Title: Things to grab for this session (in priority order)
1Things 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
2Core Ag Engineering Principles Session 1
- Bernoullis Equation
- Pump Applications
3Core Principles
- Conservation of mass
- Conservation of energy
4Assumption/Conditions
- Hydrodynamics (the fluid is moving)
- Incompressible fluid (liquids and gases at low
pressures) - Therefore changes in fluid density are not
considered
5Conservation 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
6For 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
7Example
- 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?
8Example
- D1 0.15 m D2 0.3 m
- V1 0.3 m/s V2 ?
- How do we find V2?
9Example
- D1 0.15 m D2 0.3 m
- V1 0.3 m/s V2 ?
- How do we find V2?
- We know A1V1 A2V2
10Answer
11What is the volumetric flow rate?
12Volumetric flow rate Q
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14What is the mass flow rate in the larger section
of pipe?
15Mass flow rate
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17Questions?
18Bernoullis 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.
19Bernoullis 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
20Bernoullis Theorem Special Conditions
- (situations where we can simplify the equation)
21Special 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
22Special 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
23Special Condition 3
- If no pump or fan is between the two points
chosen, W0
24Example
25- Find the total energy (ft) at B assume flow is
frictionless
A
B
125
C
75
25
26Preliminary 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?
27Preliminary 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?
28Example
- Total EnergyA Total EnergyB
Total EnergyB
hA
29Example
- Total EnergyA Total EnergyB
Total EnergyB
hA 125 Total EnergyB
30Example
- Find the velocity at point C.
31Example
- Find the velocity at point C.
0
32Try 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
33Answer
- 150 psig 62.4 lb/ft3 144 in2 / ft2 346 ft
- 1ft 346 ft 0 0 10 11 x
- X 326
34Bernoullis 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)
35Bernoullis 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
36Determining F for Piping Systems
37Step 1
- Determine Reynolds number
- Dynamic viscosity units
- Diameter of pipe
- Velocity
- Density of fluid
38Example
- 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
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42- What is viscosity? What is density?
43- Viscosity 2.13 x 10-3 Pa s
- ? 1030 kg/m3
44 45Reynolds numbers
- lt 2130 Laminar
- gt 4000 Turbulent
- Affects what?
46Reynolds 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
47Total F in piping sytem
- F Fpipe Fexpansion
- Fexpansion Ffittings
48Darcys 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
51Example
- Find f if the relative roughness is 0.046 mm,
pipe diameter is 5 cm, and the Reynolds number is
17312
52Solution
- 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
54Answer
55Energy Loss due to Fittings and Sudden
Contractions
56Energy Loss due to Sudden Enlargement
57Example
- 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.
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65- Ffittings
- Fexpansion
- Fcontraction
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68Ftotal 199.7 m
69Try 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.
70Pump Applications
71How is W determined for a pump?
- Compute all the terms in the Bernoulli equation
except W - Solve for W algebraically
72Why is W determined for a pump?
- W is used to compute the size of pump needed
73Power
- 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
74Remember
- Po the power delivered to the fluid (sometimes
referred to as hydraulic power) - Pin Po/pump efficiency
- (sometimes referred to as brake horsepower)
75To calculate Power(out)
76To calculate Power(out)
77Flow rate is variable
- Depends on back pressure
- Intersection of system characteristic curve and
the pump curve
78System 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
79Example system characteristic curve
80Pump 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
81Pump Performance Curve
Total head
Power
Efficiency
N 1760 rpm D 15 cm
82Pump Operating Point
- Pump operating point is found by the intersection
of pump performance curve and system
characteristic curve
83What 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)
86Pump 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
87Example
- 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
89Procedure
- 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
92What 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
93How do we convert Po to W?
94How 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
95Find 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
96Find 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
97Find N that corresponds to new Q and D (p. 109
equ)
98Find N that corresponds to new Q and D
- N2N1(Q2/Q1)(D1/D2)3
- N2 1770 rpm
99Try 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?
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101Answers
- 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.