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Analysis of the effects of wall perforations on the performance of a vehicle in a tube
Sequence 30
21 appropriate relations for the drag disc are 2 i - Vd. 2.4 2.12 2.15 For the inflow region ahead of the actuator disc…
Sequence 31
22 or, in normalized form, 2.32 Equations 2.30, 2.31 and 2.32 are not all independent, hence one more equation is needed -…
Sequence 32
23 P-"A a.. .3 _ 2 1 ( XL - - - - - - 2~-i - (2u3 -i)e. - 4 sinh (-?-..'L) J( ~L J2 r: + ~2U.-t) e - (…
Sequence 33
24 where Thus the entire flow field is specified for the case of matched internal propulsion. The drag, and consequently the…
Sequence 34
25 Between the actuator and drag discs, (from 4 to 1) the pressure will increase causing outflow and a decrease in velocity.…
Sequence 35
. / 26 and integration from the drag disc (X = 0) forward yields sln (-?\.X + C.3) 2.41 where At X = L, U = U3 and eq. 2.…
Sequence 36
which is of course, equal to the thrust, P a - P 3 • The critical length is given by 2.45 Equations 2.12 and 2.15 still…
Sequence 37
which then permits specifying j3. Then from the definition of t/ and an assumed value of U d , P 1 - P a can be…
Sequence 38
therefore Pl also equals Pa which further requires that u1 = u 4 = u • This is possible under two conditions. One is the…
Sequence 39
30 pressure behind the actuator disc (the thrust) is equal to the drop in pressure to atmospheric behind the drag disc (the…
Sequence 40
31 3. EXPERIMENTAL APPARATUS AND PROCEDURE Experiments were conducted for two purposes: first, to deter- mine the…
Sequence 41
connected to one side of a U-tube water manometer, give the pressure difference across the tube wall directly. 32 The rotary…
Sequence 42
33 consecutively, to 1/4, 7/16 and S/S inches and the entire procedure repeated. 3.1.3. Data Reduction. The tube axial…
Sequence 43
34 was constructed for the purpose of extending the range of tests and for testing the drag disc in a porous tube. This…
Sequence 44
35 rates was obtained by adjusting the control valve and new readings were made. Discs of different porosities were then…
Sequence 45
36 4. DISCUSSION OF RESULTS Solutions to the equations of motion governing the flow field induced by a vehicle traveling…
Sequence 46
37 All of the data points for inflow appear to lie on the same straight line through the origin corresponding to a flow…
Sequence 47
38 The viscous flow solution is for a tube-wall fricition factor of C~= .01 and a 2.5 per cent wall porosity. All solutions…
Sequence 48
39 evident even for wall porosities as low as 1 or 2.5 per cent. The drag of the disc, given by eq. 2.17, is presented in…
Sequence 49
40 U d '2. .5 and of U = .5 for Uci <'.5 is maintained. The effect of viscosity is to bring the flow to rest…
Sequence 50
41 only about 20 tube radii with very good correlation between theory and experiment. A 1/4" aluminum disc with 1/4…
Sequence 51
presented in Fig. 20 show the same general trend as the experimental results shown in Fig. 21, which has been reproduced from…
Sequence 52
43 constant area, cylindrical fairing 14• An actuator disc operating in a finite length constant area fairing produces a low…
Sequence 53
blockage. Frictional drag on the vehicle is not included. Under conditions of level motion, the thrust on the vehicle must…
Sequence 54
per cent wall porosity but with a further decreased length of disturbed flow ahead of the drag disc. Behind the actuator disc…
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