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

26.12.2012 Views

4.1.1 Flight Profiles Hopper flight profiles were entered into in the MATLAB model in terms of varying vertical and horizontal thrust. As discussed in section 3.1.3, the vertical thrust requirements throughout a hop of the desired dimensions were fairly well defined. Because the hopper would constantly lose mass during a hop as it expended nitrogen propellant, the vertical thrust levels for each phase of the hop were defined in terms of T/W, with a new vehicle weight calculated at each timestep of the solution based on previous gas usage. It was assumed that all four vertical thrusters would fire together to provide the total vertical thrust needed from the CGSE. There was more variation possible in defining the horizontal thrust for the transit phase of the hop. For all flight profiles, it was assumed that horizontal thrusters would fire in pairs, to accelerate or decelerate the hopper in the direction parallel to its Z axis (see Figure 3-2), with no steering or other rotation. However, the hopper could have short periods of acceleration and deceleration with a longer cruise at relatively low constant velocity, or longer periods of acceleration and deceleration resulting in a shorter cruise at higher velocity. In the limit, the hopper would accelerate horizontally for the entire first half of the transit phase and then decelerate over the second half, with no constant-velocity cruise in between. Several different horizontal acceleration profiles were modeled in order to judge their effect on CGSE design requirements. It should be noted that throughout all phases of the hop, attitude control was known to be necessary but not modeled. Possible sources of disturbances were identified to include gusts of wind (though it was planned to operate the TALARIS hopper indoors if possible to mitigate this), misalignments in the CGSE (i.e. a thruster mounted at a slight angle to its primary direction of force), and torques or lateral forces caused by the EDF weight relief propulsion system. The magnitude of these disturbances was not known at the time the model was written, so it was not possible to make an accurate estimate of the total amount of impulse necessary for attitude control, but it was assumed that it would be much smaller than the impulse required to perform the major planned vehicle maneuvers. Therefore, flight profiles were only considered feasible if the model indicated there was surplus gas available in the tanks at the end of a hop. It was assumed that this additional margin would be used for attitude control during a real hop. 48

4.1.2 Rocket Propulsion Equations Like all forms of rocket propulsion, a cold gas thruster produces thrust by converting the internal energy of a gas to kinetic energy in an exhaust flow by means of thermodynamic expansion in a nozzle [28]. As propellant mass is ejected from the thruster at high speeds in the exhaust flow, thrust is produced in the opposite direction to ensure conservation of momentum for the system. Thrust is also produced by any difference between the exhaust pressure and the ambient pressure. In equation form:

4.1.1 Flight Pr<strong>of</strong>iles<br />

Hopper flight pr<strong>of</strong>iles were entered into in <strong>the</strong> MATLAB model in terms <strong>of</strong> varying vertical and horizontal<br />

thrust. As discussed in section 3.1.3, <strong>the</strong> vertical thrust requirements throughout a hop <strong>of</strong> <strong>the</strong> desired<br />

dimensions were fairly well defined. Because <strong>the</strong> hopper would constantly lose mass during a hop as it<br />

expended nitrogen propellant, <strong>the</strong> vertical thrust levels <strong>for</strong> each phase <strong>of</strong> <strong>the</strong> hop were defined in terms<br />

<strong>of</strong> T/W, with a new vehicle weight calculated at each timestep <strong>of</strong> <strong>the</strong> solution based on previous gas<br />

usage. It was assumed that all four vertical thrusters would fire toge<strong>the</strong>r to provide <strong>the</strong> total vertical<br />

thrust needed from <strong>the</strong> CGSE.<br />

There was more variation possible in defining <strong>the</strong> horizontal thrust <strong>for</strong> <strong>the</strong> transit phase <strong>of</strong> <strong>the</strong> hop. For<br />

all flight pr<strong>of</strong>iles, it was assumed that horizontal thrusters would fire in pairs, to accelerate or decelerate<br />

<strong>the</strong> hopper in <strong>the</strong> direction parallel to its Z axis (see Figure 3-2), with no steering or o<strong>the</strong>r rotation.<br />

However, <strong>the</strong> hopper could have short periods <strong>of</strong> acceleration and deceleration with a longer cruise at<br />

relatively low constant velocity, or longer periods <strong>of</strong> acceleration and deceleration resulting in a shorter<br />

cruise at higher velocity. In <strong>the</strong> limit, <strong>the</strong> hopper would accelerate horizontally <strong>for</strong> <strong>the</strong> entire first half <strong>of</strong><br />

<strong>the</strong> transit phase and <strong>the</strong>n decelerate over <strong>the</strong> second half, with no constant-velocity cruise in between.<br />

Several different horizontal acceleration pr<strong>of</strong>iles were modeled in order to judge <strong>the</strong>ir effect on CGSE<br />

design requirements.<br />

It should be noted that throughout all phases <strong>of</strong> <strong>the</strong> hop, attitude control was known to be necessary<br />

but not modeled. Possible sources <strong>of</strong> disturbances were identified to include gusts <strong>of</strong> wind (though it<br />

was planned to operate <strong>the</strong> TALARIS hopper indoors if possible to mitigate this), misalignments in <strong>the</strong><br />

CGSE (i.e. a thruster mounted at a slight angle to its primary direction <strong>of</strong> <strong>for</strong>ce), and torques or lateral<br />

<strong>for</strong>ces caused by <strong>the</strong> EDF weight relief propulsion system. The magnitude <strong>of</strong> <strong>the</strong>se disturbances was not<br />

known at <strong>the</strong> time <strong>the</strong> model was written, so it was not possible to make an accurate estimate <strong>of</strong> <strong>the</strong><br />

total amount <strong>of</strong> impulse necessary <strong>for</strong> attitude control, but it was assumed that it would be much<br />

smaller than <strong>the</strong> impulse required to per<strong>for</strong>m <strong>the</strong> major planned vehicle maneuvers. There<strong>for</strong>e, flight<br />

pr<strong>of</strong>iles were only considered feasible if <strong>the</strong> model indicated <strong>the</strong>re was surplus gas available in <strong>the</strong> tanks<br />

at <strong>the</strong> end <strong>of</strong> a hop. It was assumed that this additional margin would be used <strong>for</strong> attitude control during<br />

a real hop.<br />

48

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!