Fluid Mechanics and Energy Fluid Mechanics and Energy Transport Transport BIEN 301 BIEN 301 Lecture 15 Lecture 15 Compressible Flows Continued – Isentropic Compressible Flows Continued – Isentropic Flow Flow Juan M. Lopez, E.I.T. Juan M. Lopez, E.I.T. Research Consultant Research Consultant LeTourneau University LeTourneau University Adjunct Lecturer Adjunct Lecturer Louisiana Tech University Louisiana Tech University
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Juan M. Lopez, E.I.T. Research Consultant LeTourneau University Adjunct Lecturer
Fluid Mechanics and Energy Transport BIEN 301 Lecture 15 Compressible Flows Continued – Isentropic Flow. Juan M. Lopez, E.I.T. Research Consultant LeTourneau University Adjunct Lecturer Louisiana Tech University. Isentropic Flow. Area Changes (White 9.4) - PowerPoint PPT Presentation
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Fluid Mechanics and Energy TransportFluid Mechanics and Energy TransportBIEN 301BIEN 301
Lecture 15Lecture 15Compressible Flows Continued – Isentropic FlowCompressible Flows Continued – Isentropic Flow
Juan M. Lopez, E.I.T.Juan M. Lopez, E.I.T.
Research ConsultantResearch ConsultantLeTourneau UniversityLeTourneau University
Adjunct LecturerAdjunct LecturerLouisiana Tech UniversityLouisiana Tech University
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Isentropic FlowIsentropic Flow
Area Changes Area Changes (White 9.4)(White 9.4)
Flow can be considered one-dimensional Flow can be considered one-dimensional when:when:• There is a no slip condition at the wallThere is a no slip condition at the wall• dh/dx << 1 and h(x) << R(x)dh/dx << 1 and h(x) << R(x)• V = V(x), reacts to changes in areaV = V(x), reacts to changes in area
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Isentropic FlowIsentropic Flow
Differential form of continuity for area-dependent Differential form of continuity for area-dependent 1D flow:1D flow:
0A
dA
V
dVd
This simple relationship helps us predict the behavior This simple relationship helps us predict the behavior of a compressible fluid in a 1D flow situation.of a compressible fluid in a 1D flow situation.
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Isentropic FlowIsentropic Flow
dV < 0dV < 0
dp > 0dp > 0
Subsonic Subsonic DiffuserDiffuser
dV > 0dV > 0
dp < 0dp < 0
Subsonic Subsonic NozzleNozzle
dV > 0dV > 0
dp < 0dp < 0
Supersonic Supersonic NozzleNozzle
dV < 0dV < 0
dp > 0dp > 0
Supersonic Supersonic DiffuserDiffuser
dA > 0dA > 0
dA < 0dA < 0
Ma < 1Ma < 1 Ma > 1Ma > 1
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Isentropic FlowIsentropic Flow
More relationshipsMore relationships
22
2
1
1
:flows ibleincompressFor
Sound) of (Speed
Equation) (Momentum0
V
dp
MaA
dA
V
dV
dadp
VdVdp
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Isentropic FlowIsentropic Flow
Ideal Gas Area ChangeIdeal Gas Area Change• The previous equation helps us to identify a maximum mass The previous equation helps us to identify a maximum mass
flow (choking condition) for compressible, isentropic flows:flow (choking condition) for compressible, isentropic flows:
kk
k
p
p
p
p
k
k
p
RT
A
m
RT
ARTAm
1
0
2
00
0
21
0
021
00max
11
2
:choking)(not function flow mass local aWith
6874.06874.0
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Isentropic FlowIsentropic Flow
Eq’s 9.48a-dEq’s 9.48a-d Provide good relationships for the mach number at Provide good relationships for the mach number at
different area relationships.different area relationships.
We will be skipping the sections on shock We will be skipping the sections on shock waves.waves. Read them for your own edification-the material is Read them for your own edification-the material is
good, the pictures are quite interestinggood, the pictures are quite interesting
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Blood FlowBlood Flow
From these equations to blood flow is From these equations to blood flow is quite a ways. However, I wanted to be quite a ways. However, I wanted to be sure we had the foundations before we sure we had the foundations before we saw a true blood flow solution worked out.saw a true blood flow solution worked out.
Here is a full blood flow solution for Here is a full blood flow solution for pulsatile flow. Poiseuille flow is utilized.pulsatile flow. Poiseuille flow is utilized.
Examples of Comprehensive Flow Solutions
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Isentropic FlowIsentropic Flow Converging and Diverging NozzlesConverging and Diverging Nozzles
A few examplesA few examples• Example 9.8Example 9.8• Example 9.9Example 9.9• P9.63P9.63• P9.65P9.65
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
Chapter 9 HomeworkChapter 9 Homework
DUE 2/22/2007DUE 2/22/2007
P9.11P9.11P9.43P9.43P9.78P9.78P9.88P9.88
EC: P9.114EC: P9.114
Due with the Ch. 7 and Ch. 8 HW.Due with the Ch. 7 and Ch. 8 HW.
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007
RememberRemember
Study Session tomorrow nightStudy Session tomorrow night Project Questions – Office hours today, Project Questions – Office hours today,
tomorrow, and during the study sessiontomorrow, and during the study session Report format is required on the final Report format is required on the final
projects.projects. Projects due Thursday!Projects due Thursday!
2/6/20072/6/2007 BIEN 301 – Winter 2006-2007BIEN 301 – Winter 2006-2007