Proceedings of the 3rd AEC Air Cleaning Conference, WASH-170 · 192 calculatinc grotmd...
Transcript of Proceedings of the 3rd AEC Air Cleaning Conference, WASH-170 · 192 calculatinc grotmd...
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METEOHOLOGICAL J\Dl'ECTS OF AlH CLEANING
·Althou:::;h there are many topics which ahould be mentioned while
considering meteorological aspects of air cleanine, this opportunity is
is boing used to review the effects of vertical temperature gradient on
stack eas behavior and to show s~r.ie photographs from the National Reactor
Testine Station illustrating typical conditions.
The appearance of stack effluent plumes is regulated largely by the
conficuration of the vertical gradient of air density, or temperature • .
With respect to a high stack on nearby level terrain there are five
diff crent con.figurations of the vertical temperature gradient that occur,
and these usually have a diurnal cycle.
These configurations, along with the expected behavior of an effluent
plu.'11e, is sho\m schematically in Figure 1.
Looping - occurs with a superadiabatic (very unstable) temperature lapse
rate. The stack effluent, if visible, appears to loop because .
of relatively large thermal eddies in the w-.lnd flow. Diffusion
is rapid, but sporadic puffs having strong concentrations are
occasionally brought to the ground near the base of the stack.
Loopine is favored by fair weather with r.elatively light w.inds.
- occurs with a grad:i.ent lyine between dry adiabatic and
isotherp.:i.l. The effluent stream is shaped like a cone with
axis horizontal.. Thti distance from the stack that effluent first
coraes to the ground is greater thnn with looping. Mechanical
mixiti0 predo;ninc.tes. · Al th ouch this condition is ideal for
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192
calculatinc grotmd concentrations by means of diffusion
equ.:i.tions, it docs not often persist except durinc cloudy,
windy \·reather. Durine fair weather, it is transitional and is
most likely to occur only for a brief interval about sunset as
the strong daytime lapse condition is converted to an inversion.
Fanning - occurs with temperature inversion conditions. Such laminar flow
may also occur in n·layer of air that is isothermal, depending
on wind speed and roughness of terrain. The stack effluent
diffuses practically not at all' in the vertical, and the effluent
trail may resemble a meandering river, widening very gradunlly ;
with distance from the stack. Depending on the duration of the
stable period and the wind speed at stack level, the effluent
may travel for many railes with little dilution. With level
terrain ground concentrations of effluent ·ao not occur;. however,
isolated objects which 'extend up into the pl1Ji11e, or hillsides
.which are encountered, can receive large concentrations even
though miles away from the stack.
Lofting - is usually associated with the transition from lapse to jnvcrsion,
but may persist at times for one to several hours. Occasio:ially
the inversion does not build up to stack level durine an entire
night due to interference of winds and/or cloudiness. The zone ,·
uf stronger effluent concentration, as shovm by shadin0, will
depend on the heip,ht of the inversion. It is caused by trapping
by the inversion of effluent carried into the stable layer by
turbulcr.t eddies that penetrate the layer for a short distnnce.
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I WASII-l'{O
Except \";hen the top pf tho inver:;ion is very near t.he ground,
this t;ype muy be corwidcr.:?d as the most favorable diffusion
situJ.tion to l:c cncountcn:d. IJ.'hc invl!r.:;ion prevents effluent
from re;i.chin& the nround; and at the same tiMe the cf fluent may
be rapicily dilutccl in the lapse leyer above the inversion.
Fumigating - occurs at the ti;:ie that the nocturnal inversion is being
dissipated py he at from the morning sun. The lapse layer begins
at the ground and works its 1-1<1.y upHard, rapidly· in sUJ-:L11er, but ·
slowly in winter. At some time the inversion is just above the
t~p of the stack, and actj_ng :is a lid, forces the effluent strew'l
to dilute within the shallo'.r lapse layer near.the ground. Laree
concentrations are hrougj'lt to the grotmd ai·ong the entire effluent
strea.:'Il by thermc.:.1 eddies in ~he lapse layer. Sustained conccntra-
tions near the ground will be higher with this situ~tion than
with ~r other.
Smoke experiments were pe~fon:ied by the Weather L>ureal.J. using the
' · 250-foot Chemical Plarit st::i.cl< to detcrntine the validity of the associat:i,ons
of plume behavior with the temperature gradient configurations ju$t shmm.
Pictures of smo1<e behavior during so1r.e of these experiments are shown on
the slides to follow.
Figure 2 - Looping condition. 0945 ll..ST, April 9, 1952.
Tom1~rnturo 10.poe rato was moro than throo ti.moo the dry
adiabatic ruto (which is o.r;;4°F./100 ft.) in tho lowor
250 :foot.
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Figuro 3 - Coning condi tiono. 1910 MST, l.,,Pril 16, 1952.
Lnpoo rnto in loW'.cr 250 foot wo.s slightly leoo than tho I
dry ndinbutic ro.te.
Figuro 4 - Funning condition. 0722 MST, April 111 1952.
Pronounced tompornturo i~voroion from tho surface to
eomewhero above 500 feet.
Figure 5 - Lofting condition. 1945 MST, April 16, 1952.
Inversion, surface to 200 foot, with lapse nbovo 200 feet.
Figure 6A - Fumigating condition. 0746 MST, April 11, 1952·
Lapse lnyer has worked up just to the 250-;f'oot level. Note
that eddie'.3 in the lnpse layer have begim to penetrnto the
smoke-bearing ~er, as evidenced by streamers extending
downward from the concentrated plume.
Figure 6B - Fur:ligution {continued). 0748 MST. The first
·stream.er reached tho ground about 10 stack lengths from
the stack about two m:tnutes after streamers begnn to decend.
Inversion based about 300 feot.
Figuro 6c - Fumigntion {continued). 0802 Vi.ST. By this
time otrong omoke concentrations appeared on the ground
along almost tho entire visib1e length of the plurr.e. Note
that the concontrutod arn.oke .layer aloft that wo.s vioible
in Figu1·00 l~, 6A t:md. 6B is no longor vioiblo. The entire
plurr.c n;ppeo.ro to have been mixod downward. Inversion
baaod n1Jo'..lt 380 f'oot.
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It Yns mentioned cnr~ior thnt tho typoo of tomporatu1~ gro.diont uounlly
hnvo a diurno.l cyclo. Thia io illuotro.tod by fiE:,'1.U'O 7 which givoa :plota of
tomporo.turo soundingo on o. clonr dn.y. Noto tbnt tho ~igo.ting condition
(for o. 250-:foot stuck) wno prosont nt 0900 MST. By llOO MST the inveroion
hnd disoi:patod, and looping conditions provo.iled until tho inversion begun
to form in tho evening. Lofting conditions wore present at 1830 and 2000
11..ST, and fo..nning conditions, at 0200 through 0700 MST the following morning.
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Fig. l--Scho1::ntic roprooo~tntion or stack eao behnvior undor variouo conditiona or vertical ot.ubility •
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