G22.2243-001 High Performance Computer Architecture
Lecture 4 Branch Prediction Scoreboarding September 28, 2004
Outline
Announcements
Assignment 1 due back October 5th
Reducing the impact of control hazards
Branch prediction buffers Branch target buff
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 1
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Basic Definitions
Dr. M. H. Saidi
Thermodynamics: study of the macroscopi
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 27
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Phase Equilibrium Models
Dr. M. H. Saidi
Binary phase equilibrium models
School of Mechanical Engineering
Sharif University of Technology
Convection Heat Transfer
Instructor: M.H.Saidi
PhD, Professor
Lecture #4
Fall 2011
1
Convection Heat Transfer
2
Convection Heat Transfer
Summary of second session:
vScale Analysis
vIntroduct
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 21
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Generalized Eq. of State
Dr. M. H. Saidi
Ad. Thermodynamics
Generalized E
School of Mechanical Engineering
Sharif University of Technology
Convection Heat Transfer
Instructor: M.H.Saidi
PhD., Professor
Lecture #3
Fall 2011
1
Convection Heat Transfer
2
Convection Heat Transfer
Summary of second session:
vThermodynamics laws
vAn
School of Mechanical Engineering
Sharif University of Technology
Convection Heat Transfer
Instructor: M.H.Saidi
Ph.D., Professor
Lecture #5
Fall 2011
1
Convection Heat Transfer
2
Convection Heat Transfer
Summary of previous session
vLaminar Boundary Layer
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 8
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Legendre Transformation
Dr. M. H. Saidi
Y =Y ( X )
= (P )
dY
P=
dX
= P X
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 18
Dr. M. H. Saidi
2011
Entropy
Ad. Thermodynamics
Dr. M. H. Saidi
What is the relation between Entropy, S, and the
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 22
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Generalized Properties
Generalized Equations of State
Generalized compr
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 24
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Mixtures & Solutions
Dr. M. H. Saidi
These models may be used for solid
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 7
Dr. M. H. Saidi
2011
Extreme Principles
Ad. Thermodynamics
Dr. M. H. Saidi
Postulate #2
fundamental equation can
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 28
Dr. M. H. Saidi
2011
Ad. Thermodynamics
T, P
Mix.
A, B, C, D
Chemical Equilibrium
Dr. M. H. Saidi
Equil. Comp. n
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 9
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Maxwell Relations
The Maxwell relations may be represented as:
Dr. M. H.
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 20
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Compressibility Factor
Dr. M. H. Saidi
Z=compressibility factor
PV = ZRT
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 13
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Heat Exchanger
Dr. M. H. Saidi
For simplification, consider an average t
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 26
Dr. M. H. Saidi
2011
Phase Equilibrium
Ad. Thermodynamics
Dr. M. H. Saidi
In a pure substance
dT = 0 T = const
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 15
Dr. M. H. Saidi
2011
Throttling Valve
Ad. Thermodynamics
Concept of recovering lost work.
Example:
Throttling pr
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 2
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Thermodynamics Postulates
Dr. M. H. Saidi
Postulate I:
There exist parti
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 25
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Ideal Solution Model
Dr. M. H. Saidi
Ideal solutions: VA v A = 0 , at P,
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 16
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Statistical Definitions
Dr. M. H. Saidi
Microstate: Exact specification
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 11
Dr. M. H. Saidi
2011
Heat Engine
Ad. Thermodynamics
Heat engine performance index:
QH
W QH QL
th =
=
= 1
QH
QH
Q
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 19
Dr. M. H. Saidi
2011
Translational P. F.
Ad. Thermodynamics
Dr. M. H. Saidi
Monoatomic ideal gas:
They only hav
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 23
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Generalized Fugacity Chart
Dr. M. H. Saidi
Fugacity is pseudo pressure a
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 12
Dr. M. H. Saidi
2011
Exergy Analysis for a C.V.
Ad. Thermodynamics
Q& 0
W&C .V .
m& in1
m& in 2
m& in 3
Q&1 (T1 )
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 14
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Exergy & Energy Analysis
Dr. M. H. Saidi
Exergy analysis (2nd law analys
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 6
Dr. M. H. Saidi
2011
Ad. Thermodynamics
RWS, RHS, and Reservoirs
Dr. M. H. Saidi
Reversible Work Source (RWS):
A
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 10
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Exergy
Dr. M. H. Saidi
Exergy=available reversible work
Simultaneous in
Sharif University of Technology
School of Mechanical Engineering
Center of Excellence in Energy Conversion
Advanced Thermodynamics
Lecture 17
Dr. M. H. Saidi
2011
Ad. Thermodynamics
Thermodynamic Probability
= Thermodynamic Probability
Bol .
g Nj j
= N