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Mechanics of Fluids

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550 Compressible flow <strong>of</strong> gases<br />

Fig. 11.32 Mach–Zehnder<br />

interferometer.<br />

each other, making the screen uniformly bright. The beam through the test<br />

section may be retarded by an increase <strong>of</strong> density there; if this is sufficient<br />

to put the beams out <strong>of</strong> phase by half a wavelength (or an odd multiple <strong>of</strong><br />

half a wavelength), so that the crests <strong>of</strong> waves in one beam coincide with<br />

troughs in the other, the screen is uniformly dark. Lines <strong>of</strong> maximum and<br />

minimum brightness therefore represent contours <strong>of</strong> constant density, and<br />

the density increment between successive contours corresponds to a phase<br />

shift <strong>of</strong> half a wavelength. Alternatively, the splitter plates P1 and P2 may be<br />

slightly rotated from the position that gives uniform brightness <strong>of</strong> the screen<br />

at no-flow conditions to one that gives a series <strong>of</strong> interference fringes parallel<br />

to the axes <strong>of</strong> rotation. Non-uniform density in the test section then causes<br />

local distortion <strong>of</strong> these otherwise equally spaced fringes, and measurement<br />

<strong>of</strong> the fringe displacement permits calculation <strong>of</strong> the density at that point<br />

relative to the density in an undisturbed part <strong>of</strong> the flow.<br />

The interferometer is costly and demands very high accuracy <strong>of</strong> the<br />

optical components and vibration-absorbing supports. It does, however,<br />

yield quantitative information about the density throughout the flow, and<br />

not just where the density changes rapidly.<br />

In association with a heated wire shedding a filament <strong>of</strong> warmer, less<br />

dense, gas these optical methods may also be used to indicate a filament line<br />

in gas flow otherwise at constant density.<br />

PROBLEMS<br />

(For air take γ = 1.4, R = 287 J · kg −1 · K −1 , cp = 1005 J · kg −1 · K −1 .<br />

All pressures quoted are absolute.)<br />

11.1 Atmospheric air at 101.3 kPa and 15 ◦ C is accelerated isentropically.<br />

What are its velocity and density when the Mach<br />

number becomes 1.0 and what is the maximum velocity theoretically<br />

obtainable? Why could this maximum not be achieved<br />

in practice?<br />

11.2 Air flows isentropically from atmosphere (pressure 101.5 kPa<br />

and temperature 15 ◦ C) to a 600 mm square duct where the<br />

Mach number is 1.6. Calculate the static pressure, the velocity

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