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Chapter 21 
Performance Curves for
Performance Curves for 
Individual Unit Operations
(Fluid Flow Equipment)
Department of Chemical Engineering
West Virginia University
Copyright J. A. Shaeiwitz and R. Turton - 2012 1
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton - 2012 2
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton
- 2012
3
Key Relationships
Key Relationships
2
• Turbulent flow
2
2
4
2
∝
Δ
⇒
=
Δ
m
m
v
P
D
fLv
P fr
fr
ρ
&
&
2
2
32
4
=
=
m
fL
D
m
A
m
v
ρπ
ρ
&
&
&
5
5
2
32 −
∝
Δ
⇒
=
Δ D
P
D
m
fL
P fr
fr
ρπ
&
Copyright J. A. Shaeiwitz and R. Turton - 2012 4
Key Relationships
Key Relationships
• Laminar flow
L
L
L
D
P
v
D
v
Δ
=
=
128
32
128
4
4
2
μ
π
π
&
&
v
D
P
D
L
v
D
L
v
P fr
fr ∝
∝
Δ
⇒
=
=
Δ −
and
128
32 4
4
2
π
μ
μ &
Copyright J. A. Shaeiwitz and R. Turton - 2012 5
Example 1
Example 1
• Increase velocity by 25% ‐ turbulent flow ‐
effect on ΔP
ld
1
2
25
.
1
old
1
new
2
2
=
=
=
v
v
2 2
2
1
∝
Δ
⇒
=
Δ v
P
D
fLv
P
v
fr
fr
ρ
5625
.
1
25
.
1 2
2
2
2
1
2
=
=
=
Δ
Δ
v
v
P
P
D
f
f
1
1
Δ v
P
Copyright J. A. Shaeiwitz and R. Turton - 2012 6
Example 2
Example 2
• Double diameter – turbulent flow‐ effect on 
ΔP
2
old
1
new
2
2
=
=
=
D
D
32 5
5
2
2
1
∝
Δ
⇒
=
Δ −
D
P
D
m
fL
P
D
fr
fr
ρπ
&
32
1
03125
.
0
5
.
0 5
5
5
1
1
2
=
=
=
=
Δ
Δ
D
D
P
P
D
ρπ
32
2
1
Δ D
P
Copyright J. A. Shaeiwitz and R. Turton - 2012 7
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton - 2012 8
NPSH
NPSH
NPSH N P i i S i H d
• NPSH = Net Positive Suction Head
• There is pressure drop upon entering pump, 
p p p g p p,
before mechanism that increases pressure
• If fluid is too close to vapor pressure at pump
• If fluid is too close to vapor pressure at pump 
inlet, it could flash upon entering pump
• Pumps are designed to handle liquids and do not 
behave well with vapor
Copyright J. A. Shaeiwitz and R. Turton - 2012 9
NPSH
NPSH
• NPSHA = Pinlet – P *
NPSHR
• NPSHA = NPSH “available”
NPSHR
• NPSHR = NPSH “required”
i f i li d b f
v
&
– information supplied by pump manufacturer
Copyright J. A. Shaeiwitz and R. Turton - 2012 10
NPSH
NPSH
• Common situation
• Apply MEB
1
2
0
2
2
W
e
z
g
v
P
s
f −
→
Δ
=
−
+
Δ
+
Δ
+
Δ
ρ
2
0
2
2
2
1
2
fL
D
fLv
gh
P
P
=
+
−
−
ρ
ρ
*
2
*
2
2
2
1
2
P
fLv
gh
P
P
P
NPSH
D
fLv
gh
P
P
+
=
=
−
+
=
ρ
ρ
ρ
ρ
Copyright J. A. Shaeiwitz and R. Turton - 2012 11
*
* 1
2 P
D
gh
P
P
P
NPSH A −
−
+
=
−
= ρ
NPSH
NPSH
5
2
2
1 *
32
P
D
v
fL
gh
P
NPSH A
π
ρ
ρ −
−
+
=
&
2
form
of
v
b
a
NPSH A −
= & NPSH
1
32
*
fL
b
P
gh
P
a
v
b
a
NPSH A
ρ
ρ −
+
=
NPSHA
5
2
32
D
fL
b
π
ρ
=
v
&
this is for turbulent flow
f l i fl t i ht li
Copyright J. A. Shaeiwitz and R. Turton - 2012 12
for laminar flow – straight line
with negative slope
NPSH
NPSH
2
1
2
32
*
fL
P
gh
P
a
v
b
a
NPSH A
ρ −
+
=
−
= &
• How to increase NPSHA
• base case is line (1)
increase a line (2)
5
2
32
D
fL
b
π
ρ
=
– increase a – line (2)
• increase h
• increase P1
• decrease P*
– decrease T
– decrease b – line (3) NPSHA
• decrease L
• increase D
– suction line usually larger D
1
3
2
Copyright J. A. Shaeiwitz and R. Turton - 2012 13
v
&
NPSH
NPSH
NPSHA > NPSHR
pump operates appropriately
R
NPSHA < NPSHR
pump will cavitate
inappropriate pump operation
but it will operate
NPSH
but it will operate
v
&
A
v
&
Copyright J. A. Shaeiwitz and R. Turton - 2012 14
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton - 2012 15
Pump and System Curves
Pump and System Curves
• Pump curve (centrifugal pump shown)
• Pump curve (centrifugal pump shown)
• Supplied by manufacturer
• Can be measured in lab
• centrifugal is sometimes called “constant head” pump
ΔP in pressure units
or head developed
or head developed
Copyright J. A. Shaeiwitz and R. Turton - 2012 16
v
&
Pump and System Curves
Pump and System Curves
• System curve
pump supplies pressure increase
)
(
)
( 3
2
3
1
2
1 Δ
−
+
Δ
−
+
Δ
=
Δ −
−
− P
P
P
P fr
to increase fluid pressure and to overcome all of these pressure losses
0)
(
h
)
0
or
0
be
could
(
)
0
usually
(
n
destinatio
to
source
in
-
out
3
1
Δ
<
>
Δ
+
>
Δ
=
Δ
=
Δ
−
P
z
g
P
P ρ
0)
(
valve
across
drop
pressure
frictional
0)
(
pipes
in
drop
pressure
frictional
0)
(
pump
across
change
pressure
3
2
2
1
<
=
Δ
<
=
Δ
>
=
Δ −
P
P
P
fr
0)
(
valve
across
drop
pressure
frictional
3
2 <
=
Δ −
P
Copyright J. A. Shaeiwitz and R. Turton - 2012 17
Pump and System Curves
Pump and System Curves
• To plot system curve – look at source to 
destination and frictional loss
3
1
3
1
)
0
or
0
be
could
(
)
0
usually
(
n
destinatio
to
source
in
-
out
)
(
z
g
P
P
P
P
P fr
sys
<
>
Δ
+
>
Δ
=
Δ
=
Δ
Δ
−
+
Δ
=
Δ −
ρ
5
2
2
3
1
2
3
1
3
1
so
32
2
)
o
be
cou d
(
)
usu y
(
des o
o
sou ce
D
v
fL
P
D
fLv
P
P
g
sys
&
+
Δ
=
+
Δ
=
Δ −
−
−
π
ρ
ρ
ρ
ΔPsys
( )
2
form
empirical
so
v
b
a
P
P
P
P
sys
valve
sys
pump
&
+
=
Δ
Δ
−
+
Δ
=
Δ
v
&
ΔPsys
Copyright J. A. Shaeiwitz and R. Turton - 2012 18
v
&
this is for turbulent flow
for laminar flow – straight line
Pump and System Curves
Pump and System Curves
• Often expressed as head
sys
v
fL
h
fLv
h
h +
=
+
= −
−
32
2
5
2
2
3
1
2
3
1
&
sys
D
g
gD
−
−
so
5
2
3
1
3
1
π
valve
sys
pump h
h
h +
= hsys
Copyright J. A. Shaeiwitz and R. Turton - 2012 19
v
&
Pump and System Curves
Pump and System Curves
ΔP
ΔPpump < ΔPsys
impossible operation
sys
ΔP
a = ΔPsource dest + ρgΔz if know this point
2
{
-ΔPvalve
ΔPpump
z
a ΔPsource-dest + ρgΔz
with
can find a and b
2
v
b
a
Psys &
+
=
Δ
operating
v
& v
&
pump
a
}-ΔPfr
z
ΔPpump > ΔPsys
excess pressure dissipated across partially closed valve
as open and close valve, flowrate changes
operating v
&
Copyright J. A. Shaeiwitz and R. Turton - 2012 20
as open and close valve, flowrate changes
intersection point is fully open valve
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton - 2012 21
Pumps in Series and Parallel
Pumps in Series and Parallel
• Series
– Pump curve
two pumps
Pump curve
– 2X head at 
same flowrate
ΔPpump
one pump
v
&
Copyright J. A. Shaeiwitz and R. Turton - 2012 22
Pumps in Series and Parallel
Pumps in Series and Parallel
• Parallel
P
two pumps
– Pump curve
– 2X flowrate at 
same head
ΔPpump
one pump
same head
v
&
Copyright J. A. Shaeiwitz and R. Turton - 2012 23
Pumps in Series and Parallel
Pumps in Series and Parallel
• Which 
configuration
two pumps
series
configuration 
maximizes 
flowrate?
ΔPpump z
flowrate?
– No general 
result
one pump
two pumps
parallel
z
result
Copyright J. A. Shaeiwitz and R. Turton - 2012 24
v
&
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton - 2012 25
Centrifugal – variable speed
Centrifugal  variable speed
ΔP
ΔPpump
rpm 5
rpm 3
rpm 2
rpm 4
v
&
rpm 1
rpm increases with number
more expensive pump
Copyright J. A. Shaeiwitz and R. Turton - 2012 26
p p p
cost of “wasting” pressure across valve may be less than cost of pump
Positive Displacement
fl l /
flow regulation/pump curve
ΔP in pressure units
sometimes called “constant volume” pump
p
or head developed
v
&
Copyright J. A. Shaeiwitz and R. Turton - 2012 27
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton - 2012 28
Compressors
Compressors
locus of maxima = surge line
can also draw system
Pout /Pin
rpm 5
can also draw system
curves on this graph –
must change form of left-
hand side to ratio
rpm 3
rpm 2
rpm 4
v
&
rpm 1
rpm 2
usually worth using speed control here because of compression costs
Copyright J. A. Shaeiwitz and R. Turton - 2012 29
usually worth using speed control here because of compression costs
Outline
Outline
• Flow in pipes
Flow in pipes
– laminar vs. turbulent
• NPSH
• NPSH
• Pump and system curves
– single vs. multiple pumps
– centrifugal vs. positive displacement
– compressors
Copyright J. A. Shaeiwitz and R. Turton - 2012 30

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Chapter21 performanceoffluidflowequipment-150917142659-lva1-app6892

  • 2. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 2
  • 3. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 3
  • 4. Key Relationships Key Relationships 2 • Turbulent flow 2 2 4 2 ∝ Δ ⇒ = Δ m m v P D fLv P fr fr ρ & & 2 2 32 4 = = m fL D m A m v ρπ ρ & & & 5 5 2 32 − ∝ Δ ⇒ = Δ D P D m fL P fr fr ρπ & Copyright J. A. Shaeiwitz and R. Turton - 2012 4
  • 5. Key Relationships Key Relationships • Laminar flow L L L D P v D v Δ = = 128 32 128 4 4 2 μ π π & & v D P D L v D L v P fr fr ∝ ∝ Δ ⇒ = = Δ − and 128 32 4 4 2 π μ μ & Copyright J. A. Shaeiwitz and R. Turton - 2012 5
  • 6. Example 1 Example 1 • Increase velocity by 25% ‐ turbulent flow ‐ effect on ΔP ld 1 2 25 . 1 old 1 new 2 2 = = = v v 2 2 2 1 ∝ Δ ⇒ = Δ v P D fLv P v fr fr ρ 5625 . 1 25 . 1 2 2 2 2 1 2 = = = Δ Δ v v P P D f f 1 1 Δ v P Copyright J. A. Shaeiwitz and R. Turton - 2012 6
  • 7. Example 2 Example 2 • Double diameter – turbulent flow‐ effect on  ΔP 2 old 1 new 2 2 = = = D D 32 5 5 2 2 1 ∝ Δ ⇒ = Δ − D P D m fL P D fr fr ρπ & 32 1 03125 . 0 5 . 0 5 5 5 1 1 2 = = = = Δ Δ D D P P D ρπ 32 2 1 Δ D P Copyright J. A. Shaeiwitz and R. Turton - 2012 7
  • 8. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 8
  • 9. NPSH NPSH NPSH N P i i S i H d • NPSH = Net Positive Suction Head • There is pressure drop upon entering pump,  p p p g p p, before mechanism that increases pressure • If fluid is too close to vapor pressure at pump • If fluid is too close to vapor pressure at pump  inlet, it could flash upon entering pump • Pumps are designed to handle liquids and do not  behave well with vapor Copyright J. A. Shaeiwitz and R. Turton - 2012 9
  • 10. NPSH NPSH • NPSHA = Pinlet – P * NPSHR • NPSHA = NPSH “available” NPSHR • NPSHR = NPSH “required” i f i li d b f v & – information supplied by pump manufacturer Copyright J. A. Shaeiwitz and R. Turton - 2012 10
  • 11. NPSH NPSH • Common situation • Apply MEB 1 2 0 2 2 W e z g v P s f − → Δ = − + Δ + Δ + Δ ρ 2 0 2 2 2 1 2 fL D fLv gh P P = + − − ρ ρ * 2 * 2 2 2 1 2 P fLv gh P P P NPSH D fLv gh P P + = = − + = ρ ρ ρ ρ Copyright J. A. Shaeiwitz and R. Turton - 2012 11 * * 1 2 P D gh P P P NPSH A − − + = − = ρ
  • 12. NPSH NPSH 5 2 2 1 * 32 P D v fL gh P NPSH A π ρ ρ − − + = & 2 form of v b a NPSH A − = & NPSH 1 32 * fL b P gh P a v b a NPSH A ρ ρ − + = NPSHA 5 2 32 D fL b π ρ = v & this is for turbulent flow f l i fl t i ht li Copyright J. A. Shaeiwitz and R. Turton - 2012 12 for laminar flow – straight line with negative slope
  • 13. NPSH NPSH 2 1 2 32 * fL P gh P a v b a NPSH A ρ − + = − = & • How to increase NPSHA • base case is line (1) increase a line (2) 5 2 32 D fL b π ρ = – increase a – line (2) • increase h • increase P1 • decrease P* – decrease T – decrease b – line (3) NPSHA • decrease L • increase D – suction line usually larger D 1 3 2 Copyright J. A. Shaeiwitz and R. Turton - 2012 13 v &
  • 14. NPSH NPSH NPSHA > NPSHR pump operates appropriately R NPSHA < NPSHR pump will cavitate inappropriate pump operation but it will operate NPSH but it will operate v & A v & Copyright J. A. Shaeiwitz and R. Turton - 2012 14
  • 15. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 15
  • 16. Pump and System Curves Pump and System Curves • Pump curve (centrifugal pump shown) • Pump curve (centrifugal pump shown) • Supplied by manufacturer • Can be measured in lab • centrifugal is sometimes called “constant head” pump ΔP in pressure units or head developed or head developed Copyright J. A. Shaeiwitz and R. Turton - 2012 16 v &
  • 17. Pump and System Curves Pump and System Curves • System curve pump supplies pressure increase ) ( ) ( 3 2 3 1 2 1 Δ − + Δ − + Δ = Δ − − − P P P P fr to increase fluid pressure and to overcome all of these pressure losses 0) ( h ) 0 or 0 be could ( ) 0 usually ( n destinatio to source in - out 3 1 Δ < > Δ + > Δ = Δ = Δ − P z g P P ρ 0) ( valve across drop pressure frictional 0) ( pipes in drop pressure frictional 0) ( pump across change pressure 3 2 2 1 < = Δ < = Δ > = Δ − P P P fr 0) ( valve across drop pressure frictional 3 2 < = Δ − P Copyright J. A. Shaeiwitz and R. Turton - 2012 17
  • 18. Pump and System Curves Pump and System Curves • To plot system curve – look at source to  destination and frictional loss 3 1 3 1 ) 0 or 0 be could ( ) 0 usually ( n destinatio to source in - out ) ( z g P P P P P fr sys < > Δ + > Δ = Δ = Δ Δ − + Δ = Δ − ρ 5 2 2 3 1 2 3 1 3 1 so 32 2 ) o be cou d ( ) usu y ( des o o sou ce D v fL P D fLv P P g sys & + Δ = + Δ = Δ − − − π ρ ρ ρ ΔPsys ( ) 2 form empirical so v b a P P P P sys valve sys pump & + = Δ Δ − + Δ = Δ v & ΔPsys Copyright J. A. Shaeiwitz and R. Turton - 2012 18 v & this is for turbulent flow for laminar flow – straight line
  • 19. Pump and System Curves Pump and System Curves • Often expressed as head sys v fL h fLv h h + = + = − − 32 2 5 2 2 3 1 2 3 1 & sys D g gD − − so 5 2 3 1 3 1 π valve sys pump h h h + = hsys Copyright J. A. Shaeiwitz and R. Turton - 2012 19 v &
  • 20. Pump and System Curves Pump and System Curves ΔP ΔPpump < ΔPsys impossible operation sys ΔP a = ΔPsource dest + ρgΔz if know this point 2 { -ΔPvalve ΔPpump z a ΔPsource-dest + ρgΔz with can find a and b 2 v b a Psys & + = Δ operating v & v & pump a }-ΔPfr z ΔPpump > ΔPsys excess pressure dissipated across partially closed valve as open and close valve, flowrate changes operating v & Copyright J. A. Shaeiwitz and R. Turton - 2012 20 as open and close valve, flowrate changes intersection point is fully open valve
  • 21. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 21
  • 22. Pumps in Series and Parallel Pumps in Series and Parallel • Series – Pump curve two pumps Pump curve – 2X head at  same flowrate ΔPpump one pump v & Copyright J. A. Shaeiwitz and R. Turton - 2012 22
  • 23. Pumps in Series and Parallel Pumps in Series and Parallel • Parallel P two pumps – Pump curve – 2X flowrate at  same head ΔPpump one pump same head v & Copyright J. A. Shaeiwitz and R. Turton - 2012 23
  • 24. Pumps in Series and Parallel Pumps in Series and Parallel • Which  configuration two pumps series configuration  maximizes  flowrate? ΔPpump z flowrate? – No general  result one pump two pumps parallel z result Copyright J. A. Shaeiwitz and R. Turton - 2012 24 v &
  • 25. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 25
  • 26. Centrifugal – variable speed Centrifugal  variable speed ΔP ΔPpump rpm 5 rpm 3 rpm 2 rpm 4 v & rpm 1 rpm increases with number more expensive pump Copyright J. A. Shaeiwitz and R. Turton - 2012 26 p p p cost of “wasting” pressure across valve may be less than cost of pump
  • 27. Positive Displacement fl l / flow regulation/pump curve ΔP in pressure units sometimes called “constant volume” pump p or head developed v & Copyright J. A. Shaeiwitz and R. Turton - 2012 27
  • 28. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 28
  • 29. Compressors Compressors locus of maxima = surge line can also draw system Pout /Pin rpm 5 can also draw system curves on this graph – must change form of left- hand side to ratio rpm 3 rpm 2 rpm 4 v & rpm 1 rpm 2 usually worth using speed control here because of compression costs Copyright J. A. Shaeiwitz and R. Turton - 2012 29 usually worth using speed control here because of compression costs
  • 30. Outline Outline • Flow in pipes Flow in pipes – laminar vs. turbulent • NPSH • NPSH • Pump and system curves – single vs. multiple pumps – centrifugal vs. positive displacement – compressors Copyright J. A. Shaeiwitz and R. Turton - 2012 30