Development of a Cold Gas Propulsion System for the ... - SSL - MIT
Development of a Cold Gas Propulsion System for the ... - SSL - MIT Development of a Cold Gas Propulsion System for the ... - SSL - MIT
• Neither the Joule-Thomson effect nor any other method was used to model temperature drop across the thruster solenoid valves. • The flow coefficient
The flight profile begins with maximum vertical thrust of approximately 120 N, or about 30 N produced by each of four vertical thrusters, as was calculated in section 3.1.3. This period of upward acceleration lasts for about 1.4 s, after which the vertical CGSE thrust drops to a much lower level with less than 30 N produced by the four vertical thrusters together. During this second half of the ascent, the hopper is still moving upwards due to its vertical momentum, but the total T/W is less than 1 even with the 5/6 weight relief provided by the EDFs. This causes the vertical rise of the hopper to decelerate until it reaches its operational altitude of 2 m with zero velocity approximately 2.8 s into the flight. After the ascent, the horizontal transit phase of the hop begins. Throughout this phase, the CGSE vertical thrusters and EDFs together maintain a constant T/W of 1, but because the mass of the vehicle continually decreases as propellant is expended, the thrust level can be seen to decrease with time in the plot. Meanwhile, the horizontal thrusters fire to translate the hopper. In this particular flight profile, the hopper is first given a constant horizontal acceleration of 1.33 m/s 2 for 4 s. This acceleration is provided by two of the four horizontal thrusters; as with the vertical thrusters, they must decrease their thrust over the firing period in order to maintain constant acceleration as the hopper loses mass. At about 6.8 s into the flight, the horizontal thrusters shut off, and the constant-velocity cruise begins. At this point, the hopper has translated 10.67 m from its starting point, and it has a horizontal velocity of 5.33 m/s. The hopper cruises for 1.625 s, in which time it covers 8.66 m of additional horizontal distance (assuming drag is negligible). At the end of the horizontal transit phase, the hopper again fires a pair of horizontal thrusters for 4 s. However, this time it fires the pair opposite to the pair that initially fired, so the hopper decelerates horizontally. (Note that Figure 4-3 plots thrust magnitude, not direction.) The horizontal transit phase ends about 12.4 s into the flight, with the hopper again hovering at 2 m altitude with zero velocity, but now located 30 m from its starting point. The final phase of the flight profile is the descent. It is essentially the mirror image of the ascent, with the vertical thrust first decreasing so that the hopper begins to drop but then increasing again to decelerate the hopper’s fall so that it lands with zero velocity. As illustrated in Figure 4-3, the total flight time for this profile is just over 15 s. The MATLAB model tracked the remaining nitrogen propellant mass as well as its thermodynamic state throughout this hop, and it also computed the component
- Page 14 and 15: Figure 6-6. Identification of thrus
- Page 17 and 18: Notation Acronyms and Abbreviations
- Page 19 and 20: N newton Pa pascal psi pounds per s
- Page 21 and 22: 1 Introduction The TALARIS (Terrest
- Page 23 and 24: the idea of hopping was born, and i
- Page 25 and 26: However, as stated before, this doe
- Page 27 and 28: Figure 2-3. Diagram of ACAT lander
- Page 29 and 30: An alternate approach to resolving
- Page 31 and 32: accurate conditions for testing GNC
- Page 33 and 34: Ballistic hops tend to use less pro
- Page 35 and 36: 2.3.2 Comparison of Cold Gas and Mo
- Page 37 and 38: Handling propellant There are sever
- Page 39 and 40: and if the cold gas system was foun
- Page 41 and 42: 3 TALARIS CGSE Design Framework Aft
- Page 43 and 44: Figure 3-1. Scaling of TALARIS terr
- Page 45 and 46: (3) Providing attitude control Ther
- Page 47 and 48: Figure 3-2 also shows the body coor
- Page 49 and 50: 4 Modeling and Flow Control Compone
- Page 51 and 52: 4.1.2 Rocket Propulsion Equations L
- Page 53 and 54: variables in equation (4-8) deal wi
- Page 55 and 56: equations. Equation (4-10) was then
- Page 57 and 58: that of helium (0.227 MPa = 32.9 ps
- Page 59 and 60: thruster solenoid valve, and chambe
- Page 61 and 62: where
- Page 63: discussed later in section 6.3.4, t
- Page 67 and 68: hop, any given valve or regulator o
- Page 69 and 70: esponse time was an important perfo
- Page 71 and 72: directly opens and closes the main
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- Page 75 and 76: 5 Single-Stream Component Testing A
- Page 77 and 78: the solenoid valve, and a pressure
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- Page 81 and 82: Figure 5-5. CGSE high side as const
- Page 83 and 84: Figure 5-7 illustrates several aspe
- Page 85 and 86: 6 Full Eight-Thruster Flight System
- Page 87 and 88: Figure 6-2. TALARIS CGSE assembled
- Page 89 and 90: stream tests revealed that changes
- Page 91 and 92: Figure 6-5. Original CGSE control c
- Page 93 and 94: other constraints. This was difficu
- Page 95 and 96: variables (such as number of thrust
- Page 97 and 98: One solution to this problem would
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- Page 101 and 102: or more thrusters were firing toget
- Page 103 and 104: Table 6-3. Valve timing metrics dur
- Page 105 and 106: Figure 6-11. Redesigned CGSE contro
- Page 107 and 108: The imaginary simplified thruster c
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- Page 111 and 112: Figure 7-3. GNC data from 3-DOF tes
- Page 113 and 114: Tests on this vertical stand demons
The flight pr<strong>of</strong>ile begins with maximum vertical thrust <strong>of</strong> approximately 120 N, or about 30 N produced<br />
by each <strong>of</strong> four vertical thrusters, as was calculated in section 3.1.3. This period <strong>of</strong> upward acceleration<br />
lasts <strong>for</strong> about 1.4 s, after which <strong>the</strong> vertical CGSE thrust drops to a much lower level with less than 30 N<br />
produced by <strong>the</strong> four vertical thrusters toge<strong>the</strong>r. During this second half <strong>of</strong> <strong>the</strong> ascent, <strong>the</strong> hopper is still<br />
moving upwards due to its vertical momentum, but <strong>the</strong> total T/W is less than 1 even with <strong>the</strong> 5/6<br />
weight relief provided by <strong>the</strong> EDFs. This causes <strong>the</strong> vertical rise <strong>of</strong> <strong>the</strong> hopper to decelerate until it<br />
reaches its operational altitude <strong>of</strong> 2 m with zero velocity approximately 2.8 s into <strong>the</strong> flight.<br />
After <strong>the</strong> ascent, <strong>the</strong> horizontal transit phase <strong>of</strong> <strong>the</strong> hop begins. Throughout this phase, <strong>the</strong> CGSE<br />
vertical thrusters and EDFs toge<strong>the</strong>r maintain a constant T/W <strong>of</strong> 1, but because <strong>the</strong> mass <strong>of</strong> <strong>the</strong> vehicle<br />
continually decreases as propellant is expended, <strong>the</strong> thrust level can be seen to decrease with time in<br />
<strong>the</strong> plot. Meanwhile, <strong>the</strong> horizontal thrusters fire to translate <strong>the</strong> hopper. In this particular flight pr<strong>of</strong>ile,<br />
<strong>the</strong> hopper is first given a constant horizontal acceleration <strong>of</strong> 1.33 m/s 2 <strong>for</strong> 4 s. This acceleration is<br />
provided by two <strong>of</strong> <strong>the</strong> four horizontal thrusters; as with <strong>the</strong> vertical thrusters, <strong>the</strong>y must decrease <strong>the</strong>ir<br />
thrust over <strong>the</strong> firing period in order to maintain constant acceleration as <strong>the</strong> hopper loses mass.<br />
At about 6.8 s into <strong>the</strong> flight, <strong>the</strong> horizontal thrusters shut <strong>of</strong>f, and <strong>the</strong> constant-velocity cruise begins.<br />
At this point, <strong>the</strong> hopper has translated 10.67 m from its starting point, and it has a horizontal velocity <strong>of</strong><br />
5.33 m/s. The hopper cruises <strong>for</strong> 1.625 s, in which time it covers 8.66 m <strong>of</strong> additional horizontal distance<br />
(assuming drag is negligible).<br />
At <strong>the</strong> end <strong>of</strong> <strong>the</strong> horizontal transit phase, <strong>the</strong> hopper again fires a pair <strong>of</strong> horizontal thrusters <strong>for</strong> 4 s.<br />
However, this time it fires <strong>the</strong> pair opposite to <strong>the</strong> pair that initially fired, so <strong>the</strong> hopper decelerates<br />
horizontally. (Note that Figure 4-3 plots thrust magnitude, not direction.) The horizontal transit phase<br />
ends about 12.4 s into <strong>the</strong> flight, with <strong>the</strong> hopper again hovering at 2 m altitude with zero velocity, but<br />
now located 30 m from its starting point.<br />
The final phase <strong>of</strong> <strong>the</strong> flight pr<strong>of</strong>ile is <strong>the</strong> descent. It is essentially <strong>the</strong> mirror image <strong>of</strong> <strong>the</strong> ascent, with<br />
<strong>the</strong> vertical thrust first decreasing so that <strong>the</strong> hopper begins to drop but <strong>the</strong>n increasing again to<br />
decelerate <strong>the</strong> hopper’s fall so that it lands with zero velocity. As illustrated in Figure 4-3, <strong>the</strong> total flight<br />
time <strong>for</strong> this pr<strong>of</strong>ile is just over 15 s.<br />
The MATLAB model tracked <strong>the</strong> remaining nitrogen propellant mass as well as its <strong>the</strong>rmodynamic state<br />
throughout this hop, and it also computed <strong>the</strong> component