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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:

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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

  • 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:

    Predicting the Power Loss of Reciprocating Compressor Manifolds Project MotivationCompressor Performance CalculationCompressor Performance CalculationPressure Drop Calculation… easy, right?Challenges to IndustryHow important is power loss?Overall Project ObjectivesOverall Project ObjectivesOutlineTest Setup at TCPL’s GDTF in Didsbury, AlbertaPulse GeneratorTest Setup DetailsCustom Bottle Design (donated by Peerless Mfg.)End TreatmentsSlide Number 16Slide Number 17Photos of Configuration A SetupSlide Number 19Slide Number 20Slide Number 21Slide Number 22Slide Number 23Slide Number 24Photos of Configuration B SetupSlide Number 26Slide Number 27Slide Number 28Example of Pulsating Pressure Measurements (Across the Bottle)Example of 1st Harmonic Mapping�(Configuration A)Example of 1st Harmonic Mapping�(Configuration B)Test Results�(Configuration A)Configuration A Test ScopeNormalized Pulsating Power Loss (Bottle)Normalized Velocity Oscillation urms/UNormalized Pulsating Power Loss (Orifice)Normalized Mean Flow Pressure Loss Coefficient (Bottle) – zoomed inTheoretical K Factor for the Bottle with Square End TreatmentsThoughts about why the Measured K Factor for the Bottle is Lower than Theoretical ValueQuasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating FlowQuasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating FlowQuasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating FlowQuasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating FlowQuasi-Steady Hypothesis of Mean Flow Pressure Drop in the Presence of Pulsating FlowCurrent Measurements of Mean Flow Pressure Loss Coefficient (Representative of Suction Bottle)Normalized Mean Flow Pressure Loss Coefficient (Orifice) – Referenced to NPS4Test Results�(Configuration B)Configuration B Test ScopeNormalized Pulsating Power Loss (Bottle)Current Measurements of Mean Flow Pressure Loss Coefficient (Representative of Discharge Bottle)Summary of Site Testing2014 Project PlanSuggestions for Future WorkThank You and AcknowledgementsPredicting the Power Loss of Reciprocating Compressor Manifolds