overpressure protection-low temp effects

5
I n designing and sizing relief- device and effluent-handling systems, one commonly over- looked aspect of the perfor- mance is examining the potential f or low temperatures that can cause the components of the system to reach temperatures below their respective, minimum-design metal tempera- tures (MDMT), which may result in brittle fracture with subsequent loss of containment. This article points out limitations of the typical over- pressure-protection-analysis philos- ophy, discusses common sources of low temperatures for further inves- tigation, and addresses possible de- sign remedies for MDMT concerns. The primary objectives of a process engineering evaluation of an efflu- ent handling system (such as a flare system) include ensuring that opera- tion of the pressure relief devices dis- charging into the collection system (flare headers, for example) is not ad-  versely affected; a nd that the effluent handling equipment are properly de- signed to pe rform safely. The results of an overpressure-protection design are the primary input for this engineering evaluation; however, there are several potential gaps in the ability of these data to identify situations in which the MDMT may be exceeded. Current-practice limitations Common practices for pressure re- lief and effluent handling are found in numerous references [ 1–5]. The processes for estimating a discharge temperature and performing the out- let pressure-drop calculations in the pressure-relief-device discharge pip- ing are limited in their ability to ac- curately predict flowing temperatures for many situations. First, the discharge calculations are quite often only performed for the controlling contingency for which the pressure relief device was sized, which does not necessarily represent the most likely cause of overpressure or the cause resulting in the lowest dis- charge temperatures. Second, the outlet pressure-drop calculations for individual pressure relief valves consider the outlet dis- charge piping and potentially exclude the remaining, downstream piping system. This practice can result in a temperature discontinuity between the calculated discharge temperature for the individual relief device and that calculated for the same section of piping considering the entire down- stream piping system using an efflu- ent-handling hydraulic model. Third, the temperature estimates are typically made for isothermal pressure- drop equations and do not account for effects like retrograde condensation. Fourth, some simplifications of the calculations that are used for the pur- poses of estimating the outlet pres- sure drop do not represent flashing effects (for example, highly subcooled flashing liquids are often choked at the bubblepoint; therefore, the sizing of the valve may assume the backpres- sure is at the bubblepoint). Finally, the temperature estimates tend to be based on either relieving temperatures or isenthalpic flashes from relief conditions, which do not account for kinetic energy effects. These effects can be substantial if the developed velocity in the outlet piping is high and can be compounded when there are multiple relief devices dis- charging simultaneously into a collec- tion system, or when large diameter differences exist between the tail-pipe and the main effluent header. Temperature drop. Figure 1 shows the temperature drop from the stagna- Solids Processing Understanding the inherent limitations of current overpressure- protection analyses is key to developing a more robust heuristic  Aubry Shackelford Inglenook Engineering Brian Pack BP North America  CHEMICAL ENGINEERING WWW.CHE.COM JUL Y 2012 45 Environmental Manager FIGURE 1. Temperature drop relative t o stagnation as a result of owing Overpressure Protection: Consider Low Temperature Effects in Design -60 -50 -40 -30 -20 -10 0 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0    T   e   m   p   e   r   a    t   u   r   e    d   r   o   p  ,       F k=1.1 k=1.2 k=1.3 Mach

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8/13/2019 Overpressure Protection-Low Temp Effects

http://slidepdf.com/reader/full/overpressure-protection-low-temp-effects 1/4

In designing and sizing relief-device and effluent-handlingsystems, one commonly over-looked aspect of the perfor-

mance is examining the potential for

low temperatures that can cause thecomponents of the system to reachtemperatures below their respective,minimum-design metal tempera-tures (MDMT), which may result inbrittle fracture with subsequent lossof containment. This article pointsout limitations of the typical over-pressure-protection-analysis philos-ophy, discusses common sources oflow temperatures for further inves-tigation, and addresses possible de-sign remedies for MDMT concerns.

The primary objectives of a processengineering evaluation of an efflu-ent handling system (such as a flaresystem) include ensuring that opera-tion of the pressure relief devices dis-charging into the collection system(flare headers, for example) is not ad-

 versely affected; and that the effluenthandling equipment are properly de-signed to perform safely. The results ofan overpressure-protection design arethe primary input for this engineeringevaluation; however, there are severalpotential gaps in the ability of thesedata to identify situations in whichthe MDMT may be exceeded.

Current-practice limitations

Common practices for pressure re-lief and effluent handling are foundin numerous references [1–5]. Theprocesses for estimating a dischargetemperature and performing the out-let pressure-drop calculations in thepressure-relief-device discharge pip-ing are limited in their ability to ac-curately predict flowing temperaturesfor many situations.

First, the discharge calculationsare quite often only performed for thecontrolling contingency for which the

pressure relief device was sized, whichdoes not necessarily represent themost likely cause of overpressure orthe cause resulting in the lowest dis-charge temperatures.

Second, the outlet pressure-dropcalculations for individual pressurerelief valves consider the outlet  dis-charge piping and potentially excludethe remaining, downstream pipingsystem. This practice can result in atemperature discontinuity betweenthe calculated discharge temperaturefor the individual relief device andthat calculated for the same sectionof piping considering the entire down-

stream piping system using an efflu-

ent-handling hydraulic model.Third, the temperature estimates are

typically made for isothermal pressure-drop equations and do not account foreffects like retrograde condensation.

Fourth, some simplifications of thecalculations that are used for the pur-poses of estimating the outlet pres-sure drop do not represent flashingeffects (for example, highly subcooledflashing liquids are often choked atthe bubblepoint; therefore, the sizingof the valve may assume the backpres-

sure is at the bubblepoint).Finally, the temperature estimates

tend to be based on either relievingtemperatures or isenthalpic flashesfrom relief conditions, which do notaccount for kinetic energy effects.These effects can be substantial if thedeveloped velocity in the outlet pipingis high and can be compounded whenthere are multiple relief devices dis-charging simultaneously into a collec-tion system, or when large diameterdifferences exist between the tail-pipeand the main effluent header.Temperature drop.  Figure 1 showsthe temperature drop from the stagna-

Solids Processing

Understanding the

inherent limitations of

current overpressure-

protection analyses is

key to developing a more

robust heuristic

 Aubry ShackelfordInglenook Engineering

Brian Pack BP North America

  CHEMICAL ENGINEERING WWW.CHE.COM JULY 2012 45

Environmental Manager

FIGURE 1.  Temperature drop relative to stagnation as a result of flowing

Overpressure Protection: Consider

Low Temperature Effects in Design

-60

-50

-40

-30

-20

-10

0

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0

   T  e  m  p  e  r  a   t  u  r  e   d  r  o  p ,

   °   F k=1.1

k=1.2

k=1.3

Mach

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46  CHEMICAL ENGINEERING WWW.CHE.COM JULY 2012

tion temperature (T stagnation) causedby the kinetic energy developed duringadiabatic compressible flow of an idealgas as a function of the Mach numberfor ideal gases having different ideal-gas specific-heat ratios (k) (see Ref. 6,Equation 6–128). For the purposes ofillustrating the temperature drop, astagnation temperature of 0°F (460R)was chosen.

It is useful to note that while a stag-nation temperature of 0°F seems un-likely for many cases, this stagnation

temperature is established after thefluid has been relieved into the collec-tion system (in other words, after theisentropic process of flowing throughthe pressure-relief-valve nozzle andthe subsequent adiabatic process ofexpanding from the nozzle throat tothe total backpressure that results inJoule-Thompson (JT) cooling, both ofwhich can result in significantly lowerstagnation temperatures of the fluidentering into the discharge piping). Additional limitations.  Additionalgaps in the overpressure protectionanalysis include the common practiceof not considering the potential for

pressure relief valves to leak, or theeffects of other inputs to the effluenthandling system (such as pressurecontrol valves, depressuring valves,pump seals and manual purge valves).

 A leaking pressure-relief valve is typi-cally considered an operational andmechanical issue, not a cause of over-pressure that needs to be evaluated forthe sizing of the pressure relief valveor for the effects on the downstreamcollection system; however, many of usin the warm Gulf Coast region of the

U.S. recognize an ice-covering as indic-ative of a leaking valve, and the fluidsused in the evaluation of the pressure-relief-device sizing may not be repre-sentative of the normal process fluid(for example, the external fire case,which is a common design basis).

Pressure control valves may also becalled upon to “relieve” fluids, yet arecommonly not accounted for in over-pressure protection studies based onthe desire to not include the positiveresponse of control systems in prevent-

ing overpressure. In actual situations,the basic process-control systems areexpected to function as intended, and

thus represent a more likely source offluid input to the collection system.

In addition, these control valves arenot necessarily sized to handle the fullflow of an overpressure scenario, re-sulting in flow from both the control

 valve and the pressure relief valve,thereby exacerbating velocity effects.

Finally, depressuring is a dynamicprocess, releasing fluids of differentpressures and temperatures as a func-tion of time. Considering the mostlikely behavior of a depressuring sys-

tem to be an isentropic expansion ofthe residing fluid, the inlet fluid tem-peratures can drop significantly as thedepressuring progresses.

Low temperaturesWhile the potential for low flowingtemperatures falling below the MDMTexists in a variety of processing facili-ties, the issue is especially apparent innatural-gas processing facilities wherehigh pressure, low temperature, low-molecular-weight gases and volatileliquids are present. Design considerations.  Based onrecent evaluations of several natural-

Sweetening

Sweeten-

ing

Demethanizer

Dehydration

Flash

tank 

Stabilizer

Amine still

Deethanizer

Depropanizer

Propaneloading

Refrig-

erant

NRU

HeN2LPHP Auto-

refrig-

eration

NGL

surge

Emergency storage

1

2

3

4

5

6

7

1. Process upsets in the NRU can cause low flowing temperatures to

propagate downstream to after the gas/gas exchanger, which is typically

designed based on normal operating temperatures

2. Relief of unstabilized condensate, a flashing liquid

3. Breakthrough of high pressure gas or flashing liquid into the flash tank 

4. Tube rupture in the chillers cause relief of expanded gas that starts cold

and is cooled further by JT effects

5. Valve specifications for appropriate MDMT are

common issues

6. Common discharge lines can cause increased velocities, further

reducing flowing temperatures. Also depressuring is an

isentropic process that results in low flowing temperatures

7. Potential relief of flashing volatile liquids that can cool

significantly based on flashing

FIGURE 2. Typical schematic of NGL processing facility showing common areas of potential MDMT issues

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gas processing facilities with ethanerecovery capabilities, the authorshave identified several common areasof concern that may provide a start-

ing point for other gas processors’investigations into this aspect of col-lection system design, as well as forprocess piping. These areas includethe following: multiple inputs (suchas pressure relief devices or control

 valves) discharging into subheadershaving diameters close in size to theindividual discharge piping diameter;flashing liquid relief (unstablized con-densate, natural gas liquids [NGL] orliquid propane); internal-boundary-failure cases (tube rupture, for ex-

ample) in gas chillers; cryogenic drainoperations (such as draining expandercasing for maintenance); pressure-relief-device MDMT specifications notcommensurate with discharge pipingMDMT; and pressure relief devices or

 vents on the outlet of cryogenic cold-box sections where the normal process

fluid is at elevated temperatures, yetduring process upsets may experiencesignificantly lower temperatures.

Figure 2 provides an overview of

these common areas of concern relatedto low flowing temperatures. NGLand propane processing-and-storageequipment are examples of commonlyoverlooked systems that can achievelow flowing-discharge temperatures.These equipment usually have pres-sure relief devices that are sized basedon an external fire case, yet also havethe potential for relieving the liquideither due to blocked discharges, leak-ing relief valves or depressuring. Alternative solutions.  While the

design issues related to low flowingtemperatures can be dealt with byspecifying appropriate metallurgy,there are other alternatives for con-sideration. These alternatives caninclude identifying ways to elimi-nate the cause of overpressure inthe first place (for example, preven-

tion of overfilling of vessels), mitiga-tion of relieving conditions causingthe low temperature excursion viasafety instrumented systems (SIS),

performing mechanical stress analy-ses to establish a better estimate ofthe MDMT per ASME B31.3 (with re-placement of components not coveredby stress analysis as needed), add-ing supplemental fluid (such as gasor methanol) to raise the stagnationtemperature, rerouting the dischargeto a different location (such as to theatmosphere), or conducting Charpytesting on the piping in question toestablish the actual MDMT.

For potentially leaking pressure-

relief valves, the options also includerecognizing the additional conse-quences in a risk-based inspectionprotocol, installing rupture disks, oradding skin thermocouples and lowtemperature alarms on the dischargepiping to notify personnel of leakagebefore the MDMT is crossed.

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48  CHEMICAL ENGINEERING WWW.CHE.COM JULY 2012

Environmental Manager

Final analysisIn summary, established overpressure-protection-analysis philosophies are

not well suited to identify possible ma-

terial concerns as a result of processfluid flashing and depressuring. Relief-device and effluent-handling sizingconventions and simplified calculation

methodologies limit the ability of thedesigner to recognize potential MDMT

concerns. Understanding the inherentlimitations of current overpressure-pro-

tection-analysis practice is key to devel-

oping a more robust overpressure pro-

tection analysis heuristic, which morefully recognizes the effects of low tem-perature flashing on material design.

It is the experience of the authorsthat modification of the typical over-

pressure-protection-analysis philoso-phy to identify and propose alterna-

tive solutions for conditions resultingin excursions beyond MDMT is pru-

dent in promotion of enhanced facilityprocess-safety management. ■

   Edited by Dorothy Lozowski

NoteThe views in this paper are entirelythe authors and do not necessarily re-

flect the views of BP America Produc-tion Co. or its affiliates.

 Authors Aubry Shackelford  is aprincipal engineer for Ingle-nook Engineering, Inc., whichprovides process engineer-ing consulting with a specific

focus on process safety man-agement (15306 AmesburyLane, Sugar Land, TX 77478;Email: [email protected]; Phone: 713-805-8277).He holds a B.S.Ch.E. fromNortheastern University and

is a professional engineer licensed in the state ofTexas and the province of Alberta (Canada).

Brian Pack is the area engi-neering-support team leaderfor the Mid-Continent opera-tions area in North Americagas region for BP AmericaProduction Co. (501 West-lake Park Blvd., Houston, TX77079; Email: brian.pack@ bp.com; Phone: 281-366-1604).He holds a B.S.Ch.E. from theUniversity of Oklahoma andis a professional engineer li-

censed in the states of Texas and Oklahoma.

References1. API Standard 520, “Sizing, Selection, and

Installation of Pressure-Relieving Devicesin Refineries, Part I — Sizing and Selection”,8th Ed., December 2008.

2. API Standard 520, “Sizing, Selection, andInstallation of Pressure-Relieving Devices inRefineries, Part II — Installation”, 5th Ed.,

 August 2003.

3. ISO 23251:2006 (API Standard 521), “Petro-leum, Petrochemical and Natural Gas Indus-tries — Pressure-relieving and DepressuringSystems”, 1st Ed., August 2006.

4. Coats, and others, “Guidelines for Pressure

Relieving Systems and Effluent Handling”,1st Ed., Center for Chemical Process Safetyof the American Institute of Chemical Engi-neers, 1998.

5. Gas Processors Suppliers Association, “Engi-neering Data Book”, 12th Ed., 2004.

6. Perry, R.H., D.W. Green, and J.O. Maloney,editors, “Perry’s Chemical EngineeringHandbook”, McGraw-Hill, 7th Ed., 1997.

7. ASME B31.3-2008, “Process Piping”, Decem-ber 31, 2008.

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