Difference between revisions of "Forest UCM Ch3 Rockets"
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where <math>m_0</math> is the initial Rocket mass | where <math>m_0</math> is the initial Rocket mass | ||
| + | |||
| + | ==In terms of Thrust== | ||
| + | |||
| + | Defining | ||
| + | :<math>\mbox{THRUST} = - \dot{m} u</math> | ||
| + | |||
| + | Then | ||
| + | |||
| + | :<math>m dot{v} =</math> THRUST = Force on rocket as a result of expelling fuel | ||
[[Forest_UCM_MnAM#Rockets]] | [[Forest_UCM_MnAM#Rockets]] | ||
Revision as of 13:38, 13 September 2014
Consider a rocket of mass moving at a speed ejecting rocket fuel for propulsion.
File:Forest UCM Ch3 Rockets Fig.xfig.txt
mass of Fuel + Rocket
mass of Fuel ejected over time interval ( = mass lost by rocket < 0)
velocity of Fuel relative to the Rocket
velocity of rocket relative to the ground before ejecting fuel of mass
velocity of the rocket relative to the ground after ejecting fuel
Velocity of the fuel with respect to the ground
Apply Conservation of Momentum
The velocity of the fuel with respect to the ground may be written as the vector sum of the rocket's velocity with respect to the ground and the velocity of the fuel with respect to the rocket :Galilean transormation
assuming 1-D motion and using the velocity variables defined above
substituting
solving for the velocity
where is the initial Rocket mass
In terms of Thrust
Defining
Then
- THRUST = Force on rocket as a result of expelling fuel