predicting the hp cost of reciprocating compressor manifolds

55
Predicting the Power Loss of Reciprocating Compressor Manifolds NOVA Research: Kamal K. Botros John Geerligs Beta Machinery: Kelly Eberle Brian Howes Gordon Sun Russ Barss Bryan Long TransCanada: Thomas Robinson Peerless Mfg: Dave Breindel PSC: Martin Hinchliff - chair Rainer Kurz Christine Scrivner Steve O’toole Clint Lingel Project Team:

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Predicting the Power Loss of Reciprocating Compressor Manifolds

NOVA Research: Kamal K. Botros John Geerligs

Beta Machinery: Kelly Eberle Brian Howes Gordon Sun Russ Barss Bryan Long

TransCanada: Thomas Robinson Peerless Mfg: Dave Breindel

PSC: Martin Hinchliff - chair Rainer Kurz Christine Scrivner Steve O’toole Clint Lingel

Project Team:

2 GMC Nashville Oct 5-8, 2014

Project Motivation

How much power does my

compressor need?

3 GMC Nashville Oct 5-8, 2014

Compressor Performance Calculation

Why Estimated Total Load? - Compression (ideal) power - Mechanical Efficiency - Manifold (bottle) power loss - Orifice power loss - Other system loss

How do you calculate the unknown power losses?

4 GMC Nashville Oct 5-8, 2014

Compressor Performance Calculation

How much, assume 1%, 2%? Is it accurate?

Unknown Power Losses are estimated by the pressure drop

5 GMC Nashville Oct 5-8, 2014

Pressure Drop Calculation… easy, right?

OK, but…does this work for my recip compressor?

6 GMC Nashville Oct 5-8, 2014

Challenges to Industry

• Manifolds (pulsation bottles) have complicated geometry. K-factors are not published.

• Recip compressors create high flow fluctuations.

• How to relate pressure drop to power loss?

7 GMC Nashville Oct 5-8, 2014

How important is power loss?

Inaccurate power calculation effects performance and reliability (3% to 12% error in results)

RED = Unsafe

YELLOW = Conditionally Safe

GREEN = Safe

Suction Pressure (psia)

Disc

harg

e Pr

essu

re (p

sia)

Consequences: Driver size inadequate Unable to meet

contract flow Reliability (rod load,

reversal, and discharge temperature)

Inefficient operation

Design Point move to Unsafe Zone

8 GMC Nashville Oct 5-8, 2014

Overall Project Objectives

1. Develop a methodology to predict the mean and pulsating power losses across Reciprocating Compressor Manifolds (bottles).

2. Validate the methodology via experimental means, either from:

Measurements of actual recip. compressor in the field, or

Scale-down test rig involving a custom-design bottle and a Pulse-generator.

3. Ultimate Goal is to:

Recommend a standard methodology to quantify the pulsating flow power loss.

Come up with adjustment factor(s) to be applied to the mean pressure drop coefficient (K) in the presence of pulsating flow.

9 GMC Nashville Oct 5-8, 2014

Overall Project Objectives

1. Develop a methodology to predict the mean and pulsating power losses across Reciprocating Compressor Manifolds (bottles).

2. Validate the methodology via experimental means, either from:

Measurements of actual recip. compressor in the field, or

Scale-down test rig involving a custom-design bottle and a Pulse-generator.

3. Ultimate Goal is to:

Recommend a standard methodology to quantify the pulsating power loss.

Come up with adjustment factor(s) to be applied to the mean pressure drop coefficient (K) in the presence of pulsating flow.

Completed 2013

Focus of this presentation

10 GMC Nashville Oct 5-8, 2014

Outline

1. Test Program 2. Measurements and Results 3. Key Findings 4. Next Steps

11 GMC Nashville Oct 5-8, 2014

Test Setup at TCPL’s GDTF in Didsbury, Alberta

Pipeline quality gas

Nozzle Bank

12 GMC Nashville Oct 5-8, 2014

Pulse Generator

Pulsations will be created by a hydraulically driven rotating paddle • Not a recip compressor • Operate at 300 to 1200

rpm. • Double acting • Pulse amplitude 1% to 2%

line pressure

13 GMC Nashville Oct 5-8, 2014

Test Setup Details

Configuration A: Bottle Upstream, Orifice Downstream

Configuration B: Orifice Upstream, Bottle Downstream

14 GMC Nashville Oct 5-8, 2014

Custom Bottle Design (donated by Peerless Mfg.)

15 GMC Nashville Oct 5-8, 2014

End Treatments

2” x 3”Diffuser

Taper

Normal (Square)

16 GMC Nashville Oct 5-8, 2014

Square End Treatment

17 GMC Nashville Oct 5-8, 2014

Diffuser End Treatment

18 GMC Nashville Oct 5-8, 2014

Photos of Configuration A Setup

19 GMC Nashville Oct 5-8, 2014

Sonic Nozzles Bank

Pulse Generator

20 GMC Nashville Oct 5-8, 2014

Static P & T Transducers (Upstream)

Pair of Dynamic P Transducers (1.5 m apart)

Kulite P Transducers

21 GMC Nashville Oct 5-8, 2014

Pair of Dynamic P Transducers (1.5 m apart)

Kulite P Transducers

22 GMC Nashville Oct 5-8, 2014

Rosemount Differential P Transducer

23 GMC Nashville Oct 5-8, 2014

Pair of Dynamic P Transducers (1.5 m apart)

Rosemount Differential P Transducer

24 GMC Nashville Oct 5-8, 2014

Pair of Dynamic P Transducers (1.5 m apart)

Kulite P Transducers

Static P & T Transducers (Downstream)

25 GMC Nashville Oct 5-8, 2014

Photos of Configuration B Setup

26 GMC Nashville Oct 5-8, 2014

27 GMC Nashville Oct 5-8, 2014

28 GMC Nashville Oct 5-8, 2014

Taper Diffuser

Β = 0.5

Β = 0.7

29 GMC Nashville Oct 5-8, 2014

Example of Pulsating Pressure Measurements (Across the Bottle)

-90

-60

-30

0

30

60

90

0 50 100 150 200 250

Pre

ssu

re O

scill

ati

on

(k

Pa

)

PT1

-90

-60

-30

0

30

60

90

0 50 100 150 200 250

Pre

ssu

re O

scill

ati

on

(k

Pa

)

PT2

-90

-60

-30

0

30

60

90

0 50 100 150 200 250

Pre

ssu

re O

scill

ati

on

(k

Pa

)

PT3

-90

-60

-30

0

30

60

90

0 50 100 150 200 250

Pre

ssu

re O

scill

ati

on

(k

Pa

)

Time (ms)

PT4

0

0

0

1

10

100

0 10 20 30 40 50 60 70 80 90 100 110 120

Pre

ssu

re A

mp

litu

de

(k

Pa

)

PT1PT1

0

0

0

1

10

100

0 10 20 30 40 50 60 70 80 90 100 110 120

Pre

ssu

re A

mp

litu

de

(k

Pa

)

PT2

0

0

0

1

10

100

0 10 20 30 40 50 60 70 80 90 100 110 120

Pre

ssu

re A

mp

litu

de

(k

Pa

)

PT3

0

0

0

1

10

100

0 10 20 30 40 50 60 70 80 90 100 110 120

Pre

ssu

re A

mp

litu

de

(k

Pa

)

Frequency (Hz)

PT4

30 GMC Nashville Oct 5-8, 2014

Example of 1st Harmonic Mapping (Configuration A)

kk uandP

0.00.51.01.52.02.53.03.54.04.55.05.56.06.57.07.58.0

0

10

20

30

40

50

60

70

80

90

100

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18

Velo

city

Am

plitu

de (m

/s)

Pres

sure

Am

plitu

de (k

Pa)

Distance From Upstream 8"/4" Reducer (m)

Pressure Amplitude (kPa)Velocity Amplitude (m/s)

Puls

atio

n Bo

ttle

OrificeP. Gen.

Test 27(40.5 Hz,

6 Nozzles, 0.5 Beta)

Acoustic Power= 0.2W

Acoustic Power= 334W

Acoustic Power= 380W

Acoustic Power=229W

31 GMC Nashville Oct 5-8, 2014

Example of 1st Harmonic Mapping (Configuration B)

kk uandP

0.00.51.01.52.02.53.03.54.04.55.05.56.06.57.07.58.0

0

10

20

30

40

50

60

70

80

90

100

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18

Velo

city

Am

plitu

de (m

/s)

Pres

sure

Am

plitu

de (k

Pa)

Distance From Upstream 8"/4" Reducer (m)

Pressure Amplitude (kPa)Velocity Amplitude (m/s)

Puls

atio

n Bo

ttle

Orifice

P. Gen.

Test 209(15.875 Hz,

6 Nozzles, 0.5 Beta)

Acoustic Power= 44W

Acoustic Power= 248W

Acoustic Power= 391W

Acoustic Power=100W

32 GMC Nashville Oct 5-8, 2014

Test Results (Configuration A)

33 GMC Nashville Oct 5-8, 2014

Configuration A Test Scope

TestNumber of

Sonic NozzlesEnd Treatments Orifice β Hole(s)

1 3 and 6 Square/Square 1 -

1a 3 and 6 Square/Square 0.5 Single

1b 3 and 6 Square/Square 0.5 Multiple

1c 3 and 6 Square/Square 0.7 Single

1d 3 and 6 Square/Square 0.7 Multiple

2 3 and 6 Square/Diffuser 0.5 Single

3 3 and 6 Taper/Diffuser 0.5 Single

4 3 and 6 Taper/Square 0.5 Single

4a High flow Taper/Square O.7 Single

Configuration A Test Scope

For each of the sub-configuration and flow rate, a total of 10 tests were conducted at the following frequencies: 0, 11, 13, 15, 17, 22, 27, 31, 35, and 41 Hz. (Total for Configuration A = 180 Tests).

34 GMC Nashville Oct 5-8, 2014

Normalized Pulsating Power Loss (Bottle)

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0 0.2 0.4 0.6 0.8 1 1.2 1.4

Nor

mal

ized

Puls

atio

n Po

wer

Los

s (W

P/ρc

Aurm

s2 )

Normalized Velocity Oscillation at Bottle Flange or Orifice Plate (urms/U)

Square/Square Orifice, Beta = 0.5, Single Hole

Square/Square Orifice, Beta = 0.5, Multiple Holes

Square/Square Orifice, Beta = 0.7, Single Hole

Square/Square Orifice, Beta = 0.7, Multiple Holes

Square/Square No Orifice

Square/Diffuser Orifice, Beta = 0.5, Single Hole

Taper/Square Orifice, Beta = 0.5, Single Hole

Taper/Diffuser Orifice, Beta = 0.5, Single Hole

Configuration A:Bottle

TGP St54 (Original Bottles)

TGP St54 (New Bottles)

35 GMC Nashville Oct 5-8, 2014

Normalized Velocity Oscillation urms/U

TGP Station 54: 8350 HP compressor, 6 throw • urms/U=0.7-1.3

Gathering compressor: 1775 HP, 4 throw • urms/U=0.75

Vapour Recovery Compressor: 1200 HP, 6 throw • urms/U=0.4

Test Setup: Hydraulic driven rotating paddle, 2 HP urms/U=0.3 max

Current test setup representative of lower power/throw applications. Pulse Generator modifications could generate urms/U=0.6

36 GMC Nashville Oct 5-8, 2014

Normalized Pulsating Power Loss (Orifice)

0

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

0 0.1 0.2 0.3

Nor

mal

ized

Puls

atio

n Po

wer

Los

s (W

P/ρ c

Aurm

s2 )

Normalized Velocity Oscillation at Bottle Flange or Orifice Plate (urms/U)

Square/Square Orifice, Beta = 0.5, Single Hole

Square/Square Orifice, Beta = 0.5, Multiple Holes

Square/Square Orifice, Beta = 0.7, Single Hole

Square/Square Orifice, Beta = 0.7, Multiple Holes

Square/Diffuser Orifice, Beta = 0.5, Single Hole

Taper/Square Orifice, Beta = 0.5, Single Hole

Taper/Diffuser Orifice, Beta = 0.5, Single Hole

Configuration A:Orifices

Beta = 0.5

Beta = 0.7

37 GMC Nashville Oct 5-8, 2014

10

12

14

16

18

20

22

24

26

28

30

0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4

Mea

n Fl

ow P

ress

ure

Loss

Coe

ffici

ent,

K

Normalized Velocity Oscillation at Bottle Flange or Orifice Plate (urms/U)

Square/Square Orifice, Beta = 0.5, Single HoleSquare/Square Orifice, Beta = 0.5, Multiple HolesSquare/Square Orifice, Beta = 0.7, Single HoleSquare/Square Orifice, Beta = 0.7, Multiple HolesSquare/Square No OrificeSquare/Diffuser Orifice, Beta = 0.5, Single HoleTaper/Square Orifice, Beta = 0.5, Single HoleTaper/Diffuser Orifice, Beta = 0.5, Single Hole

Configuration A:Bottle

Normalized Mean Flow Pressure Loss Coefficient (Bottle) – zoomed in

38 GMC Nashville Oct 5-8, 2014

Theoretical K Factor for the Bottle with Square End Treatments

K1

K2 K3

K4

K5

NPS 4, ID (d2) 4.026 in

Choke Tube ID (d1) 1.939 in

Vessel ID (D) 14.29 in

Choke tube (L) 26 in

Element Local K-FactorK-Factor

(Ref NPS4)

Entrance to Bottle, K1 0.85 0.85

Emtrance to Choke Tube (square), K2 0.49 9.11

Choke Tube (f=0.014), K3 0.19 3.49

Choke Tube Exit (square), K4 1.00 18.59

Entrance from Bottle to NPS4, K5 0.42 0.42

Sum (Overall K) 32.45

Measured K Factor 25

Bottle Theoretical K Coefficient

K is 21% lower than expected. Why?

39 GMC Nashville Oct 5-8, 2014

Thoughts about why the Measured K Factor for the Bottle is Lower than Theoretical Value

Flow

40 GMC Nashville Oct 5-8, 2014

Quasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating Flow

0

5

10

15

20

25

30

0

50

100

150

200

250

300

350

0 0.01 0.02 0.03 0.04

Velo

city

(m/s

)

Pres

sure

Dro

p (k

Pa)

Time (s)

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

41 GMC Nashville Oct 5-8, 2014

Quasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating Flow

0

5

10

15

20

25

30

0

50

100

150

200

250

300

350

0 0.01 0.02 0.03 0.04

Velo

city

(m/s

)

Pres

sure

Dro

p (k

Pa)

Time (s)

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

42 GMC Nashville Oct 5-8, 2014

Quasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating Flow

0

5

10

15

20

25

30

0

50

100

150

200

250

300

350

0 0.01 0.02 0.03 0.04

Velo

city

(m/s

)

Pres

sure

Dro

p (k

Pa)

Time (s)

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

op

43 GMC Nashville Oct 5-8, 2014

Quasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating Flow

0

5

10

15

20

25

30

0

50

100

150

200

250

300

350

0 0.01 0.02 0.03 0.04

Velo

city

(m/s

)

Pres

sure

Dro

p (k

Pa)

Time (s)

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

Mean Pressure DropWith Pulsation)

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

44 GMC Nashville Oct 5-8, 2014

Quasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating Flow

0

5

10

15

20

25

30

0

50

100

150

200

250

300

350

0 0.01 0.02 0.03 0.04

Velo

city

(m/s

)

Pres

sure

Dro

p (k

Pa)

Time (s)

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

Mean Pressure DropWith Pulsation)

Freq (Hz) 27Omega (rad/s) 169.646T (s) 0.037037U (m/s) 16K 25Density (kg/m3) 40Mean DP, no pulsation (kPa) 128

op

y = x2 + 1

1

1.05

1.1

1.15

1.2

1.25

1.3

1.35

1.4

1.45

1.5

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8

K effe

ctiv

e/

K no-

puls

atio

n

urms/U

45 GMC Nashville Oct 5-8, 2014

0.95

1

1.05

1.1

1.15

1.2

0 0.1 0.2 0.3 0.4

K effe

ctiv

e/

K no-

puls

atio

n

urms/U

Quasi-Steady Pressure Drop Relationship

Square/Square

Square/Diffuser

Taper/Square

Taper/Diffuser

Current Measurements of Mean Flow Pressure Loss Coefficient (Representative of Suction Bottle)

46 GMC Nashville Oct 5-8, 2014

Normalized Mean Flow Pressure Loss Coefficient (Orifice) – Referenced to NPS4

0

5

10

15

20

25

30

35

40

45

0 0.1 0.2 0.3

Mea

n Fl

ow P

ress

ure

Loss

Coe

ffici

ent,

K

Normalized Velocity Oscillation at Bottle Flange or Orifice Plate (urms/U)

Square/Square Orifice, Beta = 0.5, Single Hole

Square/Square Orifice, Beta = 0.5, Multiple Holes

Square/Square Orifice, Beta = 0.7, Single Hole

Square/Square Orifice, Beta = 0.7, Multiple Holes

Square/Diffuser Orifice, Beta = 0.5, Single Hole

Taper/Square Orifice, Beta = 0.5, Single Hole

Taper/Diffuser Orifice, Beta = 0.5, Single Hole

Configuration A:Orifices

Ktheoretical (for β = 0.5) = 29.7

Ktheoretical (for β = 0.7) = 4.3

47 GMC Nashville Oct 5-8, 2014

Test Results (Configuration B)

48 GMC Nashville Oct 5-8, 2014

Configuration B Test Scope

For each of the sub-configuration and flow rate, a total of 10 tests were conducted at the following frequencies: 0, 11, 13, 15, 17, 22, 27, 31, 35, and 41 Hz. (Total for Configuration B = 160 Tests)

TestNumber of

Sonic NozzlesEnd Treatments Orifice β Hole(s)

1 3 and 6 Square/Square 1 -

1a 3 and 6 Square/Square 0.5 Single

1b 3 and 6 Square/Square 0.5 Multiple

1c 3 and 6 Square/Square 0.7 Single

1d 3 and 6 Square/Square 0.7 Multiple

2 3 and 6 Square/Diffuser 0.5 Single

3 3 and 6 Taper/Diffuser 0.5 Single

4 3 and 6 Taper/Square 0.5 Single

Configuration B Test Scope

49 GMC Nashville Oct 5-8, 2014

Normalized Pulsating Power Loss (Bottle)

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0 0.2 0.4 0.6 0.8 1 1.2 1.4

Nor

mal

ized

Puls

atio

n Po

wer

Los

s (W

P/ρc

Aurm

s2 )

Normalized Velocity Oscillation at Bottle Flange or Orifice Plate (urms/U)

Square/Square Orifice, Beta = 0.5, Single Hole

Square/Square Orifice, Beta = 0.5, Multihole

Square/Square Orifice, Beta = 0.7, Single Hole

Square/Square Orifice, Beta = 0.7, Multihole

Square/Diffuser Orifice, Beta = 0.5, Single Hole

Taper/Square Orifice, Beta = 0.5, Single Hole

Taper/Diffuser Orifice, Beta = 0.5, Single Hole

Configuration B:Bottle

TGP St54 (Original Bottles)

TGP St54 (New Bottles)

50 GMC Nashville Oct 5-8, 2014

Current Measurements of Mean Flow Pressure Loss Coefficient (Representative of Discharge Bottle)

0.95

1

1.05

1.1

1.15

1.2

0 0.1 0.2 0.3 0.4

K effe

ctiv

e/

K no-

puls

atio

n

urms/U

Quasi-Steady Pressure Drop Relationship

Square/Square

Square/Diffuser

Taper/Square

Taper/Diffuser

51 GMC Nashville Oct 5-8, 2014

Summary of Site Testing

1. Methodology: Successful in validating the Flow Energy (acoustic power) methodology developed in Phase I.

2. Bottle: Differences measured between the bottle loss factor in steady flow and fluctuating flow as compared to published data. A 21% difference for steady flow, 5% for fluctuating flow in the test rig.

3. Orifice: Loss factor for single hole vs multi hole agreed well with published data. Some divergence at maximum test frequency of 41 Hz. Additional testing to investigate higher frequencies.

4. Pulse Generator: could create sufficient pressure fluctuations (2% of line) but flow fluctuations were lower than high power compressor cylinder (urms/U <0.3).

52 GMC Nashville Oct 5-8, 2014

2014 Project Plan

Task Status

Field Test - Design test rig - Fabricate and Install - Execute Test Plan - Data Analysis

Testing completed July 25 Data review and analysis 95% completed.

Report Complete by end of 2014

Optional Scope: Testing on reciprocating compressor facility

Need a site: TGP Stn 54, lots of information from Phase 1. Other site possible. Design test: - Fluctuation flow measurement - Compressor performance (P-V curves) and

power measurements (torque, motor power)

53 GMC Nashville Oct 5-8, 2014

Suggestions for Future Work

Addition testing proposed at the TCPL site. Redesign of pulse generator or test rig required to create high flow fluctuations. CFD analysis of components.

4 possible journal publications resulting from the work completed.

54 GMC Nashville Oct 5-8, 2014

Thank You and Acknowledgements

GMRC for Funding the Research Program PSC Oversight committee Peerless Mfg. (Dave Breindel) for fabricating and donating the

Custom Bottle Design used in the present testing program. TCPL (Thomas Robinson) for the in-kind contribution of the use

of the GDTF in Didsbury, Canada. The following individuals for assisting in conducting the tests

and data analysis: ₋ Matthew Kindree, Alex Mantey (NRTC) ₋ Bill Eckert, Mark DuBois, Mehdi Arjmand (Beta)

Predicting the Power Loss of Reciprocating Compressor Manifolds

NOVA Research: Kamal K. Botros John Geerligs

Beta Machinery: Kelly Eberle Brian Howes Gordon Sun Russ Barss Bryan Long

TransCanada: Thomas Robinson Peerless Mfg: Dave Breindel

PSC: Martin Hinchliff - chair Rainer Kurz Christine Scrivner Steve O’toole Clint Lingel

Project Team: