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

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

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436 thrust chamber<br />

At first glance, it might seem that a constant thrust would<br />

lead <strong>to</strong> a constant acceleration, but this not the case.<br />

Even when the propellant flow rate and exhaust velocity<br />

are constant, so that the thrust is constant, a rocket will<br />

accelerate at an increasing rate because the rocket’s overall<br />

mass decreases as propellant is used up. <strong>The</strong> <strong>to</strong>tal<br />

change in velocity <strong>of</strong> a rocket due <strong>to</strong> a specific thrust, acting<br />

in a straight line, is given by an important formula<br />

known as the rocket equation. In some situations, as <strong>of</strong> a<br />

rocket rising from Earth’s surface, a large thrust acting<br />

over a relatively short period is essential. But in other situations,<br />

as <strong>of</strong> a probe on a deep space mission, the key<br />

fac<strong>to</strong>r is not so much the amount <strong>of</strong> thrust, which determines<br />

only the acceleration, but the final velocity. A high<br />

final velocity can be achieved by a propulsion system<br />

that produces a low thrust but expels material over long<br />

periods at a high velocity—for example, an ion engine.<br />

Equation (1) holds true only when the pressure <strong>of</strong> the<br />

outgoing exhaust exactly equals the ambient (outside)<br />

pressure. If this is not the case, then an extra term comes<br />

in<strong>to</strong> play, and the thrust is given by:<br />

F = m pv e + ( p e − pa )A e<br />

(2)<br />

where pe is the exhaust pressure, pa the ambient pressure,<br />

and Ae the area <strong>of</strong> the exit <strong>of</strong> the rocket nozzle. <strong>The</strong> first<br />

term in this equation is called the momentum thrust and<br />

the second the pressure thrust.<br />

thrust chamber<br />

<strong>The</strong> heart <strong>of</strong> all liquid propellant rocket engines. In its<br />

simplest form, the thrust chamber accepts propellant<br />

from the injec<strong>to</strong>r, burns it in the combustion chamber,<br />

accelerates the gaseous combustion products, and ejects<br />

them from the chamber <strong>to</strong> provide thrust.<br />

thrust commit<br />

<strong>The</strong> time, when all engines <strong>of</strong> a launch vehicle on the<br />

launch pad have been running for a designated period <strong>of</strong><br />

time (typically about three seconds) and all other parameters<br />

are normal, that is the start <strong>of</strong> the final launch<br />

sequence.<br />

thrust decay<br />

<strong>The</strong> progressive decline <strong>of</strong> propulsive thrust, over some<br />

fraction <strong>of</strong> a second, after a rocket mo<strong>to</strong>r burns out or is<br />

cut <strong>of</strong>f.<br />

thrust equalizer<br />

A safety device that prevents motion <strong>of</strong> a spacecraft if its<br />

solid-fuel rocket mo<strong>to</strong>r ignites accidentally. <strong>The</strong> device is<br />

usually a vent at the <strong>to</strong>p <strong>of</strong> the thrust chamber that is left<br />

open until launch time. If the fuel ignites accidentally<br />

before launch, the gases <strong>of</strong> combustion will blow out<br />

from both the <strong>to</strong>p and bot<strong>to</strong>m <strong>of</strong> the mo<strong>to</strong>r, thus equal-<br />

izing thrust on both sides and preventing the spacecraft<br />

from launching prematurely.<br />

thrust genera<strong>to</strong>r<br />

A device that produces motive power. In an electric<br />

propulsion system, for example, it is composed <strong>of</strong> an<br />

electric power source and a device that expels a high<br />

velocity flow <strong>of</strong> the propellant.<br />

thrust misalignment<br />

Thrust directed accidentally in an undesired direction.<br />

Thrust misalignment can have serious consequences,<br />

especially during the initial stages <strong>of</strong> a spacecraft’s ascent<br />

in<strong>to</strong> orbit.<br />

thrust vec<strong>to</strong>r control<br />

Controlling the flight <strong>of</strong> a launch vehicle or spacecraft by<br />

controlling the direction <strong>of</strong> thrust.<br />

thruster<br />

A small rocket used by a spacecraft <strong>to</strong> control or change<br />

its attitude.<br />

thrust-<strong>to</strong>-Earth-weight ratio<br />

A quantity used <strong>to</strong> evaluate engine performance,<br />

obtained by dividing the thrust developed by the vehicle<br />

by the engine dry weight.<br />

tidal force<br />

A force that comes about because <strong>of</strong> the differences in<br />

gravitational pull on an object due <strong>to</strong> a large mass around<br />

which the object is moving. In the case <strong>of</strong> a space station<br />

in Earth orbit, parts <strong>of</strong> the station that are further away<br />

from the Earth are pulled less strongly, so that the centrifugal<br />

force <strong>of</strong> the orbit is not quite balanced by gravity,<br />

and there is a net upward tidal force. Similarly, for<br />

parts closer <strong>to</strong> the Earth, there is a downward tidal force.<br />

<strong>The</strong>se opposing forces try <strong>to</strong> stretch the station along a<br />

line that passes through Earth’s center. One effect is that<br />

tidal forces will make any elongated object tend <strong>to</strong>ward<br />

an orbit with its long axis pointing <strong>to</strong> the Earth’s center.<br />

Either the space station has <strong>to</strong> be designed <strong>to</strong> orbit in this<br />

way, or it must have an orientation correction system <strong>to</strong><br />

counter the orientation drift that the tidal forces will produce.<br />

Another effect will be on objects within a space<br />

station. Tidal forces are one <strong>of</strong> the reasons it is impossible<br />

<strong>to</strong> have perfectly zero-gravity conditions in orbit.<br />

<strong>The</strong> fact that microgravity always exists has important<br />

consequences for some experiments and manufacturing<br />

processes in space.<br />

Dangerous tidal effects would be most evident near<br />

highly condensed objects, such as black holes. Tidal forces<br />

are proportional <strong>to</strong> d/R 3 , where d is the density <strong>of</strong> the

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