IOWA STATE UNIVERSITY - Aerospace Engineering Notes

AER E 1600: Lecture 7 Overview

  • Presenter: Carolyn Riedel
  • Focus: Programming V - A Beginner's Guide to Rocket Math
  • Lecture Content:
    • Thrust Specific Fuel Consumption (TSFC)
    • Change in mass of the rocket
    • Force Due to Gravity
    • Forces on the Rocket
    • Acceleration of the rocket
    • Velocity of the rocket
    • Position of the rocket
    • Demonstration of the Programming Project

Thrust Specific Fuel Consumption (TSFC)

  • Definition: TSFC is a measure used to indicate rocket efficiency, specified as the rate of fuel consumption per unit thrust.
  • Key Points:
    • Important parameters in rocket propulsion include thrust and fuel efficiency.
    • TSFC is critical for understanding the efficiency of rocket engines.
    • Units: Common units for TSFC include kilograms per Newton per second in the Metric system or pounds per pound-force per hour in English units.

Change in Rocket Mass Over Time

  • Concept: As a rocket burns fuel, its total mass decreases.
  • Mathematical Representation: The change in mass over time can be expressed using the equation: dmdt=TSFCT\frac{dm}{dt} = -TSFC * T
    • Here,
      • TSFC is the thrust specific fuel consumption,
      • T is the thrust of the rocket.
  • Using Euler's Method: The change in mass can be reformulated as: δm=(TSFCT)δt\delta m = (-TSFC * T)\delta t
    • Mass of fuel at any instant in time is given by:
      m<em>fuel(t)=m</em>fuel(t0)+δmm<em>{fuel}(t) = m</em>{fuel}(t_0) + \delta m
    • Total mass at any point:
      m<em>rocket(t)=m</em>initial+mfuel(t)m<em>{rocket}(t) = m</em>{initial} + m_{fuel}(t)

Rocket Thrust and Thrust Direction

  • Understanding Thrust: Thrust is a vector and has both a magnitude (Force) and direction.
  • Equation for Thrust Direction: Tdirection=(cos(θ) sin(θ))T_{direction} = \begin{pmatrix} cos(\theta) \ sin(\theta) \end{pmatrix}
    • Direction is defined in terms of an angle ( \theta ) with reference to axes.

Rocket Global Position and Gravity

  • Gravity Force Calculation:
    • Gravitational force can be determined with:
      F<em>gravity=Gm</em>1m2r2F<em>{gravity} = \frac{G m</em>1 m_2}{r^2}
    • Here,
      • G is the gravitational constant,
      • m1 and m2 are the masses,
      • r is the distance between their centers.
  • Direction of Gravity: Represented as:
    Gdirection=positionvectorpositionvectorG_{direction} = - \frac{position\, vector}{|position\, vector|}

Forces on the Rocket

  • Total Forces Acting: The net force on the rocket is given by the combination of thrust and gravitational force:
    F<em>net=T</em>direction+GdirectionF<em>{net} = T</em>{direction} + G_{direction}
  • Newton’s Second Law: This relationship can be analyzed using:
    ΣF=ma\Sigma F = m a

Acceleration Over Time

  • Calculation of Acceleration:
    • Referring to previous equations, acceleration can be expressed as:
      a=ΣF<em>netm</em>rocketa = \frac{\Sigma F<em>{net}}{m</em>{rocket}}

Velocity Over Time

  • Velocity Relation to Acceleration: Velocity can be derived using the relationship from physics:
    a=dvdta = \frac{dv}{dt}
  • In Terms of Forces: Therefore, we have:
    a=ΣF<em>netm</em>rocketa = \frac{\Sigma F<em>{net}}{m</em>{rocket}}

Velocity Vector Change

  • Using Euler’s Method: The change in velocity vector is expressed as:
    δv=ΣF<em>netm</em>rocketδt\delta v = \frac{\Sigma F<em>{net}}{m</em>{rocket}} \delta t
  • Velocity Update: The new velocity vector at each timestep can therefore be expressed as:
    v<em>new=v</em>current+δvv<em>{new} = v</em>{current} + \delta v

Position Vector Update

  • Position Relation to Velocity: Position is related to the velocity by the equation:
    vel=dxdtvel = \frac{dx}{dt}
  • Updating Position with Euler’s Method: Changes to the position vector can be represented as: δposition=velδt\delta position = vel \delta t
    • Continuous position update would be:
      position<em>new=position</em>current+δpositionposition<em>{new} = position</em>{current} + \delta position

Programming Project Demonstration

  • A programming project demo will provide an example of the expected outcomes based on the discussed principles and equations.

References

  • Slides include images and credits (e.g., NASA's Saturn V rocket carrying humans to the moon).
  • Referenced materials from NASA/Kim Shiflett for relevant visual aids and further contexts.