then balanced

� Computer solutions!

� KYpipes

� WaterCAD

� CyberNET

� EPANET

� Pipe network divided into loops with nodes� The conditions to be satisfied in any network of pipes:

� At each node, continuity may be applied:

� Around any loop, the sum of head losses must be zero:

� The relationship between head loss and discharge must be maintained for each pipe � Darcy-Weisbach equation

� [n value ranges from 1.72 to 2.00]

∑=

=

n

iiq

1

0

∑=

=

m

ifih

1

0

n

fh rQ=

� Solution techniques� Hardy Cross loop-balancing (optimizes correction)

� Use a numeric solver (Solver in Excel) to find a change in flow that will give zero head loss around the loop

� Use Network Analysis software (EPANET)

� In this method:� A most suitable flow is assumed in such a way as to

satisfy continuity at each node� With the assumed values of Q, compute the head losses

for each pipe� Consider different loops and compute the net head loss

around each circuit� Head loss clockwise round a loop are positive andanticlockwise are negative

� If assumed distribution of flow is correct, then� If , then the assumed flows are corrected by

introducing a correction factor ∆Q, till the loop isbalanced.

∑ = 0fih

0fi

h ≠∑

Page 4: Flow through pipes PART1.ppt - Civil Engineering Explore

8/18/2012

4

� In the above eq., the denominator is a sum of absolute terms, so has no sign.

� If head losses in the CW direction are more than the CCW, ∆Q will be negative.� Subtracted from flow in CW direction� Added to flow in CCW direction

� If head losses in the CW direction are less than the CCW, ∆Q will be positive.� Subtracted from flow in CCW direction� Added to flow in CW direction

� For pipes common to two loops, corrections from both the loops are to be applied

� With the applied corrections to the flows in all pipes, a 2nd trial is made for all loops and the process repeated until the corrections become negligible

0

1

0

n

n

rQQ

rnQ −∆ = −

∑∑

� For the network shown below, the head loss is given byhf = rQ2. The values of r for each pipe, and thedischarge into or out of various nodes are shown in thesketch. The discharges are in an arbitrary unit. Obtainthe distribution of discharge in the network.

B C

A Dr = 7

r = 8

r = 4

r = 6r = 6

20 15

45 40

1st trial

LOOP ABC

Line r Q rQ2 2rQ

AB 6 15 -1350 180

CB 4 30 3600 240

CA 8 5 -200 80

∑ = 2050 500

Correction for loop ABC

∆Q = -4.1≈ - 4

LOOP ADC

Line r Q rQ2 2rQ

CD 6 5 -150 60

AD 7 10 700 140

CA 8 5 200 80

∑ = 750 280

Correction for loop ABC

∆Q = -2.67857≈ - 3

20

45 40

A D10

5

30

515

15

B C

20

45 40

A D7

9-3 = 6

26

819

15

B C

2nd trial

LOOP ABC

Line r Q rQ2 2rQ

AB 6 19 -2166 228

CB 4 26 2704 208

CA 8 6 -288 96

∑ = 250 532

Correction for loop ABC

∆Q = -0.46992≈ - 0.5

LOOP ADC

Line r Q rQ2 2rQ

CD 6 8 -384 96

AD 7 7 343 98

CA 8 6 288 96

∑ = 247 290

Correction for loop ABC

∆Q = -0.85172≈ - 0.9

20

45 40

A D7

9-3 = 6

26

819

15

B C

20

45 40

A D6.1

6.5-0.9 = 5.6

25.5

8.919.5

15

B C

3rd trial

LOOP ABC

Line r Q rQ2 2rQ

AB 6 19.5 -2281.5 234

CB 4 25.5 2601 204

CA 8 5.6 -250.88 89.6

∑ = 68.62 527.6

Correction for loop ABC

∆Q = -0.13006≈ - 0.13

LOOP ADC

Line r Q rQ2 2rQ

CD 6 8.9 -475.26 106.8

AD 7 6.1 260.47 85.4

CA 8 5.6 250.88 89.6

∑ = 36.09 281.8

Correction for loop ABC

∆Q = -0.12807≈ - 0.13

20

45 40

A D6.1

6.5-0.9 = 5.6

25.5

8.919.5

15

B C

20

45 40

A D5.97

5.73-0.13 = 5.6

25.37

9.0319.63

15

B C