Stagnation Properties and Mach...

4
1 AE3450 Stag. Props. and Mach Number -1 School of Aerospace Engineering Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved. Stagnation Properties and Mach Number Rewrite stagnation properties in terms of Mach number for thermally and calorically perfect gases Stagnation Temperature from energy conservation : no work but flow work and adiabatic R T γ γ + = 2 v 2 1 2 o M 2 1 1 T T γ + = (VI.6) 1 2 o M 2 1 1 p p γ γ ÷ ø ö ç è æ γ + = (VI.7) RT T T o γ γ + = 2 v 2 1 1 2 v 1 2 p o c T T + = 2 2 v 2 1 1 a γ + = 1 o o T T p p γ γ ÷ ø ö ç è æ = from state eq. for isen. process ÞT o (and h o ) constant for adiabatic flow Stagnation Pressure from entropy conservation : reversible and adiabatic Þisentropic (s=0) Þp o (and s o ) constant if also reversible AE3450 Stag. Props. and Mach Number -2 School of Aerospace Engineering Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved. Compressible p o and Bernoulli Equation Incompressible flow, Bernoulli eqn. also gives a stagnation pressure (static + dynamic pressure) 2 v 2 1 ρ + = p p o ( ) ... 2 1 1 1 1 2 2 1 1 1 2 1 1 2 2 2 1 2 + ÷ ø ö ç è æ γ ÷ ø ö ç è æ γ γ γ γ + γ γ γ + = ÷ ø ö ç è æ γ + = γ γ M M M p p o ( ) ( ) ... x 2 1 n n nx 1 x 1 2 n + + + = + ... 4 v 2 1 v 2 1 2 2 2 + ρ + ρ + = M p p o higher terms negligible for small M (<0.3) Bernoulli ρ γ = p M 2 2 v use Expand compressible p o in Taylor series ... v 8 v 2 1 ... 2 2 2 1 2 2 2 2 2 2 + ρ + ρ + = + ÷ ÷ ø ö ç ç è æ γ + γ + = M p p M M p p o 0.3 2 /4=0.0225

Transcript of Stagnation Properties and Mach...

1

AE3450Stag. Props. and Mach Number -1

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Stagnation Properties and Mach Number• Rewrite stagnation properties in terms of Mach number for

thermally and calorically perfect gases• Stagnation Temperature

– from energy conservation:no work but flow workand adiabatic

RT

γ−γ+=

2v2

1

2o M2

11TT −γ+= (VI.6)

12o M2

11pp −γ

γ

��

���

� −γ+= (VI.7)

RTTTo

γ−γ+=

2v2

11

2v1 2

po c

TT +=

2

2v2

11a

−γ+=

1ooTT

pp −γ

γ

��

���

�=from state

eq. for isen. process

�To (and ho) constant foradiabatic flow

• Stagnation Pressure– from entropy conservation:

reversible and adiabatic����isentropic (∆∆∆∆s=0)

�po (and so) constant ifalso reversible

AE3450Stag. Props. and Mach Number -2

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Compressible po and Bernoulli Equation• Incompressible flow, Bernoulli eqn. also gives a stagnation

pressure (static + dynamic pressure) 2v21 ρ+= ppo

( ) ...2

111122

11

12

112

2212 +��

���

� −γ��

���

� −−γγ

−γγ+−γ

−γγ+=�

���

� −γ+=−γ

γ

MMMppo

( ) ( ) ...x2

1nnnx1x1 2n +−++=+

...4

v21v

21 2

22 +ρ+ρ+= Mppo

higher terms negligible for small M (<0.3)Bernoulli

ργ=

pM

22 v use

• Expand compressible po in Taylor series

...v8

v2

1...222

1 22222

2 +ρ+ρ+=+���

����

�γ+γ+= Mpp

MMppo

0.32/4=0.0225

2

AE3450Stag. Props. and Mach Number -3

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Stagnation Density and Tables• Stagnation Density

– from To, po andideal gas law (ρ=p/RT)

– ρρρρo constant for isentropic flow

11

oo

TT −γ

��

���

�=ρρ

11

2o M2

11−γ

��

���

� −γ+=ρρ (VI.8)

• Tables– To/T and po/p tabulated in text (John) as function of M

listed as Tt/T and pt/p (t for total T and total p) – γ=5/3 (Table A.3): atoms (Ar, He, …) at “not too high” T– γ =1.4 (Table A.1): diatomics (N2, O2, …) at “moderate” T– γ =1.3 (Table A.2): more atoms or higher T– make your own?

AE3450Stag. Props. and Mach Number -4

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Stagnation versus Static Properties• Static Properties

– represent the properties you would measure if you were moving with the flow (at the local flow velocity)

– always defined in the flow’s reference frame

still air

moving air

still air

• Stagnation Properties– always defined by conditions at a point– represent the (static) properties you’d

measure if you first brought the fluid at that point to a stop (isentropically) with respect to a chosen observer

– depends on observer’s reference frame

3

AE3450Stag. Props. and Mach Number -5

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Stagnation Properties: Example• Supersonic projectile (M=2) flying through still air • Static conditions: T∞=250 K, p∞=0.003 atm

shock

A B C D

streamline

M=2T∞=250Kp∞=0.003atm

• Find:1. To at A (ToA) relative to

observer on projectile 2. ToD (same observer) <, >, = ToA ?3. poB (same observer)4. poC (same observer) <, >, = poB ?

AE3450Stag. Props. and Mach Number -6

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Stagnation Properties: Example (con’t)

4

AE3450Stag. Props. and Mach Number -7

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Stagnation Properties: Example 2• Projectile flying through still air at 170 m/s• Static conditions: T∞=288 K, p∞=1 atm• Nose of projectile = point B• Find:

1. poA (relative to observeron projectile)

2. pB

3. TB

• Hint, use RTa γ=

Bstagnationstreamline 170 m/s

A

AE3450Stag. Props. and Mach Number -8

School of Aerospace Engineering

Copyright © 2001-2002 by Jerry M. Seitzman. All rights reserved.

Stagnation Properties: Example 2 (con’t)