Non-frictional Source of Entropy Generation… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Rotational Inviscid Flows.

Slides:



Advertisements
Similar presentations
Chapter 17 Compressible Flow Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus A. Çengel and.
Advertisements

One-dimensional Flow 3.1 Introduction Normal shock
16 CHAPTER Thermodynamics of High-Speed Gas Flow.
Effect of Piston Dwell on Engine Performance P M V Subbarao Professor Mechanical Engineering Department Sufficiency of time to Execute a Process…..
Analysis of Oblique Shocks P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi A Mild, Efficient and Compact Compressor ….
Ch4 Oblique Shock and Expansion Waves
Lecture 5 Shaft power cycles Aircraft engine performance
Point Velocity Measurements
Continuum Mechanics Analysis of Supersonic Flow Submitted by Rajendra B Dubagunta Siva Prasad Rao Batchu Visweswara Mudiam Sandeep Kancharla Narayana Kalpana.
Gas Dynamics ESA 341 Chapter 3
Thermodynamic Analysis of Internal Combustion Engines P M V SUBBARAO Professor Mechanical Engineering Department IIT Delhi Work on A Blue Print Before.
Assessment of Engine Breathing Capacity P M V Subbarao Professor Mechanical Engineering Department Measure of Filling & Emptying Effectiveness….
Salient Features of Gas Dynamics
Tamed Effect of Normal Stress in VFF… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Negligible Bulk Viscosity Model for Momentum.
Deduction of Fundamental Laws for Heat Exchangers P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Modification of Basic Laws for.
Compressible Flow.
Chapter II Isentropic Flow
Analysis of A Disturbance in A Gas Flow P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Search for More Physics through.
Analysis of Disturbance P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Modeling of A Quasi-static Process in A Medium.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS Compressible Flow Over Airfoils: Linearized Subsonic Flow Mechanical and Aerospace Engineering Department Florida.
MAE 3241: AERODYNAMICS AND FLIGHT MECHANICS
P M V Subbarao Professor Mechanical Engineering Department I I T Delhi
Analysis of Expansion Waves P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Another Zero Cost Nozzle …..
Mach ’ s Measure of Flying P M V Subbarao Professor Mechanical Engineering Department Lecture - 8 A Thoughtful Measure of Speed of Fast Flyers….
Historically the First Fluid Flow Solution …. P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Second Class of Simple Flows.
One Dimensional Flow of Blissful Fluid -III P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Always Start with simplest Inventions……..
Basics of GAS DYNAMICS P M V Subbarao Associate Professor Mechanical Engineering Department I I T Delhi Alphabets of this new literature called Gas Dynamics.
The figure shows that the minimum area which can occur in a given isentropic duct flow is the sonic, or critical throat area. Choking For γ=1.4, this reduces.
One Dimensional Flow with Heat Addition
Supersonic flow and shockwaves
HIGH SPEED FLOW 1 st Semester 2007 Pawarej CHOMDEJ Jun-071.
Gas dynamics of Real Combustion in Turbo Combustor P M V Subbarao Professor Mechanical Engineering Department Make Sure that design is Acceptable to Gas.
Compressible Frictional Flow Past Wings P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Small and Significant Region of Curse.
First step in Understanding the Nature of Fluid Flow…. P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Analysis of Simplest Flow.
Dr. R. Nagarajan Professor Dept of Chemical Engineering IIT Madras
ME2213 Fluid Mechanics II Version – 1 (ME-13) Date: 23/12/2015
Design & Aerodynamics of Inlets & Nozzles P M V Subbarao Professor Mechanical Engineering Department Understanding of Real Flow Through Passive Devices…….
MAE 5380: Advanced Propulsion Thermodynamics Review and Cycle Analysis Overview Mechanical and Aerospace Engineering Department Florida Institute of Technology.
Reflection of Oblique Shocks P M V Subbarao Professor Mechanical Engineering Department I I T Delhi A Train of Waves ….. Where to End ???
Oblique Shocks -1 School of Aerospace Engineering Copyright © 2001 by Jerry M. Seitzman. All rights reserved. AE3450 Supersonic Flow Turning For normal.
Flow of Compressible Fluids. Definition A compressible flow is a flow in which the fluid density ρ varies significantly within the flowfield. Therefore,
Chapter 12 Compressible Flow
Prof. dr. A. Achterberg, Astronomical Dept., IMAPP, Radboud Universiteit.
Shock waves and expansion waves Rayleigh flow Fanno flow Assignment
Great Innovations are possible through General Understanding …. P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Thermodynamic View.
Subject Name: FLUID MECHANICS Subject Code:10ME36B Prepared By: R Punith Department: Aeronautical Engineering Date:
4th Global Engineering, Science and Technology Conference
Power Consuming Fluid Machines - II
Mach’s Vision of Flying
Entropy Generators in Simplest Flow
Oblique Shocks : Less Irreversible Thermodynamic Devices
Gas Dynamics for Design of Nozzles
A course in Gas Dynamics…………………………………. …. …Lecturer: Dr
Analysis of the Simplest Flow
The Second Extreme Gas Dynamic Activity
Gas Dynamics for Design of Intakes
Analysis of Two Extreme Gas Dynamic Activities
MAE 5350: Gas Turbines Ideal Cycle Analysis
Identification of Fundamental Design Parameter for A Wind Turbine
The Bow Shock and Magnetosheath
Prof. dr. A. Achterberg, Astronomical Dept
Prof. dr. A. Achterberg, Astronomical Dept
P M V Subbarao Professor Mechanical Engineering Department
Mach’s construction Dr Andrew French.
Section 11 Lecture 2: Analysis of Supersonic Conical Flows
CHAPTER THREE NORMAL SHOCK WAVES
Introduction to Fluid Mechanics
Control of Entropy Generation due to Shock
Introduction to Fluid Mechanics
Presentation transcript:

Non-frictional Source of Entropy Generation… P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Rotational Inviscid Flows

Inviscid-compressible Flows Above equation shows that despite the inviscid flow assumption, it contains vorticities that are inherent in viscous flows but special in inviscid flows. The vortices cause additional entropy production in inviscid flows. This can be better explained using the first law of thermodynamics.

Governing Equations for Inviscid-compressible Flows

Gibbs form of First Law of Thermodynamics For an infinitesimal flow process For a differential displacement,

First Law of Thermodynamics for Inviscid compressible flow with s as the specific entropy, h as the specific static enthalpy and p the static pressure. Inserting the above property changes into the first law of thermodynamics For a differential displacement,

The expression in the parentheses on the left-hand side of above equation is the total enthalpy. In the absence of mechanical or thermal energy addition or rejection for an adiabatic flow; h total remains constant. Meaning that its gradient vanishes. Furthermore, for steady flow cases,

Above equation is an important result that establishes a direct relation between the vorticity and the entropy production in inviscid flows. A flow field generates discontinuities as a result of the presence of shock waves. These are responsible for large jumps in velocities. These jumps cause vorticity production and therefore, changes in entropy.

Discontinuities in High Speed Flows

High Speed Jet Engines

Discontinuities Ahead of inlet

Weakening of Discontinuity : Infinitesimal Strength & Reversible Discontinuity When High speed object is either a “point” or “thin rod”, the discontinuity in an invsicd flow, the discontinuity will weaken to an isentropic flow process. This discontinuity is called as Mach Wave.

Mach’s Measure of Speed Prof. Mach initiated the art of understanding the basic characteristics of high speed flow. He proposed that one of the most important variables affecting aerodynamic behavior is the speed of the air flow over a body (V) relative to the speed of sound (c). Mach was the first physicist to recognize that dependency. He was also the first to note the sudden and discontinuous changes in the behavior of an airflow when the ratio V/c goes from being less than 1 to greater than 1. Ernst Mach ( )

The Thought Experiment

Mach’s Flow Visualization Experiments Ernst Mach's photo of a bullet in supersonic flight Mach was actually the first person in history to develop a method for visualizing the flow passing over an object at supersonic speeds. He was also the first to understand the fundamental principles that govern supersonic flow and their impact on aerodynamics.

Speed of sound in a Fluid Flow The speed of sound can be obtained easily

Moving Disturbance In A Fluid As an infinitesimal object moves through a fluid medium it creates pressure waves. Pressure waves travel out at the speed of sound which in term depends on nature of fluid. If the object is traveling significantly slower than sonic velocity, then pressure waves travel out uniformly similar to waves on the surface of a pond.

Moving Disturbance In A Fluid As the object approaches the speed of sound, it begins to catch up with the pressure waves and creates an infinitesimally weak flow discontinuity just ahead of the aircraft

Moving Disturbance In A Fluid As the vehicle breaks the speed of sound, the infinitesimally weak Shock waves begin to add up along a “Mach Line”.

Moving Disturbance In A Fluid As Mach number increases, the strength of the shock wave increases and the Angle of the shockwave becomes increasingly severe Credit: Selkirk College Professional Aviation Program

Mach Waves, Revisited A ‘’point-mass’’ object moving with Supersonic velocity Generates an infinitesimally weak “mach wave”. The direction of flow remains unchanged across Mach wave.

Irreversible Discontinuity in High Speed Inviscid Flows When generating object is larger than a “point”, shockwave is stronger than mach wave …. Oblique shock wave  -- shock angle  -- turning or “wedge angle”

High Angle Objects  max  max

Descent of A Spacecraft

Landing of A Space Craft