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: The Limitations of the Up: Normal Shock Previous: Prandtl's Condition   Index

Operating Equations and Analysis

In Figure (5.3), the Mach number after the shock, My, and the ratio of the total pressure, P0y/P0x, are plotted as a function of the entrance Mach number. The working equations were presented earlier. Note that the $ M_y$ has a minimum value which depends on the specific heat ratio. It can be noticed that the density ratio (velocity ratio) also has a finite value regardless of the upstream Mach number.

The typical situations in which these equations can be used also include the moving shocks. The equations should be used with the Mach number (upstream or downstream) for a given pressure ratio or density ratio (velocity ratio). This kind of equations requires examining Table (5.1) for $ k=1.4$ or utilizing Potto-GDC for for value of the specific heat ratio. Finding the Mach number for a pressure ratio of 8.30879 and k=1.32 and is only a few mouse clicks away from the following table.

This table was generated by Potto-GDC (in HTML)

Normal Shock Input: Py/Px k = 1.32
Mx My Ty/Tx ρy/ρx Py/Px P0y/P0x
2.7245 0.476422 2.111 3.93596 8.30879 0.381089
Figure: The ratios of the static properties of the two sides of the shock.
Image shockT-P
To illustrate the use of the above equations, an example is provided.
\begin{examl}
Air flows with a Mach number of
\begin{rawhtml}
<i>M<sub>x</sub>=...
...f the shock. Assume that
\begin{rawhtml}
<i>k=1.4</i>\end{rawhtml}.
\end{examl}
Solution

Analysis:
First, the known information Mx=3, Px=1.5[bar] and T=273 K. Using these data, the total pressure can be obtained (through an isentropic relationship Table (4.2), i.e. P0x is known). Also with the temperature, Tx the velocity can readily be calculated. The relationship that was calculated will be utilized to obtain the ratios for downstream of the normal shock.

$\displaystyle {P_x \over P_{0x} } = 0.0272237 \Longrightarrow
P_{0x} = 1.5/0.0272237 = 55.1 [bar]
$

$\displaystyle c_x = \sqrt{k R T_x} = \sqrt {1.4 \times 287 \times 273} = 331.2 m/sec
$

Normal Shock Input: Mx k = 1.4
Mx My Ty/Tx ρy/ρx Py/Px P0y/P0x
3 0.475191 2.67901 3.85714 10.3333 0.328344

$\displaystyle U_x = M_x \times c_x = 3\times 331.2 = 993.6 [m/sec]
$

Now the velocity downstream is determined by the inverse ratio of ρy = 993.6 / 3.85714 = 257.6 [m/sec].

Uy=993.6/3.85714=257.6[m/sec]

P0y = ( P0y / P0x ) * P0x = 0.32834 * 55.1 [bar] = 18.09 [bar]




Subsections
next up previous index
Next: The Limitations of the Up: Normal Shock Previous: Prandtl's Condition   Index
Created by:Genick Bar-Meir, Ph.D.
On: 2007-11-21