Upload
marylou-garrett
View
215
Download
1
Tags:
Embed Size (px)
Citation preview
Optical Sensing Systems
Gisle Vold
Slide 2© 2006 Weatherford. All rights reserved.
1870 : Principle of Total Internal Reflection discovered
1950 : Invention of first laser
1970 : First low-loss fibre produced
1974 : Launch of optical communications
1986 : Introduction of optical amplifiers
1994 : Introduction of multi-wavelength systems
2000 : Peak of Telecom bubble
History
Slide 3© 2006 Weatherford. All rights reserved.
Transmission Data Rate and Capacity
• Broadband capability of optical fiber allows multiple channel transmission
– Currently 128 channels with existing components
– Each channel can carry 10Gb/s
– Unlike electrical signals, optical signals do not interfere with each other
• Each Fiber has an aggregate data rate of 1.28Tb/s = 1,280,000,000,000 bps !
• This translates to:
– 20 million simultaneous phone connections (64kb/s each); typical telecom twisted-pair cable 300 phone calls
3
Twisted Pair Copper- MHz - 300 Phone Calls
Single Fiber - THz - Over 20 Million Phone Calls
Slide 4© 2006 Weatherford. All rights reserved.
Bandwidth !
Slide 5© 2006 Weatherford. All rights reserved.
What makes us different ?
• Operation Principle
• Suite of Sensors
• Extreme Long Term Stability
• Unmatched Durability
Slide 6© 2006 Weatherford. All rights reserved.
Bragg Grating Operating Principle
Input SpectrumInput Spectrum
P
Transmitted SpectrumTransmitted Spectrum
P
Slide 7© 2006 Weatherford. All rights reserved.
Bragg Grating Operating Principle
UV interference
UV laserbeams
photo-inscribedgrating in core
Slide 8© 2006 Weatherford. All rights reserved.
Bragg Grating Operating Principle
Reflectedcomponent
Transmittedlight
Input SpectrumInput Spectrum
P
Transmitted SpectrumTransmitted Spectrum
P
B
Reflected SpectrumReflected Spectrum
P
B
Slide 9© 2006 Weatherford. All rights reserved.
Bragg Grating Operating Principle
stretch
Strain-inducedshift in grating
resonance wavelength
Slide 10© 2006 Weatherford. All rights reserved.
Reflectedcomponent
Transmittedlight
Input SpectrumInput Spectrum
P
Transmitted SpectrumTransmitted Spectrum
P
B
Reflected SpectrumReflected Spectrum
Pstrain-induced
shift
B
Bragg Grating Operating Principle
Slide 11© 2006 Weatherford. All rights reserved.
-5
-4
-3
-2
-1
0
1
2
0 2 4 6 8 10 12 14
Time (au)
Re
lati
ve
In
ten
sit
y
Optical Wave 1
Optical Wave 2
Interference of 1 + 2
Interference of Two Optical Waves
Slide 12© 2006 Weatherford. All rights reserved.
-1.5
-1
-0.5
0
0.5
1
1.5
0 2 4 6 8 10 12 14
Time (au)
Re
lati
ve
In
ten
sit
y
-2.5
-1.5
-0.5
0.5
1.5
2.5
Interference of Two Optical Waves
Slide 13© 2006 Weatherford. All rights reserved.
-1.5
-1
-0.5
0
0.5
1
1.5
0 2 4 6 8 10 12 14
Time (au)
Re
lati
ve
In
ten
sit
y
-2.5
-1.5
-0.5
0.5
1.5
2.5
Interference of Two Optical Waves
Slide 14© 2006 Weatherford. All rights reserved.
-1.5
-1
-0.5
0
0.5
1
1.5
0 2 4 6 8 10 12 14
Time (au)
Re
lati
ve
In
ten
sit
y
-2.5
-1.5
-0.5
0.5
1.5
2.5
Interference of Two Optical Waves
Slide 15© 2006 Weatherford. All rights reserved.
-1.5
-1
-0.5
0
0.5
1
1.5
0 2 4 6 8 10 12 14
Time (au)
Re
lati
ve
In
ten
sit
y
-2.5
-1.5
-0.5
0.5
1.5
2.5
Interference of Two Optical Waves
Slide 16© 2006 Weatherford. All rights reserved.
Path 1
Path 2
=2**n*L
=2**n*L
L2-L1
Bulk-Optic Michelson Interferometer
Slide 17© 2006 Weatherford. All rights reserved.
Mirrors
Two Legs with Mirrors
Fiber Michelson Interferometer
Slide 18© 2006 Weatherford. All rights reserved.
Single Leg with Grating Reflectors
Fiber Michelson Interferometer
Slide 19© 2006 Weatherford. All rights reserved.
What makes us different ?
• Operation Principle
• Suite of Sensors
• Extreme Long Term Stability
• Unmatched Durability
Slide 20© 2006 Weatherford. All rights reserved.
The Case for Fiber Optic Sensors
• High Reliability
– No Downhole Electronics
– No Moving Parts
– Nominal Part Count
• Ideally Suited For Harsh Environments
– High Temperature Capability
– Vibration and Shock Tolerant
• High Data Transmission Capability
– Multiple Sensors on Common Fiber Infrastructure
– Technological Advances Driven by Telecom
Slide 21© 2006 Weatherford. All rights reserved.
Downhole Cable
Slide 22© 2006 Weatherford. All rights reserved.
Temperature Profiling
• Thermal profile of well
• Production and injection profiling
• Identify well problems
• Monitor water, gas, steam breakthrough
• Artificial lift monitoring
• Distributed Temperature Sensing (DTS) and Array Temperature Sensing (ATS)
0
400
800
1200
1600
2000
2400
2800
3200
0 20 40 60 80 100 120
Temperature
Perforated Interval
Distributed Sensor
Continuous Sensor
Distributed Sensor
Continuous Sensor
Quasi-Distributed Sensor
Array Temperature Sensor
Quasi-Distributed Sensor
Array Temperature Sensor
Slide 23© 2006 Weatherford. All rights reserved.
DTS - Operation Principle
Spectrometer
Laser
source
Processing
Spectral
Processing
T(z)
Fiber
T
e
m
p
e
r
a
t
u
r
e
P
r
o
f
i
l
e
T(z)
Scattered light at location z
Pulse
Modulator
Raman Stokes/Anti-Stoke Ratio
Surface Unit
Slide 24© 2006 Weatherford. All rights reserved.
Raman StokesAnti-Stokes ratio
DTS – measurement principle
Slide 25© 2006 Weatherford. All rights reserved.
Array Temperature Sensing
• Accurate/stable point measurements– 15-18 points/fiber– P/T gauge can be deployed on same
fiber• 1 P/T + 12 ATS
– <0.01°C (0.018°C) temperature resolution
– Update rate 3 – 5 seconds• Similar technology to Weatherford optical
P/T gauge– Glass microstructure– Manufactured by Weatherford– Integrated into standard ¼” Inc 825,
3-fiber cable• Temperature sensor isolated from strain• Standard deployment techniques
– Location of sensors needs to be defined in advance of installation
• Same instrument as optical P/T gauge (platform or subsea)
• Long distance (>30km) reach• Field trials planned for 2006 (land) and
2007 (subsea)
Leveraging Existing Technology
Array Temperature Sensor
Slide 26© 2006 Weatherford. All rights reserved.
Build model to evaluate DTS sensitivities to :
• total flow rate
• oil, gas and water profile differences
• flow allocation
• water breakthrough
• gas coning
• pressure drawdown
Specific input required from customer
Simulation of well candidates
Slide 27© 2006 Weatherford. All rights reserved.
• WFT-PLATO software
– Three-phase PLT analysis
– Statistical optimization
– Global statistical modeling of entire well
– Automatic determination of flow regime
– Interactive visualization
– Simultaneous use of all logs and surface information to determine production profile
– Emulation capabilities
• Temperature Profiling Design & Analysis
– Warm-back tests for injectors
– Specialized tests for producers
– Temperature array array design
– Service
– Software
WFT Temperature Profiling Analysis Capabilities
Slide 28© 2006 Weatherford. All rights reserved.
Temperature Profiling Data Viewer
• Standalone application for viewing DTS data
• SQL Database, LAS, POSC, ASCII format files
• Features
– Animations relative to baseline DTS data
– User-specified data interval density (in time)
– User-settable zooming, scaling, gridding, scrolling, smoothing, etc.
• Intended users
– Operators – for quick qualitative analysis
– Production and reservoir engineers – for identifying trends and visualizing specialized tests, e.g., warmback tests in injection wells
Slide 29© 2006 Weatherford. All rights reserved.
Why Measure Flow Downhole
• Reduce surface facilities and well tests
– Eliminates the need for test separator
– Handling of high gas rates
– Favorable measurement conditions
• Allocation from/to multiple zones
– Production and Injection well applications
– In multi-zone and multi-lateral completions
• Commingling
– Regulatory requirements
• Faster identification of production anomalies
Slide 30© 2006 Weatherford. All rights reserved.
Weatherford’s Optical Flowmeter
• Measurements
– Flow velocity (gives volumetric flow rate)
– Speed of sound (gives gas volume fraction)
• Measurement Advantages
– Liquid, gas, or multiphase
– High accuracy:
• single-phase ±1%
• multiphase ±5%
– Zero drift
– Bi-directional flow rate
– High turndown ratio, scalable to any pipe size
Turndown Ratio is the ratio of the highest to the lowest measurable flow rate
Turndown Ratio is the ratio of the highest to the lowest measurable flow rate
Slide 31© 2006 Weatherford. All rights reserved.
Weatherford’s Clarion™ In-Well Seismic System
• High Performance– Broad bandwidth, high sensitivity and
wide dynamic range
• Optical Seismic Sensors– 3-component accelerometer
– hydrophone (prototype only)
• Standard Weatherford optical backbone
– Combines with optical PT, DTS & Flowmeter
• Dry tree solutions available
– Subsea under development
ALL OPTICAL SYSTEM
LIFE OF FIELD RELIABILITY
Life of Well Seismic™
Slide 32© 2006 Weatherford. All rights reserved.
RUGGEDIZEDSENSOR CARRIER
3-C SENSOR
Clarion™ Deployment in Production/Injection Wells
ARRAY SPOOLING UNIT
SENSORMANDREL
Tubing or casing conveyed
Slide 33© 2006 Weatherford. All rights reserved.
Weatherford’s Clarion™ In-Well Seismic System
Geophysicists (benefit)
• Permanent Measurement Repeatability
• Real time on demand seismic data
• Passive event gathering
• Active Seismic event Gathering
• Calibration of Seabed Sensors
• Intended Wellbore viewing
• High resolution Imaging in 4D Timeline
• Geometry understanding
• Inversion – Porosity/ Resistivity
• Fluid Movement understanding
• Fracture Delineation
• Bypass Pay
• Cap Rock Integrity
Slide 34© 2006 Weatherford. All rights reserved.
Weatherford’s Clarion™ In-Well Seismic System
Reservoir Engineers (Benefit)
• Available with P/T, Flow and DTS systems
• Material Balance help
• Formation Activity
• Fracture Tracing
• Cross Flow
• Well Balance when shut in
• Reservoir Loss path
• Reservoir Boundaries
• Injection performance
• Interference Test greater understanding
• Uncertainty reduction
Slide 35© 2006 Weatherford. All rights reserved.
Weatherford’s Clarion™ In-Well Seismic System
• Drilling Engineer (Benefit)
• Infill well placement
• Real time seismic while drilling
• Look ahead Drilling
• Production Engineer (Benefit)
• Stimulation
Slide 36© 2006 Weatherford. All rights reserved.
1990’s DTS installations
1993 First In-well Optical P/T Gauge
1996 First Subsea Optical P/T Gauge
1999 First In-well Bragg Grating P/T Gauge
1999 First In-well Seismic Accelerometer
2000 First Non-intrusive In-well Fiber Optic Flowmeter
2001 Optical P/T Gauge and DTS in Single Completion
2002 Multiple Optical P/T Gauges in Single Completion
2003 Full 3-phase Fiber Optic Flowmeter with P/T Gauges
2003 Multi-zone Optical P/T Gauges and Remote Flow Control
2004 Multi-zone Optical P/T Gauges and Flowmeters with Remote Flow Control
2004 Casing-conveyed, Multi-station, Seismic with P/T Gauge
2005 Multiple Optical P/T Gauges and DTS Integrated with Sand Control
2006 Offshore Tubing-conveyed, Multi-station, Seismic with P/T Gauge
In-Well Optical Sensing Chronology
WORLD-FIRST DOWNHOLE FIBER OPTIC INSTALLATIONS: