me 475/675 introduction to combustion lecture 34

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ME 475/675 Introduction to Combustion Lecture 34

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Page 1: ME 475/675 Introduction to Combustion Lecture 34

ME 475/675 Introduction to

CombustionLecture 34

Page 2: ME 475/675 Introduction to Combustion Lecture 34

Announcements• Integrated BS/MS Degree• http://www.unr.edu/engineering/academics/accelerated

• Term Project• Add 2% to HW• http://wolfweb.unr.edu/homepage/greiner/teaching/MECH.475.675.Combustion/TermProjectAssignment.pdf

Page 3: ME 475/675 Introduction to Combustion Lecture 34

Midterm 2

• Scaled = 10xSqrt(Raw)• Scaled average = 82

35 45 55 65 75 85 9535

45

55

65

75

85

95

105

115

Midterm 1

Mid

term

2

35 40 45 50 55 60 65 70 75 80 85 90 95 100 1050

1

2

3

4

Unscaled

Unscaled score

# of

stud

ents

35 40 45 50 55 60 65 70 75 80 85 90 95 100 1050

1

2

3

4

Scaled

Axis Title

Axis

Title

Page 4: ME 475/675 Introduction to Combustion Lecture 34

Flame Quenching, Mixture Flammability, Ignition •What does it take to ignite a mixture? •What does it take to extinguish a flame?• “Williams Criteria” (rule of thumb)• Ignition will occur if enough energy is added to a slab of thickness (laminar

flame thickness) to raise it to the adiabatic flame temperature, Tad. • A flame will be sustained if its rate of chemical heat release insides a slab is

roughly equal to heat loss by conduction out of the slab• Example extinguishment methods

• Pass a flame through a narrow tube or slot so it losses too much heat to the surfaces• Dilute using water (or thermal?)• Interrupt chemical kinetics (halogens)• Blow reaction away (loses fuel or heat)

Page 5: ME 475/675 Introduction to Combustion Lecture 34

Cold Wall Quenching

•Quenching distance d• Smallest dimension d that allows flame to pass• Experimentally determined by shutting off flow of a premixed

stabilized flame• dtube = (1.2 to 1.5) dtube

d d

Page 6: ME 475/675 Introduction to Combustion Lecture 34

Simplified Quenching Analysis for a slot

• To quench, we need:

• , so need • If ; and since and

�̇�′ ′ ′𝑉 𝑄𝑐𝑜𝑛𝑑𝑄𝑐𝑜𝑛𝑑

𝑑

𝛿𝐿

𝑇𝑥b=2

b>2

Page 7: ME 475/675 Introduction to Combustion Lecture 34

Quenching will take place when

• , = 2 or larger• But

�̇�′ ′ ′𝑉 𝑄𝑐𝑜𝑛𝑑𝑄𝑐𝑜𝑛𝑑

𝑑

𝛿𝐿

𝑇𝑥b=2

b>2

𝑑𝛿

Page 8: ME 475/675 Introduction to Combustion Lecture 34

Data, Table 8.4 page 291

Page 9: ME 475/675 Introduction to Combustion Lecture 34

Example 8.4, page 290Turn in next time for EC

• Consider the design of a laminar-flow, adiabatic, flat-flame burner consisting of a square arrangement of thin-walled tubes as illustrated in the sketch below. Fuel-air mixture flows through both the tubes and the interstices between the tubes. It is desired to operate the burner with a stoichiometric methane-air mixture exiting the burner tubes at 300 K and 5 atm.• Determine the mixture mass flowrate per unit cross-sectional area at the design

condition. • Estimate the maximum tube diameter allowed so that flashback will be

prevented.

• Methane (CH4)/air,

Page 10: ME 475/675 Introduction to Combustion Lecture 34

Flammability Limits

• Flames only propagate within certain equivalence ratio ranges• ,

• See page 291, Table 8.4 for limits

Page 11: ME 475/675 Introduction to Combustion Lecture 34

Example 8.5, p 294 (turn in next time for EC)• A full propane cylinder from a camp stove leaks its contents of 1.02 lbm (0.464

kg) into a 12’x14’x8’ (4.66 m x 4.27 m x 2.44) room at 20C and 1 atm. After a long time, the fuel gas and room are well mixed. • Is the mixture in the room flammable?

Page 12: ME 475/675 Introduction to Combustion Lecture 34

Ignition

• The minimum electrical spark energy capable of igniting a flammable mixture.• It is dependent on the temperature, pressure and equivalence ratio of the mixture

• What is the critical (minimum) radius of a spark that will propagate

• ; ; ; ;

( 𝑑𝑇𝑑𝑥 )𝑅𝐶𝑟𝑖𝑡

Page 13: ME 475/675 Introduction to Combustion Lecture 34

Energy to bring critical volume to Tb

• • ; •

• not normally considered reliable

• Agrees with measurements at low pressure • Need lots of energy at low pressure• Hard to restart jet engines at high pressures• decreases as Tu increases• Table 8.5 page 298 Different fuels

Page 14: ME 475/675 Introduction to Combustion Lecture 34