may the force be with the particles!
DESCRIPTION
Electrical Migration. Reading: Chap15. May the force be with the particles!. Q: Difference between impaction and electrostatic collection in terms of forces acting on the system?. Millikan Experiment. (Robert Millikan, US, 1868-1953) Nobel Laureate, 1923. Electrostatic Force. - PowerPoint PPT PresentationTRANSCRIPT
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04/22/2023 1Aerosol & Particulate Research Laboratory
May the force be with the particles!
Q: Difference between impaction and electrostatic collection in terms of forces acting on the system?
Reading: Chap15
Electrical Migration
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04/22/2023 2Aerosol & Particulate Research Laboratory
Millikan Experiment
(Robert Millikan, US, 1868-1953)Nobel Laureate, 1923
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04/22/2023 3Aerosol & Particulate Research Laboratory
• Coulomb’s law
• Units (esu)
• Electric Field
221
rqqKF EE
xW
qFE E
q = ne (e: unit charge)
Statcoulomb (stC): the charge that causes a repulsive force of 1 dyne when 2 equal charges are separated by 1 cm (3.3310-10C)Unit charge: 4.8 10-10stC (1.610-19C)
Electrostatic Force
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04/22/2023 4Aerosol & Particulate Research Laboratory
Electrical Mobility• Terminal velocity in an electrical field
qEBd
qECVp
cTE
3
c
TEp
CVd
qE3
(force balance)
qBd
qCE
VZp
cTE 3
(for Re < 1)
Charging MechanismsFlame ChargingStatic Electrification: Electrolytic charging, Spray electrification, Contact chargingDiffusion ChargingField Charging
Q: physical meaning?
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04/22/2023 5Aerosol & Particulate Research Laboratory
Diffusion Charging• Random collisions between ions and particles
– No external electrical field needed; independent of materials
kTtNecd
ekTd
q iipp
2
1ln2
2
Total charge
Q: Does q depend on time? on composition? on size?
STP) @ cm/s 10(2.4
speed lion thermamean 4
ic
Ni: ion concentration
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04/22/2023 6Aerosol & Particulate Research Laboratory
Field Charging• Bombardment of ions in the
presence of a strong field
4
23 2
ps
Edq
Saturation charge
Q: Is the charging rate dependent on particle size? On field strength?
tNtNEd
qi
ip
i
i2
eZ 1eZ
4
23
Charges by field charging
Zi: ion mobility (450 cm2/stVs): dielectric constant
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04/22/2023 7Aerosol & Particulate Research Laboratory
Positive Corona Negative Corona+ - -
- +
-
-
-
+
+
+
- +
electron molecule particleCollection Plate Collection PlateElectrode Electrode
Step 1
+ -
+Step 2
+ -+Step 3
+
+
-Step 4
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04/22/2023 8Aerosol & Particulate Research Laboratory
1 2 3
(28) (24) (12)
1 2 3
Turbulent Flow with Lateral Mixing ModelElectrostatic Precipitator
Three assumptions:
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04/22/2023 9Aerosol & Particulate Research Laboratory
Electrostatic Precipitator• Deutsch-Anderson Equation
RdtV
RdtRV
NdN TETE 22
2
)2exp()(
0 RtV
NtN TE
QRLVPE
QLRt
tLRQ
TE
2exp11
22
QAVE cTEexp1area)colletion (total 2 Define RLAc
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04/22/2023 10Aerosol & Particulate Research Laboratory
Comparison of Diffusion & Field Charging
Q: How does n vary wrt dp? Which mechanism is more important?
Q: Does collection efficiency increase as particle size increase (because of a higher number of charges)?
dp (um) ndiff nfield ntotal Zdiff ZField Z (stC•s/g)0.01 0.10 0.02 0.12 0.66 0.10 0.760.02 0.30 0.06 0.36 0.49 0.11 0.600.05 1.1 0.40 1.50 0.31 0.12 0.430.1 2.8 1.6 4.38 0.23 0.13 0.360.2 7 6.5 13.2 0.18 0.17 0.350.5 21 40 61.2 0.15 0.30 0.451 48 161 209 0.16 0.52 0.682 108 646 754 0.16 0.98 1.145 311 4035 4346 0.18 2.34 2.5210 683 16140 16824 0.20 4.61 4.8020 1490 64562 66052 0.21 9.16 9.3750 4134 403510 407644 0.23 22.78 23.0
Number of Charges vs dp
dp (um)0.01 0.1 1 10
n
10-2
10-1
100
101
102
103
104
105
106
Diffusion chargingField Charging
Nit = 107 s/cm3
= 5.1E = 5 KV/cmT = 298 K
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04/22/2023 11Aerosol & Particulate Research Laboratory
ELectrical Mobility vs dp
dp (um)0.01 0.1 1 10
Z (s
tC.s
/g)
0.1
1
10 Diffusion chargingField ChargingCombined Charging
Typical fly ash size distribution
Q: If the ESP is used to collect the fly ash, how will the particle size distribution at ESP outlet look like?
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04/22/2023 12Aerosol & Particulate Research Laboratory
Equilibrium (Boltzmann) Charge Distribution
kTden
kTdef
ppn
22
exp
dp Average % of particles carrying the indicated number of charges(m) Charges < -3 -3 - 2 -1 0 +1 + 2 + 3 > +30.01 0.007 0.3 99.3 0.30.02 0.104 5.2 89.6 5.20.05 0.411 0.6 19.3 60.2 19.3 0.60.1 0.672 0.3 4.4 24.1 42.6 24.1 4.4 0.30.2 1.00 0.3 2.3 9.6 22.6 30.1 22.6 9.6 2.3 0.30.5 1.64 4.6 6.8 12.1 17.0 19.0 17.0 12.1 6.8 4.61.0 2.34 11.8 8.1 10.7 12.7 13.5 12.7 10.7 8.1 11.82.0 3.33 20.1 7.4 8.5 9.3 9.5 9.3 8.5 7.4 20.15.0 5.28 29.8 5.4 5.8 6.0 6.0 6.0 5.8 5.4 29.810.0 7.47 35.4 4.0 4.2 4.2 4.3 4.2 4.2 4.0 35.4
tNeZntn ii4exp)( 0
Number of charges on a particle after it has been exposed to a bipolar ion concentration
(dp > 0.05 m)
pdn 37.2Average equilibrium charge
(dp in µm)
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04/22/2023 13Aerosol & Particulate Research Laboratory
Bipolar Charging
Q: How to produce bipolar charges?Soft X-ray (< 9.5 keV)
• Radioactive source: Kr-85, PO-210• Alternating corona
http://en.wikipedia.org/wiki/File:Krypton_discharge_tube.jpg
Kr discharge tube
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04/22/2023 14Aerosol & Particulate Research Laboratory
Electrical Measurement: Electrical Mobility Analyzer
VLUhZ pL
22 V: potential difference between plates
U: mean flow velocityh: half the inter-plate distanceL: inlet to exit distance
Q: If monodisperse aerosols are introduced, what information can we obtain using this instrument?
hVE2
U
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04/22/2023 15Aerosol & Particulate Research Laboratory
Electrical MeasurementEAA (Electrical Aerosol Analyzer) DMA (Differential Mobility Analyzer)
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04/22/2023 16Aerosol & Particulate Research Laboratory
Smoke Detector – Ionization type
Ionization Chamber
http://en.wikipedia.org/wiki/Smoke_detector
• 241Am emitting particles as the radiation source. • particles permit a small, constant current between two
electrodes• If particles are absorbed by smoke aerosol absorbs, the
current is interrupted which sets off the alarm
http://www.cna.ca/curriculum/cna_nuc_tech/images/smoke1.gif
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04/22/2023 17Aerosol & Particulate Research Laboratory
Reflections