Launching a Rocket

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The launch of a spacecraft is fundamental to all space activity. As a rocket flies it loses mass, because most of its mass is fuel (pure hydrogen and oxygen) that provides the propulsive force.
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Contributed by: Frederick Wu (October 2008)
Open content licensed under CC BY-NC-SA
Snapshots
Details
Graphic, top right: Tsiolkovsky's rocket equation, which defines the relationship between exhaust velocity and mass ratio
Graphic, bottom right: rocket dynamic parameters of acceleration, velocity, altitude and burn-out time
Graphic, left: 3D rocket dynamic launch model with altitude function control
Snapshot 1: ideal rocket specification that surpasses first escape velocity
Snapshot 2: ideal rocket specification that surpasses second escape velocity
Snapshot 3: 3D Earth scale model, with the launch site (yellow) and rocket altitude (red)
simplified assumptions:
1. gravity and aerodynamic drag effects are neglected
2. single stage rocket, initial velocity is zero
3. vertical launch or pitch angle is 90°
4. a constant exhaust velocity
5. a constant mass flow rate
governing equations:
1. Tsiolkovsky's rocket equation or rocket velocity:
2. mass flow rate:
3. maximum flight time or fuel burn‐out time:
4. rocket altitude:
5. rocket acceleration: , from
and above governing equations 1 and 2
symbols:
is the rocket velocity.
is the efficient exhaust velocity, constrained within a range 2500-4500
, using today's liquid‐fueled rocket chemical technology.
is the initial rocket mass.
is the current or final rocket mass;
decreases during flight until all the liquid fuel is burned out.
is the final rocket mass, usually regarded as payload.
is the mass ratio,
, which is usually in the range from 3 to 8; 14 is difficult to achieve.
is the mass flow rate, which depends on rocket engine design and specification; it indicates the rate at which the mass of the rocket is decreasing. Also called "specific impulse".
is the rocket flight time,
, which is the fuel burn-out time or the maximum flight time.
is the rocket acceleration. It is difficult for the human body to withstand high acceleration; 15-20 G is the maximum tolerance limit. (1 G is the acceleration due to gravity.)
References:
J. Peraire, "Variable Mass Systems: The Rocket Equation," MIT OpenCourseWare, 2004.
M. J. L. Turner, "Newton's Third Law and the Rocket Equation," Rocket and Spacecraft Propulsion, 2nd ed., New York: Springer, 2005 pp. 14–17.
M. J. L. Turner, "Launch Vehicle Dynamics," Rocket and Spacecraft Propulsion, 2nd ed., New York: Springer, 2005 pp. 115–144.
M. Voshell, "High Acceleration and the Human Body," 2004.
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