A Survey of Computational Physics: Introductory by Rubin H. Landau PDF

By Rubin H. Landau

ISBN-10: 0691131376

ISBN-13: 9780691131375

Computational physics is a quickly transforming into subfield of computational technological know-how, largely simply because pcs can resolve formerly intractable difficulties or simulate normal methods that don't have analytic ideas. the next move past Landau's First path in medical Computing and a follow-up to Landau and Páez's Computational Physics , this article offers a huge survey of key themes in computational physics for complex undergraduates and starting graduate scholars, together with new discussions of visualization instruments, wavelet research, molecular dynamics, and computational fluid dynamics. by means of treating technology, utilized arithmetic, and computing device technology jointly, the e-book unearths how this data base might be utilized to a much wider variety of real-world difficulties than computational physics texts usually address.

Designed for a one- or two-semester path, A Survey of Computational Physics also will curiosity somebody who desires a reference on or sensible adventure within the fundamentals of computational physics. The textual content encompasses a CD-ROM with supplementary fabrics, together with Java, Fortran, and C courses; animations; visualizations; colour figures; interactive Java applets; codes for MPI, PVM, and OpenDX; and a PVM tutorial.

  • Accessible to complex undergraduates
  • Real-world problem-solving technique
  • Java codes and applets built-in with textual content
  • Accompanying CD-ROM comprises codes, applets, animations, and visualization documents
  • Companion website comprises video clips of lectures

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Additional resources for A Survey of Computational Physics: Introductory Computational Science

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17). Without using the identity sin(x + 2nπ) = sin(x), show that there is a range of somewhat large values of x for which the algorithm converges, but that it converges to the wrong answer. Show that as you keep increasing x, you will reach a regime where the algorithm does not even converge. Now make use of the identity sin(x + 2nπ) = sin(x) to compute sin x for large x values where the series otherwise would diverge.

But how do we decide when to stop summing? 15) indicates that we should calculate (−1)n−1 x2n−1 and then divide it by (2n − 1)! This is not a good way to compute. On the one hand, both (2n − 1)! and x2n−1 can get very large and cause overflows, even though their quotient may not. On the other hand, powers and factorials are very expensive (time-consuming) to evaluate on the computer. Consequently, a better approach is to use a single multiplication to relate the next term in the series to the previous one: (−1)n−1 x2n−1 −x2 (−1)n−2 x2n−3 = (2n − 1)!

P r i n t f ( "\n\n Enter new name and r in Name. dat\n" ) ; Scanner s c 2 = new Scanner ( new F i l e ( "Name. dat" ) ) ; / / Open f i l e System . out . p r i n t f ( "Hi %s\n" , s c 2 . next ( ) ) ; / / Read , p r i n t l i n e 1 r = s c 2 . nextDouble ( ) ; / / Read l i n e 2 System . out . 1f \n" , r ) ; / / Print line 2 A = PI ∗ r ∗ r ; / / Computation System . out . p r i n t f ( "Done , look in A. dat\n" ) ; / / Screen p r i n t P r i n t W r i t e r q = new P r i n t W r i t e r ( new FileOutputStream ( "A.

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A Survey of Computational Physics: Introductory Computational Science by Rubin H. Landau


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