Calculation of small rocket trajectories using only rocket-to-launcher radial velocity data
Calculating small rocket trajectories using rocket to launcher radial velocity data
SEARCH · Search NASA
Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.
Quote a phrase for an exact phrase match. Source license links do not imply unrestricted reuse.
Calculating small rocket trajectories using rocket to launcher radial velocity data
Rocket trajectory determination by tracking onboard light source against star background with image orthicon TV system
Optimal vacuum rocket trajectories over spherical earth, deriving nonlinear differential equations for position and velocity
Simulation and Optimization of Rocket Trajectories program (SORT) contains comprehensive mathematical models for simulating aircraft dynamics, freely falling objects, and many types of ballistic trajectories. Provides high-fidelity, three-degrees-of-freedom simulation for atmospheric and exoatmospheric flight. It numerically models vehicle subsystems and vehicle environment. Used for wide range of simulations. Written in machine-independent FORTRAN 77.
Simultaneous recording of rocket trajectory and rapid auroral variations using high sensitivity image orthicon TV system
Numerical method for rocket trajectory determination from multistation Doppler tracking data
Mathematical model of rocket trajectories, drag, and positive static stability
Accelerated gradient projection method applied to rocket trajectory optimization for minimizing fuel required for placing payload in circular orbits
Multistage rocket trajectories optimized by second order numerical technique and digital computer program, considering coasting, vacuum flight and transition times
Perturbation solutions of differential equations of motion for low-thrust rocket trajectories
Extremal, maximum-range, thrust limited rocket trajectory computing method with lunar transport applications
Iterative solution of least squares programming problem for finite thrust rocket trajectory optimization
The present paper deals with the problem of determining various solar eclipse variables as observed from a sounding rocket for various rocket trajectories. By applying the methods described to a set of trajectories, a set of boundary conditions, launch azimuth, quadrant elevation, and launch time may be selected to optimize any aspect of eclipse observation within the constraints imposed by rocket performance.
Interplanetary low thrust, geocentric low and high thrust trajectory optimization
Models utilizing various sub-sets of the six degrees of freedom are used in trajectory simulation. A 3-D model with only linear degrees of freedom is especially attractive, since the coefficients for the angular degrees of freedom are the most difficult to determine and the angular equations are the most time consuming for the computer to evaluate. A computer program is developed that uses three separate subsections to predict trajectories. A launch rail subsection is used until the rocket has left its launcher. The program then switches to a special 3-D section which computes motions in two linear and one angular degrees of freedom. When the rocket trims out, the program switches to the standard, three linear degrees of freedom model.
Perturbation solutions for equations of motion of vehicle subjected to low thrust acceleration
The optimal trajectories in the neighborhood of an optimal intermediate-thrust arc are investigated for the minimum-fuel orbit rendezvous problem with fixed specific impulse. Since such an arc is singular, the thrust acceleration magnitude being the singular control component, a second-variation analysis leads to the identification of a field of neighboring, singular arcs in a state space of dimension four rather than six, provided that a suitable Jacobi condition is met. A given neighboring initial six-dimensional state vector does not generally lie on a neighboring singular arc, and junction onto the appropriate singular arc must be accomplished by a short period of strong variations in the acceleration. The neighboring singular arc meets the final condition in 4 dimensions, rather than 6 dimensions, and rendezvous must be completed by another, terminal short period of strong variations in the acceleration. Implications for midcourse guidance near a singular arc are discussed.
Spacecraft guidance - multistage rocket trajectories