Mass ratio

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In aerospace engineering, mass ratio is a measure of the proportion of a rocket that is propellant. It is the ratio of the rocket's wet mass (vehicle plus contents plus propellant) to its dry mass (vehicle plus contents).

The definition arises naturally from the Tsiolkovsky rocket equation:

\Delta v = v_e \ln \frac {m_0} {m_1}

where

  • Δv is the desired change in the rocket's velocity
  • ve is the effective exhaust velocity (see specific impulse)
  • m0 is the initial mass (rocket plus contents plus propellant)
  • m1 is the final mass (rocket plus contents)

This equation can be rewritten in the following equivalent form:

\frac {m_0} {m_1} = e ^ { \Delta v / v_e }

The fraction on the left-hand side of this equation is the rocket's mass ratio by definition.

This equation indicates that a Δv of n times the exhaust velocity requires a mass ratio of en. For instance, for a vehicle to achieve a Δv of 2.5 times its exhaust velocity would require a mass ratio of e2.5 (approximately 12.2). One could say that a "velocity ratio" of n requires a mass ratio of en.

The mass ratio is a useful quantity for back-of-the-envelope rocketry calculations: it is an easy number to derive from either Δv numbers or from rocket and propellant mass numbers, and therefore serves as a handy bridge between the two. It is also a useful number to give an impression of the size of a rocket: while two rockets with mass fractions of, say, 92% and 95% may appear similar, the corresponding mass ratios of 12.5 and 20 clearly indicate that the two systems are very different.

Typical multistage rockets have mass ratios in the range from 8 to 20. The Space Shuttle, for example, has a mass ratio around 16.

[edit] References

Zubrin, Robert (1999). Entering Space: Creating a Spacefaring Civilization. Tarcher/Putnam. ISBN 0-87477-975-8.

[edit] See also