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7/22/2019 29_Cavitation_&_Flashing.ppt
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Cavitation Flashing
and
Flashing
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VaporizationEffects in
Fluid Flow
Vaporization
Effects inFluid Flow
o o
o
o
o
o
o
o
o
o
o
o
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o
o
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o o
o
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o
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FusionLine
FusionLine
Critical
PointLiquid
Phase
Vapor
Phase
Phase
Solid
Triple
Point
Pr
essure
Triple Point Diagram
Temperature
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Water 32 0.0886
oF psia
Triple Point
CO2 - 69.88 75.09
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FusionLine
FusionLine
Critical
PointLiquid
Phase
Vapor
Phase
Phase
Solid
Triple
Point
Pr
essure
Triple Point Diagram
Temperature
Water (Solid, Liquid, Vapor)
CO2 (Solid, Vapor, NO Liquid)
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Cavitation?
What is
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Cavitation?What is
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1 2 3
Varying Area Flow Channel
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Flow with Pressure RecoveryFlow with Pressure Recovery
pp
1 2 3
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V12 P1 V2
2 P2
+ + gz 1 = + + gz 2
2 1 2 2
1V1A1 = 2V2A2
Basic Equations:
Bernoullis Energy Equation
X X
Continuity
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1 2 3
11Flow Channel with sharp edge orifice
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p
1 2 3
Flow Channel with out Pressure Recovery
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ValvePressure
Drop
CavitationCavitation
PP 22(Outlet
Pressure)(Outlet
Pressure)
Single Seated Valve Pressure Recovery Diagram
oo
oo
PPvcvc (Pressure at Vena Contracta)
PV
PP 11
(InletPressure)
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
P Line( Pressure)Drop
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Bubblecollapseformation
andmechanism
14
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1 diameter from wall
Bubble Implosion
17
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1 diameter from wall
Bubble Implosion
Within a relatively
short time the total
damage can become
very signi f icant.
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CavControl trim
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CavControl trim
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316
Stainless
Steel
with
TungstenCarbide
Insert
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316
Stainless
Steel
with
TungstenCarbide
Insert
With higher magnification
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Pitting and erosion
Noise and vibration
Corrosion
Combination
Resultsof Cavitation
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V12 P1 V2
2 P2
+ + gz 1 = + + gz 22 1 2 2
Basic Equations:
Bernoullis Energy Equation
V12 P1 V22 P2+ = +
2 1 2 2
X X
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V1
A1
= V2
A2
V1 P1 V2 P2+ = +
2 1 2 2
[ ]( )A 2
2 1/2 2 PV1 = 1 +
A1
GfW
therefore
Capacity
CV TermP/Gf
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PQ = V2 A2 = CVGf
CV is defined for
units/area used
where:
Reduces to
ISA Sizing Equation
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Slope = CV
Ideal Fluid
P
q
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Actual Liquid
PP
q A
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P
Actual Liquid
CBTheoretical choking pointActual choking point
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ChokedPoint B
Pc
= FL
2 (P
1- F
FP
V)
ChokedChoked
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Pressu re drop produces no ise
and vibrat ion fromvapo r free
f low turbu lence.
No Cav itat ion :
Simp ly Flow Noise
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In term it ten t Noise and cavi ty
format ion.
Constant(o r Crit ic al)
Steady cons tant Noise and cons tant
cavi ty format ion .
Cavitat ion:
Cavitat ion
Incipient
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Increases in vib rat ion and
Noise intensi ty to the level of
"max imum v ibrat ion"
Ful l
"max imum v ibrat ion""max imum v ibrat ion""max imum v ibrat ion""max imum v ibrat ion"
Cavitat ion:
Significant Damage"oftenoccu rs somewhere in th is regime.
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`
Erosion damage from high velocity
can occur giving a damageappearance.
Super
A decrease in noise and vibration.
Choking often occurs in this
area.
oo
o
o
o
o
oo
ooo
o
o
oo
o
o
Cavitation:
o
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P1 - Pv1 =P1 - P2
P1 - based index:
Sigma1
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P2 - based index:
P2 - Pv2 =P1 - P2
Sigma2
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Testing forCavitation in
"LowPressureRecovery"
Control Valves
Testing forCavitation in
"LowPressureRecovery"
Control Valves
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Ways of
of Cavitation
Ways of
of Cavitation
MeasuringIntensity Soft Aluminum Plate
Accelerometer
MeterMeter
1 m. down
1 m. out
and
Sound
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TestingTesting1. Noise / Acceleration2. Damage3. Visual
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45
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46 = (P1- PV) / P
Acceler
ation
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47 = (P1- PV) / P
Acceler
ation
i
c
mv
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Testing1. Noise / Acceleration2. Damage3. Visual
Testing1. Noise / Acceleration2. Damage3. Visual
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Cavitation
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Velocity Erosion
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Corrosion
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Testing1. Noise/Acceleration2. Damage3. Visual
Testing1. Noise/Acceleration2. Damage3. Visual
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55 Transparent pipe Strobe Light
Visual Cavitation
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56 Transparent pipe Strobe Light
Visual Cavitation
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Control of Cavitation DamageControl of Cavitation Damage1. Remove all nuclei
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Control of Cavitation DamageControl of Cavitation Damage
2. Inject air or gas1. Remove all nuclei
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Control of Cavitation DamageControl of Cavitation Damage
2. Inject air or gas1. Remove all nuclei
3. Increase the FL value
FL = .92
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0 20 40 60 80 1000 20 40 60 80 100
% of Rated Capacity% of Rated Capacity
FL Flow-to-CloseFL Flow-to-Close
F L Flow-to-OpenFL Flow-to-Open
0 20 40 60 80 1000 20 40 60 80 100
% of Rated Capacity% of Rated Capacity
0 30 60 900 30 60 90
ValdiskValdisk
Fi Flow-to-CloseF i Flow-to-Close
F i Flow-to-OpenF i Flow-to-Open
Valve Recovery FactorsValve Recovery Factors
FL Fi FL
Globe Valve FL Values Globe Valve Fi Values Rotary Valve FL Values
1.00
0.90
0.80
0.70
0.60
0.50
0.40
1.00
0.90
0.80
0.70
0.60
0.50
0.40
1.00
0.90
0.80
0.70
0.60
0.50
0.40
Degrees Open
ShearStream
FL = .92?
FL .92Flow Under
FL = .70
Flow Over
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3. Increase the FL value
4. Hardened materials (brute force)
2. Inject air or gas1. Remove all nuclei
Estimated force = approx. 250,000# per in2
Control of Cavitation Damage
No materials available that have such strength
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62Hardened Trim
Flowserve prefers: 316 ss / #6 Stellite
Note: For2 valves and smaller, the entire plug
head and seat ring are solid Stellite.
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Control of Cavitation DamageControl of Cavitation Damage
3. Increase the FL value
4. Hardened materials (brute force)
2. Inject air or gas1. Remove all nuclei
5. Remove metal boundary
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FLOW
CavControl
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Counterbored holes from outside in.
CavControl
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Flow
CavControl
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67CAVITATION CONTROL
65
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A. Single Orifice
B. Multiple Orifice
This looses less energy
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5. Remove metal boundary
2. Inject air or gas1. Remove all nuclei
3. Increase the FL value
4. Hardened materials (brute force)
6. Multi-stage trim design
Control of Cavitation Damage
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PP
PP
PP
11
22
vcPP
Liquid
The Problem
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
Liquid and Vapor
PV
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PV
The SolutionPP
PP
11
22
Liquid
Liquid and Vapor
73
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PV
The SolutionPP
PP
11
22
Liquid
(Multi-Stage trim)
Liquid and Vapor
Since, Pressure does not go below PV ,
74
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74 doesNOToccur!Cavitation
PP
PP
11
22PV
Liquid
The Solution
(Multi-Stage trim)
Since, Pressure does not go below PV ,
76
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outside to
increase
Channelwidths
Inside.
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77 CHANNELSTREAM
NO CAVITATION
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Visual Comparison
CHANNELSTREAMCAVITATION CONTROL
CAVITATES DOES NOT CAVITATE
SINGLE STAGE MULTI-STAGE
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Tiger-Tooth
Flow
Tiger-Tooth Trim also eliminates cavitation.77
.
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8080
FlashingFlashing
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PP
FlashingFlashing
PV
Pressure)(Outlet
P2
(ValvePressureDrop)
PP
1
(Pressure at Vena Contracta)
Pressure Profile Single Seated Valve
VC
Liqu id
Liqu id / Gas combinat ion
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c. Erosion
ProblemsProblemsa. High Velocitiesa.High Velocities
b. Choking
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h1 = hf(1-x) + hg(x)
Since the Enthalpy of a control valveis considered constant between P1 & P2 :
x = % of liquid mass
flashed to vapor
Constant Enthalpy, h
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T
S
Vapor
Liquid
1
2
P2
P1
Liquid Gas
Typical T S Diagram
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P = 15 psia
Example
= 200 psia
Water @ 250o
F
P1
2
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hf1 = 218.59 B/lb m
hf2 = 181.19 B/lb m
hfg2 = 967.70 B/lb m
Enthalpies from
Steam Tables
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= 3.86% flash(218.59 - 181.19)
967.70
Enthalpy o f
Sat. Liq uid at
Inlet Temp
Enthalpy o f
Evaporat ion at
Outlet Press
Enthalpy o f
Sat. Liq uid at
Outlet Press
Percent Flash
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Sp. Vol. = (1 - x)vf+ xvg
vfm = 1.04 ft3/ lb m
vfm = .017(96.1%) + 26.29(3.09%)Liquid Vapor
61+ times as much
volume as the
original liquid.
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Flashing DamageFlashing Damage
1. Harden the trim2. Control velocities
3. Select Proper materials
To minimize
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`
Vaporization
RequiresCareful
Engineering
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Return to Performance!