Quiz 2 – 2013.11.27.

Slides:



Advertisements
Similar presentations
Chapter Four Fluid Dynamic
Advertisements

Chapter Four Fluid Dynamic
Integration Relation for Control Volume
Lecture 15: Capillary motion
Chapter 2 Introduction to Heat Transfer
Convection.
First Law of Thermodynamics - Open Systems
Chapter 4 Mass and Energy Analysis of Control Volumes (Open Systems)
The Bernoulli Equation - Work and Energy
Energy Conservation (Bernoulli’s Equation)
MASS, MOMENTUM , AND ENERGY EQUATIONS
First Law of Thermodynamics-The Energy Equation (4) Work transfer can also occur at the control surface when a force associated with fluid normal stress.
Equations of Continuity
Exergy: A Measure of Work Potential Study Guide in PowerPoint
Mass and Energy Analysis of Control Volumes. 2 Conservation of Energy for Control volumes The conservation of mass and the conservation of energy principles.
1 Lec 26: Frictionless flow with work, pipe flow.
CE 230-Engineering Fluid Mechanics Lecture # 18 CONTINUITY EQUATION Section 5.3 (p.154) in text.
CHE/ME 109 Heat Transfer in Electronics
Chapter 5 Mass and Energy Analysis of Control Volumes Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition.
Chapter 4 Fluid Flow, Heat Transfer, and Mass Transfer:
Fluid mechanics 3.1 – key points
Chapter 7 Energy and Energy Balance
PTT 201/4 THERMODYNAMIC SEM 1 (2012/2013). Objectives Apply the second law of thermodynamics to processes. Define a new property called entropy to quantify.
Conservation Laws for Continua
CHAPTER 7 ENERGY PRINCIPLE
SURVIVAL MODE Quiz 3 –
PHAROS UNIVERSITY ME 259 FLUID MECHANICS FOR ELECTRICAL STUDENTS Basic Equations for a Control Volume.
4 CHAPTER The First Law of Thermodynamics: Control Volumes.
Energy Equation. Chapter 2 Lecture 3 2 Mechanical Energy? Forms of energy that can be converted to MECHANICAL WORK completely and directly by mechanical.
Molecular Transport Equations. Outline 1.Molecular Transport Equations 2.Viscosity of Fluids 3.Fluid Flow.
Lecture slides by Mehmet Kanoglu
Lesson 21 Laminar and Turbulent Flow
Conservation of mass If we imagine a volume of fluid in a basin, we can make a statement about the change in mass that might occur if we add or remove.
Lesson 22 BERNOULLI’S EQUATION
Physics 1B03summer-Lecture 13 Final Exam April 18 2 hours long – 30 MC questions Covers all material with approximately equal weight, up to and including.
CBE 150A – Transport Spring Semester 2014 Macroscopic Mechanical Energy Balance.
Chapter 4 Control Volume Analysis Using Energy. Learning Outcomes ►Distinguish between steady-state and transient analysis, ►Distinguishing between mass.
CHAPTER 3 EXACT ONE-DIMENSIONAL SOLUTIONS 3.1 Introduction  Temperature solution depends on velocity  Velocity is governed by non-linear Navier-Stokes.
Chapter 7 Energy and Energy Balance By : Mrs. Norazian Mohamed Noor
AGUS HARYANTO 01 March  Examine the moving boundary work or P.dV work.  Identify the first law of thermodynamics for closed (fixed mass) systems.
Dr. Jason Roney Mechanical and Aerospace Engineering
Chapter 7 Energy and Energy Balance
INTRODUCTION TO CONVECTION
Work Readings: Chapter 11.
NNPC FSTP ENGINEERS Physics Course Code: Lesson 7.

MFSacedon Study of Fluids. MFSacedon Fluids in Motion Topics: Fluid flows Continuity equation Bernoulli ‘s Energy Equation.
Chapter 4 ENERGY ANALYSIS OF CLOSED SYSTEMS
Transport process In molecular transport processes in general we are concerned with the transfer or movement of a given property or entire by molecular.
Basic equations of fluid flow. The principles of physics most useful in the applications of the fluid mechanics are mass- balance, or continuity ; the.
Dr. Owen Clarkin School of Mechanical & Manufacturing Engineering Summary of Energy Topics Chapter 1: Thermodynamics / Energy Introduction Chapter 2: Systems.
Chapter 5 Part 2 Mass and Energy Analysis of Control Volumes Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 8th edition.
First Law of Thermodynamics applied to Flow processes
CE 3305 Engineering FLUID MECHANICS
Energy Conservation (Bernoulli’s Equation)
ABE 223 ABE Principles – Machine systems Bernoulli’s Law Tony Grift
Chapter 6 Energy and Energy Balance
Introduction to Fluid Mechanics
KINEMATICS 1. A nozzle is so shaped that the velocity of flow along the centre line changes linearly from 1.5 m/s to 15 m/s in a distance of m. Determine.
3.4 Continuity Equation The use of Eq. (3.3.1) is developed in this section. First, consider steady flow through a portion of the stream tube of Fig. 3.4.
Fluid kinematics Chapter 3
Chapter 5 Mass and Energy Analysis of Control Volumes Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 6th edition.
Chapter 6 THE MECHANICAL ENERGY BALANCE.
Chapter 6 THE MECHANICAL ENERGY BALANCE.
Mass and Energy Analysis of Control Volumes (Open Systems)
Chapter 6 ENERGY ANALYSIS OF CLOSED SYSTEM
FLUID MECHANICS - Review
4 CHAPTER The First Law of Thermodynamics: Control Volumes.
Ch. 4 The first law of thermodynamics: Control Volume
Energy Conservation (Bernoulli’s Equation)
Presentation transcript:

Quiz 2 – 2013.11.27

TIME IS UP!!! Questions What is the Reynolds number? Differentiate the flow patterns observed in laminar flow from those in turbulent flow. How does temperature affect the dynamic viscosity of a fluid? TIME IS UP!!!

Overall Balances

Outline Mass Balance Energy Balance Momentum Balance

Mass Balance For an overall mass balance, no mass is being generated. Why?

Mass Balance Imagine the control volume as having infinitesimal surfaces dA. We need to find the net outflow of mass across the control surface.

Mass Balance For every dA element, a streamline of velocity vector v passes through it.

Mass Balance For every dA element, a unit normal vector n exists.

Mass Balance The component of velocity vector v in the direction of the unit normal vector n is given by:

Mass Balance The rate of mass efflux through dA:

Mass Balance What do we get when we integrate over the entire control surface?

Mass Balance POSITIVE: net outflow of mass NEGATIVE: net inflow of mass ZERO: ?

Mass Balance Rate of mass outflow across control surface (and control volume): Rate of mass accumulation in control volume:

Mass Balance

Overall Mass Balance

Overall Mass Balance A well-stirred storage vessel contains 10000 kg of dilute methanol solution (xMetOH = 0.05). A constant flow of 500 kg/min of pure water is suddenly introduced into the tank and a constant rate of withdrawal of 500 kg/min of solution is started. These two flows are continued and remain constant. Assuming that the densities of the solutions are the same and that the total contents of the tank remain constant at 10,000 kg of solution, calculate the time for the alcohol content to drop to 1.0 wt.%.

Outline Mass Balance Energy Balance Momentum Balance

Forms of Energy Possessed/Carried by fluid Internal Energy Potential Energy Kinetic Energy PV-work Transferred between system and surroundings Heat Shaft work

Internal Energy (U) Intrinsic property of the fluid Molecules in random motion

Potential Energy (mgz) Position of the fluid with respect to an arbitrary reference plane

Kinetic Energy (mv2/2α) Due to fluid motion Correction factor, a To account for velocity distribution Ranges from 0.5 (laminar) to 1.0 (turbulent)

PV Work (PV) Work done by surroundings to push the fluid into the system P S d

Heat (Q) Net heat passing through the boundary of the system Positive if heat is transferred to the system from the surroundings Negative if system to the surroundings Excludes heat generated by friction

Shaft Work (Ws) Net work done on the system by the surroundings Convention (IUPAC) Positive if work done on the system Negative if work done by the system

Total Energy Balance Energy balance from point 1 to point 2: U1, v1, P1, V1, S1 Q z1 U2, v2, P2, V2, S2 Ws z2 Datum/reference plane

Total Energy Balance Energy balance from point 1 to point 2:

Total Energy Balance Water at 93.3°C is being pumped from a large storage tank at 1 atm abs at a rate of 0.189 m3/min by a pump. The motor that drives the pump supplies energy at the rate of 1.49 kW. The water is pumped through a heat exchanger, where it gives up 704 kW of heat and is then delivered to a large open storage tank 15.24 m above the first tank. What is the final temperature of the water to the second tank?

Mechanical Energy Balance A modification of the total energy balance - shaft work - kinetic energy - potential energy - flow work (PV) Does not include heat and internal energy. - Why? Energy converted to heat is lost work - loss of mechanical energy by friction

Ideal Fluids Bernoulli Equation No shear stress; zero viscosity For isothermal flow and Q=WS=0, Bernoulli Equation

Bernoulli Equation Restrictions: Valid only for incompressible fluids No devices that add/remove energy should be between points 1 and 2 No heat transfer occurring in the system No loss of energy due to friction

Real Fluids Friction losses: SF (energy dissipation) Total heat absorbed by the fluid Total work done by fluid, -W = -WS + SF Additional work must be done by the fluid to overcome fluid friction

Real Fluids Note: energy per mass units kJ/kg or ft-lbf/lbm For incompressible flow: Derivation for incompressible flow energy balance skipped