Impact pressure

In compressible fluid dynamics, impact pressure (dynamic pressure) is the difference between total pressure (also known as pitot pressure or stagnation pressure) and static pressure.[1][2] In aerodynamics notation, this quantity is denoted as q c {\displaystyle q_{c}} or Q c {\displaystyle Q_{c}} .

When input to an airspeed indicator, impact pressure is used to provide a calibrated airspeed reading. An air data computer with inputs of pitot and static pressures is able to provide a Mach number and, if static temperature is known, true airspeed.[citation needed]

Some authors in the field of compressible flows use the term dynamic pressure or compressible dynamic pressure instead of impact pressure.[3][4]

Isentropic flow

In isentropic flow the ratio of total pressure to static pressure is given by:[3]

P t P = ( 1 + γ 1 2 M 2 ) γ γ 1 {\displaystyle {\frac {P_{t}}{P}}=\left(1+{\frac {\gamma -1}{2}}M^{2}\right)^{\tfrac {\gamma }{\gamma -1}}}

where:

P t {\displaystyle P_{t}} is total pressure

P {\displaystyle P} is static pressure

γ {\displaystyle \gamma \;} is the ratio of specific heats

M {\displaystyle M\;} is the freestream Mach number


Taking γ {\displaystyle \gamma \;} to be 1.4, and since P t = P + q c {\displaystyle \;P_{t}=P+q_{c}}


q c = P [ ( 1 + 0.2 M 2 ) 7 2 1 ] {\displaystyle \;q_{c}=P\left[\left(1+0.2M^{2}\right)^{\tfrac {7}{2}}-1\right]}


Expressing the incompressible dynamic pressure as 1 2 γ P M 2 {\displaystyle \;{\tfrac {1}{2}}\gamma PM^{2}} and expanding by the binomial series gives:


q c = q ( 1 + M 2 4 + M 4 40 + M 6 1600 . . . ) {\displaystyle \;q_{c}=q\left(1+{\frac {M^{2}}{4}}+{\frac {M^{4}}{40}}+{\frac {M^{6}}{1600}}...\right)\;}

where:

q {\displaystyle \;q} is dynamic pressure

See also

  • Dynamic pressure
  • Pitot-static system
  • Pressure
  • Static pressure

References

  1. ^ "Definition of impact pressure". answers.com. Archived from the original on 2008-08-29. Retrieved 2008-10-01.
  2. ^ The Free Dictionary Retrieved on 2008-10-01
  3. ^ a b L. J. Clancy (1975) Aerodynamics, Section 3.12 and 3.13
  4. ^ "the dynamic pressure is equal to half rho vee squared only in incompressible flow."
    Houghton, E.L. and Carpenter, P.W. (1993), Aerodynamics for Engineering Students, Section 2.3.1