Experiments have shown that the transition from laminar to turbulent conditions for flow normal to the axis of a long cylinder occurs at a critical Reynolds number of Re D , c ≈ 2 × 10 5 , where D is the cylinder diameter. Moreover, the transition from incompressible to compressible flow occurs at a critical Mach number of M a c ≈ 0.3. For air at a pressure of p = 1 atm and temperature T = 27 ° C, determine the critical cylinder diameter D c below which, if the flow is turbulent, compressibility effects are likely to be important.
Experiments have shown that the transition from laminar to turbulent conditions for flow normal to the axis of a long cylinder occurs at a critical Reynolds number of Re D , c ≈ 2 × 10 5 , where D is the cylinder diameter. Moreover, the transition from incompressible to compressible flow occurs at a critical Mach number of M a c ≈ 0.3. For air at a pressure of p = 1 atm and temperature T = 27 ° C, determine the critical cylinder diameter D c below which, if the flow is turbulent, compressibility effects are likely to be important.
Experiments have shown that the transition from laminar to turbulent conditions for flow normal to the axis of a long cylinder occurs at a critical Reynolds number of
Re
D
,
c
≈
2
×
10
5
,
where D is the cylinder diameter. Moreover, the transition from incompressible to compressible flow occurs at a critical Mach number of
M
a
c
≈
0.3.
For air at a pressure of
p
=
1
atm and temperature
T
=
27
°
C,
determine the critical cylinder diameter
D
c
below which, if the flow is turbulent, compressibility effects are likely to be important.
determine the Mach number, total pressure, and total
temperature after the heat interaction for the following gases:
a) y= 1.4 and cp 0.24 Btu/(lbm- °R)
b) y= 1.325 and cp = 0.28 Btu/(1bm · °R)
%3D
Consider a cone at zero angle of attack in a hypersonic flow. (Hypersonic flow is very high-speed flow, generally defined as any flow above a Mach number of 5.) The half-angle of the cone is θc, as shown inthe figure. An approximate expression for the pressure coefficient on the surface of ahypersonic body is given by the newtonian sine-squared law : Cp = 2 sin2 θcNote that Cp, hence, p, is constant along the inclined surface of the cone. Along the base of the body, we assume that p = p∞. Neglecting the effect of friction, obtain an expression for the drag coefficient of the cone, where CD is based on the area of the base Sb.
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