Astrodynamics/Basic Rocketry

This section of the introduction will cover the basic ideas and theory of how rockets fly and leave the atmosphere as well as introduce the rocket equation.

The Ideal Rocket Equation

Rockets are momentum exchange devices the function by expelling some fluid (usually very hot gas or plasma) which "pushes" the rocket via Newtons third law of motion. Rockets are technically all around us ranging from simple water bottle rocket, to fireworks, to more sophisticated rockets like the Saturn V. The Tsiolkovsky Rocket Equation, derived below, is basic and fundamental principle of how rockets fly and shows the maximum change in velocity, ${\displaystyle \Delta V}$ (Delta V), that can be achieved by a rocket provided no external forces act on it.

${\displaystyle \Delta V=v_{e}\ln {\left({\frac {m_{0}}{m_{f}}}\right)}=I_{SP}g_{0}\ln {\left({\frac {m_{0}}{m_{f}}}\right)}}$

Where,

• ${\displaystyle v_{e}}$ is the effective exhaust velocity (out of the nozzle) equal to ${\displaystyle I_{SP}g_{0}}$.
• ${\displaystyle I_{SP}}$ is the specific impulse of measuring in seconds. It's a measure of solid rocket fuel efficiency specifically the impulse created per unit weight (on Earth) of propellant.
• ${\displaystyle g_{0}}$ is the standard gravity on Earth near ground level.
• ${\displaystyle m_{0}}$ is the mass of the rocket before firing it's engines. Commonly the initial total mass is used (wet mass).
• ${\displaystyle m_{f}}$ is the mass of the rocket after the engines stop burning. Commonly the final total mass is used (dry mass).

The Rocket Equation states that with a faster exhaust velocity the greater finally velocity of the rocket; however, due to the natural logarithm there is an exponential increase in the initial mass of the rocket. Therefore, it is not beneficial to increase the mass of rocket as it will have negligible return and instead the uses of stages (multiple rocket stacked on top of each other) is more beneficial. Further, it's important to state that it might be misleading thinking that more efficient rockets (higher ${\displaystyle I_{SP}}$) are better at launch, since the rocket may not lift of the ground if the thrust force propelling it up is too small. This is due to the fact that the equation functions with no external forces acting on it.

Picture a rocket or a mass in space of mass, ${\displaystyle m}$, traveling at a velocity, ${\displaystyle v}$. If we take a small lump of the mass, ${\displaystyle dm}$, and throw it, as a speed of ${\displaystyle v_{e}}$ relative to the rocket, opposite to the direction of the flight (anti-colinear with velocity). We can expect a small change in velocity, ${\displaystyle dv}$, of the mass in space. Since, there are no other forces acting on this the momentum of the mass before expelling of the smaller mass and the one after must be equal due to the conservation of momentum. Let ${\displaystyle P_{1}}$ and ${\displaystyle P_{2}}$ denote the linear momentum before and after respectively.

${\displaystyle P_{1}=mv}$
${\displaystyle P_{2}=(m-dm)(v+dv)+dm(v+dv-v_{e})}$

Note, that both moments are taken from a stationary observer not on either of the masses, hence why the dv is added to the small masses momentum. Setting these two equations equal to one another the equation becomes:

${\displaystyle mv=(m-dm)(v+dv)+dm(v+dv-v_{e})}$
${\displaystyle mv=mv-vdm+mdv-dmdv+vdm+dmdv-v_{e}dm}$

After cancellations,

${\displaystyle mdv=v_{e}dm}$

It would be unfair to not mention here that this equation can create two useful equations in itself, an ODE (first one shown below) of a 1D rocket dynamics, and the Tsiolkovsky equation (second one shown below). These equations are achieved by making the time between the two moments ${\displaystyle P_{1}}$ and ${\displaystyle P_{2}}$ smaller. In other words taking the limit as time approaches zero.

${\displaystyle m(t){\frac {dv}{dt}}={\dot {m}}v_{e}}$
${\displaystyle \Delta v=v_{f}-v_{0}=v_{e}\ln {\left({\frac {m_{0}}{m_{f}}}\right)}}$

Although the Rocket Equation has it's limitations it is a useful resources for explaining future topics such as transfers. However, to elaborate on reason why the efficiency might be misleading it's worth noticing that in the derivation we have found the ${\displaystyle F=ma}$ equation. Hence, the instantaneous thrust force on the rocket in 1D is shown below. As can be seen if the ISP is high and the rocket motor is efficient it will not mean much if the mass flow rate, ${\displaystyle {\dot {m}}}$, is low and the thrust cannot surpass gravity and aerodynamical drag.

${\displaystyle T=v_{e}{\dot {m}}=g_{0}I_{SP}{\dot {m}}}$

Rocket Staging

The rocket's propulsion system can only consist of one fuel tank and one engine, however, such a system cannot be used to get into earth's orbit, as for that we would need a very long fuel tank, which is impractical since it would lower the engine's thrust to weight ratio(Except for the hypothetical spaceplane single stage to orbit or SSTO designs like Skylon). Such a problem is solved by adding multiple stages, with each stage consisting of a propellant tank and an engine, along with a separation system(Sometimes along with other things like an electronic guidance system or parachutes). When the propellant of one stage runs out, that section is removed, thus reducing onboard dry mass. Staging can be used for reasons such as:

• Reducing onboard dry mass
• Using engines more fit to the situation(Certain engines are optimized for certain altitudes, so they can be put on different stages)

This makes staging an expensive, but effective method to go to earth's orbit and beyond. There are also efforts to make stages reusable to reduce the cost of using these rockets.