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Three notes on propulsion and braking of tubeflight vehicles
Sequence 77
-2- the only steady-flow solution of the nonlinear differential equations governing the flow downstream of the vehicle is one…
Sequence 78
-3- h ~'( s ou1d -- the flow in the tube will be nonsteady. Since the pressure drag at subsonic and moderate…
Sequence 79
-4- conservation equations relating flow conditions immediately upstream and immediately downstream of a tubeflight vehicle…
Sequence 80
-5- at fixed distances behind the flame approach each other as time progresses, although it is not clear that their…
Sequence 81
-6- (Ref. 15), and of realistic assumptions concerning the internal ducting losses. The calculated performance is presented…
Sequence 82
-7- VEHICLES, TUBES, AND OPERATING CONDITIONS CONSIDERED IN THE ANALYSIS All vehicles considered in the present analysis have…
Sequence 83
-8- (a) it would restrict the freedom of transverse motion of the vehicle that the support and suspension mechanisms are…
Sequence 84
-9- Boundary layer suction is provided at appropriate locations on the surface of the vehicle for three main purposes: (a)…
Sequence 85
DRAG ANALYSIS 1. Drag of the body -- Unchoked flow. Fig. 1 identifies the main regions and dimensions of the analytical…
Sequence 86
-11- where C 1: is the nondimensional fric tion fac tor, defined as the frictional force per unit wetted area, divided by…
Sequence 87
-12- The boundary layer removal has the same effect on the transfer flow as an area expansion and, if it is carried out in…
Sequence 88
-13- Eq. (9) also yields p:z. = P, e Therefore, the buoyancy drag is ;2.. = TT d v 4- P, The ratio between frictional…
Sequence 89
-14- simplification, the body drag equations reduce to ::t Fa, .oG5 Pi M, Lv for dt 15 ft Fb .05~ P' M,l. Lv for dt…
Sequence 90
-15- computed in a later section. An accurate prediction of the parasite drag of the support system can- not be made at this…
Sequence 91
-16- signals generated by the flow inducer in the rear. Under these conditions, pumping of the transfer flow must take place…
Sequence 92
-17- F Ve'J ( '-d;l.. Trd V 4 f- C p (21) For the conditions selected in this analysis, = (22) The…
Sequence 93
-18- in the transfer passage, Fv > Fy , and the power required increases e~ with speed at a faster rate, along curve b-c…
Sequence 94
-19- shown that full recovery of the curtain momentum is possible with two- dimensional peripheral-jet pads in supercritica1…
Sequence 95
-20- At the highest speeds, the drag due to lift becomes a very small fraction of the total drag. When the flow is choked, it…
Sequence 96
-21- been made here with regard to the allocation of frictional forces and to the magnitude of certain parasite drag…
Sequence 97
-22- power demands of the tubeflight scheme exceed, at very low speeds, those of more conventional modes. Figs. 3, 4, and 5…
Sequence 98
-23- REFERENCES 1. Foa, J.V., "Propulsion of a vehicle in a tube," Rensselaer Polytechnic Institute, Rept. TR AE…
Sequence 99
-24- 13. Skinner, J.H., "Plane-flame simulation of the wake behind an internally propelled vehicle -- Part 2 --…
Sequence 100
- ----fN\ - - \::.J - - - - ----8 > ..J
Sequence 101
shock line Fig. 2
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