Computer Simulation of An Optically Pumped Methyl Fluoride Laser
Computer Simulation of An Optically Pumped Methyl Fluoride Laser
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61 Pressure broadened C0 2 Figure 22 . Broadened C0 2 in resonance with methyl fluoride.
CHAPTER V RESULTS Numerical solutions of the equations described in the last chapter were carried out at the University of Florida on an I.B.M. 360-75 computer. The numerical technique employed was Hamming's modification of the Milne predictor -corrector method. A fourth order Runge-Kutta method is used to generate the first time-increment solution since the predictor -corrector method is not self -starting.... Hamming's method is a stable fourth order integration procedure which has the advantage of a variable step size. This saves computing time without sacrificing accuracy.
The accuracy for all the results was kept between one part in 10 3 to one part in 10 4 . This is better than actually required; however it facilitates faster overall integration since solutions were not allowed to start diverging at any point. The time step was between .5 and .01 measured in units of time where one unit was the time for one collision.
What to read after Computer Simulation of An Optically Pumped Methyl Fluoride Laser?
You can find similar books in the "Read Also" column, or choose other free books by Schau, Harvey Charles to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
61 Pressure broadened C0 2 Figure 22 . Broadened C0 2 in resonance with methyl fluoride.
CHAPTER V RESULTS Numerical solutions of the equations described in the last chapter were carried out at the University of Florida on an I.B.M. 360-75 computer. The numerical technique employed was Hamming's modification of the Milne predictor -corrector method. A fourth order Runge-Kutta method is used to generate the first time-increment solution since the predictor -corrector method is not self -starting.... Hamming's method is a stable fourth order integration procedure which has the advantage of a variable step size. This saves computing time without sacrificing accuracy.
The accuracy for all the results was kept between one part in 10 3 to one part in 10 4 . This is better than actually required; however it facilitates faster overall integration since solutions were not allowed to start diverging at any point. The time step was between .5 and .01 measured in units of time where one unit was the time for one collision.
What to read after Computer Simulation of An Optically Pumped Methyl Fluoride Laser?
You can find similar books in the "Read Also" column, or choose other free books by Schau, Harvey Charles to read onlineMoreLess
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