Compressible Flow credits Logo credits
Potto Home Contact Us

Potto Home

About Potto

Chapters:

  Content
  Introduction
  Sound
  Isentropic
  Shock
  Gravity
  Isothermal
  Fanno
  Rayleigh
  Tank
  Piston
  Oblique
  Prandtl-Meyer
  Hard copy
  Gas Dynamics Tables

Other things:
Other resources
Download Area
calculators

Other Resources

  FAQs
  Compare Other Books
  Articles

Potto Statistics

License

Feedback

next up previous index
Next: Application of Oblique Shock Up: Detached Shock Previous: Issues Related to the   Index

Oblique Shock Examples


\begin{examl}
Air flows at Mach number ($M_1$) or $M_x= 4$ is approaching a wed...
... the weak, the strong
Mach numbers, and the respective shock angles.
\end{examl}
Solution

The find maximum wedge angle for ($ M_x= 4$ ) $ D$ has to be equal to zero. The wedge angle that satisfies this requirement by equation (13.28) is the solution (a side to the case proximity of $ \delta = 0$ ). The maximum values are:
$ \rule[-0.1in]{0.pt}{0.3 in}\mathbf{M_x} $ $ \mathbf{M_y} $ $ \mathbf{\delta_{max}} $ $ \mathbf{\theta_{max}} $
4.0000 0.97234 38.7738 66.0407
<>


To obtain the results of the weak and the strong solutions, utilize either equation (13.28) or the Potto-GDC, which yields the following results:

$ \rule[-0.1in]{0.pt}{0.3 in}\mathbf{M_x} $ $ \mathbf{{M_y}_s} $ $ \mathbf{{M_y}_w} $ $ \mathbf{\theta_s} $ $ \mathbf{\theta_w} $ $ \mathbf{\delta } $
4.0000 0.48523 2.5686 1.4635 0.56660 0.34907
<>


Figure: Oblique shock occurs around a cone. This photo is courtesy of Dr. Grigory Toker, a Research Professor at Cuernavaco University of Mexico. According to his measurement, the cone half angle is $ 15^\circ$ and the Mach number is 2.2.
Image sharpNose

\begin{examl}
A cone shown in Figure \eqref{oblique:fig:sharpNose} is exposed
to...
...s the photo taken
based on the assumption that the cone is a wedge.
\end{examl}
Solution

The measurement shows that cone angle is $ 14.43^\circ$ and shock angle is $ 30.099^\circ$ . With given two angle the solution can be obtained utilizing equation (13.59) or the Potto-GDC.

$ \rule[-0.1in]{0.pt}{0.3 in} \mathbf{M_1} $ $ \mathbf{{M_y}_s} $ $ \mathbf{{M_y}_w} $ $ \mathbf{\theta_s} $ $ \mathbf{\theta_w} $ $ \mathbf{\delta } $ $ \mathbf{{P_0}_y \over {P_0}_x } $
3.2318 0.56543 2.4522 71.0143 30.0990 14.4300 0.88737
<>


Because the flow is around Cone it must be a weak shock. Even if the cone was a wedge, the shock will be weak because the maximum (transition to a strong shock) occurs at about $ 60^{\circ}$ . Note that Mach number is larger than the predicted by the wedge.


Figure: $ \;$ Maximum values of the properties in an oblique shock
\begin{figure}\centerline{\includegraphics
{calculations/figures/obliqueMax}}
\end{figure}

Figure: Two variations of inlet suction for supersonic flow.
\begin{figure}\centerline{\includegraphics
{cont/oblique/inletSuction}}
\end{figure}

next up previous index
Next: Application of Oblique Shock Up: Detached Shock Previous: Issues Related to the   Index
Created by:Genick Bar-Meir, Ph.D.
On: 2007-11-21


If you want the whole book or parts in pdf or other formats, then click here. You also can get the best and the largest gas dynamics tables in the world.

About Potto Project

Potto Project has been created by Dr. Genick Bar-Meir and friends to build free software and textbooks for college students.

Potto Project is under open content licenses, which means that you will always have the freedom to use it, make copies of it, and improve it. You are encouraged to make use of these freedoms and share the textbooks and program with your family and friends!