Fundamentals of Gas Dynamics (NOC16 - ME05) Assignment - 8 : Solutions

Similar documents
Fundamentals of Gas Dynamics (NOC16 - ME05) Assignment - 10 : Solutions

6.1 According to Handbook of Chemistry and Physics the composition of air is

In which of the following scenarios is applying the following form of Bernoulli s equation: steady, inviscid, uniform stream of water. Ma = 0.

SUPERSONIC WIND TUNNEL Project One. Charles R. O Neill School of Mechanical and Aerospace Engineering Oklahoma State University Stillwater, OK 74078

One-Dimensional Isentropic Flow

IX. COMPRESSIBLE FLOW. ρ = P

1. (20 pts total 2pts each) - Circle the most correct answer for the following questions.

Lecture-2. One-dimensional Compressible Fluid Flow in Variable Area

P 1 P * 1 T P * 1 T 1 T * 1. s 1 P 1

Introduction to Fluid Mechanics. Chapter 13 Compressible Flow. Fox, Pritchard, & McDonald

Please welcome for any correction or misprint in the entire manuscript and your valuable suggestions kindly mail us

Review of Fundamentals - Fluid Mechanics

for what specific application did Henri Pitot develop the Pitot tube? what was the name of NACA s (now NASA) first research laboratory?

AEROSPACE ENGINEERING DEPARTMENT. Second Year - Second Term ( ) Fluid Mechanics & Gas Dynamics

SPC 407 Sheet 2 - Solution Compressible Flow - Governing Equations

Introduction to Aerospace Engineering

Applied Gas Dynamics Flow With Friction and Heat Transfer

Signature: (Note that unsigned exams will be given a score of zero.)

Lecture with Numerical Examples of Ramjet, Pulsejet and Scramjet

Compressible Flow. Professor Ugur GUVEN Aerospace Engineer Spacecraft Propulsion Specialist

Chapter 17. For the most part, we have limited our consideration so COMPRESSIBLE FLOW. Objectives

2013/5/22. ( + ) ( ) = = momentum outflow rate. ( x) FPressure. 9.3 Nozzles. δ q= heat added into the fluid per unit mass

GAS DYNAMICS AND JET PROPULSION

UNIT 1 COMPRESSIBLE FLOW FUNDAMENTALS


Figure 1. Mach cone that arises upon supersonic flow around an object

DESIGN & COMPUTATIONAL FLUID DYNAMICS ANALYSES OF AN AXISYMMETRIC NOZZLE AT TRANSONIC FREE STREAM CONDITIONS

Gas Dynamics and Jet Propulsion

Isentropic Duct Flows

SPC 407 Sheet 5 - Solution Compressible Flow Rayleigh Flow

THEORETICAL AND EXPERIMENTAL INVESTIGATIONS ON CHOKING PHENOMENA OF AXISYMMETRIC CONVERGENT NOZZLE FLOW

SPC 407 Sheet 6 - Solution Compressible Flow Fanno Flow

Civil aeroengines for subsonic cruise have convergent nozzles (page 83):

GAS DYNAMICS. M. Halük Aksel. O. Cahit Eralp. and. Middle East Technical University Ankara, Turkey

Rocket Thermodynamics

Supersonic air and wet steam jet using simplified de Laval nozzle

AOE 3114 Compressible Aerodynamics

Final 1. (25) 2. (10) 3. (10) 4. (10) 5. (10) 6. (10) TOTAL = HW = % MIDTERM = % FINAL = % COURSE GRADE =

Notes #4a MAE 533, Fluid Mechanics

Introduction to Aerospace Engineering

1. For an ideal gas, internal energy is considered to be a function of only. YOUR ANSWER: Temperature

Jet Aircraft Propulsion Prof. Bhaskar Roy Prof. A.M. Pradeep Department of Aerospace Engineering

MCE380: Measurements and Instrumentation Lab

Chapter 3 Bernoulli Equation

HOMEWORK ASSIGNMENT ON BERNOULLI S EQUATION

Aerothermodynamics of High Speed Flows

Steady waves in compressible flow

Effects of Disturbances on Quiet Flow in the Mach 4 Ludwieg Tube

the pitot static measurement equal to a constant C which is to take into account the effect of viscosity and so on.

Fluid Mechanics c) Orificemeter a) Viscous force, Turbulence force, Compressible force a) Turbulence force c) Integration d) The flow is rotational

ME 440 Aerospace Engineering Fundamentals

2 Navier-Stokes Equations

Introduction. In general, gases are highly compressible and liquids have a very low compressibility. COMPRESSIBLE FLOW

Simulation of Condensing Compressible Flows

High speed wind tunnels 2.0 Definition of high speed. 2.1 Types of high speed wind tunnels

Aerodynamics. Basic Aerodynamics. Continuity equation (mass conserved) Some thermodynamics. Energy equation (energy conserved)

Introduction to Chemical Engineering Thermodynamics. Chapter 7. KFUPM Housam Binous CHE 303

Compressible Fluid Flow

Design and Optimization of De Lavel Nozzle to Prevent Shock Induced Flow Separation

William В. Brower, Jr. A PRIMER IN FLUID MECHANICS. Dynamics of Flows in One Space Dimension. CRC Press Boca Raton London New York Washington, D.C.

Flow Characteristic Through Convergent-Divergent Nozzle

AME 436. Energy and Propulsion. Lecture 15 Propulsion 5: Hypersonic propulsion

FUNDAMENTALS OF GAS DYNAMICS

WALL ROUGHNESS EFFECTS ON SHOCK BOUNDARY LAYER INTERACTION FLOWS

Experimental Study of Steam Flow in a Convergent-Divergent Nozzle

AER210 VECTOR CALCULUS and FLUID MECHANICS. Quiz 4 Duration: 70 minutes

Introduction to Gas Dynamics All Lecture Slides

Influence of Molecular Complexity on Nozzle Design for an Organic Vapor Wind Tunnel

Fluid Mechanics - Course 123 COMPRESSIBLE FLOW

Gasdynamics 1-D compressible, inviscid, stationary, adiabatic flows

Fanno Flow. Gas Dynamics

Richard Nakka's Experimental Rocketry Web Site

Transient Temperature Probe Measurements. in a Mach 4 Nitrogen Jet

The Interaction of a Supercritical Fluid Free-Jet Expansion With a Flat Surface

AerE 344: Undergraduate Aerodynamics and Propulsion Laboratory. Lab Instructions. Pressure Measurements in a de Laval Nozzle

Chapter 4 DYNAMICS OF FLUID FLOW


5 ENERGY EQUATION OF FLUID MOTION

Shock and Expansion Waves

The E80 Wind Tunnel Experiment the experience will blow you away. by Professor Duron Spring 2012

Mass of fluid leaving per unit time

Part A: 1 pts each, 10 pts total, no partial credit.

Analyses of Diamond - Shaped and Circular Arc Airfoils in Supersonic Wind Tunnel Airflows

DECAY OF SUPERSONIC RECTANGULAR JET ISSUING FROM A NOZZLE WITH DIAGONAL EXPANSION RAMPS

Brown Hills College of Engineering & Technology

4 Compressible Fluid Dynamics

Unified Quiz: Thermodynamics

Compressed Air Discharge from a Blowing Unit

c Dr. Md. Zahurul Haq (BUET) Thermodynamic Processes & Efficiency ME 6101 (2017) 2 / 25 T145 = Q + W cv + i h 2 = h (V2 1 V 2 2)

FLUID MECHANICS D203 SAE SOLUTIONS TUTORIAL 2 APPLICATIONS OF BERNOULLI SELF ASSESSMENT EXERCISE 1

Introduction to Aerospace Engineering

2 Internal Fluid Flow

Aerothermodynamics of high speed flows

Lecture 55 Compressible Flows (Contd.)

IMPACT OF FLOW QUALITY IN TRANSONIC CASCADE WIND TUNNELS: MEASUREMENTS IN AN HP TURBINE CASCADE

Numerical investigation on the effect of inlet conditions on the oblique shock system in a high-speed wind tunnel

Contents. Preface... xvii

Objectives. Conservation of mass principle: Mass Equation The Bernoulli equation Conservation of energy principle: Energy equation

The Computations of Jet Interaction on a Generic Supersonic Missile

Introduction to Aerodynamics. Dr. Guven Aerospace Engineer (P.hD)

Transcription:

Fundamentals of Gas Dynamics (NOC16 - ME05) Assignment - 8 : Solutions Manjul Sharma & Aswathy Nair K. Department of Aerospace Engineering IIT Madras April 5, 016 (Note : The solutions discussed below are just one of the ways of solving the problem. Your method is right as long as the final answers match!!) 1) Air at Mach number 1.8, static pressure of 0.8 bar and static temperature of 373 K passes through a normal shock wave. Determine its density after the shock. Answer : (p) ρ y = 1.76 kg/m 3 Given : M x = 1.8; = 0.8 bar; T x = 373 K To find : ρ y From Normal Shock Tables for γ = 1.4, corresponding to M x = 1.8, P y = 3.613 & T y T x = 1.53 P y =.8904 bar & T y = 571.436 K ρ y = P y RT y = 1.76 kg/m 3 ) A normal shock occurs in the diverging section of a C-D nozzle. The throat area is one-third of the exit area and the static pressure at the exit is 0.4 times the stagnation pressure at the entry. The flow is throughout isentropic except across the shock. Determine the area of cross-section of the nozzle (in terms of throat area) where the normal shock occurs. Answer : (t).84 times the throat area Given : = 3; P e = 0.4P 0i To find : 1

Since the flow is isentropic everywhere except at the shock, = ; = ; A 1 = = ; A y = = = 3 = A A But, P = 0.4 = P 0.4 A 1 = A 1 = = A A A = 1 A = 3 P = 3 0.4 = 1. From Isentropic tables, corresponding to P = 1., M = 0.47 From Normal Shock tables, for = 0.466, & 0.4 = 0.859 P = 0.859 = 0.4 0.859 = 0.466 M x =.58

From Isentropic tables, for M x =.58, =.84 =.84 3) A C-D nozzle is supplied air kept in a reservoir at pressure 500 kpa. The throat area is 8 cm and exit area is 30 cm. A normal shock stands at a section where the area is 10 cm. Assuming flow to be isentropic everywhere except at the shock, find the static pressure at the exit. Answer : (g) P e = 48 kpa Given : P 0 = 500 kpa; = 8 cm ; A s = 10 cm ; = 30 cm To find : P e = = A 1 = 8 cm Assuming shock is a very thin region, A s = = A y = 10 cm = 10 8 = 1.5 From Isentropic tables, for = 1.5, M x = 1.6 Since flow is isentropic, P 0 = = = 500 kpa From Isentropic Tables, for M x = 1.6, From Normal Shocks tables, for M x = 1.6, = 0.35 = 117.5 kpa M y = 0.668 P y =.80 P y = 331.35 kpa = 0.895 = 447.5 kpa = A y A y = 11.98 cm = A y = 11.98 cm = 30 11.98.505 3

From Isentropic tables, for =.505, M e = 0.33 & P e P 0e = 0.956 P e 48 kpa 4) Find the entropy change across the normal shock for an incoming flow of air with Mach number.5. Answer : (c) s = 137. J/kg K Given : M x =.5 To find : s From Normal Shocks Tables, corresponding to M x =.5, T y T x =.138 & P y = 7.15 s = C P ln ( Ty T x ) Rln ( Py ) s = 137. J/kgK 5) A pitot-static probe is used for measurement in a supersonic flow in a wind tunnel. If the readings of the probe are 600 kpa and 40 kpa, determine the static pressure of the supersonic flow in the wind tunnel. Answer : (k) = 19.3 kpa Given : = 600 kpa; P y = 40 kpa To find : Py = 0.7 From Isentropic tables, corresponding to P y = 0.7, M y = 0.73 From Normal Shocks Tables, corresponding to M y = 0.73, M x = 1.4 & = 3.1 = 19.3 kpa 6) Air from a reservoir at 0 and 500 kpa flows through a duct and forms a normal shock downstream of a throat of area 10 cm. By an odd coincidence it is found that the stagnation pressure downstream of this 4

shock exactly equals to the throat pressure. What is the area where shock stands? Answer : (e) A s = 4.7 cm Given : T 0 = 93 K; P 0 = 500 kpa; = 10 cm ; = P t To find : A s = = A 1 = 10 cm Since flow is isentropic everywhere except at the shock, = ; = ; A 1 = = ; A y = Assuming shock is a very thin region, A s = = A y From Isentropic tables, corresponding to M t = 1, P t = 0.58 P t = 64 kpa = = P t = 0.58 From Normal Shock tables, corresponding to = 0.58, M x =.4 From Isentropic tables, for M x =.4, =.448 =.448 =.448 4.7 cm 7) A C-D nozzle, discharging a jet of air into the atmosphere (1.0135 bar, 300 K), has a ratio of exit area to throat area equal to.5. What should be the reservoir pressure to drive this nozzle if a normal shock stands at an area ratio (area where shock stands to the throat area) of in the divergent section? Answer : (z) P 0 = 161 kpa Given : = 1.0135 bar; T 0 = 300 K; To find : =.5; A s =.0 5

Since flow is isentropic everywhere except at the shock, = ; = ; A 1 = = ; A y = A s = = From Isentropic tables, corresponding to =, M x =. From Normal Shocks tables, for M x =., M y = 0.547 & = 6.716 = 6.716 = 15.087 kpa From Isentropic tables, for M x =., = 0.0935 = 0.0935 161 kpa 8) A large tank with compressed air is attached to a C-D nozzle at pressure 4 bar and temperature of 35. The nozzle throat area is 3 cm and the exit area is 9 cm. A shock occurs at a location where the cross section area is 6 cm. Calculate the back pressure and temperature of the flow. Answer : (m) P b =.34 bar & T b = 300 K Given : = 4 bar; T 01 = 308 K; = 3 cm ; = 9 cm ; A s = 6 cm To find : P b, T b = = A 1 = 3 cm Since flow is isentropic everywhere except at the shock, = ; = ; A 1 = = ; A y = Assuming shock is a very thin region, A s = = A y = 6 cm A s = = 6 3 = From Isentropic tables, corresponding to =, M x =. 6

From Normal Shocks tables, for M x =., M y = 0.547 & = 0.68 = 0.68 =.51 bar Also, = A y A y = 4.777 cm = 9 4.777 1.884 From Isentropic tables, corresponding to = 1.884, M = 0.374 ; P = 0.985 ; T T 0 = 0.9785 P.34 bar & T 300 K 9) For the previous problem find the critical values of back pressure P cr1 and P cr3 respectively as defined in the class. Answer : (w) 3.97 bar,1.67 bar Given : = 4 bar; T 01 = 308 K; = 3 cm ; = 9 cm ; A s = 6 cm To find : P cr1, P cr3 = = A 1 = 3 cm = = 9 3 = 3 From Isentropic tables, corresponding to = 3, M,cr1 = 0.1975 & M,cr3 =.64 And, P,cr1,cr1 = 0.9735 & P,cr3,cr3 = 0.0471 P,cr1 3.9 bar & P,cr3 1.67 bar 7