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The Complete Book of Spaceflight: From Apollo 1 to Zero Gravity

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nuclear reac<strong>to</strong>r, <strong>to</strong> reach speeds <strong>of</strong> about 95 km/s (20<br />

astronomical units per year), enabling it <strong>to</strong> travel 1,000<br />

AU (0.016 light-years) within a 50-year mission time. Its<br />

primary science objective would be <strong>to</strong> measure directly<br />

the distance <strong>to</strong> stars throughout our galaxy using stellar<br />

parallax. Secondary science goals would include particles<br />

and fields measurements, a search for the heliopause, a<br />

search for the Oort Cloud (a postulated ring <strong>of</strong> ice-rock<br />

bodies, which, when perturbed by the passage <strong>of</strong> nearby<br />

stars, may fall in<strong>to</strong> the inner solar system <strong>to</strong> become<br />

comets), tests <strong>of</strong> gravitational effects based on changes <strong>to</strong><br />

the spacecraft’s trajec<strong>to</strong>ry (which could be caused by a<br />

tenth planet or other dark companions in the solar system),<br />

and tests <strong>of</strong> relativity. TAU would be equipped with<br />

a 10-W laser communications system capable <strong>of</strong> transmitting<br />

20 kilobits/s from interstellar space.<br />

three-axis stabilization<br />

A type <strong>of</strong> stabilization in which a spacecraft maintains a<br />

fixed attitude relative <strong>to</strong> its orbital track. This is achieved<br />

by nudging the spacecraft back and forth within a deadband<br />

<strong>of</strong> allowed attitude error, using small thrusters or<br />

reaction wheels. With a three-axis stabilized spacecraft,<br />

solar panels can be kept facing the Sun and a directional<br />

antenna can be kept pointed at Earth without having <strong>to</strong><br />

be de-spun. On the other hand, rotation maneuvers may<br />

be needed <strong>to</strong> best utilize fields and particle instruments.<br />

Three-Corner Constellation<br />

A constellation <strong>of</strong> three nanosatellites due <strong>to</strong> be<br />

launched from the Space Shuttle in 2003. <strong>The</strong> mission is<br />

Data for Various Thor-Based Launch Vehicles<br />

Thor ICBM Thor-Able Thor-Able Star Thor-Agena D<br />

Length (m) 22.0 26.9 29.0 31.0<br />

Diameter (m) 2.4 2.4 2.4 2.4<br />

Mass (kg)<br />

Thrust (N)<br />

49,300 51,600 53,000 56,500<br />

Stage 1 670,000 670,000 761,000 759,000<br />

Stage 2 — 33,700 35,100 71,200<br />

Stage 3<br />

Propellants<br />

— 12,300 — —<br />

Stage 1 RP-1/LOX RP-1/LOX RP-1/LOX RP-1/LOX<br />

Stage 2 — IRFNA/UDMH IRFNA/UDMH IRFNA/UDMH<br />

Stage 3<br />

Payload (kg)<br />

— solid — —<br />

LEO — 140 450 1,200<br />

thrust 435<br />

sponsored by the Air Force Research Labora<strong>to</strong>ry, DARPA<br />

(Defense Advanced Research Projects Agency), and<br />

NASA, and supported by design teams at Arizona State<br />

University, the University <strong>of</strong> Colorado, and New Mexico<br />

State University. Among its goals are <strong>to</strong> experiment with<br />

stereo-imaging <strong>of</strong> the atmosphere and <strong>to</strong> test formationflying<br />

techniques. <strong>The</strong> satellites will each have a mass <strong>of</strong><br />

about 15 kg and be placed in<strong>to</strong> a 380-km-high orbit<br />

inclined at 51°.<br />

throat<br />

In rocket and jet engines, the most constricted section <strong>of</strong><br />

an exhaust nozzle.<br />

throatable<br />

A nozzle whose size and pr<strong>of</strong>ile can be varied. A throatable<br />

nozzle can be especially useful in a solid-fuel rocket<br />

mo<strong>to</strong>r <strong>to</strong> maintain uniform thrust throughout the burn<br />

time <strong>of</strong> the fuel.<br />

thrust<br />

<strong>The</strong> forward force generated by a rocket. Thrust is produced<br />

by the expulsion <strong>of</strong> a reaction mass, such as the<br />

hot gas products <strong>of</strong> a chemical reaction.<br />

In an optimum situation (see below), thrust equals the<br />

product <strong>of</strong> the mass expelled from the rocket in unit time<br />

(the propellant mass flow rate) and the exhaust velocity<br />

(the average actual velocity <strong>of</strong> the exhaust gases). If F is the<br />

thrust, mp the propellant flow rate, and ve the effective<br />

velocity, then<br />

F = m pv e<br />

(1)

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