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The one - dimensional linear wave equation can be written as We wish to adopt a second - order in time and second - order

The one-dimensional linear wave equation can be written as
We wish to adopt a second-order in time and second-order in space finite difference scheme, and a candidate is given by
The stability condition for this scheme is the Courant Friedrichs Lewy (CFL) condition, hence 0<=\sigma <=1, where \sigma =c\Delta t /\Delta x is the Courant number. In order to reduce the computational time, the \Delta t is usually kept as large as possible, hence reducing the number of time steps taken.
The problem is furthermore normalized such that an approximation error of =1 for a discretisation size \Delta x=1 is obtained. You may assume you are using a computer with a 64 bit processor, for which you can expect a floating point accuracy (i.e. machine precision) of 1016.
If we choose a \Delta x=0.001. What is the expected error when computing for the above discretisation? [ans1]
Subsequently you perform a mesh convergence study, and hence you refine the grid resolution. What is the smallest value of \Delta x you can afford before you encounter errors when computing due to the machine precision? [ans2]
Having performed the tests for the one-dimensional problem, you decide to perform the simulations on a three-dimensional problem with \Delta x=103 for a domain of unit size in each dimension and periodic boundary conditions, and 5 seconds of physical simulation time are needed for the problem. Considering an 800 mflops (mega flops) capability, and that each discretisation point requires 8 floating point operations per time step, what is the total run time for the simulation, to the nearest hour. [ans3]

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