chemical engineering 374 - ira a. fulton college of...

16
1 Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows Big whorls have little whorls That feed on their velocity And little whorls have lesser whorls And so on to viscosity --Lewis Richardson I am an old man now, and when I die and go to heaven there are two matters on which I hope for enlightenment. One is quantum electrodynamics, and the other is the Turbulent motion of fluids. About the former I am rather optimistic. --Attr. to Horace Lamb

Upload: dinhnguyet

Post on 03-May-2018

214 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

1

Chemical Engineering 374Fluid Mechanics

Turbulent Pipe Flows

Big whorls have little whorls

That feed on their velocity

And little whorls have lesser whorls

And so on to viscosity

--Lewis Richardson

I am an old man now, and when I die and go to heaven there are

two matters on which I hope for enlightenment.

One is quantum electrodynamics, and the other is the

Turbulent motion of fluids.

About the former I am rather optimistic.

--Attr. to Horace Lamb

Page 2: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Spiritual Thought

“Marriage is the foundry for social order, the

fountain of virtue, and the foundation for

eternal exaltation. Marriage has been

divinely designated as an eternal and

everlasting covenant. Marriage is sanctified

when it is cherished and honored in

holiness. That union is not merely between

husband and wife; it embraces a partnership

with God.”

President Russell M. Nelson

2

Page 3: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Fluids Roadmap3

Page 4: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Turbulence examples4

Page 5: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Turbulent Mixing Layer5

Flow

Flow

Page 6: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Instability Flow6

Page 7: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Turbulent Flow

• Turbulent Velocity?

• Turbulent Profile?

• Properties:

– Higher τw

– Higher Friction

– Higher Δploss

– Shear Stress?

7

Page 8: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Channel Flow Simulations8

Page 9: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Turbulent Eddies

• Average Shear Stress…

• Too small!

• Add new term for eddy motion

• Transport momentum:

– ሶ𝑚𝑜𝑚 = ሶ𝑚 ∙ 𝑢′ = 𝜌𝐴𝑣′ 𝑢′ = 𝜏𝑡 = 𝜌𝑣′𝑢′

• Units of stress – F/A

• Reynolds Stress

• Don’t know it… have to model it

• 𝜏𝑡 = −𝜇𝑡𝑑ഥ𝑢

𝑑𝑦

9

Page 10: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Channel Flow Simulation10

Wall

Wall

Flow

Page 11: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Roughness11

Page 12: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Instantaneous and Mean12

Shape of Regions I and III from dimensional analysis!

Page 13: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Moody Chart13

Page 14: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Example

• Consider pipe flow.

• Question: How to simplify the

above equation?

• Friction balances pressure drop.

• To find pressure drop for

pipe/fluid, and velocity (flow rate):

– Get f

• f = f(Re)

• Get Re = rDv/m

– Plug solve equation for DPL

14

Colebrook

Haaland

Page 15: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Example

• Water flow in a smooth pipe:

r = 1000 kg/m3,

m = 0.001 kg/m*s

n=1E-6 m2/s

• Find DPL, hL, Power

• Question: What is happening physically?

• Question: What do I know?

• Question: What do I want?

• Question: What relationships do I have?

• Solve Re f DPL hL Power

• Re = rDv/m:

– Need v:

– v =V / A = V / (pD2/4) = 2 m/s

Re = 100,000

• Colbrook f = 0.0178

DP = fLrv2/2D = 35600 Pa

• hL =DP/rg = 3.63 m

• Power = VDP = 140 W

15

L=50 m

D=0.05 m

V = 0.003927 m3/s

Colebrook

Haaland

Page 16: Chemical Engineering 374 - Ira A. Fulton College of ...mjm82/che374/Fall2016/LectureNotes/Lecture_18... · Chemical Engineering 374 Fluid Mechanics Turbulent Pipe Flows ... everlasting

Turbulent Flow Problem Types

• 3 Main problem types:1. Find ΔP, given D, L, v

2. Find ሶ𝑉 given D, L, ΔP

3. Find D given v, L, ΔP

16