PRV Stability Project Overview PERF ... - mycommittees.api.org Document… · API 2011 Fall Meeting...
Transcript of PRV Stability Project Overview PERF ... - mycommittees.api.org Document… · API 2011 Fall Meeting...
API 2011 Fall Meeting - November 14, 2011
Ron Darby, PhD, PE and Abdul Aldeeb, PhD
Presented to theAPI 2011 Fall Meeting
November 14, 2011Los Angeles, CA
PRV Stability Project OverviewPERF 99-05
API 2011 Fall Meeting - November 14, 2011
Project Objective
To develop a method of predicting the instability or “chatter” of a relief valve that is based on sound fundamental scientific principles, to replace the API “3% Rule.”
API 2011 Fall Meeting - November 14, 2011
API “3% Rule”
Assumption:valve will not re-close (or “chatter”) if the nozzle pressure does not fall more than 3% of PRV set pressure, due to non-recoverable friction loss in the inlet line.
Fact:This criterion is based on static conditions and does not account for other dynamic factors that affect valve stability. Thus, it is not sufficient to consider static conditions only for avoiding chatter.
API 2011 Fall Meeting - November 14, 2011
Program Goals
Develop a mathematical model to predict stability characteristics (e.g., disc lift vs. time) of a PRV in vapor/gas service, accounting for effects that may contribute to instability.
Obtain experimental data on various PRV’s for the purpose of validating the predictive accuracy of the model.
Incorporate the model into an easily-used computer program.
API 2011 Fall Meeting - November 14, 2011
Factors Influencing Disc Response
Valve disc dynamic response (damped spring-mass oscillatory system)
Pressure and fluid momentum forces on disc
Blow-down setting and backpressure effects
Dynamics of fluid response in inlet line (friction, capacitance, and acoustic coupling)
Dynamics of fluid response in outlet line
Lift-flow characteristics of the valve Geometry of flow path leaving the disc
d
Dc
Dd
API 2011 Fall Meeting - November 14, 2011
Mathematical Model
The model consists of a number of coupled nonlinear differential and algebraic equations which are solved numerically in a spreadsheet. The output is displayed as the disc lift vs. time, on a millisecond time scale.
API 2011 Fall Meeting - November 14, 2011
Mathematical Model
Factors considered in the model:
Forces on disc: Total fluid pressure on disc Fluid momentum force on disc Propagating acoustical pressure wave in inlet line Blowdown and backpressure effects
Dynamic response of disc vs. time: Spring-mass impulse response Capacitance of vessel and inlet line
API 2011 Fall Meeting - November 14, 2011
Model Assumptions
Choked gas flow
Valve opens at set pressure (Psg)
Relief mass flow determined at 1.1 Psg=Po
Max lift when Acurtain = Anozzle (choke point shifts from annulus to nozzle)
Pressure on disc determined by mass flow rate and:
Friction loss in inlet line;
Capacity of vessel and inlet line;
Expansion shock – (speed of sound, Li, Di, opening time).
Update force (magnitude and phase) on disc determined by PN, AD, momentum transfer from fluid to disc (geometry of disc and exit chamber).
Valve closes when P < PBD
API 2011 Fall Meeting - November 14, 2011
Governing Equations
5 coupled nonlinear equations for disc dynamic response:
x
N B
o N
x
x N B N
N o N
B o N
N N B
x= valve lift , F = force on disk , t=time
P ,P = pressure at nozzle , backpressure
m = relief mass rate , m =nozzle mass rate
x = fn F ,t,x,xF = fn P ,P ,mP = fn m ,m ,tP = fn m ,m ,t
m = fn x,P ,P
API 2011 Fall Meeting - November 14, 2011
Model Input Parameters
1. Mass of moving parts
2. Spring constant
3. Damping of moving parts
4. Discharge coefficient (at full and partial lift)
5. Geometry of nozzle, disc, and fluid flow path
1. Inlet piping length and diameter
2. Outlet piping length and diameter
3. Friction loss in fittings
4. Capacity of vessel and inlet line
5. Inlet and outlet piping roughness factor
1. Set pressure and overpressure
2. Vessel pressure and temperature
3. Discharge pressure and temperature
4. Relief mass flow rate
5. Gas molecular weight and isentropic exponent
ValveParameters
DesignParameters
OperatingConditions
API 2011 Fall Meeting - November 14, 2011
Stability Criterion
Valve is stable if x(t) is monotonic, or oscillatory with small decreasing amplitude
Stable
0.0
0.1
0.2
0.3
0.4
0.000 0.005 0.010 0.015Time (s)
Dis
k Li
ft
Flutter
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.000 0.005 0.010 0.015Time
Dis
k Li
ft
0.0
0.1
0.2
0.3
0.4
0.5
0.0 0.5 1.0 1.5 2.0 2.5 3.0Time (s)
Val
ve L
ift (i
n.) Low frequency
oscillations
Is this stable lift?
API 2011 Fall Meeting - November 14, 2011
Stability Criterion
Valve is unstable if x(t) is oscillatory with a large or increasing amplitude
0 5 10 15-0.1
0
0.1
0.2
0.3
Time (secs)
Val
ve L
ift (i
n)
API 2011 Fall Meeting - November 14, 2011
Factors Impacting Stability
Stability is affected by the following factors: damping of the moving parts stiffness of the spring opening time of the valve blowdown setting diameter of inlet piping diameter of discharge piping length of inlet piping length of outlet piping mass of moving parts geometry of valve/disc
Because the system is highly nonlinear, all of
these factors interact and cannot therefore be
considered separately or in isolation from all the others.
Thus it is not possible to generalize about the
effect of any one "parameter" in isolation
from the others.
API 2011 Fall Meeting - November 14, 2011
Experimental Program
Three different size valves (1E2, 2J3, and 3L4) from three manufacturers were tested in gas service.
Disc lift vs. time data obtained at 50 and 250 psig set pressure for each valve.
More than 250 unique test runs were completed with: No inlet piping - determine opening time
characteristics.
Inlet piping - three different lengths.
Discharge piping – two different lengths.
API 2011 Fall Meeting - November 14, 2011
Experimental Program
API 2011 Fall Meeting - November 14, 2011
Experimental Program – Collected Data
API 2011 Fall Meeting - November 14, 2011
Testing Observations – No Inlet Piping
3L4 @ 250 psig
80% Capacity
Valves were tested at flow rates ranging from 10 to 100% of their measured flowing capacities and all valves operated without signs of chattering (high frequency opening and closing)
1E2 @ 50 psig
100% Capacity
API 2011 Fall Meeting - November 14, 2011
Testing Observations – No Inlet Piping
For the same valve, the transient disc lift response profiles were nearly identical for most of the tests, regardless of the pressure rise rate and the percentage of valve capacity
API 2011 Fall Meeting - November 14, 2011
Testing Observations – No Inlet Piping
Mfg. F - 1E2 - 250 psig - No Inlet Piping
0.00
0.04
0.08
0.12
0.16
0.20
0.00 0.02 0.04 0.06 0.08 0.10 0.12 0.14Time (s)
Val
ve L
ift (i
n)
10% Capacity_1.13 psi/sec
24% Capacity_3.20 psi/sec
48% Capacity_6.26 psi/sec
72% Capacity_9.66 psi/sec
96% Capacity_12.46 psi/sec
96% Capacity_0.96 psi/sec
72% Capacity_0.72 psi/sec
48% Capacity_0.46 psi/sec
Mfg. F - 1E2 - 250 psig - No Inlet Piping
0.00
0.04
0.08
0.12
0.16
0.20
0.00 0.02 0.04 0.06 0.08 0.10 0.12 0.14Time (s)
Val
ve L
ift (i
n)
10% Capacity_1.13 psi/sec
24% Capacity_3.20 psi/sec
48% Capacity_6.26 psi/sec
72% Capacity_9.66 psi/sec
96% Capacity_12.46 psi/sec
96% Capacity_0.96 psi/sec
72% Capacity_0.72 psi/sec
48% Capacity_0.46 psi/sec
API 2011 Fall Meeting - November 14, 2011
Testing Observations – Inlet Piping
18 valves were tested at flow rates ranging from 30 to 100% of their measured flowing capacities.
The range of testing is not significant but results illustrate complexity of stability problem.
For the same valve at a specific inlet piping length, the transient disc lift responseprofiles were nearly identical for most of the tests.
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
6.1 6.12 6.14 6.16 6.18 6.2 6.22 6.24Correlated Time (Secs)
Valv
e Li
ft (i
n)
Run 46 - 30% Capacity
Run 47 - 50% Capacity
Run 48 - 100% Capacity
Repeat Run 48*
* The repeat of Run 48 showed that theset pressure of the valve had changedto approximately 232 psig. Testing was then terminated with this valve.
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
6.1 6.12 6.14 6.16 6.18 6.2 6.22 6.24Correlated Time (Secs)
Valv
e Li
ft (i
n)
Run 46 - 30% Capacity
Run 47 - 50% Capacity
Run 48 - 100% Capacity
Repeat Run 48*
* The repeat of Run 48 showed that theset pressure of the valve had changedto approximately 232 psig. Testing was then terminated with this valve.
API 2011 Fall Meeting - November 14, 2011
Testing Observations – Inlet Piping
44 valves tested valves at 100% capacity:
50 psig valves: 8 of 9 were stable at all “tested” lengths with inlet pressure drop ranging from 1.1 to 4.6% of set pressure (the only unstable case has pressure drop of 4.3%).
250 psig valves: 6 of 9 valves were not tested at 6 foot inlet lines (presumably because of damage during earlier testing).
4 valves became unstable at higher inlet piping lengths: 3 of the unstable PRVs had inlet pressure drops < 3% of set pressure (all were < 5%).
API 2011 Fall Meeting - November 14, 2011
Testing Observations – Inlet Piping
44 valves tested valves at 100% capacity:
10 of the 18 tested valves had measured blowdown less than 7% of set pressure.
5 valves had a difference between blowdown and inlet pressure drop (w/ 6 foot inlet length) that was < 2% (4 of the 5 valves became unstable).
API 2011 Fall Meeting - November 14, 2011
Testing Observations – Inlet and Outlet Piping
J and L valves set only at 50 psig were tested due to damaged 250 psig valves.
Dynamic backpressure was ~8% of set pressure.
Stability was not impacted by adding outlet piping.
7 7.1 7.2 7.3 7.4 7.5 7.6 7.7 7.8 7.9 80
0.05
0.1
0.15
0.2
0.25
Correlated Time (secs)
Lift
(in)
No Exit Pipew/ Exit Pipe
7.6 7.62 7.64 7.66 7.68 7.7 7.72 7.74 7.76 7.780
0.02
0.04
0.06
0.08
0.1
0.12
0.14
0.16
0.18
0.2
Correlated Time (secs)
Lift
(in)
No Exit Pipew/ Exit Pipe
2J3 @ 50 psig
2-foot Inlet Piping
API 2011 Fall Meeting - November 14, 2011
Testing Program Results
Valve Number
Valve Size&
Set Pressure
Inlet Piping Length and Pressure Drop
Measured Blowdown
2 FeetValve Initial
Lift(Test)
Inlet Pressure Drop
% of Set Pressure
4 FeetValve Initial
Lift(Test)
Inlet Pressure Drop
% of Set Pressure
6 FeetValve Initial
Lift(Test)
Inlet Pressure Drop
% of Set Pressure
1 1E2 - 50 psig Stable 1.2 Stable 2.0 Stable* 2.7 5.32 1E2 - 250 psig Stable 1.0 Unstable 1.7 Unstable 2.2 5.63 2J3 - 50 psig Stable 2.2 Stable 3.2 Unstable 4.3 8.04 2J3 - 250 psig Stable 2.0 Test Failed 3.0 Not Tested 4.0 7.65 3L4 - 50 psig Stable 2.3 Stable 3.3 Stable 4.5 4.36 3L4 - 250 psig Stable 1.8 Stable 2.7 Not Tested 3.5 11.97 1E2 - 50 psig Stable 1.1 Stable 1.9 Stable 2.6 7.18 1E2 - 250 psig Stable 1.0 Unstable 1.7 Unstable 2.3 2.59 2J3 - 50 psig Stable 2.3 Stable 3.5 Stable 4.6 9.110 2J3 - 250 psig Stable 1.9 Not Tested 2.8 Not Tested 3.8 6.411 3L4 - 50 psig Stable 2.3 Stable 3.3 Stable 4.6 5.612 3L4 - 250 psig Stable 1.8 Not Tested 2.7 Not Tested 3.6 5.713 1E2 - 50 psig Stable 1.1 Stable 1.9 Stable 2.7 9.914 1E2 - 250 psig Stable 1.0 Stable 1.7 Stable 2.2 6.415 2J3 - 50 psig Stable 2.3 Stable 3.4 Stable 4.5 11.816 2J3 - 250 psig Stable 1.9 Not Tested 2.8 Not Tested 3.7 5.617 3L4 - 50 psig Stable 2.5 Stable 3.5 Stable 4.6 10.618 3L4 - 250 psig Stable 1.8 Unstable 2.7 Not Tested 3.5 4.4
Valve Number
Valve Size&
Set Pressure
Inlet Piping Length and Pressure Drop
Measured Blowdown
2 FeetValve Initial
Lift(Test)
Inlet Pressure Drop
% of Set Pressure
4 FeetValve Initial
Lift(Test)
Inlet Pressure Drop
% of Set Pressure
6 FeetValve Initial
Lift(Test)
Inlet Pressure Drop
% of Set Pressure
1 1E2 - 50 psig Stable 1.2 Stable 2.0 Stable* 2.7 5.32 1E2 - 250 psig Stable 1.0 Unstable 1.7 Unstable 2.2 5.63 2J3 - 50 psig Stable 2.2 Stable 3.2 Unstable 4.3 8.04 2J3 - 250 psig Stable 2.0 Test Failed 3.0 Not Tested 4.0 7.65 3L4 - 50 psig Stable 2.3 Stable 3.3 Stable 4.5 4.36 3L4 - 250 psig Stable 1.8 Stable 2.7 Not Tested 3.5 11.97 1E2 - 50 psig Stable 1.1 Stable 1.9 Stable 2.6 7.18 1E2 - 250 psig Stable 1.0 Unstable 1.7 Unstable 2.3 2.59 2J3 - 50 psig Stable 2.3 Stable 3.5 Stable 4.6 9.110 2J3 - 250 psig Stable 1.9 Not Tested 2.8 Not Tested 3.8 6.411 3L4 - 50 psig Stable 2.3 Stable 3.3 Stable 4.6 5.612 3L4 - 250 psig Stable 1.8 Not Tested 2.7 Not Tested 3.6 5.713 1E2 - 50 psig Stable 1.1 Stable 1.9 Stable 2.7 9.914 1E2 - 250 psig Stable 1.0 Stable 1.7 Stable 2.2 6.415 2J3 - 50 psig Stable 2.3 Stable 3.4 Stable 4.5 11.816 2J3 - 250 psig Stable 1.9 Not Tested 2.8 Not Tested 3.7 5.617 3L4 - 50 psig Stable 2.5 Stable 3.5 Stable 4.6 10.618 3L4 - 250 psig Stable 1.8 Unstable 2.7 Not Tested 3.5 4.4
API 2011 Fall Meeting - November 14, 2011
Model Prediction
Valve parameters, design parameters, and test conditions were utilized as inputs to the mathematical model for valve stability modeling.
All parameters are known or measured except for fluid deflection angel and damping factor. These were estimated.
Generally, the mathematical model was found to predict the actual test data reasonably well.
d
Dc
Dd
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. E - 3L4 - 50 psig - Large Tank - 3.52 psi/s - 100% of Capacity - 0 ft Inlet Piping
0.0
0.1
0.2
0.4
0.5
0.6
0.7
0.8
1.0
1.1
0.0 0.1 0.2 0.3 0.4 0.5Time (s)
Val
ve li
ft (in
)
Model Prediction
Test Run - Cycle 1
Test Run - Cycle 2
Mfg. E - 3L4 - 50 psig - Large Tank - 3.52 psi/s - 100% of Capacity - 0 ft Inlet Piping
0.0
0.1
0.2
0.4
0.5
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0.8
1.0
1.1
0.0 0.1 0.2 0.3 0.4 0.5Time (s)
Val
ve li
ft (in
)
Model Prediction
Test Run - Cycle 1
Test Run - Cycle 2
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. D - 3L4 - 50 psig - Large Tank - 3.53 psi/s - 100% of Capacity - 0 ft Inlet Piping
0.0
0.1
0.2
0.3
0.4
0.5
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0.8
-0.5 -0.4 -0.3 -0.2 -0.1 0.0 0.1 0.2 0.3 0.4 0.5Time (s)
Val
ve L
ift (i
n)
Model Prediction
Test Data
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. F - 2J3 - 50 psig - Large Tank - 1.57 psi/s - 100% of Capacity - 6 ft Inlet Piping
0.0
0.1
0.2
0.3
0.4
0.5
0.6
-0.1 0.0 0.1 0.2 0.3 0.4 0.5Time (s)
Val
ve L
ift (i
n.)
Model Prediction
Test Data
Mfg. F - 2J3 - 50 psig - Large Tank - 1.57 psi/s - 100% of Capacity - 6 ft Inlet Piping
0.0
0.1
0.2
0.3
0.4
0.5
0.6
-0.1 0.0 0.1 0.2 0.3 0.4 0.5Time (s)
Val
ve L
ift (i
n.)
Model Prediction
Test Data
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. D - 2J3 - 50 psig - Large Tank - 1.57 psi/s - 100% of Capacity - 6 ft Inlet Piping
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.0 0.5 1.0 1.5 2.0
Time (s)
Val
ve L
ift (i
n)
Model Prediction
Test Data
Mfg. D - 2J3 - 50 psig - Large Tank - 1.57 psi/s - 100% of Capacity - 6 ft Inlet Piping
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.0 0.5 1.0 1.5 2.0
Time (s)
Val
ve L
ift (i
n)
Model Prediction
Test Data
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. D - 1E2 - 250 psig - Small Tank - 12.29 psi/s - 74% of Capacity - 6 ft Inlet Piping
-0.05
0.00
0.05
0.10
0.15
-0.5 0.0 0.5 1.0 1.5 2.0Time (s)
Val
ve L
ift (i
n) Model Prediction
Test Data
Mfg. D - 1E2 - 250 psig - Small Tank - 12.29 psi/s - 74% of Capacity - 6 ft Inlet Piping
-0.05
0.00
0.05
0.10
0.15
-0.5 0.0 0.5 1.0 1.5 2.0Time (s)
Val
ve L
ift (i
n) Model Prediction
Test Data
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. D - 3L4 - 250 psig - Large Tank - 11.2 psi/s - 76% of Capacity - 0 ft Inlet Piping
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.0 0.1 0.2 0.3 0.4 0.5Time (s)
Val
ve L
ift (i
n)
Model Prediction
Test Data
Mfg. D - 3L4 - 250 psig - Large Tank - 11.2 psi/s - 76% of Capacity - 0 ft Inlet Piping
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
0.80
0.0 0.1 0.2 0.3 0.4 0.5Time (s)
Val
ve L
ift (i
n)
Model Prediction
Test Data
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. D - 2J3 - 250 psig - Large Tank - 6.51 psi/s - 100% of Capacity - 2 ft Inlet Piping
0.0
0.1
0.2
0.3
0.4
0.5
0.6
-0.5 -0.4 -0.3 -0.2 -0.1 0.0 0.1 0.2 0.3 0.4 0.5
Time (s)
Val
ve L
ift (i
n)
Model Prediction
Test Data
Mfg. D - 2J3 - 250 psig - Large Tank - 6.51 psi/s - 100% of Capacity - 2 ft Inlet Piping
0.0
0.1
0.2
0.3
0.4
0.5
0.6
-0.5 -0.4 -0.3 -0.2 -0.1 0.0 0.1 0.2 0.3 0.4 0.5
Time (s)
Val
ve L
ift (i
n)
Model Prediction
Test Data
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
Mfg. E - 1E2 - 50 psig - Small Tank - 3.02 psi/s - 100% of Capacity
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.0 0.1 0.2 0.3 0.4 0.5
Time (s)
Val
ve L
ift (i
n)
Test Data - 0 ft Inlet Piping
Test Data - 2 ft Inlet Piping
Test Data - 4 ft Inlet Piping
Test Data - 6 ft Inlet Piping
Mfg. E - 1E2 - 50 psig - Small Tank - 3.02 psi/s - 100% of Capacity
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.0 0.1 0.2 0.3 0.4 0.5
Time (s)
Val
ve L
ift (i
n)
Model Prediction - 0 ft Inlet Piping
Model Prediction - 2 ft Inlet Piping
Model Prediction - 4 ft Inlet Piping
Model Prediction - 6 ft Inlet Piping
Mfg. E - 1E2 - 50 psig - Small Tank - 3.02 psi/s - 100% of Capacity
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.0 0.1 0.2 0.3 0.4 0.5
Time (s)
Val
ve L
ift (i
n)
Test Data - 0 ft Inlet Piping
Test Data - 2 ft Inlet Piping
Test Data - 4 ft Inlet Piping
Test Data - 6 ft Inlet Piping
Mfg. E - 1E2 - 50 psig - Small Tank - 3.02 psi/s - 100% of Capacity
0.00
0.05
0.10
0.15
0.20
0.25
0.30
0.35
0.40
0.0 0.1 0.2 0.3 0.4 0.5
Time (s)
Val
ve L
ift (i
n)
Model Prediction - 0 ft Inlet Piping
Model Prediction - 2 ft Inlet Piping
Model Prediction - 4 ft Inlet Piping
Model Prediction - 6 ft Inlet Piping
API 2011 Fall Meeting - November 14, 2011
Model Prediction - Examples
2J3 - 50 psig - Large Tank - 1.57 psi/s - 100% of Capacity - 4 ft Inlet Piping & 31.42 ft Oulet Piping
0.0
0.1
0.2
0.3
0.4
0.5
0.6
-1.8 -1.6 -1.4 -1.2 -1.0 -0.8 -0.6 -0.4 -0.2 0.0 0.2 0.4 0.6Time (s)
Valv
e Li
ft (in
.)
Model Prediction
Test Data
2J3 - 50 psig - Large Tank - 1.57 psi/s - 100% of Capacity - 4 ft Inlet Piping & No Outlet Piping
0.0
0.1
0.2
0.3
0.4
0.5
0.6
-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5
Time (s)
Val
ve L
ift (i
n.)
Model Prediction
Test Data
API 2011 Fall Meeting - November 14, 2011
Conclusions & Path Forward
PRV stability appears to be affected by several parameters including valve specifications, system design, and operating conditions.
Based on the tested valves, mathematical modeling of valve lift response was possible.
Additional work to test valves of different sizes from other manufacturers will be required to establish reliable methods to estimate the unknown parameters outside the range of sizes and conditions of those tested.
API 2011 Fall Meeting - November 14, 2011
Questions
Thank you for your attention!