Non Isentropic Flow 1

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  NON-ISENTROPIC FLOW  

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non isentropic

Transcript of Non Isentropic Flow 1

  • NON-ISENTROPIC FLOW

  • 2

    MENU

    1. Non-Isentropic flow : Real flow 2. Shockwave & Expansion waves Normal shockwave Oblique shockwave Prandtl Meyer expansion

    3. Duct Flow with Friction without Heat Transfer (Fanno flow)

    4. Duct Flow with Heat Transfer and Negligible Friction Force (Reyleigh Flow)

  • 3

    Non-Isentropic flow : Real flow

    What is Non-Isentropic Flow ?

    1. Irreversible ( there is viscous effect) only 2. Non Adiabatic ( There is heat transfer) only 3. Combination of Both

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    Non-Isentropic flow : Real flow

    What is Non-Isentropic Flow ?

    2 1 = ln0201

    ln0201

    1. Irreversible ( there is viscous effect) only 01 02 and 01 = 02

    2. Non Adiabatic ( There is heat transfer) only 01 02 and 01 = 02

    3. Combination of Both 01 02 and 01 02

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    Isentropic flow

    Flow through Convergent Divergent Duct

    (1) 0= 1 ,

    0= 1 ,

    0= 1

    Flow conditions

    Is there an flow through the duct?

    How is about the following flow through the duct?

    (2) 0= 1 ,

    0= 0.9725,

    0= 0.7 5

    (3) 0= 0.95 ,

    0= 0.85,

    0= 0.528

    (4) 0= 0.95 ,

    0= 0.1278,

    0= 0.528

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    Isentropic flow

    Flow through Convergent Divergent Duct

    Mach number and Mass flow rate

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    Non-Isentropic flow

    Flow through Convergent Divergent Duct

    Normal shock wave

    If the pressure at exit , pe is less than p3 and greater than pd so the normal shock wave will appear inside the divergent duct

    The shock wave occurs in supersonic speed

    The Mach number change from supersonic to subsonic

    The flow properties change abruptly

    pc

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    Non-Isentropic flow

    Normal Shock Normal shockwave : shock waves that

    occur in a plane / cross section normal to the direction of flow

    A supersonic flow across a normal shock wave becomes subsonic

    Total enthalpy remains constant across the shock (conservation energy principle)

    01 = 02 = 1 + 1

    2

    2= 2 +

    22

    2

    Continuity equation

    = 11 = 22

    Momentum equation

    1 2 =

    (2 1)

    Entropy

    2 1 > 0

    01 = 02

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    Non-Isentropic flow

    Prandtl Relation

    Flow relation between before shock wave and after shock wave

    2 =

    1

    1

    1 2

    5.0

    2

    *

    )1(2

    1

    MMM

    where

    22 =

    2 + ( 1)12

    2 12 ( 1)

    ()2 = 12

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    Non-Isentropic flow

    Prandtl Relation

    Flow relation between before shock wave and after shock wave

    1 2

    22 =

    2 + ( 1)12

    2 12 ( 1)

    What is happen if M1

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    Non-Isentropic flow

    Prandtl Relation

    Flow relation between before shock wave and after shock wave

    2

    1

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    Non-Isentropic flow

    Static Properties Relation

    Properties relation between before shock wave and after shock wave

    Pressure

    21

    =2 1

    2 ( 1)

    ( + 1)

    Density

    21

    =12

    =( + 1)1

    2

    2 + ( 1) 12

    Temperature

    21

    = 2 1

    2 1 [2 + 1 12]

    ( + 1)2 12

    What is happen if M1

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    Non-Isentropic flow

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    Non-Isentropic flow

    Entropy

    2 1

    = ln0102

    0201

    =21

    2 ( 1)

    ( + 1)

    1/(1)( + 1)1

    2

    2 + ( 1) 12

    /(1)

    2 1

    =1

    ( 1)

    2 12

    ( + 1) 1

    + 1+

    ( 1)

    2 + ( 1) 12

    ( + 1)12

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    Non-Isentropic flow

    Entropy

    1

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    Non-Isentropic flow

    Air Speed Measurement in Supersonic flight

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    Non-Isentropic flow

    1. A blunt nose missile is flying at Mach 2 at standard sea level. Calculate the temperature and pressure at the nose of the missile

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    Non-Isentropic flow

    Air Speed Measurement in Supersonic flight

    Pressure ratio

    1

    )1(2

    124

    1 211

    2

    1

    2

    1

    2

    1

    02

    M

    M

    M

    p

    p

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    Non-Isentropic flow

    2. Air with initial stagnation conditions of 700 kPa and 530 K passes through a frictionless CD nozzle Th troat area is 5 cm2 and the exit area is 12.5 cm2. The back pressure is 350 kPa, and a normal shock wave occurs within the diverging section. determine

    (a) The Mach number at the exit (b) The change in stagnation pressure (c) Mach number before and after the shock (d) the nozzle area at the point of shock (e) The back pressure if the flow were isentropic throughout

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    Non-Isentropic flow

    QUIZ 3 Air with initial stagnation conditions of 700 kPa and 330 K passes

    through a CD nozzle at the rate of 1 kg/s. At the exit are of the nozzle the stagnation pressure is 550 kPa and the stream pressure is 550 kPa. The nozzle is insulated and there is no irreversibility except for the occurrence of a shock

    (a) What is the nozzle throat area ? (b) What is Mach number before and after the shock ? (c) What is the nozzle area at the point of shock and at the exit (d) What is the stream density at the exit (e) The back pressure if the flow were isentropic throughout

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    Non-Isentropic flow

    Rankine-Hugoniot Relations

    Combining continuity equation and momentum equation

    2 1 = 112 22

    2 = 112(1

    12)

    21

    =

    + 1 1

    12

    1

    + 1 1

    12

    21

    =

    + 1 1

    21

    1

    + 1 1

    21

  • Non-Isentropic flow

    Duct Flow with Heat Transfer (Reyleigh Flow)

    Combining continuity, momentum and energy equations

    21 00TCqTC pp

    Is the following isentropic gas law still valid ?

    u1 u2

    p1, r1 p2, r2

    Fire

    q

    With Heat Addition

  • Non-Isentropic flow

    Static Properties relations

    2

    2

    2

    1

    1

    2

    1

    1

    M

    M

    p

    p

    Pressure Temperature

    2

    1

    2

    2

    2

    2

    2

    1

    1

    2

    1

    1

    M

    M

    M

    M

    T

    T

    Density

    2

    2

    1

    2

    1

    2

    2

    1

    2

    1

    1

    M

    M

    M

    M

    r

    r

    Total Properties relations

    1

    2

    12

    1

    2

    22

    1

    2

    2

    2

    1

    10

    20

    1

    1

    1

    1

    M

    M

    M

    M

    p

    p

    Total Pressure Total Temperature

    2

    12

    1

    2

    22

    12

    1

    2

    2

    2

    2

    2

    1

    10

    20

    1

    1

    1

    1

    M

    M

    M

    M

    M

    M

    T

    T

  • Non-Isentropic flow

    Critical Static Properties relations

    Pressure Temperature Density

    Critical Total Properties relations

    Total Pressure Total Temperature

    2* 1

    1

    Mp

    p

    2

    2

    2

    * 1

    1

    MM

    T

    T

    r

    r

    1

    112

    2*

    M

    M

    1

    1

    )1(2

    1

    12

    2*

    0

    0

    M

    Mp

    p

    2

    22

    2

    *

    0

    0 121

    1M

    M

    M

    T

    T

  • Non-Isentropic flow

    Graph of Total Temperature at Various Mach number

    Adding heat will increase flow velocity or Mach number in Subsonic flow and decrease flow velocity of Mach number in Supersonic flow

    Extracting heat (cooling of the flow) will decrease flow velocity or Mach number in Subsonic flow and increase flow velocity of Mach number in

    Supersonic flow

    0.0

    1.0

    2.0

    3.0

    0.0 0.5 1.0 1.5

    T0/T0*

    Mach

    2

    22

    2

    *

    0

    0 121

    1M

    M

    M

    T

    T

    Supersonic

    Subsonic

  • Non-Isentropic flow

    Graph of Total Pressure at Various Mach number

    Supersonic

    Subsonic

    1

    1

    )1(2

    1

    12

    2*

    0

    0

    M

    Mp

    p

    0

    1

    2

    3

    0 1 2 3 4 5 6

    p0/p0*

    Ma

    ch

  • Non-Isentropic flow

    Graph of Static Pressure at Various Mach number

    0.0

    1.0

    2.0

    3.0

    0.0 0.5 1.0 1.5 2.0 2.5 3.0

    p/p*

    Ma

    ch

    2* 1

    1

    Mp

    p

    For subsonic flow (M1), adding heat will increases pressure

    Supersonic

    Subsonic

  • Non-Isentropic flow

    Graph of Density at Various Mach number

    Supersonic

    Subsonic

    r

    r

    1

    112

    2*

    M

    M

    0.0

    1.0

    2.0

    3.0

    0.0 2.0 4.0 6.0 8.0 10.0 12.0

    r /r *

    Mach

  • Non-Isentropic flow

    Graph of Static Temperature at Various Mach number

    2

    2

    2

    * 1

    1

    MM

    T

    T

    0.0

    1.0

    2.0

    3.0

    0.0 0.5 1.0 1.5

    T/T*

    Mach

    0.0

    1.0

    2.0

    3.0

    0.0 0.5 1.0 1.5

    T/T*

    Mach

    Supersonic

    Subsonic

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    Non-Isentropic flow

    Rankine-Hugoniot Relations

    Combining continuity equation and momentum equation

    1 2 + 12 =1

    2 (1 2)(

    1

    2+

    1

    1)

    1 2 + 12 =1

    2 (1 2)(2 + 1)

    1 2 + 12 =1

    2 (1 + 2)(

    1

    1

    1

    2)

    1 2 + 12 =1

    2 (1 + 2)(1 2)