metallic layers in the mesosphere - cedarweb.vsp.ucar.edu file1992 annual cedar meeting metallic...
TRANSCRIPT
1992 Annual CEDAR Meeting
Metallic Layers in the Mesosphere
John M.C. Plane
School of Environmental Sciences
University of East Anglia
Norwich
United Kingdom
This work has been supported by NSF Atmospheric Sciences (Aeronomy)
and the SERC of the United Kingdom
3 a o P w o 13 P O a O C in n tr
o 0-
»-•
•
1-t
fD to
Per
seid
met
eor
ions
inat
mos
pher
e
t
G
} I f it r
y JSr r
2 p̂f
I' i
XI
o r-^
o'
o -♦<
3 (t
r*+
-
o o 5* o =r
-1 o D Ql
• (6
Rat
ioof
free
met
al/N
oin
nn
eso
sph
ere
f 1 Metol precursor4
in tantalum Doat
Thermocouple
Photomultiplier
1^1 Quortz end—window^—^*~and interference filter
in
Dye loser
Suprosil window
set ot Brewster's ongle
CENTRAL
CHAMBERPUMP
Suprcsil window->>y—^
Excimer loser
Thermocouple
HeaterControl
ThermocoupleRead-out
HV
Power
Supply
Piooam
meter
Excimer
Laser
Li
t-e-
Beam—steerer
Iris
Lt
Filter
/ Beam-7 steerer
Beamsteerer
Beamexpander
Pump
HV
Power
Svpply
Photodiode
..J.
Boxcar
Averaging System
o
#
cr^
rn
Po
tv
Hj
Cl p 1J
u-1
prt
f
^1-
rx
}i-
r T
•s
?s-
s>
I
1 a_
o P
rrr>
Oo
•-
+O
O(>
>g
..o
I p Od 3 <
»
I—1
.0"S
>5r ?
>V
*"
LIF
sign
al(a
rb.
unit
s)
LIF
aign
al(o
rb.
unit
s)
I- t?
S o s: (A 0
t:
^ to r
O r
lo
IOT
CM
IJ)DU
So
ECO
Eo
1.0E-29::
1.0E-30-:
l.OE-31
150
Li + O2 + N2
No + O2 + N2
K + O2 + N2
2000
V)
i?3O
o
Eto
Eo
T/K
400 300 250
1.0E-9"__^ T-t T• I •
i
200
• Kolb et al.
• Ager and Howard
T
Na + O3 (this work)
NaO + O3 (this work)
1.0E-10--
5.0E-112.5E-3
i
Ager and Howard
—I3.0E-3 3.5E-3
44.0E-3
1 /T(K-1)
+
4.5E-3 5.0E-3
Co'6lirtg colls and
insulation \
Waeeif-tftJdled metal
vdpeut injector
Carrier gasinlet
No- + Oj^ ♦ K)j —• •*•
NaO^ ♦ O KkOf O.
Pressure
Photomultipliertube \
VSfltnplingorifice
QutdrupoleiMaat
Photoionizatlonport
Pre filter
jLonsource
hil86 eHUKtlTi^ehflflHeltfWh
Turbo molecular
pump housing
Reactant gas Qinlets
Ion transfer' optics
Mechanicalbooster pump
CU ctwMttj-k,. [n«] |[0»l[W|i"l(r'ja-M)M
=: (i t t 0-4)^10""^300 K.
Neutral and lonii
Rg^ctiQjo
Neutral Chemistry with Oxygen only
* 1. Na+ O3 --> NaO + O2
* 2. NaO + O --> Na(2p,2S) + O^
* 3.
4a.
4: 41b.
* 5.
6.
* 7.
Na +Oj + M --> NaOj +M
NaO + Oj -> Na+202
NaO + O3 ~> NaOj + Oj
NaOj + O --> NaO +Oj
NaO + Oj+ Nj -> NaOj + Nj
Na03 +0 --> NaO +Cy,
Neutral Qtemdstry wiitli H, O and COj
* 8. NaO + Hp --> NaOH + OH
* 9a. NaO + H^ --> NaOH + H
* 9b. NaO + Hj -> Na + H^O
* 10. NaO + H --> Na + OH
ixtfe CO'XSt'ftAt
in the Mesosphere
Rate Coefficient
i.5 X10''exp(-220/tenip)
1.5 X10-'exp(-383/temp)(branchingratio^ = 0.2)
4.7 X10-»(temp/200)-'
3.2 X10-'° exp(-550/temp)
1.5 X10'' exp(-^36/tenip)
1.0 X10-'eKp(-1300/temp)
5.3xl0^(200/temp)
3 XlO"'** sqr(temp/290)
8 X10 '̂° exp(-374/temp)
l.'l X10-'exp(-1100/temp)
1.1 X10-'exp(-1400/temp)
3 X10-'° exp(-668/temp)
o 11. NaOj +H --> NaOH +0 3x10"'" exp(-2000/temp)
12. NaOH + H -> Na + HjO 5 X10"'° exp(-1000/temp)
* 13. NaO + COj +Nj --> NaCOj +Nj 1.3x 10-"(200/temp)
o 14. NaCOj + O -> NaOj +CO, 1 X10-'exp(-1400/teinp)
o 15. NaCOj +H --> NaOH +CO^ 1 X10-9exp(-1400/temp)
*- 16. NaOH +CO2 +Nj -> NaHCOj +N^ 1.9 X10"^* (200/temp)
17. NaHCOj +H --> Na +HjO +CO, 1 X10''exp(-1800/teinp)
Ionic Chemistry
* 18. Na + Oj* -> Na+ +02 1.4 X 10"'
* 19. Na + NO* --> Na* + NO 1 X 10'
c 20. Na^ +Nj +N^ -> NaN,* +N, 2.5 X10" (teinp/200)-' ^
0 21. Na.X+ + e- --> Na + X 1 X10^ (200/tetnp)''̂
nK)tcx:lieiniical reactions
* 22. NaO^ +hC5 —> Na02 + O2 4 X 10"'
23. NaOH + hOJ --> Na + OH 1 X 10-5
c 24. NaOj + htD -> NaO +O2 1 X 10^
* 25. Na + hGJ -> Na+ 2 X 10-5
D
o
Cp.\u*WJ (^HtUcr ei/JUiuX^ 4/c
Jiv^ydf b«A h iJLAJ^Ot^/lt
Meteors
X = N2 Ablation
ondensation
Na.X
NaHCQ
C0..11
COo ,M NaOH
NaCOo
-0.2^
+0.8
l^y
-0.jZ,
Sodium Superoxide
0 Y+0.3
Sodium Ozonide
-0.74-0.79 +0.85
+0.98+0.43 +0.95
-0.32-0.72
(a) NaHC03(^A') (b) NaC03(2A')
-0.77-0.72
+0.37 +0.87
-0.43
-0.78
(c) HCO3" (U') (d) CO3 (202)
Model of Sodium in the Mesosphere
n^teoric input of Na of (1 ±0.2) x10^ atoms cm'̂ -s ' (Hughes. Gadsden)ablation profile from Hunten et al. (1980)
M 11 " ""vertical mixing
be solved as afunction of altitude
panWonlng of sodiun, is g.«r«d b, the o.ly.He seasonal ..d lafi»de dependence of ,.n,>e,a..re, p«ss»e. edd, dlffus.oncoefficient is included
seasonal de^ndenc of nUno, spedes O, Hand 0, is included
variable parameters.meteoric input flux
total Na at 65 km
/c(NaOH + H)
the photolysis cross-section of NaOHjt(NaHCO, + H)
aX
Q)
s
0)•d
105--
100--
00
105"
100--
40ON, Summer, Noon
10 100 1000
Concentration / cm""^
40ON, Summer, Midnight
10 100 1000
Concentration / cm~^
NaHCOs^
1E4
NaHCOsN "
1E4
•d^3
105"
100"
90"
85"
40®N, Summer
I r . I Mitl
Noon
Midnight
100 1000 1E4
Concentration / cm""^
6
•P
Comparison between Model and Tilgner and von Zahn (1988)70ON, Winter. Midnight
110 . . L. ^
100--
Column density = 5.0 (5.5±1.0) x lO^ cm 2Halfwidth (FWHM) = 10.5 (10.810.4) km i
I
Scale height =2.0 (2.5) km |I
Peak Na = 4680 (4940±560) cm~^~
Peak altitude =89 (B9.0±0.9)^^Scale height = -1.9 (—3.0) km
.(Scale height = -0.7 (-0.3) km
1— —I \—
2000 4000 6000
Concentration cm ^
-L
I
I
4-
8000
110-^
106
6looA
95"
-d13. %
90"
< 85-L
AH JiOU -I
75-
winter 35/86
suBMr 87
sunaer 88
OA «. y/cA~K"ury.
Sodium Density Profiles at
4 »-
winter (midnight)
- suunamer (noon)
1000 2000 3000 4000
Concentration / cm*"^
5000
lU,r
c\2
I
6o
m
aV
o
ou
(d
Temperature Dependence of Na Column Density, 40®N
7E9
6E9"
5E9-
4E9"
3E9 -
2E9-0^
1E9--
O BiUs and Gardner (1991)
# Model prediction
o o
o
170 180 190 200 210
Average Temperature (85 - 95 km) / K
220
Characteristics of Sudden Sodium Layers (SSLs)
form explosively at altitudes between 93 and 102 km, i.e. several
kilometres above the permanent global Na layer
have lifetimes of tens of minutes to a few hours, and then disappear
rapidly
the Na atom density in SSLs can be up to 40 times greater than in the
background Na layer: SSLs appear to come from a fresh source of Na
can extend over several hundred kilometres horizontally
appear most commonly between 1500 and 0000 hrs local time
occur quite frequently at low and high latitudes, but very rarely at mid-
latitudes cf. sudden Fe layers
strong correlation between sporadic-^ and SSLs
also appear when there is strong local heating (e.g. from 170 to 220 K in
under an hour) e.g. due to the passage of a tidal wave
o
2100 LST 2314 LST105
^e" 1 i—
!100 "
>— 1
95 -<^ _
^ Na90
851 I
80
1
1
30 March 1989^ : 1 1 I ^
0 3000 10000 20000 30000 40000
Density (cm"^)
K6^€ ^Gwi-dACr^ oaA Tey Lu.^
2 Chemical mechanisms
The striking correlation between SSLs and sporadic-£ suggests thatSSLs could be formed by the action of electrons or ions on a reservoir.
These charged particles could have large kinetic energies if they were causedby auroral precipitation, although this would only explain SSLs at high latitudes. Possible reservoirs include:
• neutral so<Mnin compounds involved in dissociative electron
attachment reactions (von Zahn and Murad, 1990)
e.g. NaHCOj + e" --> Na + HCO3-
Our recent ab initiocalculations (Rajasekhar and Plane, 1992) indicate
that this reaction is about 50 kJmol ' endothermic, so that NaHCOj is
stable with respect to thermal electrons. Reaction with atomic O mayalso be important; we have recently shown that the reactionNaO, +O --> NaO +Oj, k(300 K) = 1.6 x 10"" cm'molecule 's '
is fast (Helmer and Plane, 1992), so that a sudden increase in [O] willproduce Nafrom NaOj.
• Na* ions; these recombine with electrons extremely slowly, so the rate
of formation of molecular Na ions is important
e.g. Na* + X + N2 --> Na.X-^ + N^
Na-' + Oj --> Na0* + 02
The formation of the molecular Na ions would then be followed by
dissociative recombination with electrons;
e.g. Na.X'" + f --> Na + X
The rates for the clustering reactions are not known. However, this
mechanism may work if the rate of re-ionisation of Na by the reactions
e.g. Na + NO^, O2* --> Na-^ + NO.Oj
was slowed down by the removal of and O2* by the high electron
density in a sporadic-^ layer.
Also, if a large concentration of negative ions could be produced
(Swider, 1992):
e.g. e" (fast, 6eV) + O, -> O" + O
then O' + Na'^ -> O + Na
Unfortunately, O" also reacts very rapidly with O;
0 +0 -> 0, + e"
so that the concentration of negative ions will be limited.
Na cluster ions on the surface of dust particles. These are formed
from the recondensation of meteoric silicates, and are thought to be
about 10 nm in diameter:
(Na,Y,r (aos, +charged particle -> (Na^Yy)"^(Na^Y^r (g) +e- --> x.Na +y.Y
Thus, several Na atoms are formed for every electron that is consumed,
in accord with very recent observations (Gardner and coworkers, 1992).
Mesospheric Chemistries of Other Meteoric Metals
Potassium
• seasonal column abundance appears to be constant cf. sodium
• difficult to explain since the alkalis should all have very similarchemistries
• only the reaction K+Oj +Nj has been measured -twice as fast asNa reaction
Calcium
depleted relative to sodium by about 120, although the Ca/Na ratioin meteorites is about unity
the reaction Ca +O, + has apositive temperature dependence atlow temperatures -tnis could explain the summertime enhancementof Ca to Na
the reaction Ca +O, --> CaO +O, is very fast - perhaps furtherreactions such as
CaO + CO2 + N2 --> CaCO, + Nj
CaO + HjO + N2 --> Ca(0H)2 +
remove Ca permanently
Metal + O2 + N2
1.OE-29 V
m 1.0E-3p^|
0/ 1.0E-31
1.0E-32
1 .OE-33 - -
1 .OE-34
200 1000
/K
500.0
o
o 400.0
0)
C 300.0
X)c
^ 200.0o
D
•\ 100,0D
0.0
X 19820 1983• 1984• 1985
X
JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC
< 80
70-
Ca X 120
1000 2000 3000Number Density (cm-3)
4000
Magnesium
cannot be seen spectroscopically from the ground because of theHartley band of ozone
the reaction Mg + Oj + Nj ~> MgOj + Nj is extremely slow
the reaction Mg + O3 remains to be measured; if MgO formation israpid, then formation of MgCOj and Mg(0H)2 may remove Mg
the ionic chemistry of Ca and Mg is more complex than Na, becausethe Group 2 metals can form stable oxide cations:
Mg+ + 02 + N2 --> MgOj"^
Mg^ + Oj --> Mg0+ + 02
However,Mg02'̂ + 0 -> Mg0"^ + 02
MgO'̂ + O -> Mg+ + 02
compete very effectively with dissociative recombination withelectrons.
Iron
• Fe is depleted relative to Na by factors ranging from 3 to 20; the Felayer is more variableand is a few kilometres lower
• recent lidar observations (Gardner and coworkers) indicates largeenhancements at the equinoxes (comprehensive winter observationsyet to be reported?)
• Fe, like Mg and Ca, has a closed electronic s shell. Thus, it reactsvery slowly with O2. The O3 reaction is unknown at present.