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Title: Things to grab for this session (in priority order)


1
Things to grab for this session (in priority
order)
  • Pencil
  • Henderson, Perry, and Young text
  • (Principles of Process Engineering)
  • Calculator
  • Eraser ?
  • Scratch paper
  • Units conversion chart
  • Tables of fluid properties
  • Moody diagram
  • Pump affinity laws

2
Core Ag Engineering Principles Session 1
  • Bernoullis Equation
  • Pump Applications

3
Core Principles
  • Conservation of mass
  • Conservation of energy

4
Assumption/Conditions
  • Hydrodynamics (the fluid is moving)
  • Incompressible fluid (liquids and gases at low
    pressures)
  • Therefore changes in fluid density are not
    considered

5
Conservation of Mass
  • If the rate of flow is constant at any point and
    there is no accumulation or depletion of fluid
    within the system, the principle of conservation
    of mass (where mass flow rate is in kg/s)
    requires

6
For incompressible fluids density remains
constant and the equation becomes
  • Q is volumetric flow rate in m3/s
  • A is cross-sectional area of pipe (m2) and
  • V is the velocity of the fluid in m/s

7
Example
  • Water is flowing in a 15 cm ID pipe at a velocity
    of 0.3 m/s. The pipe enlarges to an inside
    diameter of 30 cm. What is the velocity in the
    larger section, the volumetric flow rate, and the
    mass flow rate?

8
Example
  • D1 0.15 m D2 0.3 m
  • V1 0.3 m/s V2 ?
  • How do we find V2?

9
Example
  • D1 0.15 m D2 0.3 m
  • V1 0.3 m/s V2 ?
  • How do we find V2?
  • We know A1V1 A2V2

10
Answer
  • V2 0.075 m/s

11
What is the volumetric flow rate?
12
Volumetric flow rate Q
13
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14
What is the mass flow rate in the larger section
of pipe?
15
Mass flow rate
16
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17
Questions?
18
Bernoullis Theorem (conservation of energy)
  • Since energy is neither created nor destroyed
    within the fluid system, the total energy of the
    fluid at one point in the system must equal the
    total energy at any other point plus any
    transfers of energy into or out of the system.

19
Bernoullis Theorem
W work done to the fluid h elevation of
point 1 (m or ft) P1 pressure (Pa or psi)
specific weight of fluid v velocity of fluid F
friction loss in the system
20
Bernoullis Theorem Special Conditions
  • (situations where we can simplify the equation)

21
Special Condition 1
  • When system is open to the atmosphere, then P0
    if reference pressure is atmospheric (gauge
    pressure)
  • Either one P or both Ps can be zero depending on
    system configuration

22
Special Condition 2
  • When one V refers to a storage tank and the other
    V refers to a pipe, then V of tank ltltltlt V pipe
    and assumed zero

23
Special Condition 3
  • If no pump or fan is between the two points
    chosen, W0

24
Example
25
  • Find the total energy (ft) at B assume flow is
    frictionless

A
B
125
C
75
25
26
Preliminary Thinking
  • Why is total energy in units of ft? Is that a
    correct measurement of energy?
  • What are the typical units of energy?
  • How do we start the problem?

27
Preliminary Thinking
  • Feet is a measure of pressure it can be
    converted to more traditional pressure units.
  • Typical units of energy energy work Nm or
    ft-lb. If we multiply feet or meter by the
    specific weight of the fluid, we obtain units of
    pressure.
  • How do we start the problem?

28
Example
  • Total EnergyA Total EnergyB

Total EnergyB
hA
29
Example
  • Total EnergyA Total EnergyB

Total EnergyB
hA 125 Total EnergyB
30
Example
  • Find the velocity at point C.

31
Example
  • Find the velocity at point C.

0
32
Try it yourself
Water is pumped at the rate of 3 cfs through
piping system shown. If the energy of the water
leaving the pump is equivalent to the discharge
pressure of 150 psig, to what elevation can the
tank be raised? Assume the head loss due to
friction is 10 feet.
9
1
x
pump
1
33
Answer
  • 150 psig 62.4 lb/ft3 144 in2 / ft2 346 ft
  • 1ft 346 ft 0 0 10 11 x
  • X 326

34
Bernoullis Equation
  • Adding on how do we calculate F (instead of
    having it given to us or assuming it is
    negligible like in the previous problems)

35
Bernoullis Theorem
h elevation of point 1 (m or ft) P1
pressure (Pa or psi) specific weight of
fluid v velocity of fluid F friction loss in
the system
36
Determining F for Piping Systems
37
Step 1
  • Determine Reynolds number
  • Dynamic viscosity units
  • Diameter of pipe
  • Velocity
  • Density of fluid

38
Example
  • Milk at 20.2C is to be lifted 3.6 m through 10 m
    of sanitary pipe (2 cm ID pipe) that contains two
    Type A elbows. Milk in the lower reservoir
    enters the pipe through a type A entrance at the
    rate of 0.3 m3/min. Calculate Re.

39
  • Step 1 Calculate Re number

40
  • Calculate v ?
  • Calculate v2 / 2g, because well need this a lot

41
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42
  • What is viscosity? What is density?

43
  • Viscosity 2.13 x 10-3 Pa s
  • ? 1030 kg/m3

44
  • So Re 154,000

45
Reynolds numbers
  • lt 2130 Laminar
  • gt 4000 Turbulent
  • Affects what?

46
Reynolds numbers
  • To calculate the f in Darcys equation for
    friction loss in pipe need Re
  • Laminar f 64 / Re
  • Turbulent Colebrook equation or Moody diagram

47
Total F in piping sytem
  • F Fpipe Fexpansion
  • Fexpansion Ffittings

48
Darcys Formula
49
  • Where do you use relative roughness?

50
  • Relative roughness is a function of the pipe
    material for turbulent flow it is a value needed
    to use the Moody diagram (e/D) along with the
    Reynolds number

51
Example
  • Find f if the relative roughness is 0.046 mm,
    pipe diameter is 5 cm, and the Reynolds number is
    17312

52
Solution
  • e / D 0.000046 m / 0.05 m 0.00092
  • Re 1.7 x 104
  • Re gt 4000 turbulent flow use Moody diagram

53
  • Find e/D , move to left until hit dark black line
    slide up line until intersect with Re

54
Answer
  • f 0.0285

55
Energy Loss due to Fittings and Sudden
Contractions
56
Energy Loss due to Sudden Enlargement
57
Example
  • Milk at 20.2C is to be lifted 3.6 m through 10 m
    of sanitary pipe (2 cm ID pipe) that contains two
    Type A elbows. Milk in the lower reservoir
    enters the pipe through a type A entrance at the
    rate of 0.3 m3/min. Calculate F.

58
  • Step 1

59
  • Step 1
  • Re 154,000

60
  • f ?
  • Fpipe

61
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62
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63
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64
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65
  • Ffittings
  • Fexpansion
  • Fcontraction

66
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67
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68
Ftotal 199.7 m
69
Try it yourself
  • Find F for milk at 20.2 C flowing at 0.075 m3/min
    in sanitary tubing with a 4 cm ID through 20 m of
    pipe, with one type A elbow and one type A
    entrance. The milk flows from one reservoir into
    another.

70
Pump Applications
71
How is W determined for a pump?
  • Compute all the terms in the Bernoulli equation
    except W
  • Solve for W algebraically

72
Why is W determined for a pump?
  • W is used to compute the size of pump needed

73
Power
  • The power output of a pump is calculated by

W work from pump (ft or m) Q volumetric flow
rate (ft3/s or m3/s) ? density g gravity
74
Remember
  • Po the power delivered to the fluid (sometimes
    referred to as hydraulic power)
  • Pin Po/pump efficiency
  • (sometimes referred to as brake horsepower)

75
To calculate Power(out)
  • What we know
  • What we need

76
To calculate Power(out)
  • What we know
  • What we need
  • W
  • ?
  • g
  • Q

77
Flow rate is variable
  • Depends on back pressure
  • Intersection of system characteristic curve and
    the pump curve

78
System Characteristic Curves
  • A system characteristic curve is calculated by
    solving Bernoullis theorem for many different
    Qs and solving for Ws
  • This curve tells us the power needed to be
    supplied to move the fluid at that Q through that
    system

79
Example system characteristic curve
80
Pump Performance Curves
  • Given by the manufacturer plots total head
    against Q volumetric discharge rate
  • Note these curves are good for ONLY one speed,
    and one impeller diameter to change speeds or
    diameters we need to use pump laws

81
Pump Performance Curve
Total head
Power
Efficiency
N 1760 rpm D 15 cm
82
Pump Operating Point
  • Pump operating point is found by the intersection
    of pump performance curve and system
    characteristic curve

83
What volumetric flow rate will this pump
discharge on this system?
84
  • Performance of centrifugal pumps while pumping
    water is used as standard for comparing pumps

85
  • To compare pumps at any other speed than that at
    which tests were conducted or to compare
    performance curves for geometrically similar
    pumps (for ex. different impeller diameters or
    different speeds) use pump affinity laws (or
    pump laws)

86
Pump Affinity Laws (p. 106)
  • Q1/Q2(N1/N2)(D1/D2)3
  • W1/W2(N1/N2)2(D1/D2)2
  • Po1/Po2(N1/N2)3(D1/D2)5(?1/?2)
  • NOTE For changing ONLY one property at a time

87
Example
  • Size a pump that is geometrically similar to the
    pump given in the performance curve below, for
    the same system. Find D and N to achieve Q
    0.005 m3/s against a head of 19.8 m?

0.01 m3/s
88
(Watt)
N 1760 rpm D 17.8 cm
89
Procedure
  • Step 1 Find the operating point of the original
    pump on this system (so youll have to plot your
    system characteristic curve (calculated) onto
    your pump curve (given) or vice-versa.

90
P(W)
N 1760 rpm D 17.8 cm
91
P(W)
882.9 W
0.01 m3/s
N 1760 rpm D 17.8 cm
92
What is the operating point of first pump?
  • N1 1760
  • D1 17.8 cm
  • Q1 0.01 m3/s Q2 0.005 m3/s
  • W1 W2 19.8 m

93
How do we convert Po to W?
94
How do we convert Po to W?
  • W Po/Q?g
  • W(882.9 Nm/s)/(0.01 m3/s 1000 kg/m3 9.81
    m/s2)
  • W 9 m

95
Find D that gives both new W and new Q
  • (middle of p. 109 cant use p. 106 for two
    conditions changing)
  • D2D1(Q2/Q1)1/2(W1/W2)1/4
  • D2
  • D2

96
Find D that gives both new W and new Q
  • (middle of p. 109)
  • D2D1(Q2/Q1)1/2(W1/W2)1/4
  • D20.178m(.005 m3/s/0.01m3/s)1/2(9 m/19.8 m)1/4
  • D20.141 m

97
Find N that corresponds to new Q and D (p. 109
equ)
  • N2N1(Q2/Q1)(D1/D2)3
  • N2

98
Find N that corresponds to new Q and D
  • N2N1(Q2/Q1)(D1/D2)3
  • N2 1770 rpm

99
Try it yourself
  • If the system used in the previous example was
    changed by removing a length of pipe and an elbow
    what changes would that require you to make?
  • Would N1 change? D1? Q1? W1? P1?
  • Which direction (greater or smaller) would they
    move if they change?

100
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101
Answers
  • Removing pipe elbow would reduce F and
    therefore reduce W (increase Q). System curve
    would move to the right.
  • N would likely change. D- no. Q- yes. P depends
    on the shape of the power curve but likely it
    will change.
  • N would increase (N2N1(Q2/Q1)(D1/D2)3)
  • Q increase P depends.
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