ML17174A105

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Proposed Tech Spec Changes 1.1-3.2.3 to Permit Reactor Power Ascension to Proceed Along Modified Power/Flow Line,For Dresden Facility
ML17174A105
Person / Time
Site: Dresden Constellation icon.png
Issue date: 11/01/1979
From:
COMMONWEALTH EDISON CO.
To:
Shared Package
ML17174A103 List:
References
NUDOCS 7911060334
Download: ML17174A105 (6)


Text

  • .

ATTACHMENT 1 PROPOSED TECHNICAL SPECIFICATION CHANGES FOR DRESDEN 2 s ..

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DPR-19 1.1 SAFETY LIMIT 2.1 L:IMITING SAFETY SYS'l'EM SETTING

1. APRM Flux Scram Trip Setting (Run Mode)

When the reactor mode switch is in the run position, the APRM flux scram settinq shall be:

S'= ~.SBW0 + 61 ~~;F]

with a maxium set potnt of 120% for core

' flow equal to 98 x 10 lb/hr and greater.

where:

S

.w 0

~ settinq in percent of rated power

=percent of drive flow required to produce a rated core flow of 98.

Mlb/hr. .

I TPF - LTPF un1ess the combination of power and peak LHGR is above the curve in Figure 2.1-2 at which point the actual peakinq factor value shall be used.

  • LTPF = 3.05 (7x7 fuel assemblies) 3.01 (8x8 fuel assemblies) 2.98 (8x8 R fuel assemblies)
2. APRM Flux Scram Trip Setting (Refuel or Startup and Hot Standby Mode)

When the reactor mode switch is in the refuel or startup/hot standby position, the APRM scram shall be set at less than or equal to .15% of rated neutron flux.

6

.. ************** ****** _, ........... ___ ..... -----**-*- .. **-*-* .... -*- -*-* --* -- -- -- ***-. ~*

DPR-19 1.1 SAFETY LIMIT 2.1 LIMITING SAFETY SYSTEM SETTING .,

Core Thermal Power Limit (Reactor B.

Pressure = 800 psig) 3.

  • IRM Flux Scram Trip Setting When the reactor pressure is ~eoo psig The IRM flux scram setting shall be or core flow. is less than 10% of rated, set at less than or equal to 120/125 the core* thermal power shall not exceed of full scale.

25% of rated thermal power.

c. Power Transient B~ APRM Rod Block Setting
1. The neutron flux shall not exceed the scram setting established in Specif ica- The APRM rod block setting shall be:

tion 2.1.A for lon<Jer than*1.s seconds as indicated by the process canpute~.

2. When the process ~omputer is out of SL f~o*sawD sol-1 . fi.TPF]

+

\2'PF service, this safety limit shall be assumed to be exceeded if the neutron The definitions u~ed above for the APRM flux'exceeds the scram settin<J scram trip apply. .

established by Specification 2.1.A and a control rod scram does not occur.

o. Reactor Water Level (Shutdown Condition)

Whenever the reactor is in the shutdown condition with irradiated fuel in the reactor vessel, the water level shall not be less than that correspondinq to 12 inches above the top of the active fuel when it is seated in the core.*

  • Top of active fuel is defined to be 360" above vessel zero. (see Bases 3.2) 7

DPR-19 ROD BLOCK APRM BACKUP SCRAM INTERCEPT LINE

.. .:..:.... - - - . -,- - -r--

/

100

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Oi'lf1Al1NG RIGION SUl'i'Oi-ll D II BY N.r.n 0. - 24167 Op:*rating on Single Loop I or Natural* Circuletion is I.imi.ted per Tech Specs.

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DPR-19 ll(SA'F..O~'"l'AT!~i~ 'IF.:\T I~!ITL'\".L-l:S ~C!> ~L~< ._ '-~

TC!lble 3.2.3

~~:::-i'.!>l~ In:tt.

cr..~~:;~ls Pc=

~::-!.*> 5,.,*::t~(l)

  • I:1str._:=cr.t Tri-:> t.~vel S-"'~~i~~

.-::..::..:;;...;...r_.:;..o..;=-=-..=..;...;;..:..:::..:-4---~-?-:---.:-*:JJ-__ -~.:-::-:.-c-a-1-~-:;;..;cr-:;;.*,. .; ;._.;: ;. , . ;: ;. ;.;.b;.; i; ;.c:o;.,=-:::...>--

. (-7-,---------~, L-
r=--,_,;;.;;;_ * ** '.1 ** Lrwwm:.

1-L:0.5Sw0 + SOJ ~ ( 2)

TPF

.. 1 II ~ 12/125 *.fUil. scale I

2

  • 1* 2 J/12; ~full .scale bi~s} (7l ;- ~ o.65Wo 1

l Red blo:i<.

~o~ bloc~ ~onito~ tlO-*-:l:iC~le

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+ 42 ( 2)

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  • > 5/125 !-::1:!. ~cal-:?

3 3 ~103/125 full.sc~l~

.. 3 IR?! cfot~cto~ not fulJ.}* in3~rted in t~c co::-~

2(5) SP.n cli:?tcctor not in nto.rt:\:p po::.H:io:i (4) 7.(5 (6

\*

DPR-19* '-

TA3~~ 3.2.3 (c6ht)

t::otc5:
  • 1. For the St<?.rtl.:p/~ot St<:tndby a:ld Run po~itio:lz of tho F.eactor W~C!e Selector Switch.*

therc :;h~~-1 be tv.:o cp':'!runic or t::::-:..ppc:c\ t::-i? ~y:::;'.::c~3 f~r c;;a.ch fu:-.ctior.; c:::*:ccpt t~c 4

Si:..'~ r.od bloc!~s, IP..M tlp5c<:ll~, IR:*1 ciown:.:c;.tl.:? ar,d l?J*i d~t~ct-:>r r.o~ ful~y ir.s~::::-tcd in t!:~ co;::-c n~~ci not. b~ opcrublc i'1 th0 "r~*.lT!." po::;i'd.0:1 u:icl id~~1 C:o*.-msculc, .i\??.:*1 upscale (flow bias), RBt.f *upscule, and RBI-I downscale need not be operable in the Startup/Hot

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opcr~hle sys te:-a is fl.i;-i(: tio:1<:llly tcs'<.:ccl irr.:71(!Uic). t.c ~y ci.~:1 d~i ly th~rc~£tcr; if this .

co::C.i t. ic;1 la 5tz lons'2:::- th.~n ~c*.-c:l d;::y:; the ~ys ~cD s'hull b~ tr ip9sd. If the fir.st colu:r.:1 c.'.ln;1ot be m~'.: for both trip ~y*~tc::i::;~ th~ sy:;tc:ns shull :Oc t:ripp\!ci.

Wo - perci?nt nf drive flO:*; req:..i1red to produce a r<!ted core flow of 98 Mlbuihr*.

3.  !~1 down~cole m~y be bypassed when it is on its lowest r~nge.
4. This function may be bypass.~d *.when th~ cc'.lnt rat~ is ~100 cps.

S. One cf the fo*..ir* S?,H. inputs r.iu.y be oyp:lsscci.

This SP""'1 .functio:1*ma:-r~ be *byp<l:;scd in t;1c higher IRH =~ns-es ,,.,.hen the IR.L'1 u?scale red 6;.

block is opcrub!.~. e

7. Not requirc::d v/hile perfonning low pow~r physics tests at utmosphcr.ic pressure during or after rcfucli~g at power levels n6t to cxc~~d 5 ~~1{t}.