los angeles november 10, 2008 api 73 rd fall refining and equipment standards meeting
TRANSCRIPT
Los Angeles November 10, 2008
API 73rd Fall Refining and Equipment Standards Meeting
Combustion Analysis Options for Process Heaters
David Fahle – VP of Marketing Hydrocarbon Processing
ENABLE YOU TO GO FURTHER
precision and expertise
• Industrial Gas
• Hydrocarbon Processing
• OEM Transducers
• Product Support
• Committed to your Success
• Quality Focus
• Process Oxygen
• Photometric
• Combustion
• Laser
• OEM transducers
• Analytical Systems
Experts in Gas Analysis
• Paramagnetic
• Zirconia
• Photometric
• Thick Film
• Tuneable Diode Laser
Markets Products Technology Support
Gas Analysis is what we do - And we do it best
Servomex Proud 50 Year History
• Servomex Controls Limited formed 1952• First paramagnetic cells made based on licence from
Distillers 1961• Bought by Sybron Corporation and integrated into Taylor
Instruments Group 1971 • MBO from Sybron Corporation 1987• Stock market flotation (London Stock Exchange) 1989• Acquired by The Fairey Group 1999• The Fairey Group renamed as Spectris plc 2001
Global PresenceGlobal Presence
Combustion Applications
Index of Applications
Thermal power generation
Incineration
Hydrocarbon Processing
Industrial Gases
Specialty Chemicals and Pharmaceuticals
Cement
Iron and steel
Hydrocarbon Processing
Process HeatersDirect-fired heat exchanger that usesthe hot gases of combustion to raise the temperature of afeed flowing through coils of tubes aligned throughout theheater. Typical temperatures 400°C-550°C (800-1000°F)
Thermal Crackers Heat exchanger where reactions take place while the feedtravels through the tubes, i.e. Ethylene cracking furnace. Typical temperatures 980°C-1200°C (1800-2200°F)
On-site IncineratorsDesigned to combust both solid and liquid chemical waste. The type depends upon the type of waste being disposedand include fluidized bed, multiple hearth and rotating kiln incinerators.Typical temperatures 1100°C (2000°F) or greater.
Application Types Hydrocarbon Processing
Application Types Hydrocarbon Processing
Process Heaters and Thermal Crackers -pipes run inside heating chamber to transfer heat
•Why measure gases during combustion?
•Detecting oxygen rich conditions: O2 measurement
•Detecting fuel rich conditions: CO measurement
•Combustion Analyzer Types
Complete Combustion
CxHy + (x+(y/4))O2 xCO2 + (y/2)H2O + HEAT
FUEL + OXYGEN CARBON DIOXIDE + WATER + HEAT
Combustion:Why measure gases?
0 10 20-10-20
Ideal
CO
O2
FUEL RICH
incomplete combustion
Too little oxygen = some fuel not burnt:
2000ppm excess CO above ideal means 1% extra
fuel cost
%
Combustion Efficiency
% Excess Air
% Excess Air0 10 20-10-20
Ideal
CO
O2
AIR RICH
complete combustion
Too much air
= cooling effect:
1.5% excess oxygen above
ideal means 1% extra fuel cost
FUEL RICH
incomplete combustion
Too little oxygen = some fuel not burnt:
2000ppm excess CO above ideal means 1% extra
fuel cost
%
Combustion Efficiency
NOx
-20 -10 0 10 20
20
16
FUEL RICH AIR RICH
IDEAL
EFFICIENCY
O2
12
8
4
CO
Combustion Efficiency
% Excess Air
Review - Breakthrough Concept
Example 1: Coal data, 10h sample
Typical COe 'Breakthrough' Event - 10 hour data period
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
1400
1500
0 1 2 3 4 5 6 7 8 9 10
Time (hours)
CO
e r
ea
din
g (
pp
m)
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
10.0
O2
Re
ad
ing
(%
)
COe Reading (ppm) O2 Reading (%)
See Detail Zoom
Review - Breakthrough Concept
Example 1: Coal data, 1h
Typical COe 'Breakthrough' Event - 1 hour data period
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
1400
1500
6.0 6.1 6.2 6.3 6.4 6.5 6.6 6.7 6.8 6.9 7.0
Time (hours)
CO
e R
ead
ing
(p
pm
)
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
10.0
O2
Rea
din
g (
%)
COe Reading (ppm) O2 Reading (%)
2. COe 'breakthrough' event. Oxygen level
drops 2% COe level increases
3. Oxygen level returns to 'excess air'. COe reading drops quickly to base level
1. Process stable. Oxygen level controlled at approx 5%. COe at low background levels.
Review - Breakthrough Concept
Example 1: Coal data, 5mins
0
100
200
300
400
500
600
700
800
900
1000
1100
1200
1300
1400
1500
384 385 386 387 388 389 390 391 392 393 394
Time (mins)
CO
e R
ead
ing
(p
pm
)
0.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
10.0
O2
Rea
din
g (
%)
COe Reading (ppm) O2 Reading (%)
Review - Breakthrough Concept
Example 2: Gas data, 3 week sample
0
5
10
15
20
25
0 50 100 150 200 250 300 350 400 450 500
TIME (hours)
Oxy
gen
(%
)
-100
0
100
200
300
400
500
CO
e (p
pm
)
Oxygen (%) AI05005.PV COeq (ppm) AI05041.PV
Review - Breakthrough Concept
Example 2: Gas data, 10h sample
0
5
10
15
20
25
420 421 422 423 424 425 426 427 428 429 430
TIME (Hours)
OX
YG
EN
(%
)
-100
0
100
200
300
400
500
CO
e (
pp
m)
Oxygen (%) AI05005.PV COeq (ppm) AI05041.PV
NOx
-20 -10 0 10 20
20
16
FUEL RICH AIR RICH
IDEAL
EFFICIENCY
O2
12
8
4
CO
Combustion Efficiency
% Excess Air
How can oxygen be measured?
Paramagnetic• High accuracy• Need extractive sample system with moisture removed
“Zirconia” (zirconium oxide, ZrO2) based analysers
• Suitable accuracy, measure hot and wet• Fast analysis, low maintenance and low cost
Tuneable Diode Laser• In-situ analysis• Hot, corrosive, particulate latent samples
Combustion Control: O2 Measurement Detecting air rich conditions
Paramagnetic Paramagnetic TechnologyTechnology
Combustion Control: O2 Measurement Detecting air rich conditions
Oxygen is unique.
It is strongly attracted
into a magnetic field.
It is described as being “ paramagnetic ”
O2
O2
O2
O2
O2
O2
O2
O2
O2
O2
O2
O2O2
O2
O2
O2
CO
COCO2 CO2
SO2 HCl HCl
N2
NO NO
N2
O2
O2
COCOCO2 CO2
SO2 SO2
HCl N2
NO2 NO2 NO2
O2
O2
O2
COCO
CO2 CO2
SO2 SO2
HCl N2
Paramagnetic Cell
Magnet pole pieces
Nitrogen filled spheres
Feed back coil
Suspension & mirror
LED source
Photocell sensor
Paramagnetic Technology Provides:Performance
• Fast response
• Exceptional linearity and repeatability
• High stability & accuracy
Economics• Long operational life
• Extractive sample system required
• Simple validation / calibration
Combustion Control: O2 Measurement Detecting air rich conditions
Zirconia Oxide Zirconia Oxide TechnologyTechnology
Combustion Control: O2 Measurement Detecting air rich conditions
At high temperatures, zirconia conducts electricity through the movement of oxygen ions.
Heated Chamber
Zirconium oxide (zirconia) based techniques
Zirconia disk
Electrodes
Combustion Control: O2 Measurement Detecting air rich conditions
0 100
ReferenceSample
7000C
When the oxygen concentration
on each side is different,
an emf related to oxygen
concentration is generated.
Nernst Equation
Cell output, E = K x Ln ( Pr/ Ps) mV
assuming a constant cell temperature
Zirconium oxide (zirconia) based techniques
Combustion Control: O2 Measurement Detecting air rich conditions
Zirconia Oxide Technology Provides:Performance
• Fast response
• Unaffected by background gases
• Sample at hot / wet conditions
Economics• Very acceptable operational life
• Low maintenance requirements
• Simple validation / calibration
Combustion Control: O2 Measurement Detecting air rich conditions
TDLTDLTechnologyTechnology
Combustion Control: O2 Measurement Detecting air rich conditions
Optical Absorption Spectroscopy
• Based on Beer-Lambert law• Used both in UV and IR• Typical wideband techniques have low spectral resolution and
sensitivity is limited by cross-interference• The alternative is single line spectroscopy using tuneable
diode lasers (TDL)• TDL are available for a range of gases of interest
Optical Absorption Spectroscopy
• Beer Lambert law: T = exp(-Sg(f)NL)– T is transmission– S is the absorption strength– g(f) is the line shape function– N is the concentration of absorbing molecules– L is the optical path length
• Measuring T and knowing S, g(f) and L, N can be found• Use single absorption lines in the NIR
Single Line Spectroscopy
Gas under test, typical absorption linewidth 0.05 nm
Absorption lines from other (background) gases
Laser scan range, typically 0.2 - 0.3 nm, note Laser spectral line width is ca. 0.0001 nm
UV / IR absorption spectroscopy linewidth > 2 nm
Single Line Spectroscopy
• Choose a single absorption line from available databases• Ensure no cross interference from other gases
Typical Gas Mix for Waste Incinerator– 10 mg/m3 HCl– 15% H2O
– 6% O2
– 500 mg/m3 SO2
– 350 mg/m3 NOx
– 100 mg/m3 CH4
– 150 mg/m3 CO– 10% CO2
0.9986
0.9988
0.9990
0.9992
0.9994
0.9996
0.9998
1.0000
5700 5720 5740 5760 5780 5800
Wavenumber (cm^-1)
Tra
nsm
issi
on
H2O
CH4
HCl
Single Line Spectroscopy
0.9986
0.9988
0.9990
0.9992
0.9994
0.9996
0.9998
1.0000
5737 5738 5739 5740 5741 5742
Wavenumber (cm^-1)
Tra
nsm
issi
on
H2O
CH4
HClLaser scan range
A single HCl line
Absorption spectrum for offgas from waste incinerator
Measurement influences
• Measurement influenced by:– Pressure– Temperature– Background gas composition
• Just like conventional IR measurements!
• Due to inter-molecular collisions, which strongly affect the absorption line:
– its amplitude– Its width– Its shape (asymmetry)
• Note: 2f WMS signal is just filtered version of line shape, so all information above is still available (non-linear relations however)
4
3
2
1
0
-2 -1 0 1 2
amplitude
width
asymmetry
• Pressure influence– Frequency of collisions increases with gas density i.e. total pressure– Causes line broadening, hence the term “pressure broadening”– Line amplitude (per molecule) is unchanged– Small line centre shift occurs also– Maximum measurement pressure limited by pressure broadening smearing the
line so as to overlap an adjacent line
8
6
4
2
0
-2
lock
-in a
mpl
ifier
out
put (
V)
-0.015 -0.010 -0.005 0.000 0.005 0.010 0.015wavelength scan (nm)
background 1.25 bar 1.0 bar 1.5 bar 2.0 bar 2.5 bar 3.0 bar 4.0 bar 5.0 bar
0.014
0.012
0.010
0.008
0.006lin
e w
idth
(nm
)
3.02.52.01.51.0abs. pressure (bar)
Pressure broadening measured for 2f WMS spectroscopy of O2 in N2
• Temperature influence– Changes gas density and molecular velocity distribution, hence collision
frequency and line width– Temperature also changes thermal excitation of molecular vibrations, hence the
line amplitude (per molecule)– Can be exploited to distinguish hot gas from cold gas e.g. 2900 (NEO) oxygen
analyser
8x10-24
6
4
2
0
line
inte
nsity
/(cm
/mol
)
775770765760wavelength/nm
800K 300K 1300K
Oxygen lines at high temperature
From HITRAN database
TDL (Tuneable Diode Laser) Provides:Performance
• Fast response
• In-situ measurement at process conditions
• Temperature and moisture measurement possible
Economics• Long operational life
• Low maintenance requirements
• Inferred validation
Combustion Control: O2 Measurement Detecting air rich conditions
How can CO be measured?
Thick film• High accuracy at process conditions• Cost effective measurement in combination with O2
Tuneable Diode Laser• In-situ analysis• Hot, corrosive, particulate latent samples
Combustion Control: CO Measurement Detecting breakthrough and flooding
Very thin platinum tracks are printed onto a ceramic disk.
Combustion Control: CO via Thick Film Sensor
Very thin platinum tracks are printed onto a ceramic disk.
Combustion Control: CO via Thick Film Sensor
These form resistors in a “Wheatstone bridge”, an arrangement that allows small changes in resistance to be accurately detected.
Each quadrant is thermally isolated from next by slots.
Combustion Control: CO via Thick Film Sensor
Very thin platinum tracks are printed onto a ceramic disk.
These form resistors in a “Wheatstone bridge”, an arrangement that allows small changes in resistance to be accurately detected.
A special catalyst that is selective to CO is then
printed over two quadrants
Combustion Control: CO via Thick Film Sensor
Any CO in the sample will burn on the surface of the catalytic material, creating a change in temperature.
CO
CO
CO
COCO
CO
CO
COCO
COCO
COCO
Combustion Control: CO via Thick Film Sensor
CO
CO
CO
COCO
CO
CO
COCO
COCO
COCOThe change in temperature is detected by the platinum tracks
underneath, changing their resistance, which can be detected.
Combustion Control: CO via Thick Film Sensor
ServoTOUGH Fluegas
Servomex Combustion Analyzer History
700 B / N
700 Ex
2700
Model 700 Combustion Analyzer
• Model 700 was introduced circa 1987• Two Models 700B & 700EX• Key Features:
– Separate sensor head and remote control unit– Oxygen only or with combustibles option– Rugged design (IP55)/wide range of applications– Comprehensive range of probes and filters– Fast dynamic response– Low flow (300 ml) extractive design
• 700B was discontinued in 1998• 700EX was discontinued in 2003
700 B / N
700 Ex
Model 2700 Combustion Analyzer
• The 2700 was Introduced 1998• Three Models 2700, 2700B & 2700C• The 2700C was introduced in 2006• Key Features:
– Same basic principal of operation– Standard flame traps– Simple Intuitive User Interface– Auto Calibration and assignable alarm relays– Integral auxiliary air supply– Introduced the TFx combustible sensor for COe– Easy access to servable parts
Sensor Head and Remote Controller
Auxiliary Air
Aspirator Air
AutoCal &BlowBack
SampleInlet
Aspirator& Sample
Outlet
HeatedEnclosure
Flame Trap
InternalFilter
O2 Cell
COeSensor Breather
Low Flow Extractive
Aspirator
Flame Trap
Solenoid Valve
Principal of Operation 2700B
Aux Air
Rest.
Aspirator Air
AutoCal &BlowBack
SampleInlet
200ml/min
Aspirator& Sample
Outlet
HeatedEnclosure
Flame Trap
InternalFilter
O2 Cell
COe Cell
Breather
Aspirator
Flame Trap
Solenoid Valve
Probe
100 ml/min
Principal of Operation 2700C
Servomex Zirconia Cell
mV
Sample in
Servomex 2700 ZrO2 Zirconia Sensor
Heater
Reference Air In
Platinum Electrodes Zirconia Crucible
Diaphragm Springs
Servomex Thick Film Sensor
Sample enters and is heated by sensor body
Hot sample reaches sensor and CO combusts - calibrated as CO equivalents (COe)
Heater
Heater
Heater band
PRT
Headerassembly
Sensor housingOutlet
Inlet
Sensor disc
Thick Film Sensor Structure
CombustiblesSensor
OxygenCell
Internalfilter
FlameTrap
Aspirator
Heater
Thick Film Sensor Location
Thick Film Sensor Location
ZirconiaSensor
Thick FilmSensor
Insulatedcover keeps wetted components above
210°C
Keep it hot =Increase performance.
Stop condensation.Stop blockage.Stop corrosion.
Increase life.
InternalSample
Filter(5 micron)
FlameArrestor(tested by
external agency)
2700 Flame Traps and Filter
Flame traps prevent risk of sensors igniting unburnt fuel at start up and causing an explosion
Modular Design• Open, standard filter or large filter• Variable lengths, with or without probe retention• Wide range of temperatures: <700°C to 1750°C (<1300°F to 3182°F) • Special materials eg ceramics or alloys• 4” ANSI Standard, 3” ANSI, JIS, DIN, 700B or Thermox flanges
2700 Probes
Sample Tube
½” NPT Probe Fitting
Filter Element
InternalFilter &
Flame TrapAssembly
°F
Stainless Steel 316 Probe can be used up to 1292F at any probe length
Haynes Alloy 556 Probe used for temperatures < 1832F Max temp will be dependent upon probe length
High Temperature Ceramic Probe for temperatures < 3182F
°C
0
500
1000
1500
32
932
1832
2732
3182 1750
1292 700
Cer
amic
Hay
nes
All
oy
556
S.S
316
2700 Probes
Questions on Analyzer Operation
• How does the analyzer respond in a low oxygen and /or high combustible conditions?– The analyzer will continue to measure what it sees. The combustible measurement is
maintained by the auxiliary air. The oxygen reading is maintained but will be reduced from the true reading by an amount which is dependent on the combustible gas species and concentration. The sensors will not be adversely affected.
• What are the analyzer/sensor response times?– When installed with a typical probe for heater applications and unfiltered software the T90
response time for oxygen is 10 seconds and 20 seconds for combustibles at 300 ml/min sample rate.
• Is output signal damping available?– The software allows dampening of both the oxygen and combustible outputs and displays. It
can be applied by differing amounts and can be switch out if required.• How does the analyzer measure combustibles?
– The combustibles analysis is wet and is optimized and calibrated for carbon monoxide to enhance its use for combustion control. The combustibles sensor will respond to most flammable gases apart from methane. Its response to hydrogen is twice that of carbon monoxide.
Questions on Analyzer Operation
• What is the recommended testing frequency?– The initial calibration intervals are 3 months for oxygen and 1 month for combustibles but
after operational experience this may typically be extended to 12 months and 2 months• What are the known failure modes for the analyzer?
– Internal failures• Temperature control oxygen• Temperature control combustibles• Sensor heads• Wiring faults• Block heater
– External failures• Aspirator air supply• Restricted probe• Sensor head temperature
– External issues• Mounting flange temperature• Radiated heat from process• Ambient temperature hot and cold
Questions on Analyzer Operation
• What are the common known failure modes for the analyzer?– Loss of sample flow due to probe blockage– Loss of air pressure for aspiration, purging, etc.– Controller power– Sensor head power– Sensor head block heater
Best Practice for Installation
• Serviceable location• Ensure ambient temperature is within specifications• Protect from wind chill• Protect from radiant heat• Minimize flange distance from wall to insulation• Use correct cable• Minimize distance between sensor head and controller• Insure proper wiring termination• Use probe retention flange when temperature is above 700C• Locate utilities in a stable ambient environment• Consider blowback for high sulfur high particulate samples• Leave sensor head off process until ready to power up
ServoTOUGH Laser
ServoTOUGH Laser Gas II
Dual Modulation Technique
• Laser wavelength chosen to match absorption line, fine tuning with temperature and current
• Tune diode laser by temperature to pin-point the centre wavelength of a single absorption line (+/-5mK)
• Laser wavelength scanned by applying ramp current• High frequency modulation added for 2nd harmonic detection• 2nd harmonic signal extracted by use of mixer• CPU computes gas concentration
Dual Modulation Technique
Diodecurrent
Diodelaserpower
Rampcurrent
High freq.modulation
() (2)
DetectorProcess
gas Signalprocessing
Temp. contr.Diode laser
Det. current
Mixer
Filter
Second harm.
Direct signal
Differences from conventional IR spectroscopy
• Laser radiation is monochromatic i.e. a specific wavelength, whereas conventional IR source is “multi-chromatic”
• Allows TLDS to measure a single absorption line by scanning across it• Signal is the line shape or a filtered version of it (2f WMS)• Free of cross interfering absorptions if suitable line is chosen i.e. no other lines nearby.
3
2
1
0
-1
lock
-in s
igna
l (V
)
0.0100.000-0.010wavelength scan (nm)
Second harmonic WMS,2nd derivative of line shape
Direct absorption scan
Process gas
Flanges Transmitter
Diode Laser
Purg e gas inlet
Receiver Purge gas
inlet Detector Focusing lens
Instrument window
Process gas
Flanges Flanges Flanges Transmitter
Diode Laser
Purg e gas inlet
Receiver Purge gas
inlet Detector Focusing lens
Instrument window
Loop cable
Collimating lens
Set-up for a in-situ cross stack TDLAS system
HARNESS THE POWER OF
expertise
SERVOTOUGH Combustion Solutions