ML030700448
| ML030700448 | |
| Person / Time | |
|---|---|
| Site: | Point Beach  |
| Issue date: | 02/06/2003 |
| From: | Khurana S Florida Power & Light Co |
| To: | Office of Nuclear Reactor Regulation |
| References | |
| FOIA/PA-2003-0094 | |
| Download: ML030700448 (22) | |
Text
4-i.
WATER HAM ME R/CAVITATIO N Assessment & Prevention
"* WHAT IS WATERHAMMER
"* WATERHAMMER CATEGORIES
"* WATERHAMMER PHENOMENON
"* WATERHAMMER ASSESSMENT
"* WATERHAMMER PREVENTION
"* INDUSTRY EXPERIENCES 0
0 S
0 0
WHAT IS CAVITATION WHERE IT OCCURS HOW TO IDENTIFY EFFECTS OF CAVITATION CAVITATION DAMAGE DESIGN CONSIDERATIONS SUBHASH C. KHURANA FLORIDA POWER & LIGHT L
Cavitaiton Trng.
Page 1 of 6 CAVITATION 1.0 What is Cavitation In a flowing liquid if the static pressure is dropped below the vapor pressure corresponding to the liquid temperature (or the temperature is increased above the saturation temperature corresponding to the liquid pressure), vapor bubbles (cavities) will be generated. If these bubbles are carried downstreams by the liquid to a region of higher static pressure (or lower temperature) then the bubbles will collapse. the region of the flow where bubbles exist is the cavitating region, whereas the observed damage is at the location of the bubble collapse.
Cavitation is distinguished from flashing or boi-in-flow in that no pressure recovery occurs downstream in the latter type of flow, and therefore no bubble collapse occurs.
2.0 Where Cavitation is likely to occur in Systems a
Orifices (Pressure profile across an Orifice, Figure-l)
Valves Venturies Pump Suction 0
Pipe Fittings (Elbows, TEEs, etc.),
(Figures 2 and 3) 0 Bumps 3.0 Identification of Cavitation This process of bubble formation, growth, and collapse produces oscillation in the flow regime that can be identified by distinct sound. The sound may range from occasional popping (at the onset of cavitaion) to a sound like frying bacon as cavitation level increases. Extensive cavitation sounds like gravel flowing through the system. Because the flow oscillation associated with cavitation is broad band, pipe vibtation will also be associated with cavitation.
Cavitaiton Trng.
Page 2 of 6 4.0 Effects of Cavitation/Damage Cavitation produces undesirable effects on piping system and components.
It generates undesirable noise, may cause erosion, restrict flow capacity of the system, and may cause pipe failure due to pipe failure.
The erosion observed in cavitating fluid is due to bubble collapse near the pipe wall. Studies have shown that as a result of bubble collapse the liquid jets with velocities of 300 to 2000 feet per second will impact the pipe wall. At this high impact velocity, the local pressure at the wall could be as high as 10,000 atm. The continuous bomardment of the metal surface will result in the pitted configuration observed in most damaged components.
5.0 Design Considerations For system susceptible to cavitation, the designer should ensure that under operating conditions, the system is either free from cavitation or has acceptable level of cavitation. Levels of cavitation are defined below.
Incipient Cavitation Critical Cavitation Incipient Damage Choking Cavitation -
The onset of cavitation. No objectionable noise and no damage.
Continuous light cavitation usually adopted as the design criterion. Noise and vibtation are acceptable and only minor damage after long periods.
Onset of surface pitting after short period of operation.
Flow is not increased if downstream pressure is decreased. Maximum vibration and noise.
Cavitation at pump suction is well taken care by satisfying Vendor's NPSH requirements. Valves and Orifices are genarally the common source of cavitation problems encountered in power plants.
The following sections provide basic guidance on how to avoid cavitation of orifices and valves.
- m Cavitaiton Trng.
Page 3 of 6 ORIFICES (See Figure-1 for a pressure profile across an Orifice)
Cavitaiton Index a =
(Pd PV)/(P- -
Pd)
(Pd Pv)/AP (Reference 1)
Where:
a
=
Orifice Cavitation Index Pu
=
Upstream Pressure, psia Pd
=
Downstream Pressure, psia Pv
=
Vapor Pressure, psia The above calculated "cavitation Index" is compared to accepatable "Cavitation Level" (see Figure 5) which is experimently determined.
If the cavitaion index is equal to, or higher than the cavitaion level, the orifice size is acceptable.
If a single orifice fails to satisfy cavitation criterion, multiple orifices are required. The spacings between orifices must allow complete pressure recovery, which is achieved by placing the orifices 6-8 pipe diameters apart. The "f," ratio (orifice diameter/pipe inside diameter) of orifices shall be in increasing order along the flow. Sample Problem-I illustrates selection of orifice(s) to have cavitation free operation.
When enough space is not available, multi hole type orifice plate (perforated plate),
or a cone type orifice is 'recommended.
Other definitions of Cavitation Parameter (hu-h.)
a =
and U2/2g (hu-hv) a =
(Reference 2)
(hu-hd)
Where:
a
= Cavitation parameter hu
= Upstream head hv
= Vapor head hv
= Downstream head U
= Upstream velocity g
= Gravitational constant
Cavitaiton Trng.
Page 4 of 6 Reference-2 utilizes reference velocities for a component size and upstream head at which a type of cavitation commences. These velocities are then corrected to other component sizes and upstream head conditions using empirical relationships with experimentally derived coefficients.
VALVES Colorado State University tested some valves for Hydraulic and Cavitation characteristics. The test data indicate that the critical cavitation index does not only depend on the valve opening (area ratio) but is also dependent on VALVE SIZE, UPSTREAM PRESSURE, and VALVE TYPE. Figure-9 through-12 show results of such tests. Figure-12 also includes a curve for the critical cavitation index for a thin orifice plate for comparison to that of a valve.
For a valve to operate completely cavitation free, operating conditions should never approach those corresponding to the critical cavitation index. Operation beyond critical cavitation is never recommended.
Analytically, it may not always be possible to accurately predict when a valve will start to cavitate. Therefore, monitoring for noise and vibration levels at the required operating point is recommended.
Reference 2 provides guidelines for determining cavitation parameter for valves. Sample Problem-2 is used as an illustration for a butterfly valve.
6.0 References
- 1.
Technical Paper, "Eliminating cavitation from pressure reducing orifices", CHEMICAL ENGINEERING DECEMBER 12,1983
- 2.
INTERNAL FLOW SYSTEMS, by Donald S. Miller, Volume 5 in the BHRA ( British Hydromechanics Research Association )Fluid Engineering Series
Cavitaiton Trng.
Page 5 of 6 SAMPLE PROBLEM-I
-/- / &'-- -
I0.
Pump discharges water to atmosphere (See Figure-4).
Pipe size:
14-inch, Schedul Flow:
4500 gpm Pressure drop across orifice(s):
Fluid temperature:
e 40 120 psid 1600 F Determine the size of orifice(s) for cavitation free operation.
Neglect piping friction loss. Use Figure 5 for comparing calculated cavitation index (a).
SAMPLE PROBLEM-2 Water flows from a reservoir at higher elevation to the reservoir at lower elevation, and flow is to be controlled by a butterfy valve (See Figure-6).
Determine the cavitation free range of control for the A-type butterfly valve from fully closed to fully open position. Loss coefficients for butterfly valve types are shown in Figure-7. Accepatance criteria is critical cavitation velocity..
Pipe Size:
Valve Size:
Water Temperature:
K-for Piping between "A" to "B" :
K-for Piping between "C" to "D" :
K-for butterfly valves types:
30-inch, Schedule-40 30-inch diameter 900 F 17 7
Shown in Figure-7 Based on Reference-2, Cavitation velocities for a butterfly valve are determined as follows:
Ui or U, = Cl. (Ur or Ucr).[(hu-hv)/50]
0.39 and Uch = Urch [ (hu-hb)
/50] 0.5
Cavitaiton Trng.
Page 6 of 6 Where:
U1, U,,
and Uch are incipient, critical or choking cavitation velocity (to be determined) for a given butterfly valve.
C1 is correction factor for the valve size used, Figure-8 Ui,. U,,,
and Uch are the reference cavitation velocities (incipient, critical, or choking as applicable) for the base valve, shown in Figure-B.
h
=
upstream head of the valve (meters) h,
=
vapor head (meters)
"50"
=
"h,-hv" value (in meters) for the base valve (size 0.3m diameter)
CAUTION:
USE DIMENSIONAL UNITS APPROPRIATELY
ORIFICE I
I Pu Pd PvP PRESSURE PROFILE OF A SINGLE-ORIFICE SYSTEM Pu = Pressure upstream of the orifice Pc = Pressure at the vena-contracta A473 Pd = Pressure downstream of the orifice Pv = Vaper pressure of the flowing fluid FIGURE -
1
VAPOR FILLED CAVITY 7,
SB ELBOW A472 FIGURE -
2 OA
Brim I FIGURE -
3 I,
ti
INCORRECT SOLUTION:
(1 stage orifice)
CORRECT SOLUTION:
(2 oriface stages) 2nd 1st
_ 7 Ii0
-2P -2 A471 FIGURE -
4
I-Critical Cavitation Index for Thin Plate Orifice FIGURE -
S 1*
9 -
I -
+
1 I iT
-i I.
I--t-I-t-4-I-I-I t-t-1-I I
NO CAVITATION
/
CAVITATION L_~
0.0 0.1 0.2 0.3 0.4 0.5 0.6 DIAMETER RATIO (d/D) 0.7 0.8 0.9 1.
70 FT.
RESERVOIR D
RESERVOIR B
REFERENCE VALVE
-0 FT.
FIGURE -
6 A477 200 FT.
Pt
1000 C
100 50 A
10 1.0 0.1 0
10 20 30 40 50 60 70 80 go Vahv owniN (deg,)
Loss Coefficients for Butterfly Valves (from Reference 2, Figure 14.19)
FIGURE -
7 lI
)
L=s coeffi~ent K Cavitation Velocities for Butterfly Valves (from Reference 2, Figure 6.22)
U IA.
C C
a U
10.2 1.4 7
2m---"
1.0 m
a oO."
0.1 10 1
LOU coff
@Mc KV Correction Factors for Valve Size (from Reference 2, Figure 6.23)
FIGURE -
8 i
I i
I.......
- 11. FPiGURE -
9 12-in. Rjuttes4L.VVv?! with 24-in. expansion downstream Upstream pressure 00 psi 0
1 0
10 Normal tests Air injection into stem
-J S....
rnRf 70 t
z0 iu "IU "Test Valve Opening'-
9o 11 6
5 4
3 2
I (1
SiSr
'0 6
- ,.Iv
"FIGURE -
10 to 20 30 40 50 60 70 80 Test Valve Opening - 7 6
5 4
0 u
u; u
3 z
i 0
0 4
MA
)',C*,
'z-
FIGURE-12 3.0 8-in.
Nqg1j&.y e
1.,xpansion P u o
14-in.
153 psi 14-in.
65 psi 12-in.
153 psi o
12-In.
65 psi 14-in.
153 psi (swOeep tests)
S2.0 A
12-in.
153 psi (sweep tests) 0 8-in.
65 psi
>0 u
"u.
- o.
F//
0 20 40 60 80 103 Test Valve Opening -
I
FIGURE -
12 10 20 30 40 50 60 70
'rest Valve Opening - I Orifice Area Ratio (d/D) 0/0 6
5 t
U La4 u
2 I
0 0
80
Cavitation Trng.
Attachment Page 1 of 3 Eliminating cavitation from pressure-reducing orices Multiple orifices can avert the cavitation, and resulting noise and vibration, caused by single orifices in hydraulic systems P.ztiik C. Tuisg.. d Miltd MQiuie, Ouarw Hydro o Fig I illustrates flow through a sing orifice in a pipe: P. is the pressure upstream of the orifice; P, the vena-contracta pressure; and P,. the pressure dow'n stream of the orifice. The last pressure. Pj. must be higher than the vapor pressure. P,. of the flowing fluid.
If PA falls belou P,. bubbles form. the first stage of c,,vitation. As the fluid moves downstream, the bubbles collapse under the higher pressure. Pg. in the final stage of ca-itation. The implosions generate noise and vibra tion. and accelerate the erosion of the piping [)).
If P, is kept below P,. t'o-phase flow continues down stream as a flashing mixture without cavitation.
Cavitation criterion To avoid orifice camitation. the orifice size selected for the pressure-drop requirement must be checked against an orifice cavitation index, which is then compared to a cavitation level If the index is equal to. or higher than.
the cavitation level. the orifice size is acceptable.
The index was defined b. Tullis and Govindarajan 12]:
0, -
(P4 -
PY(.W.
Pd) -
(pd - P.-AP (1)
They also experimentally determined acceptable cavita tion levels. These. ',. vs. orifice-to-pipe-dia. raitios. P. for
%anous pipe sizes are shou n in Fig. 2. At these cavitation Levels, noise is io, and stead% and no damage will result.
When a single orifice fails to satisf' the cas'itation crite rion.two or more orifices in series are required. In multi pke-orifice systems. the spacings between orifices must allow complete pressure recover)', which is achieved when'the circumference of the orifice jet expanding to ward the pipe ^-all equals that of the inside pipe. Fig. 3 relates these distances to P [3].
Design of single-orifice systems To design a single-orifice system free from cavitation:
- 1. Size the orifice for the required flowrate and pres sure drop by means o7 !-.
(2):
Ah- - X(V412)p (2)
Determine the resistance factor. K. for the orifice by inserting the floeate and orifice pressure drop into Eq.
(2). Having the K value, find the orifice size from Fig.1LX"
- 2. Check that the orifice size obtabwd from Step I sat-is'ies the cavitation criterion. Calculate the cavitation index. o'. for the orifice %ia Eq (1), and get the corre sponding acceptable cavitation level, a,,. from Fig. 2.
Compare a' to a',: If a ý c',. the size of the single orifice is acceptable; if o < a,. multiple orifices are required Design of multiple-orifice systems Each orifice in a multiple system (illustrated in Fig. 4) is sized to meet the c*vitation criterion I. Assume a P value for the fast orifice. OR1 (the one furthest downstream). With this 9 value, determine the corresponding resistance factor. K. from Fig 5.
- 3. Substitute this calculated AP into Eq. (1) to deter mine the ca2itation index. a,.
- 4. With the Pvalue assumed in Step 1. find the accept able caiLtation leveL o in Fig. 2.
- 5. Compare oto o',. If ao:q the assumed 0 i satis factory. (To have the minimum number of orifices for a specific flourate and pressure-drop requirement. the value of a should be kept as dose as possible to Or.) If 0r< 0o, choose a larger p value and repeat Steps I through 5 until a 'o'.r
- 6. The downstream pressure. PIM. of the second ori 69 CMUKAL LXWALLIUWG ZNWEMM U. Mo Pressure profile of a single-orifice system Fig. 1 I~P.
p P.
Acceptable cavitation level related -
to orifice-to-pipe-dia. ratio 121 Fig. 2
. 2*
.cL I..:
0.2 1
-0 2~
vistarne downstfeano for compltce pressure ri I"\\
I ' I P11 1
I I
OR3 OR2 oR, A
Pipe flow W=. V X
Resistance factor
!n Man, Gowra. igh p~d 3akpreuuur. L~a P. OrirKr upavam prm=a.
kPM P. Vapor prmur.
M*
A, Pipe internial radlus,
-V Tho.w Vktiz). =Vs a
Dinanc for orie jet drcuzmfu to fm pipe &
¢mlference. =
I Du-ner rato o oroif/"tpipe
- *-*). hem 4r Cavitation budes w,
AmzpLabk tavisaog kevel fKce. OR-,. is set equal to the uptream pressure. PI.. of the first orifice. OR,. etc. (as indicated in Fig. 4)
- 7. The last orifice (the one funhest uPTreim) is sized as was described for a single-orifice system
- 8. After all the orifices have been sized. determine the neccssarý distances between the orifices for cavitation free operation b% means of Fig. 3. For example. find the proper distance bet% een ORI and OR2 (Fig 4j. enter the value of J for OR2 into Fig. 3 and obtain the correspond ing value of x!Rr Having the pipe radius. R,. determine the proper distance;-x, between OR, and OR.
Example illustrates the procedure Design an orifice system for a 186 0-kg s floTate of water through a NPS12 Sch. 80 pipe. The upstream pressure and temperature are 10.340 kPa and 138'C.
respec-ve.. and the orifice backpressure is 690 IPi The vapor pressure and density of water at I 38'C: are 340 L)It and 928.0 Ig'm'. respectivel.. The pipe's inside radius is 0.145 m. and its flou' area is 0.066 mi.
First determine the flow velocity through the pipe.
V - m'pA = 186.0:(928 00X0.066, - 3.0 m s
- 1. Trý a single orifice, sizing it via Eq. (21.
(10.340 - 690()
I.SM = A(3.0"2] 92F 0 SWith K - 2.300. P = 0.186. from Fig. 5.
- 2. Check whether the orifice size P = 0.186 satisfies the cavitation criterion. Via Eq. (1):
arn (69 - 340)'00.340 - 690. = 0.036 With P - 0.186. Fig 2 gives: a, 1 I.I.
As (a -- 0.036) < (ct-
- 1. 1). one onficr system does not meet the criterion, and a multiple s%stem must be designed:
- l. Assume that 1, = 0.4 for the first orifice. OR, (the one furthest downstream). With this 191. A - 90
- 2. Determine the pressure drop via Eq (21.
AP - 90 1(3.0)2f2] 92.0 - 375.8 LRa
- 3. Substitute this AP value into Eq. (1):
a, - (690 - 340)f375.8 - 0.93
- 4. With
,0.41,
A,-.3, from Fig. 5.
- 5. Because (0, - 0.9) < (q, -
1.3). the cavitation cr*te riOn has no( been met. Tr" a larger orifice size--e.g-.
P-Ps - 0.45. Repeating the "foregoing procedure tields
-, 1.62-and a, = 1.6. which satisf% thecrflterion.
-6 The sizes of the remaining orifices are determined SPr:or'usl described-i.e. the downstream pressure.
i (Ca Tr1 "I af a multiple-orifice system Fig 4 I
Cavitation Trng.
Attachment Page 2 of 3
10 0.1 O-OWAI RetationshiP of rnistame factor to cwific&-to-pipe-dia. ratio for "rp-edged orificn 141 CKLUSCAL gw.&ýP*G DICU"" $2. IM3 cavitation Trng.
Attachment Page 3 of 3 DIM a 0 fig. S Ibe, siý ravick C lr;ýj'ý des;r eftw-M wW Orwww Hvdro (700 L ftwrmn.-AC Torama Cku-MSG Dfi-CjMWA,,:,
I plimot 416-W--=W HOVý7.-ý - I mpmuWam wchý V-d Md Lr dnwn of PTUM %-k-p- -
and mWed eq-Prwww2HOkI" Of A wwd'W&Cd earrwrmw from shi-ý t;nrmm *(%%w=wn wWw-USA,;
In= the Vwwrwn Of M-wt-Ow a '70"'d CArrw" in Omano. a VwvIkw of the Anwn= Sm 0( M-M--J J'r'w' WW the Othm O(wrrAI muck, in wdwwW Pubb WICU MAUAWOM S & wneac deW"
,pm-1 ý,h OnL&rw 14-ldfu H*
map--b-b-widude drWn ww "Mm of Vwjw-2' "Pup-"
,d d..---J P-- Wj
'(' IS " wwC"r-Kw CDC--q imm aw U-V'w- -( bar'Ide TwjadrAL jw a a =,ed Lw=
Onmb" of Lhe
. S:
Im rni.-r-w b'r-a'd Ow a`
St a Undboa affhad r-,
T.Imbýwl MW O(bM--'
7 p2d. of the d OrifiCC-OR2. is Wt equal to dW UP SET'CaM pressure. PI.. of the first orifikx. Mi. CM
- 7. Size the final oTifice. as his been dcscrR)ed.
- 8. Lasd). find the dis=ccs beturctm the orifices.
J. Adadry. EAw References
- 1. Jaime. Ir-C&wwxan in eancral Vamjawww-ant Ca-d5rWars. VaL 34.
No.vmbrr 1961 2 TW6 j ?..NW GOVWAMYUL R. Cavaum WW SOW-5-k VISM SM Or6CCL:'
- j df Piv"wfir Dn. Anwn= Sm. Ci Crei Lngwwcm MwCh 1273 T"Wd=. a G-MW %-*m U P. M ri, ei L'w Ve" GWWN=7 AwwrIMA Sm. of MechanciJ Engvwo-L P*v he 73-%AITM-9
- 4. XaAwwkv-U- mid Twq. T C-Ssmg of TW*mbag Onfa=L. Saw%4PYOW Ar GPft&bowwC. D"mub" IM LwAvr=mn.Wj-wd 'Aabs. L W-nuid TlwwTbrwACIýTwoorifiaw is soon.
Toom Awný Sm 4(XFAwmwd Lnmwm jounn 1157 OL IcnpffwL M 'Wý and MMn. j G-The Fkp-of Sowrxwd VAw TbrONO ThrombM CwVcm TvoL Amomm SK #f AdmArmait LegwAm JWY M 1
- 7. WummdL j ?- et aL. Cawwwwan Elko m Wbc Dodwav Ckeffamm Od dw DwpEdCW Onf- "wNj t(Sa-X%--4 Man:h IM TwIsLj. r-et aL hvkrwd Pbm a HvdrAK EmeThDo
=n Sm-a( 04 L-4wwm JOW 9 vAjwwL w. w., tvakwoona(Mubynsinve Wacj dfhýOý V&ýAwý Sw-or Cr#j &Wmmjuw 1977.
W TwLj.T
=n Sor-of 04 Lasww"L P-Oftf 1971.
t I. DrubeL L-CAwad Vshq Sm% W" ZA Fwmdm& few. raL. Jay "M