1998
DOI: 10.1063/1.882306
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Computational Physics: Problem Solving with Computers

Abstract: Computing Software Basics 7 2.1 Making Computers Obey 7 2.2 Computer Languages 7 2.3 Programming Warmup 9 2.3.1 Java-Scanner Implementation 10 2.3.2 C Implementation 11 2.3.3 Fortran Implementation 12 2.4 Shells, Editors, and Programs 12 2.5 Limited Range and Precision of Numbers 13 2.6 Number Representation 13 2.7 IEEE Floating Point Numbers 14 2.8 Over/Underflows Exercise 20 2.9 Machine Precision 21 2.10 Determine Your Machine Precision 23 2.11 Structured Program Design 24 2.12 Summing Series 26 2.13 Numeric… Show more

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Cited by 57 publications
(68 citation statements)
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“…Thus, in order to generalize the study of the properties of this model by a nonextensive approach, we modified the Metropolis method for the nonextensive statistics. To proceed the single spin flip MC calculations [36] and to obtain the physical quantities of interest of the system (magnetization, susceptibility, specific heat, and other quantities), we have changed the usual statistical weight to [21] w q = P i,af ter…”
Section: Nonextensive Statistics and Monte Carlo Simulationmentioning
confidence: 99%
“…Thus, in order to generalize the study of the properties of this model by a nonextensive approach, we modified the Metropolis method for the nonextensive statistics. To proceed the single spin flip MC calculations [36] and to obtain the physical quantities of interest of the system (magnetization, susceptibility, specific heat, and other quantities), we have changed the usual statistical weight to [21] w q = P i,af ter…”
Section: Nonextensive Statistics and Monte Carlo Simulationmentioning
confidence: 99%
“…Based on this information, one can obtain the positions r in+1/2 , corresponding to the midpoint of the integration interval h (Euler method The energy conservation is not explicitly built in the algorithm. The precision could be thus checked by plotting [1] …”
Section: Program Descriptionmentioning
confidence: 99%
“…The equations (1) are solved using a second order Runge-Kutta algorithm [1]. We calculated first the resultant force F i (t n ) acting on each particle.…”
Section: Program Descriptionmentioning
confidence: 99%
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