Behavior of Isentropic Flow in Quasi-1D

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  • 8/13/2019 Behavior of Isentropic Flow in Quasi-1D

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    Behavior of Isentropic Flow in Quasi-1D

    Recall cons. of mass:.constuA=

    Consider a perturbation in the area

    0

    ...

    ))()((

    =++

    ++++=

    +++=

    udAAduuAd

    TOHudAAduuAduA

    dAAduuduA

    Or

    (1)

    Similar manipulations to x-momentum gives:

    (2)

    Also, since the flow is assumed isentropic, we can use the definition of the speedof sound to relate d and dp :

    =

    = .

    2

    consts

    pa

    AA

    uu

    pp

    L

    L

    L

    L

    =

    =

    =

    =

    Lx

    Rx

    dAAA

    duuu

    dppp

    d

    LR

    LR

    LR

    LR

    +=

    +=

    +=

    +=

    0=+ ududp

    dadp2=

    0=++A

    dA

    u

    dud

    Since we have assumed .consts= in the flow (3)

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    Behavior of Isentropic Flow in Quasi-1D

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    We are interested in how the flow properties change when the area changes. So,we use (2) and (3) to eliminate terms from (1). For example, lets determine how

    u changes with A :

    0)1(

    0

    0

    0

    2

    2

    2

    =+

    =++

    =++

    =++

    A

    dA

    u

    duM

    A

    dA

    u

    du

    a

    udu

    A

    dA

    u

    du

    a

    dp

    A

    dA

    u

    dud

    When 1u

    duwhen 0M : 0> u

    du

    when 0>A

    dA

    u increases when A increases!

    0M ? Clearly, u must behave the opposite of A

    regardless of the Mach number. So, what must be happening is that changes

    more rapidly than A for 1>M and, thus u behaves opposite of what we expect

    from subsonic flow behavior. Lets check this:

    A

    dA

    Mu

    dp

    A

    dA

    Mu

    du

    22

    2

    1

    1

    1

    1

    =

    =

    A

    dA

    Mu

    du21

    1

    =

    A

    dA

    Mu

    dp22 1

    1

    =

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    Behavior of Isentropic Flow in Quasi-1D

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    A

    dA

    Mu

    da22

    2

    1

    1

    =

    These results show that, regardless of whether 1>M or 1 ,:1 pM when A

    ,p when A

    Which are the opposite of how u behaves. It is also useful to consider the

    magnitudes of the different changes:

    A

    dA

    M

    Md2

    2

    1

    =

    ,p when A

    ,p when A

    A

    dA

    Mu

    dp22 1

    1

    =

    A

    dA

    M

    Md2

    2

    1=

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    Behavior of Isentropic Flow in Quasi-1D

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    0=++A

    dA

    u

    dud

    Flow low ,M changes are small compared to u changes. But for ,1>M

    changes more rapidly.

    Also, of interest is that ,,dpd and du become extremely large as 1M .

    In fact, this requires that 1=M must occur at a minimum in the area where

    0=dA .

    Lets consider a converging-diverging duct:

    Whenbachp is only a little less than 0p , the flow will be subsonic:

    As bachp is lowered from op , we will eventually hit the bachp at which 1=M at

    the throat.

    What happens if bachp is lowered further?

    There is one other isentropic flow through this geometry which occurs when

    bachp is very low. In this situation, the flow will become supersonic in the divergent

    section:

    0p bachp

    M

    1

    0

    decreasing

    bachp

    01

    1

    1 22

    2

    =+

    A

    dA

    A

    dA

    MA

    dA

    M

    M

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    Behavior of Isentropic Flow in Quasi-1D

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    M

    1

    0

    Supersonicisentropic flow(very low

    bachp )

    Subsonicisentropic flows