SlideShare uma empresa Scribd logo
1 de 8
Baixar para ler offline
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
Lesson 4: 
Bernoulli's Theorem 
Objective 
In this lesson we will discuss the relationships of "fluid mechanics" and how it APPLIES to flow and 
pressure or head. The flow of ground water is controlled by the laws of physics and thermodynamics. We 
will discuss a variety of concepts that apply to ground water flow and hydro-geology, and also flow in a 
pipe as well as, the concept of pressure or "head." We will also discuss the Bernoulli equation or theorem. 
Reading Assignment 
Read the online lesson as well as Chapter 3 in your textbook. 
Lecture 
Introduction 
The flow of groundwater is controlled by the laws of physics, thermodynamics and hydro-geology. In this 
lesson we will assume that the water temperature is nearly constant and is not very warm. Most drinking 
water sources are not very warm even in the summer months. Thermodynamics is more important in 
industrial WATER TREATMENT , where boiler water is often treated, and is usually very hot to begin 
the process. We will study the process of mechanical energy. Water contains energy due to 1- elevation, 2- 
pressure and 3- velocity. Head is the amount of energy possessed by a unit quantity of water expressed in 
feet. (Example: A 30 ft. tank will have a head of 30 ft.) Simply put head is the vertical distance between 
two levels in a fluid. Another term for velocity pressure is dynamic pressure. 
We will briefly discuss some terms and relationships, which will help you to better understand the rest of 
this lesson. 
Velocity pressure = total pressure - static pressure. 
Velocity Head - the energy of motion; the vertical distance or height through which water must fall 
freely, under the force of gravity, to acquire the velocity that it possesses. It is theoretically equal to the 
square of the velocity divided by twice the acceleration of gravity. V2/ 2g 
Static Head - Head due to elevation: the actual elevation difference between water surfaces or a water 
surface and some other reference point. Example: If one WATER TANK is at the elevation of 2300ft., 
1 dari 8 24/10/2014 23:35
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
while another is at the elevation of 2100 ft., the static head would be 200 ft. 
Pressure Head - the head represented by the expression of pressure over weight (p/y ) where p is 
pressure and y is weight. Where p is in pounds /sq. ft. and y is the weight of the liquid per cubic feet, h is 
head in feet. 1 psi = 2.31 ft. and 1 ft. = 0.433 psi. These are very helpful conversions to use. 
For a unit volume of fluid, the mass, m, is numerically equal to the density, p, since density is defined as 
mass per unit volume. The total energy of the unit volume of fluid is the three components; 1- kinetic, 2- 
gravitational, 3- fluid pressure energy. 
E tv = ½ pv2 + pgz + P 
g = the acceleration of gravity 
z = the elevation of the center of gravity of the fluid 
v = velocity above the reference elevation. 
where Etv is the total energy per unit volume. If this equation is divided by p, the result is the total energy 
per unit mass..... 
E tm = v2/2 + gz + P/p )which is the BERNOULLI equation). 
The Bernoulli Theorem says that total pressure = the same at any two points along a streamline, in a 
flow. 
Total Pressure - static pressure + ½ × density × velocity squared. 
Total pressure = static pressure + dynamic pressure 
Static pressure = pressure that is measured when water is at rest. 
The Theory of Bernoulli 
This theory, which forms part of the study of hydraulic principles, states that the static pressure of a 
moving fluid varies inversely as its velocity, which means that as velocity increases, the static pressure 
decrease. 
The principle of the relationship between velocity and pressure is illustrated below. Two vessels (a) and 
(b), of the same shape and cross-sectional area, are joined together by a small-bore pipe, (c). If fluid is 
added to vessel (b) and gradually find its own level, this level will still be maintained if two positions (d) 
and (e) of the same size and weight are placed on the liquid in the vessels (a) and (b), respectively. 
If a force of 1N is exerted on piston (d), in a downward direction, fluid in (a) will flow through the pipe (c) 
into vessel (b). The velocity of the fluid will increase as it passes through (c), because the cross-sectional 
2 dari 8 24/10/2014 23:35
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
area of the pipe (c) is much less than that of (a), and the same volume of fluid must pass through (c) as 
leaves (a) in the same time. 
Some of the 1N pressure in (a) will be converted into velocity pressure in pipe (c), and a pressure gauge 
situated at (f) would REGISTER a pressure less than that equivalent to 1N. When the fluid reaches the 
vessel (b), its velocity will reduce to its original rate and some of the kinetic energy is reconverted into 
potential energy." 
Total Pressure: In flowing are, it is the sum of the static and velocity pressures. 
Velocity Pressure: In flowing air, it is the pressure due to velocity and density of air. 
Static Pressure: In flowing air, it is the total pressure minus velocity pressure, pushing equally in all 
directions. 
Pressure Static measures elevation change in feet. 
Static Pressure 
Static pressure is the difference between the air pressure on the inside of your barn and the air pressure 
outside your barn. 
The static pressure is an indicator of how much negative pressure the fans are creating and how effective 
they will be at drawing fresh air in through your inlets. An overly high static pressure can also indicate 
that you do not have enough inlets in your barn. 
In terms of your barn, the static pressure should be around 0.04" wc (inches of water column) to 0.10" 
wc. When it is warm outside, such as during the summer, and your fans are running on or near their 
maximum speed, you want your static pressure to be around 0.05". In the winter, you want the static 
pressure higher so that the air pulled through the inlets enters the room faster, promoting thorough mixing 
of incoming air with the air already in the barn. 
To measure static pressure in a barn you would use a manometer. 
The following diagrams indicate the changes in static pressure when your fans are off and when they are 
running. 
Fig. 4-1: This diagram shows a u-tube manometer measuring an equal pressure between the outside of the barn and the inside of 
the barn. This happens when the fans are off. 
3 dari 8 24/10/2014 23:35
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
Fig. 4-2: This diagram shows a u-tube manometer measuring a decreased pressure in the barn compared to outside due to the fans 
running. Note that compared to figure one the tube closest to the wall is lower because the greater pressure is pushing the liquid 
in the tube downward. 
Reference: BSM Agri Ltd. 
Velocity Pressure 
Tank Gauge - 20 psi = Line Gauge 
4 dari 8 24/10/2014 23:35
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
Swap gauges 
Tank Gauge - 20 psi = Line Gauge 
Velocity pressure is then 20 psi 
Velocity of water would be 57 feet/sec 
The faster the molecules flow, the harder it is to make a turn into the line gauge. 
Calculation of Velocity of a Fluid Through a Pipeline 
The speed or velocity of a fluid flowing through a channel or pipeline is related to the cross-sectional area 
of the pipeline and the quantity of water moving through the line. 
For example, if the diameter of a pipeline is reduced, then the velocity of the water in the line must 
increase to allow the same amount of water to pass through the line. 
SAMPLE Problem: 
If the flow through a 2 foot diameter pipe is 8 MGD, the velocity is: 
If this same 8 MGD flow is transferred to a pipe with a 1 foot diameter, the velocity would be: 
5 dari 8 24/10/2014 23:35
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
Based upon this example problem, we can see that if the cross-sectional area decreased, the velocity of 
the flow must increase. Mathematically we can say that the velocity and cross-sectional area are 
inversely proportional when the amount of flow (Q) is constant. (Fig. 4-3). 
This is extremely important in the operation of a centrifugal pump. 
6 dari 8 24/10/2014 23:35
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
Differential Pressure 
Molecular velocity energy is transferred directly to gauge. 
Much higher pressure. 
Review 
In this lesson we studied the concepts involved with fluid mechanics, such as total pressure, velocity 
pressure, and static pressure. Simply put HEAD is the vertical distance between two levels in a fluid. Total 
pressure is the sum of the static and velocity pressures, and velocity pressure is the pressure due to 
velocity and density of air, and static pressure is the total pressure minus velocity pressure, pushing 
equally in all direction. As well as, velocity head, static head, pressure head. Velocity head is the energy of 
motion, while static head is the actual head due to elevation, while pressure head is the ratio of pressure 
over weight, if pressure is in pounds per square foot and weight is in cubic feet, and head is in feet. We 
also discussed the calculation of velocity of a fluid through a pipeline, and conversions from feet of water 
to head in psi. 
Sources 
Water Distribution Operator Training Handbook - AWWA 
APPLIED Hydro-geology - Merrill Publishing Co., C.W. Fetter 
Operator Certification Study Guide - AWWA 
7 dari 8 24/10/2014 23:35
Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm 
LEGO Design & PROGRAMMING Systems - "Ask an Engineer" 
BSM Agri Ltd. 
Assignment 
Answer the following questions and either email or fax to the instructor. 
The total dynamic head against which 1. a pump must operate is ______________. 
A well is pumping into a reservoir at 300 gpm while the service pumps are pumping from the 
reservoir at 400 gpm. Which direction is the reservoir (tank) level going: 
2. 
In a well the static water level is 15 feet. The pumping water level is 45 feet. The drawdown is how 
much? 
3. 
A venturi tube increases the velocity and decreases the pressure as water flows through it. This type 
of tube is used to ______________. 
4. 
5. 
If one tank in a system is at 2100 ft. elevation, and another tank, same size, is at 2300 ft. elevation, 
what is the static head? 
8 dari 8 24/10/2014 23:35

Mais conteúdo relacionado

Mais procurados

Applications of the Bernoulli Equation
Applications of the Bernoulli EquationApplications of the Bernoulli Equation
Applications of the Bernoulli EquationMahmudul Hasan
 
Bernoulli's Principle and its applications
Bernoulli's Principle and its applicationsBernoulli's Principle and its applications
Bernoulli's Principle and its applicationsTanumoy Dey
 
Venturimeter : Working,Construction,Applications ,Numerical
Venturimeter : Working,Construction,Applications ,NumericalVenturimeter : Working,Construction,Applications ,Numerical
Venturimeter : Working,Construction,Applications ,NumericalSINY MARY LONA
 
VENTURIMETER -Application of Bernoulli's Law
VENTURIMETER -Application of Bernoulli's LawVENTURIMETER -Application of Bernoulli's Law
VENTURIMETER -Application of Bernoulli's LawKundan Kumar
 
New microsoft office power point presentation
New microsoft office power point presentationNew microsoft office power point presentation
New microsoft office power point presentationGokul R
 
Bernoulli’s principle
Bernoulli’s principleBernoulli’s principle
Bernoulli’s principleVyvian Leow
 
Bernoulli’s equation
Bernoulli’s equationBernoulli’s equation
Bernoulli’s equationSajjad Ahmad
 
Bernoulli's principle
Bernoulli's  principleBernoulli's  principle
Bernoulli's principleAng Sovann
 
Bernoulli’s Theorem
Bernoulli’s Theorem Bernoulli’s Theorem
Bernoulli’s Theorem Habib Rahman
 
Bernoullis Theorem (proof and explaination)
Bernoullis Theorem (proof and explaination)Bernoullis Theorem (proof and explaination)
Bernoullis Theorem (proof and explaination)Deepanshu Chowdhary
 
class 11 Physics investigatory project(cbse)
class 11 Physics investigatory project(cbse)class 11 Physics investigatory project(cbse)
class 11 Physics investigatory project(cbse)Ayan sisodiya
 
Bernoullis theorem
Bernoullis theoremBernoullis theorem
Bernoullis theoremRajeev kumar
 
Bernoulli’s principle
Bernoulli’s principleBernoulli’s principle
Bernoulli’s principleVyvian Leow
 
Bernoulli's Principle
Bernoulli's PrincipleBernoulli's Principle
Bernoulli's Principleeliseb
 
Bernoulli’s principle
Bernoulli’s principleBernoulli’s principle
Bernoulli’s principleSheeRa Aya
 

Mais procurados (20)

Applications of the Bernoulli Equation
Applications of the Bernoulli EquationApplications of the Bernoulli Equation
Applications of the Bernoulli Equation
 
Bernoulli's Principle and its applications
Bernoulli's Principle and its applicationsBernoulli's Principle and its applications
Bernoulli's Principle and its applications
 
Venturimeter : Working,Construction,Applications ,Numerical
Venturimeter : Working,Construction,Applications ,NumericalVenturimeter : Working,Construction,Applications ,Numerical
Venturimeter : Working,Construction,Applications ,Numerical
 
Bernoulli's Principle
Bernoulli's PrincipleBernoulli's Principle
Bernoulli's Principle
 
VENTURIMETER -Application of Bernoulli's Law
VENTURIMETER -Application of Bernoulli's LawVENTURIMETER -Application of Bernoulli's Law
VENTURIMETER -Application of Bernoulli's Law
 
New microsoft office power point presentation
New microsoft office power point presentationNew microsoft office power point presentation
New microsoft office power point presentation
 
Bernoulli’s principle
Bernoulli’s principleBernoulli’s principle
Bernoulli’s principle
 
Bernoulli’s equation
Bernoulli’s equationBernoulli’s equation
Bernoulli’s equation
 
Bernoulli theorm
Bernoulli theormBernoulli theorm
Bernoulli theorm
 
Bernoulli's principle
Bernoulli's  principleBernoulli's  principle
Bernoulli's principle
 
Bernoulli Theorem
Bernoulli  TheoremBernoulli  Theorem
Bernoulli Theorem
 
Bernoulli’s Theorem
Bernoulli’s Theorem Bernoulli’s Theorem
Bernoulli’s Theorem
 
Bernoullis Theorem (proof and explaination)
Bernoullis Theorem (proof and explaination)Bernoullis Theorem (proof and explaination)
Bernoullis Theorem (proof and explaination)
 
class 11 Physics investigatory project(cbse)
class 11 Physics investigatory project(cbse)class 11 Physics investigatory project(cbse)
class 11 Physics investigatory project(cbse)
 
Bernoullis theorem
Bernoullis theoremBernoullis theorem
Bernoullis theorem
 
PRESSURE & HEAD (PART-1)
PRESSURE & HEAD (PART-1)PRESSURE & HEAD (PART-1)
PRESSURE & HEAD (PART-1)
 
Bernoulli’s principle
Bernoulli’s principleBernoulli’s principle
Bernoulli’s principle
 
Bernoulli's Principle
Bernoulli's PrincipleBernoulli's Principle
Bernoulli's Principle
 
Fluid Mechanics
Fluid MechanicsFluid Mechanics
Fluid Mechanics
 
Bernoulli’s principle
Bernoulli’s principleBernoulli’s principle
Bernoulli’s principle
 

Destaque (19)

Bagaimana tidak untuk he...tware basis pengetahuana
Bagaimana tidak untuk he...tware basis pengetahuanaBagaimana tidak untuk he...tware basis pengetahuana
Bagaimana tidak untuk he...tware basis pengetahuana
 
Airflow ac 2
Airflow ac 2Airflow ac 2
Airflow ac 2
 
Subcool 2
Subcool 2Subcool 2
Subcool 2
 
Aliran dan penurunan tek...resistensi dan diameter
Aliran dan penurunan tek...resistensi dan diameterAliran dan penurunan tek...resistensi dan diameter
Aliran dan penurunan tek...resistensi dan diameter
 
Btu
BtuBtu
Btu
 
10 fluid dynamics
10 fluid dynamics10 fluid dynamics
10 fluid dynamics
 
Sediment Transport
Sediment TransportSediment Transport
Sediment Transport
 
Presentation on bernoulli
Presentation on bernoulliPresentation on bernoulli
Presentation on bernoulli
 
Stages Of A River
Stages Of A RiverStages Of A River
Stages Of A River
 
Sediment transport
Sediment transportSediment transport
Sediment transport
 
Fluvial Geomorphology
Fluvial GeomorphologyFluvial Geomorphology
Fluvial Geomorphology
 
Bernoulli and continuity equation
Bernoulli and continuity equationBernoulli and continuity equation
Bernoulli and continuity equation
 
Center of pressure and hydrostatic force on a submerged body rev
Center of pressure and hydrostatic force on a submerged body revCenter of pressure and hydrostatic force on a submerged body rev
Center of pressure and hydrostatic force on a submerged body rev
 
Fluids lab manual_2
Fluids lab manual_2Fluids lab manual_2
Fluids lab manual_2
 
River Channel Processes & Landforms
River Channel Processes & LandformsRiver Channel Processes & Landforms
River Channel Processes & Landforms
 
Power point presentation on kinetic energy and potential energy
Power point presentation on kinetic energy and potential energyPower point presentation on kinetic energy and potential energy
Power point presentation on kinetic energy and potential energy
 
Fluid mechanic white (cap2.1)
Fluid mechanic   white (cap2.1)Fluid mechanic   white (cap2.1)
Fluid mechanic white (cap2.1)
 
Rural Marketing, Basics
Rural Marketing, BasicsRural Marketing, Basics
Rural Marketing, Basics
 
ENERGY FLOW IN ECOSYSTEM
ENERGY FLOW IN ECOSYSTEMENERGY FLOW IN ECOSYSTEM
ENERGY FLOW IN ECOSYSTEM
 

Semelhante a Lesson 4 bernoulli's theorem

432491132-Physics-Project-Class-11.pdf bb
432491132-Physics-Project-Class-11.pdf bb432491132-Physics-Project-Class-11.pdf bb
432491132-Physics-Project-Class-11.pdf bbpixelyuo
 
unit 5 Principals of hydraulics.pptx
unit 5 Principals of hydraulics.pptxunit 5 Principals of hydraulics.pptx
unit 5 Principals of hydraulics.pptxshyleshkumar15
 
Bernoulli’s equation and its significance
Bernoulli’s equation and its significanceBernoulli’s equation and its significance
Bernoulli’s equation and its significanceRUDRASHISBISWAS
 
Lecture 10 Fluid Mechanics.pptx
Lecture 10 Fluid Mechanics.pptxLecture 10 Fluid Mechanics.pptx
Lecture 10 Fluid Mechanics.pptxOnofreAlgaraJr2
 
Ppa6 Lecture Ch 10
Ppa6 Lecture Ch 10Ppa6 Lecture Ch 10
Ppa6 Lecture Ch 10josoborned
 
Lecture 3 (1).pptx
Lecture 3 (1).pptxLecture 3 (1).pptx
Lecture 3 (1).pptxRobert Zedd
 
MECHANICAL_PROPERTIES_OF_FLUIDS.ppt
MECHANICAL_PROPERTIES_OF_FLUIDS.pptMECHANICAL_PROPERTIES_OF_FLUIDS.ppt
MECHANICAL_PROPERTIES_OF_FLUIDS.pptAryan979811
 
Lecture 3 bernoulli_s_theorm_it_s_applications
Lecture 3 bernoulli_s_theorm_it_s_applicationsLecture 3 bernoulli_s_theorm_it_s_applications
Lecture 3 bernoulli_s_theorm_it_s_applicationsRaghubir Singh
 
Fluids mechanics class 1 -Module 1
Fluids mechanics class 1 -Module 1Fluids mechanics class 1 -Module 1
Fluids mechanics class 1 -Module 1Mujeeb Muji
 
CH7 PC and SR.pptx
CH7 PC and SR.pptxCH7 PC and SR.pptx
CH7 PC and SR.pptxDawit Girma
 
SPM Physics - Solid and fluid pressure
SPM Physics - Solid and fluid pressureSPM Physics - Solid and fluid pressure
SPM Physics - Solid and fluid pressureTimothy Denis
 
Bernoulli's principle disputation 2016
Bernoulli's principle disputation 2016Bernoulli's principle disputation 2016
Bernoulli's principle disputation 2016Mity Wongkit
 
Pharmaceutical Engineering: Flow of fluids
Pharmaceutical Engineering: Flow of fluidsPharmaceutical Engineering: Flow of fluids
Pharmaceutical Engineering: Flow of fluidsParag Jain
 
Force pressure n 3 principles
Force pressure n 3 principlesForce pressure n 3 principles
Force pressure n 3 principlesSyiera Rahman
 
Pressure in still water and gases Experiment No. 3.pdf
Pressure in still water and gases Experiment No. 3.pdfPressure in still water and gases Experiment No. 3.pdf
Pressure in still water and gases Experiment No. 3.pdfKaiwan B. Hamasalih
 
Applications Of Fluid Mechanics In Different Engineering Fields
Applications Of Fluid Mechanics In Different Engineering FieldsApplications Of Fluid Mechanics In Different Engineering Fields
Applications Of Fluid Mechanics In Different Engineering FieldsYasmine Anino
 

Semelhante a Lesson 4 bernoulli's theorem (20)

432491132-Physics-Project-Class-11.pdf bb
432491132-Physics-Project-Class-11.pdf bb432491132-Physics-Project-Class-11.pdf bb
432491132-Physics-Project-Class-11.pdf bb
 
unit 5 Principals of hydraulics.pptx
unit 5 Principals of hydraulics.pptxunit 5 Principals of hydraulics.pptx
unit 5 Principals of hydraulics.pptx
 
Pressure
PressurePressure
Pressure
 
Bernoulli’s equation and its significance
Bernoulli’s equation and its significanceBernoulli’s equation and its significance
Bernoulli’s equation and its significance
 
Lecture 10 Fluid Mechanics.pptx
Lecture 10 Fluid Mechanics.pptxLecture 10 Fluid Mechanics.pptx
Lecture 10 Fluid Mechanics.pptx
 
Flow of fluids
Flow of fluidsFlow of fluids
Flow of fluids
 
Imegate4u
Imegate4uImegate4u
Imegate4u
 
Ppa6 Lecture Ch 10
Ppa6 Lecture Ch 10Ppa6 Lecture Ch 10
Ppa6 Lecture Ch 10
 
Lecture 3 (1).pptx
Lecture 3 (1).pptxLecture 3 (1).pptx
Lecture 3 (1).pptx
 
Mechanics of fluids
Mechanics of fluidsMechanics of fluids
Mechanics of fluids
 
MECHANICAL_PROPERTIES_OF_FLUIDS.ppt
MECHANICAL_PROPERTIES_OF_FLUIDS.pptMECHANICAL_PROPERTIES_OF_FLUIDS.ppt
MECHANICAL_PROPERTIES_OF_FLUIDS.ppt
 
Lecture 3 bernoulli_s_theorm_it_s_applications
Lecture 3 bernoulli_s_theorm_it_s_applicationsLecture 3 bernoulli_s_theorm_it_s_applications
Lecture 3 bernoulli_s_theorm_it_s_applications
 
Fluids mechanics class 1 -Module 1
Fluids mechanics class 1 -Module 1Fluids mechanics class 1 -Module 1
Fluids mechanics class 1 -Module 1
 
CH7 PC and SR.pptx
CH7 PC and SR.pptxCH7 PC and SR.pptx
CH7 PC and SR.pptx
 
SPM Physics - Solid and fluid pressure
SPM Physics - Solid and fluid pressureSPM Physics - Solid and fluid pressure
SPM Physics - Solid and fluid pressure
 
Bernoulli's principle disputation 2016
Bernoulli's principle disputation 2016Bernoulli's principle disputation 2016
Bernoulli's principle disputation 2016
 
Pharmaceutical Engineering: Flow of fluids
Pharmaceutical Engineering: Flow of fluidsPharmaceutical Engineering: Flow of fluids
Pharmaceutical Engineering: Flow of fluids
 
Force pressure n 3 principles
Force pressure n 3 principlesForce pressure n 3 principles
Force pressure n 3 principles
 
Pressure in still water and gases Experiment No. 3.pdf
Pressure in still water and gases Experiment No. 3.pdfPressure in still water and gases Experiment No. 3.pdf
Pressure in still water and gases Experiment No. 3.pdf
 
Applications Of Fluid Mechanics In Different Engineering Fields
Applications Of Fluid Mechanics In Different Engineering FieldsApplications Of Fluid Mechanics In Different Engineering Fields
Applications Of Fluid Mechanics In Different Engineering Fields
 

Lesson 4 bernoulli's theorem

  • 1. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm Lesson 4: Bernoulli's Theorem Objective In this lesson we will discuss the relationships of "fluid mechanics" and how it APPLIES to flow and pressure or head. The flow of ground water is controlled by the laws of physics and thermodynamics. We will discuss a variety of concepts that apply to ground water flow and hydro-geology, and also flow in a pipe as well as, the concept of pressure or "head." We will also discuss the Bernoulli equation or theorem. Reading Assignment Read the online lesson as well as Chapter 3 in your textbook. Lecture Introduction The flow of groundwater is controlled by the laws of physics, thermodynamics and hydro-geology. In this lesson we will assume that the water temperature is nearly constant and is not very warm. Most drinking water sources are not very warm even in the summer months. Thermodynamics is more important in industrial WATER TREATMENT , where boiler water is often treated, and is usually very hot to begin the process. We will study the process of mechanical energy. Water contains energy due to 1- elevation, 2- pressure and 3- velocity. Head is the amount of energy possessed by a unit quantity of water expressed in feet. (Example: A 30 ft. tank will have a head of 30 ft.) Simply put head is the vertical distance between two levels in a fluid. Another term for velocity pressure is dynamic pressure. We will briefly discuss some terms and relationships, which will help you to better understand the rest of this lesson. Velocity pressure = total pressure - static pressure. Velocity Head - the energy of motion; the vertical distance or height through which water must fall freely, under the force of gravity, to acquire the velocity that it possesses. It is theoretically equal to the square of the velocity divided by twice the acceleration of gravity. V2/ 2g Static Head - Head due to elevation: the actual elevation difference between water surfaces or a water surface and some other reference point. Example: If one WATER TANK is at the elevation of 2300ft., 1 dari 8 24/10/2014 23:35
  • 2. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm while another is at the elevation of 2100 ft., the static head would be 200 ft. Pressure Head - the head represented by the expression of pressure over weight (p/y ) where p is pressure and y is weight. Where p is in pounds /sq. ft. and y is the weight of the liquid per cubic feet, h is head in feet. 1 psi = 2.31 ft. and 1 ft. = 0.433 psi. These are very helpful conversions to use. For a unit volume of fluid, the mass, m, is numerically equal to the density, p, since density is defined as mass per unit volume. The total energy of the unit volume of fluid is the three components; 1- kinetic, 2- gravitational, 3- fluid pressure energy. E tv = ½ pv2 + pgz + P g = the acceleration of gravity z = the elevation of the center of gravity of the fluid v = velocity above the reference elevation. where Etv is the total energy per unit volume. If this equation is divided by p, the result is the total energy per unit mass..... E tm = v2/2 + gz + P/p )which is the BERNOULLI equation). The Bernoulli Theorem says that total pressure = the same at any two points along a streamline, in a flow. Total Pressure - static pressure + ½ × density × velocity squared. Total pressure = static pressure + dynamic pressure Static pressure = pressure that is measured when water is at rest. The Theory of Bernoulli This theory, which forms part of the study of hydraulic principles, states that the static pressure of a moving fluid varies inversely as its velocity, which means that as velocity increases, the static pressure decrease. The principle of the relationship between velocity and pressure is illustrated below. Two vessels (a) and (b), of the same shape and cross-sectional area, are joined together by a small-bore pipe, (c). If fluid is added to vessel (b) and gradually find its own level, this level will still be maintained if two positions (d) and (e) of the same size and weight are placed on the liquid in the vessels (a) and (b), respectively. If a force of 1N is exerted on piston (d), in a downward direction, fluid in (a) will flow through the pipe (c) into vessel (b). The velocity of the fluid will increase as it passes through (c), because the cross-sectional 2 dari 8 24/10/2014 23:35
  • 3. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm area of the pipe (c) is much less than that of (a), and the same volume of fluid must pass through (c) as leaves (a) in the same time. Some of the 1N pressure in (a) will be converted into velocity pressure in pipe (c), and a pressure gauge situated at (f) would REGISTER a pressure less than that equivalent to 1N. When the fluid reaches the vessel (b), its velocity will reduce to its original rate and some of the kinetic energy is reconverted into potential energy." Total Pressure: In flowing are, it is the sum of the static and velocity pressures. Velocity Pressure: In flowing air, it is the pressure due to velocity and density of air. Static Pressure: In flowing air, it is the total pressure minus velocity pressure, pushing equally in all directions. Pressure Static measures elevation change in feet. Static Pressure Static pressure is the difference between the air pressure on the inside of your barn and the air pressure outside your barn. The static pressure is an indicator of how much negative pressure the fans are creating and how effective they will be at drawing fresh air in through your inlets. An overly high static pressure can also indicate that you do not have enough inlets in your barn. In terms of your barn, the static pressure should be around 0.04" wc (inches of water column) to 0.10" wc. When it is warm outside, such as during the summer, and your fans are running on or near their maximum speed, you want your static pressure to be around 0.05". In the winter, you want the static pressure higher so that the air pulled through the inlets enters the room faster, promoting thorough mixing of incoming air with the air already in the barn. To measure static pressure in a barn you would use a manometer. The following diagrams indicate the changes in static pressure when your fans are off and when they are running. Fig. 4-1: This diagram shows a u-tube manometer measuring an equal pressure between the outside of the barn and the inside of the barn. This happens when the fans are off. 3 dari 8 24/10/2014 23:35
  • 4. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm Fig. 4-2: This diagram shows a u-tube manometer measuring a decreased pressure in the barn compared to outside due to the fans running. Note that compared to figure one the tube closest to the wall is lower because the greater pressure is pushing the liquid in the tube downward. Reference: BSM Agri Ltd. Velocity Pressure Tank Gauge - 20 psi = Line Gauge 4 dari 8 24/10/2014 23:35
  • 5. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm Swap gauges Tank Gauge - 20 psi = Line Gauge Velocity pressure is then 20 psi Velocity of water would be 57 feet/sec The faster the molecules flow, the harder it is to make a turn into the line gauge. Calculation of Velocity of a Fluid Through a Pipeline The speed or velocity of a fluid flowing through a channel or pipeline is related to the cross-sectional area of the pipeline and the quantity of water moving through the line. For example, if the diameter of a pipeline is reduced, then the velocity of the water in the line must increase to allow the same amount of water to pass through the line. SAMPLE Problem: If the flow through a 2 foot diameter pipe is 8 MGD, the velocity is: If this same 8 MGD flow is transferred to a pipe with a 1 foot diameter, the velocity would be: 5 dari 8 24/10/2014 23:35
  • 6. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm Based upon this example problem, we can see that if the cross-sectional area decreased, the velocity of the flow must increase. Mathematically we can say that the velocity and cross-sectional area are inversely proportional when the amount of flow (Q) is constant. (Fig. 4-3). This is extremely important in the operation of a centrifugal pump. 6 dari 8 24/10/2014 23:35
  • 7. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm Differential Pressure Molecular velocity energy is transferred directly to gauge. Much higher pressure. Review In this lesson we studied the concepts involved with fluid mechanics, such as total pressure, velocity pressure, and static pressure. Simply put HEAD is the vertical distance between two levels in a fluid. Total pressure is the sum of the static and velocity pressures, and velocity pressure is the pressure due to velocity and density of air, and static pressure is the total pressure minus velocity pressure, pushing equally in all direction. As well as, velocity head, static head, pressure head. Velocity head is the energy of motion, while static head is the actual head due to elevation, while pressure head is the ratio of pressure over weight, if pressure is in pounds per square foot and weight is in cubic feet, and head is in feet. We also discussed the calculation of velocity of a fluid through a pipeline, and conversions from feet of water to head in psi. Sources Water Distribution Operator Training Handbook - AWWA APPLIED Hydro-geology - Merrill Publishing Co., C.W. Fetter Operator Certification Study Guide - AWWA 7 dari 8 24/10/2014 23:35
  • 8. Lesson 4: Bernoulli's Theorem http://water.me.vccs.edu/courses/CIV240/lesson4_print.htm LEGO Design & PROGRAMMING Systems - "Ask an Engineer" BSM Agri Ltd. Assignment Answer the following questions and either email or fax to the instructor. The total dynamic head against which 1. a pump must operate is ______________. A well is pumping into a reservoir at 300 gpm while the service pumps are pumping from the reservoir at 400 gpm. Which direction is the reservoir (tank) level going: 2. In a well the static water level is 15 feet. The pumping water level is 45 feet. The drawdown is how much? 3. A venturi tube increases the velocity and decreases the pressure as water flows through it. This type of tube is used to ______________. 4. 5. If one tank in a system is at 2100 ft. elevation, and another tank, same size, is at 2300 ft. elevation, what is the static head? 8 dari 8 24/10/2014 23:35