Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer...

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Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth

Transcript of Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer...

Page 1: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Particle Control Technologies

Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin

Thayer School of Engineering at Dartmouth

Page 2: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Design Criteria• Design of a system which remove solid or liquid

particulate matter from a gaseous medium• Chacacteristics of gaseous medium and

particulate matter to consider in the design:

• Size T,P,Q,• Chem. Composition Chem. Composition• Resistance Pressure Drop

PM Control Device

Page 3: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency• Considering the wide range of size of

particulates, efficiency will be different for each size.

• The overall efficiency (can be calculated on a basis of total number (or mass) of particles

• Generally regulations are written based on mass, and efficiencies are calculated on mass basis.

Page 4: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency

• Efficiencies calculated on mass basis: i

ei

i

ei

L

LL

M

MM

: overall collection efficiency (fraction)

Mi: total mass input rate (g/s or equivalent)

Me: total mass emission rate (g/s or equivalent)

Li: particulate loading in the inlet gas to the device (g/m3)

Le:particulate loading in the exit gas stream, (g/m3)

Page 5: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency

• When the particulate size distribution is known, and the efficiency of the device is known as a function of particle size, the overall collection efficiency can be calculate:

jjm where

j: collection efficiency for the jth size

mj: mass percent of particles in the jth size

Page 6: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example 3.1 from the book

Page 7: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

1. Gravity Settler

2. Cyclones

3. ESP

4. Filters and Baghouses

5. Wet Scrubbers

PM Control Devices

Page 8: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Settling Chamber

• Efficient for particles with diameter of 10-50 m (depending on its density)

• Velocity through chamber < 0.3-3 m/s (to prevent reentrainment)

V

H

L

Page 9: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Settling Chamber

• Settling time < transit time through chamber

• t = H/vt = L/v

v

H

L

Lw

Qdv

L

vHdv

pt

pt

)(

)(

Settling chambers are cheap to build and operate but not preferred due to their large space requirement

Page 10: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Settling Chamber• Assuming unit density sphere at STP, vt and chamber Lw

are tabulated below: Assumed flow rate Q = 150 m3/min

Dp (um) Vt (m/s) Required Area

0.1 8.6 (10)-7 3 km2

0.5 1.0 (10)-5 0.25 km2

1.0 3.5 (10)-5 71000 m2

5 7.8 (10)-4 3200 m2

10 3.1 (10)-3 810 m2

Lw

Qdv pt )(

Page 11: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Settling Chamber

• Baffled Settling Chamber– Large particles can not

make sudden direction change and settle into dead space of chamber

– Baffle chambers are used as precleaners

Page 12: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclones

• :

Page 13: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclones

• :

Page 14: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclone Geometry

Page 15: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclone Geometry

Page 16: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclone Theory

Page 17: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclone Theory

Page 18: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclone Theory

2/3

2

D

mVVddragforce itp

Page 19: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclone Theory

Page 20: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency

Page 21: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency

(i) increase Vt (expensive, since DP Vt2, as we will see in the next slides

Page 22: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency

Page 23: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency

Page 24: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Pressure Drop

K: a constant depends on cyclone configuration and operating conditions. Theoretically K can vary considerably but for air pollution work with standard tangential-entry cyclones values of K are in the range of 12 to 18

Cyclone pressure drops range from about 0.5 to 10 velocity heads (250 to 4000 Pa)

Page 25: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Cyclone Analysis

Page 26: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example

Page 27: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example

Conventional Type (No:3) N=(1/H) (Lb+Lc/2) = (1/0.5)(2+2/2)=6

•Vi=Q/WH =150 /(0.25*0.5) =1200 m/min 20 Vi=20 m/s

Page 28: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ExampleCalculate efficiency for each size range witch dpc = 5.79 um:

2)/(1

1

pjpcj dd

Page 29: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example 4.5

Page 30: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example 4.5

Page 31: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example 4.5

Page 32: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP

Page 33: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP

Page 34: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.
Page 35: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Geometry

Page 36: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 37: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Corona Power vrs Efficiency

Page 38: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 39: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP THEORY

Page 40: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 41: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 42: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 43: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 44: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 45: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 46: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 47: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 48: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ESP Theory

Page 49: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Efficiency

Page 50: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Efficiency

Page 51: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Effect of Resistivity

Page 52: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

ResistivityResistivity (P) is resistance to electrical conduction and can vary widely

P of a material is determined experimentally by establishing a current flow through a slab (of known geometry) of the material

P = (RA/L)=(V/i)(A/L) [ohm-cm]

R:resistance, ohm

A: area normal to the current flow, cm2

L:path length in the direction of current flow, cm,

V: voltage, i: current, A

Page 53: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Resistivity

Page 54: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Resistivity

Page 55: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Sparking

Page 56: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Internal Configuration• Internal configuration design is more art than

science• The even distribution of gas flow through the

ducts is very important to the proper operation of an ESP

• The number of ducts (Nd) is equal to one less than the number of plates (n-1)

Nd = Q/uDH (eq 5.15)

u: linear gas velocity (m/min)D Channel width (plate separation), mH: plate height, m

Page 57: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Internal Configuration• At the start of the design, use 5.15 to

estimate Nd by assuming a value for H and choosing representative values of u and D

Page 58: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Typical Values for the Fly-Ash ESP

• Table 5.1

Parameter Range of Values

Drift velocity 1-10 m/min

Channel (Duct) Width, D 15-40 cm

Specific Collection Area Plate area/Gas Flow

0.25-2.1 m2/(m3/min)

Gas velocity u 1.2-2.5 m/s

Aspect Ratio (R)

Duct Length/Plate Height

0.5-1.5

Corona Power Ratio Pc/Q 1.75-17.5 W/(m3/min)

Corona Current Ratio (Ic/A) 50-750 A/m2

Plate area per electrical set As 460-7400 m2

Number of electrical sections 2-6

Page 59: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Internal Configuration• The overall length of the precipitator (Lo)

– Lo=NsLp + (Ns-1)Ls + Len +Lex

• Lp:: length of plate

• Ls: spacing between electrical sections (0.5-1.0 m)

• Len: entrance section in length (several meters)

• Lex:exit section in length (several meters)

• Ns: number of mechanical fields

Ns ranges between 2 and 6.

Ns=RH/Lp R is the aspect ratio

Page 60: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Internal Configuration• When the numbers of ducts and sections

have been specified, the actual collection area (Aa) can be calculated as:

Aa=2HLpNsNd

• During the design process several plate sizes and numbers of ducts are tried until one combination is found such that Aa is equal to the required collection area.

Page 61: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Collection Efficiency vrs Particle Diameter

Page 62: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

An Example

Page 63: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example

Page 64: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Example

Page 65: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

POWER REQUIREMENT

Page 66: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

POWER REQUIREMENT

k: an adjustable constant in the range of 0.5-0.7 for we in ft/sec and Pc/A in W/ft2

Page 67: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.
Page 68: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Problem 5.10Provide a reasonable design for a 99.4% efficient ESP treating 30,000 m3/min of gas. The dust has a resistivity of 7.1 (10)10 ohm-cm. Specify the total plate area, channel width, number and size of plates, number of electrical sections (total and in the direction of flow), and total corona power to be supplied, and estimate the overall dimensions.

Page 69: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

SOLUTION

Page 70: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

SOLUTION

Page 71: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

SOLUTION

Page 72: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

SOLUTION

Page 73: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.
Page 74: Particle Control Technologies Lecture notes adapted from Prof. Dr. Benoit Cushman-Roisin Thayer School of Engineering at Dartmouth.

Video Demonstration on Electrostatic Precipitation

http://www.youtube.com/watch?v=y5w0IGuLR3A

http://www.youtube.com/watch?v=9kauc7OmmLQ

http://www.youtube.com/watch?v=x5YFK8mmeRQ

http://www.youtube.com/watch?v=BdRk3op2zpE

http://www.youtube.com/watch?v=iUXHzYLgrB0