2019 TRC-B&C-02-19 MEASUREMENTS TO QUANTIFY THE EFFECT OF A - - PowerPoint PPT Presentation

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Interim May Report 2019 TRC-B&C-02-19 MEASUREMENTS TO QUANTIFY THE EFFECT OF A REDUCED FLOW RATE ON TILTING PAD JOURNAL BEARING PERFORMANCE STATIC AND DYNAMIC Dr. Luis San Andrs Jon Toner Graduate Research Assistant Mast-Childs


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SLIDE 1

MEASUREMENTS TO QUANTIFY THE EFFECT OF A REDUCED FLOW RATE ON TILTING PAD JOURNAL BEARING PERFORMANCE – STATIC AND DYNAMIC

  • Dr. Luis San Andrés

Mast-Childs Chair Professor

Jon Toner

Graduate Research Assistant

Interim Report

TRC-B&C-02-19

1

May 2019

TEES Project # 28-258124-00135

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SLIDE 2

TRC interest

how low is a low flow rate enough to maintain reliability (and energy efficient) TPJB

  • peration ?

2

Reduction in flow rate  reduction in drag power loss and more efficiency, though with increased pad temperatures & drop in damping. Savings in pumping and lubricant storage make the case for low flow…

Too low

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SLIDE 3

Objective and tasks

  • To quantify the effects of lubricant flowrate on

tilting pad bearing performance:

  • Drag power & load capacity
  • Pad metal temperatures
  • Force coefficients (K, C, M)

Prior art

[1] Decamillo, S., Brockwell, K., 2001 “A Study of Parameters That Affect Pivoted Shoe Journal Bearing Performance in High-Speed Turbomachinery”, Proc. TPS, Texas A&M. [2] Dmochowski, W. M., Blair, B., 2006, “Effect of Oil Evacuation on the Static and Dynamic Properties of Tilting Pad Journal Bearings”, Trib. Trans., 49. [3] Nichols, B., 2017, “Experimental Measurements and Modeling of Tilting-Pad Bearing Performance and System Stability Under Reduced Oil Supply Flow Rates”, Thesis, UVA.

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SLIDE 4

Test Rig

4

Legacy of D. Childs & students

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SLIDE 5

Test Rig Features

Test-Rig Capabilities

  • Max. rotor speed

16 kRPM

  • Max. applied static load

20 kN

  • Max. measurable torque

100 Nm

  • Max. supply oil flow rate

~20 GPM Available shaft OD sizes 3.5”, 4”, 4.5”

  • Max. bearing length

3.5” 5

Strain gage torquemeter & coupling directly measures drag torque. Floating bearing on rigid rotor.

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SLIDE 6
  • Pneumatic cylinder applies static load.
  • Pair of hydraulic actuators deliver

dynamic loads via stingers.

Test Rig Load Devices

Pneumatic Cylinder Hydraulic Actuator

6

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SLIDE 7

Test Bearing

7

TL bearing tested by Coghlan (D. Childs team) in 2015-ff

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SLIDE 8

L/D

0.6

Shaft diameter

4.0 in (101 mm)

Length

2.4 in (61 mm)

B radial cold clearance

4.52 mil (0.115 mm)

hot clearance (6 & 12 krpm)

4.20 mil (0.106 mm)

Design pad preload

0.3

Spherical Pivot Offset

0.5

Pad Arc Length (°)

72°

AISI 1018 Pad Thickness

0.75 in

Babbitted pad surface Lubrication condition

Single Orifice b/w pads,

Flooded (with end seals)

Test bearing – load between pads

8

Thermocouples in pad and in oil supply outer annulus

ISO VG46 oil at 60C 16.4 cPoise & 837 kg/m3

Applied Load, W

2,135, 6,405, 12,810 N

Specific Load, W/(LD)

345, 1,034, 2,068 kPa  303 psi

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SLIDE 9

4 8 12 16 10 20 30 40 50

Shaft speed (rpm) Flow rate (LPM)

6 12

*

flow rate ~ shaft speed

Np = number of pads Ω = shaft speed (rad/s) D = shaft diameter (m) L = bearing axial length (m) Cr = bearing radial clearance (m) l = hot-oil carry over coefficient.

Oil supplied flow rate - theory

Nominal (100%) 150% 50% Low  rotor speed (krpm)  High

9

Tests at two shaft speeds

1. 6 krpm (32 m/s) 2. 12 krpm (64 m/s surface speed)

Q =Np ½ ( ½ W D) L Cr (1- l) VARY Flow from 150%  100% (nominal)  20% or less (if safe)

~14. 4 LPM ~28.8 4 LPM

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SLIDE 10

Test Results

10

Load between pads (LBP) 2 shaft speeds x 3 static loads

Shaft speed

6 and 12 krpm

Specific Load, W/(LD)

345, 1,034, 2,068 kPa

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SLIDE 11

Eccentricity is nearly parallel to load direction and increases with load and is much smaller as shaft speed doubles. Journal eccentricity increases slightly as flow rate decreases  small impact on film thickness.

Journal locus vs. speed vs. flow

6 kRPM 12 kRPM

L

  • a

d

11

L

  • a

d

eY eX

ISO VG46 inlet T = 60C

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SLIDE 12

Shaft eccentricity vs. flow vs. load

6 kRPM

Flow (LPM) Flow (LPM)

L

  • a

d

12

12 kRPM Eccentricity decreases with shaft speed and increases with load. Journal eccentricity increases slightly as flow rate decreases. (semi-log scale). Low flow does not produce a too small film thickness.

L

  • a

d

Y X e

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SLIDE 13

A very low flow (50% & below) does produce large increase in pad peak temperature. Load and shaft speed have minor effect. Inflection in temperature vs flow due to uneven thermal field in supply annulus (more later).

Maximum (Loaded) pad temperature rise

6 kRPM

Flow (LPM) Flow (LPM)

L

  • a

d

13

12 kRPM

ISO VG46 inlet T = 60C

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SLIDE 14

A low flow (50% or less of nominal) produces a quick temperature rise. Load and shaft speed have negligible effect. Larger than 100% flow rate produces no changes.

Maximum (unloaded) pad temperature rise

6 kRPM 12 kRPM

Flow (LPM) Flow (LPM)

14

ISO VG46 inlet T = 60C

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SLIDE 15

Shaft speed has an effect on exit oil temperature; more so than load. Low flow rates produce a significant oil exit temperature rise. Alarming only for very low flows (20% nominal or less).

Oil exit temperature rise vs. flow vs. speed

12 kRPM

Flow (LPM) Flow (LPM)

15

6 kRPM

ISO VG46 inlet T = 60C

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SLIDE 16

Drag torque drops quickly as flow rate decreases. Twice shaft speed  ~ 2 x drag torque.

Drag torque vs. flow vs. speed

6 kRPM 12 kRPM

Flow (LPM) Flow (LPM)

L

  • a

d

16

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SLIDE 17

Drag power drops quickly as flow rate decreases. Savings of 50% or more in drag power with low flow rate (40% or lower). Overflow (> 100%) increases power consumption (~20%) for

  • peration at 12 krpm (64 m/s).

Drag power vs. flow vs. speed

6 kRPM 12 kRPM

Flow (LPM) Flow (LPM)

L

  • a

d

17

Power = Torque x shaft speed

ISO VG46 inlet T = 60C

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SLIDE 18

Force Coefficients

18

Load between pads (LBP) 2 shaft speeds x 3 static loads

Shaft speed

6 and 12 krpm

Specific Load, W/(LD)

345, 1,034, 2,068 kPa

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SLIDE 19

Procedure for force coefficients identification

Step 1: Apply loads and measure bearing motions

1 1

Re

i t X

F e                 F

2 2

Re

i t Y

e F

             F

1 1 (t) 1 1 (t) i t

x X e y Y

               

1

z

2 2 (t) 2 2 (t) i t

x X e y Y

               

2

z

2

a

1

a

2

[ ]

S

i M       K C M z F a

2

i       H K M C

Record bearing displacement z and acceleration a Apply forces with shakers  pseudo-random frequency EOM: Frequency domain Find parameters:

19 CCW

X Y

X force

CCW

X Y

Y force

ω is a set of frequencies =(1, 2, 3,…, 17) x 9.77 Hz.

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SLIDE 20

Procedure for force coefficients identification

Step 2: Estimate dry structure parameters

2

[ ]

S S S

i      K M C z F

2 S S S S

i       H K M C

20

NO lubricant

Step 3: Bearing force coefficients = Lubricated system – Dry system (K, C, M)bearing = (K, C,M)L – (K, C, M)S

Bearing Test system (Lubricated) Dry structure

L O A D

Y X

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SLIDE 21

Direct stiffness KYY is a function of load more than shaft speed or even flow rate.

Direct stiffness vs. flow rate

6 kRPM 12 kRPM

Flow (LPM) Flow (LPM)

L

  • a

d

21

Y - Load direction ISO VG46 inlet T = 60C

L

  • a

d

Y X

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SLIDE 22

Direct damping CYY decreases as flow rate decreases (all pads starve). Significant drop for lowest load (345 kPa [50 psi])

Direct damping vs. flow rate

6 kRPM 12 kRPM

Flow (LPM) Flow (LPM)

L

  • a

d

22

Y - Load direction

L

  • a

d

Y X Advent of SSV?

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SLIDE 23

Low frequency spectrum (SSV hash) recorded for operation with berry-berry  low flow rates (and small load). SSV “breathed in” and need to be excited.

SSV Subsynchronus vibrations

6.5 kRPM, 345 kPa (50 psi) load, 0.36 LPM (4%)

SSV 1X (108 Hz)

23

L

  • a

d

Y X

100% flow ~ 14.4 LPM

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SLIDE 24

Complete Set of Force Coefficients (X & Y) ….

24

upcoming

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SLIDE 25

Other issues

25

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SLIDE 26

Thermocouples affixed to bearing OD facing feed annulus near inlet

  • rifices.

Inlet Oil Supply Temperature

Gravity Inlet Port

26

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SLIDE 27

For very low oil flow rates supplied  Temperatures around annulus not uniform & unsteady (likely not wetted surface). Difficult to control flow & oil inlet temperature (set 140F).

Temperatures in Oil Supply Annulus

6kRPM, 2068 kPa (300 psi) load

D C B A

3.6 LPM 2.6 LPM 2.1 LPM 2.6 LPM 3.2 LPM Temperature (°F)

Time span = 17 min

250 F 200 F 150 F 120 F set inlet T = 60C= 140F

27

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SLIDE 28

Low flow limit found by reducing oil flowrate at a constant rotor speed and specific load until:

  • 1) Pad Temperature exceeds 121C (250F) or
  • 2) SSV vibration appears
  • 3) Inlet temperature below target 60°C and/or annulus temperatures

not uniform  Cannot maintain control flowrate and/or oil inlet temperature)

Results of Low Flow Limit Tests

Limit of Low Oil Supply

Load Flow Limit

6 kRPM (32 m/s) Flow=14.4 LPM

345 kPa 2% (0.36 LPM) 3 1034 kPa 10% (1.4 LPM) 3 2068 kPa 5% (1 LPM) 1

12 kRPM (64 m/s) Flow=28.8 LPM

345 kPa 15% (4.3 LPM) SSV 1034 kPa 15% (4.3 LPM) 1 2068 kPa 23% (6.8 LPM) 1 28

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SLIDE 29

Reducing flow rate reduces power consumption.

Yet How low is too low?

Results- Low Flow Limit Tests

0.4 LPM 3.8 LPM Recall nominal flow rate at 6 krpm: ~ 14.4 LPM

The minimum flow is application specific but must prevent too large pad/film temperatures to avoid:

  • Babbitt failure
  • Varnishing of pads or (long term) degradation of oil
  • Collapse of load capacity with excessive reduction in

stiffness and damping coefficients

29

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SLIDE 30

Continuation Proposal to TRC

FURTHER MEASUREMENTS TO QUANTIFY THE

EFFECT OF A REDUCED FLOW RATE ON TILTING PAD JOURNAL BEARING PERFORMANCE – STATIC

AND DYNAMIC (LOP & EVACUATED ENDS)

how low is a low flow rate enough for safe (and energy efficient) TPJB

  • peration ?

30

Year II

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SLIDE 31

Tasks - Year II

(a) Install bearing w/o end seals  evacuated configuration (b) Conduct measurements at shaft speed=6 krpm and 12 krpm,

and three static loads (50 psi to 300 psi), and decreasing flow rate to limit determined by (a) excessive pad temperatures (above 250F), or (b) onset and persistence of SSV, (c) inability to control set flow and

  • il

inlet temperature.

 drag torque (power loss), journal eccentricity, oil exit temperature, and pad (sub surface) temperatures. (c) Perform dynamic load measurements  bearing stiffness, damping and virtual mass coefficients. (d) Produce predictions of bearing performance for (flooded & evacuated) TPJBs. (e)Correlate measurements against predictions & write technical report (MS Thesis).

31

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SLIDE 32

Budget 2019-20 (Year II)

Support for graduate student (20 h/week) x $ 2,300 x 12 months

$ 26,400

Fringe benefits (2.4%) and medical insurance ($422) x 12 months

$ 5,698

Tuition & fees three semesters (24 ch) * Legacy student

$ 13,275

Conference travel and registration

$ 1,800

Supplies: bearing parts and rig ancillary parts

$ 2,827

Total BUDGET

$ 50,000 QUANTIFY THE EFFECT OF A REDUCED FLOW RATE ON TILTING PAD JOURNAL BEARING PERFORMANCE – EVACUATED BEARING

32

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SLIDE 33

Questions (?)

QUANTIFY THE EFFECT OF A REDUCED FLOW RATE ON TILTING PAD JOURNAL BEARING PERFORMANCE – STATIC AND DYNAMIC

33

Early Summer 2019: Upcoming Technical Report TRC-B&C-02-19