연세대학교 화학공학과 이 태 규 제 4 회 광촉매 연구회 2004 년 2 월 26 일...
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연세대학교 화학공학과이 태 규
제 4 회 광촉매 연구회2004 년 2 월 26 일
Comparison of Mercury Removal Efficiency from a Simulated Exhaust Gas by Several Types of TiO2 under Variou
s Light Sources
Mercury
• Toxic properties
• High volatility
• Tendency to bio-accumulate
IntroductionIntroductionIntroductionIntroduction
Emission resources
• 80% of the total emission from the combustors (Coal Combustors, Waste Incinerators, etc.)
Hg Emissions Control MethodsHg Emissions Control Methods
IntroductionIntroductionIntroductionIntroduction
• Oxidized mercury can be captured relatively easily because of its high solubility in weak acidic solution
• Elemental mercury is difficult to capture
• Unusual non-reactivity compared to other metals– 5d106s2 closed shell electronic structure for Hg atom– extremely slow or no oxidation at high temperatures
– possible oxidation by strong oxidants (NO2, Cl2)
=> most widely used
Activated Carbon
Hg removal by adsorbents
IntroductionIntroductionIntroductionIntroduction
Photocatalyst TiO2
high removal efficiency for low concentrations of toxic compounds
disadvantagedisadvantage
Low applicable temperature range Low regeneration rate & slow adsorption rate
Hg removal under UV
light
IntroductionIntroductionIntroductionIntroduction
- high energy strength- harmful- development of improved photocatalysts activating
under the visible light!!!
UV light
Hg removal using a TiO2
under the fluorescent light
Intermediate
step
Hg capture by TiOHg capture by TiO22
TheoryTheoryTheoryTheory
Hg TiO2 HgO
OH•
H2O
O2
O2-
Hg HgO
Light
e-
+
+
H+
TiO2(s) + light → TiO2·OH + Hg(g) → TiO2·HgO(complex)
ApparatusApparatus
ExperimentalExperimentalExperimentalExperimental
ParticleFree Air
N2
Oilbath
ElementalMercury
(Hg0)
TemperatureController
MFC
MFC
Mixing
Light Source
TiO2
Filter
HoodOn-line
Hg Analyzer
GlassBead
Ontario- Hydro Method
• UV black lightUV black light
• UV sterilizing lightUV sterilizing light
• fluorescent lightfluorescent light
• blue lightblue light
• UV black lightUV black light
• UV sterilizing lightUV sterilizing light
• fluorescent lightfluorescent light
• blue lightblue light
• pure anatase pure anatase (Ishihara co.)(Ishihara co.)
• P25 P25 (Degussa co.)(Degussa co.)
anatase : rutile = 80 : 20anatase : rutile = 80 : 20
• pure rutile pure rutile (Junsei co.)(Junsei co.)
• pure anatase pure anatase (Ishihara co.)(Ishihara co.)
• P25 P25 (Degussa co.)(Degussa co.)
anatase : rutile = 80 : 20anatase : rutile = 80 : 20
• pure rutile pure rutile (Junsei co.)(Junsei co.)
Light Sources TiO2 Powder
ExperimentalExperimentalExperimentalExperimental
Wave lengthWave length
ExperimentalExperimentalExperimentalExperimental
wave length (nm)
200 300 400 500 600 700 800
co
un
ts
0
1000
2000
3000
4000
5000
blue lightfluorescent lampUV black lightUV sterilizing light
UV-C UV-B UV-A Visible Light Infrared Ray
time (s)
0 1000 2000 3000 4000 5000 6000
Hg
re
mo
va
l e
ffic
ien
cy (
%)
0
20
40
60
80
100
Ishihara (anatase)Degussa (P25)Junsei (rutile)
Off
On
[a] UV black light[a] UV black light
ResultsResultsResultsResults
time (s)
0 1000 2000 3000 4000 5000 6000
Hg
re
mo
va
l e
ffic
ien
cy (
%)
0
20
40
60
80
100
Ishihara (anatase)Degussa (P25)Junsei (rutile)
Off
On
[b] UV sterilizing light[b] UV sterilizing light
ResultsResultsResultsResults
time (s)
0 1000 2000 3000 4000 5000 6000
Hg
re
mo
va
l e
ffic
ien
cy (%
)
0
20
40
60
80
100
Ishihara (anatase)Degussa (P25)Junsei (rutile)
Off
On
[c] fluorescent light[c] fluorescent light
ResultsResultsResultsResults
time (s)
0 1000 2000 3000 4000 5000 6000
Hg
re
mo
va
l e
ffic
ien
cy (
%)
0
20
40
60
80
100
Ishihara (anatase)Degussa (P25)Junsei (rutile)
Off
On
[d] blue light[d] blue light
ResultsResultsResultsResults
Breakthrough ExperimentBreakthrough Experiment
ResultsResultsResultsResults
TiO2 activated
carbon
average time to reach 80% of the initial Hg conc.
~ 570 hrs ~ 40 hrs
amount of Hg per gramof adsorbent
~ 48.0 mg ~ 2.5 mg
cost per gram of adsorbent
3~5 원 2~4 원
estimated costper gram of Hg
~ 104.2 원 ~ 1600 원
XRD pattern of (TiOXRD pattern of (TiO22-Hg) Complex-Hg) Complex
ResultsResultsResultsResults
ConclusionConclusionConclusionConclusion
The removal efficiency was close to 100% under most light sources tested.
More than 99% of initial Hg was removed under all the light sources tested except for the blue light still achieving a Hg removal efficiency close to 80%.
High efficiency was achieved even under the low concentration.
Easily maintainable and cost-effective fluorescent light can be used.
Hg removal by sunlight
Future WorksFuture WorksFuture WorksFuture Works
• Verification of Hg removal efficiency with crystallinity, surface area, and particle size
• Verification of Hg
adsorption mechanism
under the visible light
• Hg removal by TiO2
directly coated on beads
• Application of TiO2
coated ferro-powder to
water treatment
• Furnace 온도가 증가함에 따라 크기가 커지지만 open structure 를 가진 입자를 생성
• 입자의 크기가 증가할수록 수은의 제거효율 증가
• NH3 를 이용하여 TiOx-Ny 를 제조 , 가시광선에의
반응성 측정 및 촉매 특성 분석
Structural Effect of In Situ Generated TiO2 on Hg0 Removal in a Simulated Combustion Flue Gas
Hood
On- lineHg Analyzer
HgQuartzReactor
Air
Nitrogen
TiPrecursor
SecondaryFurnace
Filter
UV Lamp
TemperatureController DMA
CPC
Argon
PrimaryFurnace
OilBath
Structural Effect of In Situ Generated TiO2 on Hg0 Removal in a Simulated Combustion Flue Gas
Ti Precursor (g) TiO2 (g) TiO2 (s) Hg0 (g) UVHgO (g)
Ti(OCTi(OC33HH77))44 + 18O + 18O22 → TiO → TiO22+12CO+12CO2 2 +14H+14H22OO
Structural Effect of In Situ Generated TiO2 on Hg0 Removal in a Simulated Combustion Flue Gas
1.88 1.81 1.70Df 1.761.93
175 188 201 225 247
55.18 74.86 90.98 108.73 129.01
dg (nm)
Rg(nm)
14.2 25.3 62.5Hg captureefficiency(%)
41.43.3
Structural Effect of In Situ Generated TiO2 on Hg0 Removal in a Simulated Combustion Flue Gas
raman cm-1
100 200 300 400 500 600 700
cts
4000
6000
8000
10000
12000
14000
pure TTIPHAB; 5cm
Preparation of Column Shape TiO2 Fiber by a Diffusion Flame Reactor
• Height above burner (HAB) 에 따른 particle shape / crystallinity ; fibrous / anatase
• Raman Spectroscopy
Apparatus
Figure 1. Schemetic diagram of multiport diffusion with particle collection system
Controllerto Move mat
TTIPPrecursor
&Heatingmantle
DiffusionBurner
Slide Glass
MFC
MFC
MFC
MFC
N2
O2
LPG
Air
SEM I
<Figure 1. Pure TTIP, HAB=3cm> <Figure 2. Pure TTIP, HAB=5cm>
<Figure 4. Pure TTIP, HAB=10cm> <Figure 3. Pure TTIP, HAB=7.5cm>
SEM II
The End