Page 70 - Intro to Space Sciences Spacecraft Applications
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Propulsion
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                      forces will be opposite the direction of motion, such as atmospheric drag,
                      but  some may  have positive  components in  the  direction of  intended
                      motion as can happen with solar pressure. Another external force, due to
                      a  difference between  the  propellant exhaust pressure  and  the  external
                      ambient pressure, may also exist as we will soon see.
                        The remaining term represents the change in momentum of  the exhaust
                      gases. This exchange of momentum is the main contributor to the accelera-
                      tion of the rocket and this last quantity is known as the thrust term (T). Note
                      that the (vector) quantity Vo - 5 would be negative since the exhaust gasses
                      are ejected opposite the direction of the original velocity. Rewritten as B - V,,,
                      this quantity describes the velocity of the exhaust gasses relative to the rock-
                      et itself. We can define this term as the exhaust velocity %.
                        With the definition of terms given above, equation 3- 1 can be rewritten as:

                           dij   -
                        m-    = F,,, + ?;                                         (3 - 3)
                           dt
                      which, in this simple form, is known as the rocket equation.

                      Rocket Thrust

                        Looking more closely at the results of  the last section, it can be seen
                      that the thrust term of the rocket equation is proportional  to both the pro-
                      pellant exhaust velocity (f - To = V,,)  and the mass flow rate of propel-
                      lant  (dddt = m). We  can  rewrite the thrust term to better  show this
                      dependency:




                        To increase the thrust of a rocket then, one could try to increase either
                      the exhaust velocity of the propellant or the mass flow rate of propellant
                      through the rocket. To see how these quantities can be changed we must
                      consider the characteristics of a typical rocket system such as that shown
                      in Figure 3-2.

                      Mass Flow Rate. A rocket differs from a jet engine in that a rocket must
                      carry its own oxidizer as well as fuel supply, although there are some sys-
                      tems which simply use a single (mono) propellant. In many propulsion
                      systems, liquid propellants are used and are delivered to the combustion
                      chamber by mechanical pumps as depicted in the figure. The pumps con-
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