may the force be with the particles!

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7/04/2022 1 Aerosol & 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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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 Presentation

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Page 1: May the force be with the particles!

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

Page 2: May the force be with the particles!

04/22/2023 2Aerosol & Particulate Research Laboratory

Millikan Experiment

(Robert Millikan, US, 1868-1953)Nobel Laureate, 1923

Page 3: May the force be with the particles!

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

Page 4: May the force be with the particles!

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?

Page 5: May the force be with the particles!

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

Page 6: May the force be with the particles!

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

Page 7: May the force be with the particles!

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

Page 8: May the force be with the particles!

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:

Page 9: May the force be with the particles!

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

Page 10: May the force be with the particles!

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

Page 11: May the force be with the particles!

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?

Page 12: May the force be with the particles!

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)

Page 13: May the force be with the particles!

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

Page 14: May the force be with the particles!

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

Page 15: May the force be with the particles!

04/22/2023 15Aerosol & Particulate Research Laboratory

Electrical MeasurementEAA (Electrical Aerosol Analyzer) DMA (Differential Mobility Analyzer)

Page 16: May the force be with the particles!

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