lectures 1&2 f. morrison cm3110 11/3/2019fmorriso/cm310/lectures/2019 fluids...

Lectures 1&2 F. Morrison CM3110 11/3/2019

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© Faith A. Morrison, Michigan Tech U.1

As teachers we can choose between

(a) sentencing students to thoughtless mechanical operations and (b) facilitating their ability to think.

If students' readiness for more involved thought processes is bypassed in favor of jamming more facts and figures into their heads, they will stagnate at the lower levels of thinking. But if students are encouraged to try a variety of thought processes in classes, then they can … develop considerable mental power. Writing is one of the most effective ways to develop thinking.

—Syrene Forsman

Reference: Forsman, S. (1985). "Writing to Learn Means Learning to Think." In A. R. Gere (Ed.), Roots in the sawdust: Writing to learn across the disciplines (pp. 162-174). Urbana, IL: National Council of Teachers of English.Professor Faith A. Morrison

Department of Chemical EngineeringMichigan Technological University

Transport/Unit Operations

© Faith A. Morrison, Michigan Tech U.2

Professor Faith A. Morrison


CM2120—Fundamentals of ChemE 2 (Steady Unit Operations Introduction, MEB)CM3110—Transport/Unit Ops 1 (Momentum & Steady Heat Transport, Unit Operations)CM3120—Transport/Unit Ops 2 (Unsteady Heat Transport, Mass Transport, Unit

Operations


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© Faith A. Morrison, Michigan Tech U.

Why study transport/unit ops?

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Why study transport/unit ops?

•Modern engineering systems are complex and often cannot be operated and maintained without analytical understanding

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•Design of new systems will come from high-tech innovation, which can only come from detailed, analytical understanding of how physics/nature works

Image: wikipedia.org

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ca


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Where are we now?

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Where are we now?

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CM2110

CM2120

Summary

CM21101. Steady mass balances2. Steady energy balances (how to calc. energy)3. MEB‐Mechanical Energy Balance (no friction)

CM2120/CM32151. MEB‐Mechanical Energy Balance (with friction)2. Pumps3. Introduction to Unit Operations4. Staged Unit Operations (distillation, absorption)


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Where are we now?

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CM3110Summary

CM31101. Steady momentum balances (macro

and micro)2. Rate‐based heat transfer processes

(Fourier’s law, heat transfer coefficients, radiation)

3. Unit Operations involving heat transfer (Heat Exchangers)


CM3110

Transport Processes and Unit Operations I

Professor Faith Morrison


www.chem.mtu.edu/~fmorriso/cm310/cm310.html

CM3110 - Momentum and Heat Transport

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EMERGENCY EVACUATION PROCEDURES

Important: The Michigan Bureau of Fire Services has adopted new rules for colleges and universities effective 2015

1. Only residence halls are required to hold fire and tornado drills.2. In lieu of fire drills in other university buildings all faculty and instructional staff are required to do the following on the first day of class:

- Explain the university fire evacuation procedures to the class (see below).- Explain the locations of the primary and secondary exit routes for your class

location.- Explain your designated safe location where the class will meet after evacuating

the building.3. The class instructor is responsible for directing the class during a building evacuation.

General evacuation procedure:- Use the nearest safe exit route to exit the building. The nearest safe exit from room 07-0100 is the back (south) entrance that is close to the Portage Canal and just outside our door, to the right. The secondary exit is the campus (north) exit, that exits near the Husky. The nearest safe exit from Fisher 139 is - Close all doors on the way out to prevent the spread of smoke and fire.- After exiting, immediately proceed to a safe location at least 100 feet from the building. Our designated safe location is in front of the MUB, near the circle drive.- Do not re-enter the building until the all-clear is given by Public Safety or the fire department.

TR Section


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EMERGENCY EVACUATION PROCEDURES

Important: The Michigan Bureau of Fire Services has adopted new rules for colleges and universities effective 2015

1. Only residence halls are required to hold fire and tornado drills.2. In lieu of fire drills in other university buildings all faculty and instructional staff are required to do the following on the first day of class:

- Explain the university fire evacuation procedures to the class (see below).- Explain the locations of the primary and secondary exit routes for your class

location.- Explain your designated safe location where the class will meet after evacuating

the building.3. The class instructor is responsible for directing the class during a building evacuation.

General evacuation procedure:- Use the nearest safe exit route to exit the building. The nearest safe exit from room 15-139 is the front (south) entrance that is close to highway 41. The secondary exit is the campus (north) exit, that connects to the main path through campus.- Close all doors on the way out to prevent the spread of smoke and fire.- After exiting, immediately proceed to a safe location at least 100 feet from the building. Our designated safe location is east of Fisher, in the parking lot of the Center for Diversity and Inclusion.- Do not re-enter the building until the all-clear is given by Public Safety or the fire department.

MW Section


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Why study fluid mechanics?

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•It’s required for my degree

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•It’s required for my degree (too literal)

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•Fluids are involved in engineered systems

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Image from: money.cnn.com

Image from: newegg.com


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•Fluids are involved in engineering systems (many devices that employ fluids can be operated and maintained and sometimes designed without detailed mathematical analysis)

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•Modern engineering systems are complex and often cannot be operated and maintained without analytical understanding

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•Design of new systems will come from high-tech innovation, which can only come from detailed, analytical understanding of how physics/nature works

Image: wikipedia.org

Imag

e: p

lane

tforw

ard.

ca

•It’s all part of learning to think and perform like an engineer. We will be intentionally ordering our knowledge and practicing asking relevant questions.


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O2 heat

exchanger

pump

membrane oxygenator – oxygen goes into blood; carbon dioxide comes out

O2

MO

spent blood

fresh blood

Membrane Oxygenator, MO(Heart-Lung Machine)

Secondary flow drives the O2 mass transfer

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© F

aith

A.

Mor

rison

, M

ichi

gan

Tech

U.

Artificial Heart

Image: health.howstuffworks.com/medicine/modern/artificial-heart.htm

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Microfluidics – Lab on a Chip

© F

aith

A.

Mor

rison

, M

ichi

gan

Tech

U.

www.nature.com/nmeth/journal/v4/n8/full/nmeth0807-665.html

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Sensors, diagnostics

And more. . . .

© F

aith

A.

Mor

rison

, M

ichi

gan

Tech

U.

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HelicoptersAirplanesQuieter fansFlexible body armorUndersea oil drillingSurgeryFood processingPlastics2D and 3D printingBattery manufactureCelestial explorationVolcanos Biomedical devices (stents, artificial organs, prosthetics)Sensor development…

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Where to start?

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Where to start?

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We’ve already started.


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1. We’ve learned fluid statics.

www.youtube.com/watch?v=zeNQOqr63cc

DrMorrisonMTU on YouTube: Introduction to Manometers: Two Essential Rules

On 3Sept19 #views >134,000!



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2. There are flow problems that can be addressed with one type of macroscopic energy balance:

2

,

2 2

, ,212 1 2 12 1 21

ΔΔΔ

2

p p(z z )

2

s on

s on

Wvpg z F

vg

m

m

v WF

1. single-input, single output2. Steady state3. Constant density (incompressible fluid)4. Temperature approximately constant5. No phase change, no chemical reaction6. Insignificant amounts of heat transferred

The Mechanical Energy Balance

Assumptions:

𝐹 friction


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Flow in Pipes

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For example:

pump

ID=3.0 in ID=2.0 in

75 ft

tank

50 ft 40 ft

20 ft

8 ft

1

2

1. Single-input, single output2. Steady state3. Constant density (incompressible fluid)4. Temperature approximately constant5. No phase change, no chemical reaction6. Insignificant amounts of heat transferred

Mechanical Energy Balance


)( ftH

)(1,2 VH

)(, VH sd

)/( mingalV

valve 50% open

valve full open

pump

system

Centrifugal Pumps

What flow rate does a centrifugal pump produce?

Answer: Depends on how much work it is asked to do.

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For example:

Calculate with the Mechanical Energy

Balance(CM2110, CM2120,

CM3215)


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We can apply the MEB to many important engineering systems

1. single-input, single output2. Steady state3. Constant density (incompressible fluid)4. Temperature approximately constant5. No phase change, no chemical rxn6. Insignificant amounts of heat

transferred

MEB Assumptions:

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Image from: www.directindustry.com

Image from: www.processindustryforum.com

Image from: www.directindustry,com

Calculate: Work,

pressures, flows


Example 1

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How many horsepower (hp) will it take to raise water at 4.0 𝑔𝑝𝑚 from a flooded basement to the surface (see figure)? The hose is smooth; as a first calculation we can neglect friction.

37.0𝑚Inner diameter=0.50𝑖𝑛

0.46𝑚

𝑊 , shaft work


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Example 1

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ANSWER: 0.12 hp

(our TA has the solution: HW/Example help session Sunday 6:30-7:30, 19-211)

How many horsepower (hp) will it take to raise water at 4.0 𝑔𝑝𝑚 from a flooded basement to the surface (see figure)? The hose is smooth; as a first calculation we can neglect friction.


30pages.mtu.edu/~fmorriso/cm310/convert.pdf

Handy Sheet for Unit Conversions


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31pages.mtu.edu/~fmorriso/cm310/MorrisonCoverMatter(c)2011.pdf

Handy Sheet of Fluid Mechanics Equations from inside cover of Morrison


Example 2

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What is the volumetric flow rate at the drain from a constant-head tank with a fluid level h? You may neglect frictional losses.


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Example 2

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What is the volumetric flow rate at the drain from a constant-head tank with a fluid level h? You may neglect frictional losses.

ANSWER: 𝜋𝑅 2ℎ𝑔

For more examples: see CM2110/20 notes; HW1;

Prerequisite review readings

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Exam 1: Next Tues 6:30-8:00pm, Dow 641The exam and solution from 2017 is on the web. TA help session is Sunday night. Exam topics: vectors, linear algebra, integration, balances, MEB, fluid statics

(Rev

iew

)

© F

aith

A.

Mor

rison

, M

ichi

gan

Tech

U.

HW1 (online and in Canvas)


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© F

aith

A.

Mor

rison

, M

ichi

gan

Tech

U.

• It is limited in application:

• It cannot determine flow patterns

• It does not model momentum exchanges

• It cannot be adapted to systems other than those for which it was designed (see list above)


The Mechanical Energy Balance (MEB) is a macroscopic analysis.

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1. single-input, single output2. Steady state3. Constant density (incompressible fluid)4. Temperature approximately constant5. No phase change, no chemical rxn6. Insignificant amounts of heat transferred

2 2

, ,212 1 2 12 1 21

p p(z z )

2s onv v W

g Fm

𝐹 friction


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CM3110

Transport Processes and Unit Operations I

Professor Faith Morrison


www.chem.mtu.edu/~fmorriso/cm310/cm310.html

CM3110 - Momentum and Heat TransportCM3120 – Heat and Mass Transport

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Part 1:


Energy balances (the MEB) can only take us so far with fluids modeling (due to assumptions).

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To understand complex flows, we must use

the MOMENTUM balance.

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Image from: commons.wikipedia.orgNaruto Whirlpools, Japan

Image from: www-math.mtu.edu


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Momentum Balance: Newton’s 2nd Law of Motion

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𝑓 𝑚𝑎

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: w

ww

.te

xtu

rex.

com

PH 2100: apply momentum

conservation to individual bodies

CM 3110: apply momentum conservation

to a continuum

See also: http://youtu.be/6KKNnjFpGto


Fluid Mechanics

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• Continuum (density, velocity, stress fields)

• Control volume

• Stress in a fluid at a point (stress tensor)

• Stress and deformation (Newtonian constitutive equation)

• Microscopic and macroscopic momentum balances

• Internal flows – pipes, conduits

• External flows – drag, boundary layers

• Advanced fluid mechanics – complex shapes

𝑣𝑣𝑣𝑣

𝜏𝜏 𝜏 𝜏𝜏 𝜏 𝜏𝜏 𝜏 𝜏

𝜌 𝑥,𝑦, 𝑧

control volume

(calc3, differential equations)

(engineering quantities of

interest)


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Momentum . . .

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𝜌𝑣𝜌𝑣𝜌𝑣𝜌𝑣

is a vector

Microscopic momentum balance

gvPvvt

v

2

Macroscopic momentum balance

2# #

1 1

cosˆ ˆ

ii

streams streams

CVi i A

A

A vdv pAn R M g

dt

P

So we need vector math.

Ch 6

Ch 9

𝐶𝑎𝑙𝑐 3

zrz

r

xyzz

y

x

v

v

v

v

v

v

v

v

v

v

1233

2

1

Same vector, different coordinate systems, different components.

magnitudevectorvv

vectorunitv

v

v ˆ


We choose coordinate systems for convenience.

Vectors

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1x rv v v Note:

(usually)


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creeping flow (sphere)

0.

01

0.2

0.6

1.2

2.0

3.0

Vector plot of the velocity field in slow flow around a

sphere

The flow is a steady upward flow; the length and direction of the vector indicates the velocity at that location.

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Fluid velocity is a vector field

𝑣 𝑣 𝑥,𝑦, 𝑧

(calc3)

Vectors – Cartesian coordinate system


•We do algebra with the basis vectors the same way as with other quantities

•The Cartesian basis vectors are constant (do not change with position)

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(three ways of writing the same thing, the Cartesian basis vectors)

𝑣𝑣𝑣𝑣

𝑣 �̂� 𝑣 �̂� 𝑣 �̂�

𝑣𝑣𝑣𝑣

𝑣 �̂� 𝑣 �̂� 𝑣 �̂�

𝑣 𝚤̂ 𝑣 𝚥̂ 𝑣 𝑘


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Vectors – Cylindrical coordinate system

•The cylindrical basis vectors are variable (depend on position)

ˆ ˆ ˆcos sin

ˆ ˆ ˆsin cos

ˆ ˆ

r x y

x y

z z

e e e

e e e

e e

cos

sin

x r

y r

z z

P

x

y

z

r

z

45

(see inside back cover of

text; also, supplemental

handouts)

𝑣𝑣𝑣𝑣

𝑣 �̂� 𝑣 �̂� 𝑣 �̂�


Vectors – Spherical coordinate system

•The spherical basis vectors are variable (with position)

ˆ ˆ ˆ ˆsin cos sin sin cos

ˆ ˆ ˆ ˆcos cos cos sin ( sin )

ˆ ˆ ˆsin cos

r x y z

x y z

x y

e e e e

e e e e

e e e

sin cos

sin sin

cos

x r

y r

z r

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handouts)

𝑣𝑣𝑣𝑣

𝑣 �̂� 𝑣 �̂� 𝑣 �̂�

Note: spherical coordinate system in use by the fluid mechanics community uses 0 𝜃 𝜋

as the angle from the 𝑧=axis to the point.

In your calc 3 class, they probably called this 𝜙and the other one 𝜃


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creeping flow (sphere)

0.

01

0.2

0.6

1.2

2.0

3.0

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Fluid Velocity is a Vector Field

Velocity magnitude and direction vary with position

𝑣 𝑣 𝑥,𝑦, 𝑧

Example 3: At positions (1,45o,0) and (1,90o,0) in the 𝑟,𝜃, 𝑧coordinate system, the velocity vector of a fluid is given by


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What is this vector in the usual 𝑥𝑦𝑧 coordinate system?

𝑣𝑣𝑣𝑣

010


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49

𝑣

0

𝑣1

00

ANSWERS:

ℎ𝑖𝑛𝑡: 010

�̂�

Example 3: At positions (1,45o,0) and (1,90o,0) in the 𝑟,𝜃, 𝑧coordinate system, the velocity vector of a fluid is given by

What is this vector in the usual 𝑥𝑦𝑧 coordinate system?

𝑣𝑣𝑣𝑣

010


We use Calculus in Fluid Mechanics to:

1. Calculate flow rate, 𝑄

2. Calculate average velocity, ⟨𝑣⟩

3. Express forces on surfaces due to fluids (vectors)

4. Express torques on surfaces due to fluids (vectors)

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These are quantities of interest.These items are what we are learning to calculate.


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2

0 0

ˆ( ) ( )

( )

area

R

z

Q v n d area

Q v r rdrd

1. Calculate Flow rate: or VQ

is the component of v in the direction normal to the area

ˆv n

General:

Tube flow:

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Common surface shapes in the standard coordinate systems:

2

: ( )

: ( )

: ( )

: ( ) ( ) sin sin

rectangular d area dxdy

circular d area r drd

surface of cylinder d area Rd dz

spherical d area rd r d r d d

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handouts)


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Example 4: Calculate the flow rate in flow down an incline plane of width W.

53

22

2

)cos()( xH

gxvz

HMomentum balance calculation gives:

(we will learn how to get this equation for 𝑣 𝑥 ; here it is given)


Example 4: Calculate the flow rate in flow down an incline plane of width W.

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22

2

)cos()( xH

gxvz

HMomentum balance calculation gives:

ANSWER:

𝑄𝐻 𝜌𝑔𝑐𝑜𝑠𝛽

3𝜇

(we will learn how to get this equation for 𝑣 𝑥 ; here it is given)


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2. Calculate Average velocity:

2

Qv

area

Qv

R

v

“area” is the cross-sectional area normal to flow

General:

Tube flow:

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Example 5: The shape of the velocity profile for a steady flow in a tube is found to be given by the function below. Over the range 0 <r<10 mm, (R=10mm), what is the average value of the velocity?

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ANSWER: 𝑣2

Example 5: The shape of the velocity profile for a steady flow in a tube is found to be given by the function below. Over the range 0 <r<10 mm, (R=10mm), what is the average value of the velocity?


3. Express forces on surfaces due to fluids

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𝐹 𝑛 ⋅ Π 𝑑𝑆Total fluid force on a

surface

Π ≡ 𝜏 𝑝�̳� Total stress tensor(calc3)


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Example 6: In a liquid of density , what is the net fluid force on a submerged sphere (a ball or a balloon)? What is the direction of the force and how does the magnitude of the fluid force vary with fluid density?

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(p81)

H0f

air

x

z


Solution: We will be able to do this in this course (Ch4, p257).

From expression for force due to fluid, obtain: (in spherical coordinates)

We can do the math from here. (Calc 3)

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surface

𝐹 𝜌𝑔𝑅 𝐻 𝑅𝑐𝑜𝑠𝜃 �̂� sin𝜃 𝑑𝜃𝑑𝜙


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Solution: We will be able to do this in this course (Ch4, p257).

From expression for force due to fluid, obtain: (in spherical coordinates)

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ANSWER: (see p83)

𝑓

00

4𝜋𝑅 𝜌𝑔3


surface

𝐹 𝜌𝑔𝑅 𝐻 𝑅𝑐𝑜𝑠𝜃 �̂� sin𝜃 𝑑𝜃𝑑𝜙


4. Express torques on surfaces due to fluids

ˆS at surface

total fluid torqueR n dS

on a surfaceT

R lever arm

We will learn to write the stress tensor for our systems; then we can calculate stresses, torques.

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pI total stress tensor

(Points from axis of rotation to position where torque is applied)


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Example 7, Torque in Couette Flow: A cup-and-bob apparatus is widely used to measure viscosities for fluids. For the apparatus below, what is the torque needed to turn the inner cylinder (called the bob) at an angular speed of ?


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Torque in Couette FlowSolution:

1. Solve for velocity field (microscopic momentum balance)

2. Calculate stress tensor3. Formulate equation for torque (an integral)4. Integrate5. Apply boundary conditions

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See problem 6.22 p487

2

2

0

1

0r z

R r Rv

R r

Velocity solution:

Tv v

pI

ˆS at surface


on a surfaceT

What is lever arm, R?

etc…

𝜏𝜏 𝜏 𝜏𝜏 𝜏 𝜏𝜏 𝜏 𝜏



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See problem 6.22 p487

ˆS at surface


on a surfaceT

ANSWER: (see p308)

𝑇4𝜋𝑅 𝜅 𝐿𝜇Ω𝜅 1

001


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Summary of Quick Start

A: Mechanical Energy Balance

B): Use Calculus in Fluid Mechanics to

1. Calculate flow rate 2. Calculate average velocity3. Express forces on surfaces due to fluids4. Express torques on surfaces due to fluids

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1. SI-SO, steady, incompressible, no rxn, no Δ𝑇, no 𝑄2. Macroscopic, based on energy (not momentum)3. Choose points 1 and 2 wisely4. Solve for 𝐹 or 𝑊 , or 𝑝, velocity, elevation

𝐹 friction2

,

2 2

, ,212 1 2 12 1 21

ΔΔΔ

2

p p(z z )

2

s on

s on

Wvpg z F

vg

m

m

v WF


68

Summary of Quick Start

A: Mechanical Energy Balance

B): Use Calculus in Fluid Mechanics to

1. Calculate flow rate 2. Calculate average velocity3. Express forces on surfaces due to fluids4. Express torques on surfaces due to fluids

1. SI-SO, steady, incompressible, no rxn, no , no 2. Macroscopic3. Choose points 1 and 2 wisely4. Solve for or or , velocity, elevation

End of Quick Start.

We have reviewed:• MEB (an energy balance)• Math tools

Now, on to Fluid Mechanics, i.e. momentum transport.


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lectures 1&2 f. morrison cm3110 11/3/2019fmorriso/cm310/lectures/2019 fluids...

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