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Second Computational Aeroacoustics (CAA) Workshop on ...

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2. Find the pressure envelope inside the duct al<strong>on</strong>g the four radial lines r = 0, 0.34, 0.55,<br />

0.79. The pressure envelope, P(x), is given by<br />

P(x)= max p(r,¢,x,t).<br />

over time<br />

Give P(x) from x = -6 to x = 0 at Ax = 0.1.<br />

For both parts of the problem, c<strong>on</strong>sider <strong>on</strong>ly n = 0, m = 2 and the two cases<br />

(a) co = 7.2<br />

(b) = 10.3<br />

Note: #o2 = 7.0156. You are to solve the linearized Euler equati<strong>on</strong>s.<br />

Category 3 m Turbomachinery Noise<br />

The purpose of these problems is to study the computati<strong>on</strong>al requirements for modeling<br />

the aeroacoustic resp<strong>on</strong>se of typical rotor-stator interacti<strong>on</strong>s that generates t<strong>on</strong>al noise in<br />

turbomachinery. You may solve either the full Euler or Ilne_(zedEuier equati<strong>on</strong>s. Be sure<br />

to specify the grid size, the total CPU time required, the CPU t:[me per period, and the<br />

type of computer used for each problem.<br />

and<br />

. :=<br />

This problem ........ is designed to test the ability of a numerical scheme to model the acoustic<br />

resp<strong>on</strong>se ofacascade to an incident "frozen gust_,',_<br />

C<strong>on</strong>slaeT_h_-c_scaae of flat-plate airfoils Shown in figure41 The mean flow is uniform<br />

and axial wi{h inflow velocity Uoo and s{atiC density po_. The inflow Mach number M_:{S<br />

0.5. The length (chord) of each plate is c, and {he gap-ico-chord ratio g/c is i.0.<br />

: We will use n<strong>on</strong>-dimensi<strong>on</strong>al variables with U_ as velodty scale, c as length scale,<br />

c/U_ as time scale, poo as density scale and pooU_ as pressure scale.<br />

The incident:vortical gust, which is carried al<strong>on</strong>g by the mean flow; has z and y<br />

velocities givefi by ......<br />

. L<br />

: : : : :: : Z72 L ::<br />

v = cos( x + av (2)<br />

respectiveiy;::where vG = 0.01. C<strong>on</strong>sider two cases. For CaSe 1, the Wavenumber/3 is<br />

g_r[2 Corresp<strong>on</strong>d{ng:{o an "interblade phase angle!' a of 5rr/2. The frequency w (same<br />

as the reduced frequency based <strong>on</strong> chord, k)_is equal to 5rr/2 (_ 7'864). For Case 2,<br />

a = k = 13_r/2 (_ 20.42). The gust is c<strong>on</strong>vected by the mean flow. Therefore, the<br />

x-wavenumber _ for both cases is equal to co.:<br />

7;<br />

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