ML20024C659
| ML20024C659 | |
| Person / Time | |
|---|---|
| Site: | Crane |
| Issue date: | 05/05/1978 |
| From: | Rogers L BABCOCK & WILCOX CO. |
| To: | Geoffrey Miller METROPOLITAN EDISON CO. |
| References | |
| TASK-*, TASK-GB GPU-2048, SOM-II-143, NUDOCS 8307120933 | |
| Download: ML20024C659 (4) | |
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Reactor Trip /I.S./Cooldown Incident of 23 April 1978 Subjects g
ogg 5,W Dear Gary fdy??+-
m Information relative to the BW evaluations of W subject transient is CMY continuing to be developed and accumlated at both the Nuclear Service section in Zynchburg and the T(I Site Cffice. The fo11oving information DM
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naq cautains conc 1usions rega.rding h-level transient in the pressuriser g
$q euring the subject plans transient.
M C
lusions Cenee@r Voidint of Pressurizar k~;g-gf,
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bD
, there are four observations or calculations which can be drawn to ascertain L%)M i,,)
vbether or not the pressuriser-surge line emptied during h transient.
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g 3hch of these suggests that. in fact, no steen hbble was drawn into the pg.;
Reactor Coozant Systen proper fran h pressuriser of forned spor.taneously i
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during the depressurisstion.
parsaeters to deternir.e the rate of and enount of Reactor Coolant,3ysten y[g.g etg Caletlations were made eased on W measured Reactor Coolant Systes
'e coolaat shrinkage er. ring the first two ainutes of the transient, which p..
includes most of W period when pressuriner level' was low-off-seale.
These en1culations considered h effects of the Makeup System and the
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opera *.or initiation of EPI, estimations of the effects of temperature p
measurement arrars, and flashing and subsequent cooling of liquid in the a
prassuriser as W pressure rapidly dropped. Using conservative estinates i@:V=d
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for these effects. the emiculation showed that the 3ressuriser steen ma wm. -hed m.,,er s.cmn.f the sur,e 2ine, i.e., m,ressuri.er M
w.
did empty kt the kbble did act reach W bot leg.
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De second iten of note is ht the Reactor Coolant System pressure was q$75 In-house codes 3.$
a smoothly varying parameter throughout the transions.
(e.g., Tinp2) have shown that following the pressuriser-surge line 4*C e.. <r%;
emptying, the Reactor Coolant System pressure promptly flattens as bot
%g{
f less flash to steen, thus maintaining the Reactor coolant Systen at T
saturation pressure for the highest temperature in the Reactor Coolant k;%g d
g This sort of phencc:enon did not occur at ':MI-II as can be seen h]P System.
from the loop Reactor Coolant System pressure traces.
The third indication that no bubble was drawn in the Reactor Coolant system
@d dy M
is that the botter of the two Reactor Coolant System hot legs (loop "A")
hw;g.
~
nner got within 20*F of saturation temperature as the Reactor CoolantAt the 3 4';
~ ~~ V Systas pressure fell. turned sharply upward and this aspect of the problem ceased to be a con
.,v.h, M
y The fourth itus is a qualitative agreasent based on the reactineter data l@r,@
- l*th yor purposes of explanation, the plot of pressuriner
$@1'W h
from the site.
level, Reactor Coolant System pressure and pressuriser temperature are P3 QQ Q
. W IPI isolation valves ware opeiied and the second makeup pump was started.
p,%
attached.
b[U Design his point is marked with sa "A" on the pressuriser level plot. stroke tim
,g f.$
s 6 Derefore, it seems reasonable to assume that
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makeup pumps is 6 seconds.
Since the full EPI flow was achieved well before the 1 minute mark.
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TY makeup pumps are centrifugal pumps, their flow rate increases as ReactorNotice on 4.U
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k@*d?y
{gG Cralant System pressure decreases.
that when it comes back on scale (t = 2.2 minutes), its slope is relativelyAt t =
ii gg,
linear for abcut half a minute.Eotice that, at that time,the slope decreased as one vould z,
How look at the dashed curve which covers that range in time when p@r.
down EPI flow.
i For the level to have behaved in this way, makeup erpect.
level was off scale.
tiov rate would have had to decrease sometine before level cane b y.g:
T y
g#"H,
throughout this time, and the EPI valves were at 'a fixed position, this M
scale.
The only curve shape cone.lusion does not seus physically realizable.which meets the physical cc i
iN According to the EPI flow Q
1i >
49 This alternative is shown as a dotted line.versus Reactor Coolant System pres Ym ing, the HPI flow rate should be continuous 3y increasind as the Reactor >
Coolant Systes pressure falls, thus a concave curve shape seems most logical.
fit;r De conclusion from this line of reasoning is that pressuriser level could
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M not have dropped very far below the lower level tap when MPI turned the Y6!
level decrease around.
l two fact of W lower level tap.
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5/5/78
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D 3ased on the arguments and observations outlined above, 3W's conclusion T-4 P
It appears that only the h:$
is that the pressuriser was never emptied.
operator's timely initiation of EPI prevented this from occurring, but 4 ?. % :
the data seems to support our contention that the pressuriser was never
$m$e h,
g';,
J.E entirely drained.
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-r As a&iitional information becomes available. I will forward it ta you 1 :
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for your reports saa files.
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If you have may further questions, ple.ase do not hesitate to cantact ze.
h I
Very truly yours.
j f.C.
.gige r
L C. Rogers s"
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.Jtite Operations Managar
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