Problem № 2 “Aerosol” презентация

Содержание

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Review IYPT , 2019 Introduction to the production and properties

Review

IYPT , 2019

Introduction to the production and properties of the aerosol

Assemble

an experimental setup

Studying of the break-up mechanisms of the jet into drops. The role of air.

Aerosol properties.

Analysis of the work and conclusions.

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Experimental Setup Theory Model Optimization IYPT Basic concepts Aerosol is

Experimental Setup

Theory Model

Optimization

IYPT

Basic concepts

Aerosol is a dispersed system which consists of

small particles suspended in a gaseous medium. Size of particles in aerosols vary from a few millimeters to ten to the power of minus 7 m.
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The method of producing aerosol Condensation aerosol Cooling and the

The method of producing aerosol

Condensation aerosol
Cooling and the formation of supersaturated

vapor, some chemical reactions

Dispersing aerosols
Disintegration of solid and liquid substances

The type of aerosol and the way of it`s producing uniquely defined by the condition of the problem - spraying a jet of water as it passes through a small aperture.(dispersing aerosol)

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Scheme of jet disintegration Fath, A., Fettes, C., and Leipetz,

Scheme of jet disintegration

Fath, A., Fettes, C., and Leipetz, A. 1998.

Investigation of the Diesel Break - up Close to the Nozzle at Different Injection Conditions, The Fourth International Symposium COMODIA 98, p.p. 429 - 434, Kyoto, Japan

Vapor bubbles and turbulence

Waves on the free surface of the fluid

The gaseous bubbles

Droplets

several sticky droplets

Reasons:

Instabilities and perturbations, which arise in the jet itself:
Cavitation
Turbulent flows

Jet disintegration due to interaction with the air

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Aerodynamic regimes *Ohnesorge V.W. Anwendung eines kinematographischen Hochfrequenzaparates mit mechanischer

Aerodynamic regimes

*Ohnesorge V.W. Anwendung eines kinematographischen Hochfrequenzaparates mit mechanischer Regelung der

Belichtung zur Aufnahme der Tropfenbildung und des Zerfalls flüssiger Strahlen//Dissertation Techn. Hochschule Berlin 1937
*Reitz R.D. Atomization and other Breakup Regimes of a liquid jet//
Ph.D. Thesis, Princeton University, 1978

Different sizes of the particles

Relay-Plato break-up mode

First aerodynamic regime

Second aerodynamic regime

Spray

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REVIEW OF INVESTIGATION Process of disintegration of the jet into

REVIEW OF INVESTIGATION

Process of disintegration of the jet into droplets, depending

on the flow rate;
Find out the role of air;
Determination of droplet size in an aerosol;
Optical and electrical properties of aerosol
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nozzle Experimental setup tripod tube pump

 

 

 

nozzle

Experimental setup

tripod

tube

pump

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The depth of field DETERMINATION OF DROPLET SIZE 15 – 20 сm 3 – 5 mm

The depth of field

DETERMINATION OF DROPLET SIZE

15 – 20 сm

3 –

5 mm
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IYPT

IYPT

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Jet flow mode Viscous friction force and dynamic pressure force of liquid jet

Jet flow mode

Viscous friction force and dynamic pressure force of liquid

jet
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INVESTIGATING JET`S BREAK-UP PROCESS Laminar flow Semi-turbulent flow Turbulent flow

INVESTIGATING JET`S BREAK-UP PROCESS

Laminar flow

Semi-turbulent flow

Turbulent flow

Experimental Setup

Theory Model

Optimization

IYPT

Re < 2100

2100

< 2300

Re >2300

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Rayleigh-Plateau instabilities The jet devides into separate drops. Laminar flow

Rayleigh-Plateau instabilities

The jet devides into separate drops.

Laminar flow

The characteristic time of

jet disintegration of the initial radius Rₒ is equal to

 

The length of the unbroken jet is equal to

**Atomization and Sprays
Arthur H. Lefebvre and Vincent G. McDonell

L

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Quality explanation of the Rayleigh-Plateau instability 14 Experimental Setup Theory Model Optimization IYPT

Quality explanation of the Rayleigh-Plateau instability

 

 

 

 

 

14

Experimental Setup

Theory Model

Optimization

IYPT

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Experimental Setup Theory Model Optimization IYPT L is the length

Experimental Setup

Theory Model

Optimization

IYPT

L is the length of the unbroken part of

the jet

INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO DROPS. LAMINAR FLOW.

L

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Experimental Setup Theory Model Optimization IYPT INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO DROPS. SEMI-TURBULENT FLOW.

Experimental Setup

Theory Model

Optimization

IYPT

INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO DROPS. SEMI-TURBULENT

FLOW.
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Experimental Setup Theory Model Optimization IYPT U,m/s 2100 L,m Diameter

Experimental Setup

Theory Model

Optimization

IYPT

U,m/s

2100 < Re <2300

L,m

Diameter of aperture
Density of the fluid
Surface

tension
coefficient

INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO DROPS. SEMI-TURBULENT FLOW.

L

U

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INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO DROPS. TURBULENT FLOW.

INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO DROPS. TURBULENT FLOW.

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Qualitative explanation of the turbulent jet 21 Experimental Setup Theory Model Optimization IYPT

Qualitative explanation of the turbulent jet

21

Experimental Setup

Theory Model

Optimization

IYPT

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Experimental Setup Theory Model Optimization IYPT Зависимость угла разлёта от скорости при турбулетном течении

Experimental Setup

Theory Model

Optimization

IYPT

Зависимость угла разлёта от скорости при турбулетном течении

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Qualitative explanation of the angle of expansion

Qualitative explanation of the angle of expansion

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d=0,8mm Turbulent flow INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO

d=0,8mm

Turbulent flow

INVESTIGATION OF THE PROCESS OF DISINTEGRATION INTO DROPS

22

Experimental Setup

Theory Model

Optimization

IYPT

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The role of air(assumptions) for the diameter of the jet:

The role of air(assumptions)

for the diameter of the jet:
2.5 mm the

velocity is 10m/s
1 mm the velocity is 16 m / s

Effect of entrainment of water by air flow is significant

An estimation for the airflow velocity required for this situation is approximately 830 m/s.

air flow is capable of deforming the jet, thereby increasing the disturbance that has arisen.

23

Experimental Setup

Theory Model

Optimization

IYPT

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Why can the jet be devideed into small drops? why

Why can the jet be devideed into small drops? why do

droplet sizes depend on the jet velocity?

 

Internal perturbations (turbulent motion) are required to break up the droplet

Number of Weber is necessary.

 

24

Experimental Setup

Theory Model

Optimization

IYPT

Surface tension and dynamic pressure force of liquid jet

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Воропай П.И., Шленов А.А. Повышение надежности поршневых насосов. М., Недра,

Воропай П.И., Шленов А.А. Повышение надежности поршневых насосов. М., Недра, 1980,

359 с.

Why can the jet be devided into small drops? why do droplet sizes depend on the jet velocity?

Internal perturbations (turbulent motion) are required to break up the droplet

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Average diameter is 0,129 mm 26 Experimental Setup Theory Model

Average diameter is 0,129 mm

26

Experimental Setup

Theory Model

Optimization

IYPT

Aerosol isn’t monodispersed

Probability

Size of

the droplets, mm
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DETERMINATION OF THE DROPLET`S SIZE d=2,5мм, water d=0,8мм, water d=0,8мм,

DETERMINATION OF THE DROPLET`S SIZE

d=2,5мм, water
d=0,8мм, water
d=0,8мм, glycerin

f

27

Experimental Setup

Theory Model

Optimization

IYPT

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The booger — Lambert — ber law will determine the

The booger — Lambert — ber law will determine the attenuation

of a monochromatic beam of light when passing through an absorbing medium.

 

aerosol

х

I0

I(х)

Source of the light

photosensor

kλ – the absorption rate depends on the wavelength λ of the absorbed light and the aerosol concentration

х

Source of the light

photosensor

OPTICAL PROPERTIES OF AN AEROSOL

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OPTICAL PROPERTIES OF AN AEROSOL 29 Experimental Setup Theory Model Optimization IYPT

OPTICAL PROPERTIES OF AN AEROSOL

29

Experimental Setup

Theory Model

Optimization

IYPT

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Experimental Setup Theory Model Optimization IYPT ELECTRICAL PROPERTY

Experimental Setup

Theory Model

Optimization

IYPT

ELECTRICAL PROPERTY

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Conclusions: a method of obtaining aerosol by simple mechanical spraying

Conclusions:

a method of obtaining aerosol by simple mechanical spraying destruction through

a small aperture;
the mechanism of the jet disintegration into droplets and the dependence of droplet sizes on the liquid velocity was studied;
at the qualitative level, the influence of air flows is understood and estimates are made for speeds in situation when the aerodynamic effect is significant;
a technique for estimating the size of droplets, studied the optical and electrical properties of the aerosol.
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7. Fath, A., Fettes, C., and Leipetz, A. 1998. Investigation

7. Fath, A., Fettes, C., and Leipetz, A. 1998. Investigation of

the Diesel Break - up Close to the Nozzle at
Different Injection Conditions, The Fourth International Symposium COMODIA 98, p.p. 429 - 434, Kyoto, Japan
8. Воропай П.И., Шленов А.А. Повышение надежности поршневых насосов. М., Недра, 1980, 359 с.
9. РАСЧЕТ ТРАЕКТОРИИ ДВИЖЕНИЯ КАПЛИ ЖИДКОСТИ В ГАЗОВОМ ПОТОКЕ  С УЧЕТОМ ЕЕ ДЕФОРМАЦИи.В.И. Рублев, В.В. Логинов
10. Study of the effects of the injector length/diameter ratio on the surface properties of
turbulent liquid jets in still air using X-ray imaging
A.R. Osta a, J. Lee a, K.A. Sallam a,, K. Fezzaa b Break-up length of liquid jets produced by short nozzles
M. Etzold ∗, A. Deswal , L. Chen , F. Durst
11. Atomization and Sprays
Arthur H. Lefebvre and Vincent G. McDonell

1. Береснев С.А., Грязин В.И.  Физика атмосферных аэрозолей: Курс лекций. – Екатеринбург:  Изд-во Урал. ун-та, 2008.
2. Фукс Н.А. Механика аэрозолей. М.: Изд. АН СССР, 1955.
3. К.И. Белоусов, А.А. Евстрапов,  И.В. Кухтевич, Я.С. Посмитная  ОСНОВЫ НАНОТЕХНОЛОГИЙ. ЧАСТЬ 1
4. A.R. Osta a, J. Lee a, K.A. Sallam a,, K. Fezzaa b Break-up length of liquid jets produced by short nozzles
M. Etzold ∗, A. Deswal , L. Chen , F. Durst
5. Sustainable Solutions for Energy and Environment, EENVIRO - YRC 2015, 18-20 November2015, Bucharest, Romania
Breakup of Liquid Jets
Ioana Laura Omoceaa*, Claudiu Patrascua, Mihaela Turcanua, Corneliu Balana
6. Manuel A. Reddemann · Florian Mathieu ·Reinhold Kneer «Transmitted light microscopy for visualizing the turbulent primary breakup of a microscale liquid jet»

Bibliography:

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There are some interesting things…(done, but not shown) Estimation for

There are some interesting things…(done, but not shown)

Estimation for the number

of Weber for droplet which rotate;
The measurements of the velocity of the laminar jet; for turbulent jet;
Droplet divide;
Instability of the Rayleigh- plateau;
The losses of energy;
The device of the spray;
The determination of the average diameter of the particles;
lifetime of the aerosol and droplet. The estimation of the critical radius for evaporation and condensation;
The concentration of the droplets.
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***Manuel A. Reddemann · Florian Mathieu ·Reinhold Kneer «Transmitted light

***Manuel A. Reddemann · Florian Mathieu ·Reinhold Kneer «Transmitted light microscopy

for visualizing the turbulent primary breakup of a microscale liquid jet»

Theory of Castleman

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F h We move in frame of reference associated with

F

 

h

We move in frame of reference associated with the jet. Select

the item Δm

 

 

 

 

 

 

AERODYNAMIC EFFECTS

the jet is compressed by the air flow

jet diameter grows

forces in equilibrium, critical flow velocity

gas

gas

sur

sur

sur

sur

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critical velocities significantly lower than velocities that we working with.

 

 

 

 

 

 

critical velocities significantly lower than velocities that we working with.

Not our

effect

thickness of the reduced mass layer (cylinder)

crit

crit

crit

gas

Aerodynamic effects

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Consider the effect of entrainment of liquid air flow. Let

Consider the effect of entrainment of liquid air flow. Let the

jet arose disturbance

 

 

 

 

 

 

 

 

 

thickness of the reduced mass layer (cylinder)

Aerodynamic effects

fr

sur

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