Advanced Programming in Engineering Saurabh Srivastava, Thomas Weinhart Martin Robinson, and Stefan Luding MSM, CTW, UTwente, NL

Size: px
Start display at page:

Download "Advanced Programming in Engineering Saurabh Srivastava, Thomas Weinhart Martin Robinson, and Stefan Luding MSM, CTW, UTwente, NL"

Transcription

1 Advanced Programming in Engineering Saurabh Srivastava, Thomas Weinhart Martin Robinson, and Stefan Luding MSM, CTW, UTwente, NL Contents Why is this class important for me? What will I learn in this class? When is this class? Where is this class? 1

2 Introduction! Why is the class important for me?! Computations are everywhere in engineering problems. Many problems are resolved with the aid of computers and dedicated programs today. It is important to be able to implement numerical algorithms It is really important for an engineer to be familiar with computers and programming languages. Introduction! 2

3 Introduction! What can we do with the computer? Ø Evaluation of (experimental) data Ø Solving physical/engineering problems Ø Numerical experiments How do we do that?! Ø Compiler languages (C, C++, Fortran,...) Ø Interpreter languages (MATLAB, ) What do we learn? Ø Translate problems to algorithms Ø Practical experiences (exercises,debugging ) Introduction! Program:! Algorithms to solve differential equations Finite element method Molecular dynamics with Lennard-Jones for fluids Measuring pressure, temperature and diffusion in MD! Random numbers & Fractals Monte-Carlo for solving integrals and PDEs Finite Volume SPH 3

4 Introduction! When is the class? From 14 November Monday Morning ½ Theory Monday Morning ¾ Practice Introduction! When is the class? From 14 November Monday Morning ½ Theory Monday Morning ¾ Practice Stefan Ordinary Differential Equations Thomas Debugging, object orientation, profiling, Stefan Molecular Dynamics for Solids Saurabh FEM for Solids Saurabh FEM for Solids Saurabh Nonlinear FEM Stefan Random Numbers and Applications reserve 4

5 Introduction! When is the class? From 14 November Monday Morning ½ Theory Monday Morning ¾ Practice Thomas Martin Martin Thomas Thomas MD for Fluids and Statistical Analysis SPH (Smooth Particle Hydrodynamics) 1 SPH (Smooth Particle Hydrodynamics) 2 free day FV (Free Volume) Methods 1 FV (Free Volume) Methods 2 reserve reserve Introduction! Where is the class? OH 112 5

6 Introduction! Questions? Flow with friction & rolling resistance µ = 0.5 µ = 0.5 µ = 0.2 r 6

7 Sintering Vibration test p=100 p=10 tension kt k 2 = 12 7

8 P-wave animation P-wave animation 8

9 Anisotropy 3D 3D 3-dimensional modeling of sound propagation Sound P-wave shape and speed 9

10 Preparation p=20000 p=2000p=200 p=20 p=2 Contents Introduction Examples 1&2 1st Days Goal: Solve Differential Equations (ODE) 2nd Days Goal: Debugging and Matlab Optimization 3rd Days Goal: 1D/2D Molecular Dynamics (ODE) Morning 3/4: Practical Exercises 10

11 Introduction to Advanced Programming in Engineering Examples 1 (Stefan) Saurabh Srivastava, Thomas Weinhart, Stefan Luding MSM, TS, CTW, UTwente, NL 5. int main(int argc, char *argv[]) 6. { 7. const int ipmax=20; 8. int inum; 9. cout << Type number: ; 10. cin >> inum; if(inum < pow(2.0,ipmax)) // check number 13. { 14. cout << Base 10: << inum << endl; 15. cout << Base 2: ; // perform binary check for 2^ipmax 18. for(int i=ipmax; i>=0; i--) 19. { 20. if(inum >= pow(2.0,i)) 21. { 22. inum -= pow(2.0,i); 23. cout << '1'; 24. } 25. else 26. cout << '0'; 27. } 28. cout << endl; 29. } 30. else 31. { 32. cout << ERROR: input-number << inum << > 33. << pow(2.0,ipmax) << too large! << endl; 34. } 35. system(pause); 36. return EXIT_SUCCESS; 37. } Previous Course PiE: Exercise 2 0 no INPUT Loop: i=20,,0 inum>=2 i 1 END yes inum=inum 2 i 11

12 Differential Equations Physical examples Mass-spring system Pendulum Methods Euler and Euler-Cromer Verlet and friends Runge-Kutta Predictor-Corrector etc. 1. #include<iostream> 2. #include<fstream> 3. #include<cmath> 4. using namespace std; 5. int main(int argc, char *argv[]) 6. { 7. // Define field x(t) with length double x[1000], t; // output variables 9. // initial conditions 10. double A, delta; // A=ampl, delta=phase 11. double mass; // mass=mass 12. double ksprng; // ksprng=spring-const. 13. double t_max, dt; // t_max=max-time 14. // dt=time-interval 15. // Request input of the parameters 16. cout << amplitude ; cin >> A; 17. cout << phase-angle ; cin >> delta; 18. cout << mass ; cin >> mass; 19. cout << spring-const. ; cin >> ksprng; 20. cout << max-time ; cin >> t_max; 21. cout << time-interval ; cin >> dt; Exercise double omega=sqrt(ksprng/mass); 23. // Loop from t=0 to t=t_max 24. t=0.0; 25. for( int i=0; i<=t_max/dt; i++ ) 26. { 27. // compute function 28. x[i]=a*sin(omega*t+delta); 29. t=t+dt; // Step to next time 30. } 31. ofstream outfile(plot.data); 32. // Output-start 33. t=0.0; 34. for( int i=0; i<=t_max/dt; i++ ) 35. { 36. outfile << t << 37. << x[i] << endl; 38. t=t+dt; 39. } 40. } 12

13 Differential Equations Mass-spring system Differential Equations 1 Mass spring system 13

14 Differential Equations 1 Mass-spring system Differential Eqs Mass-spring system 14

15 Differential Equations 2 Pendulum Differential Equations Physical examples Mass-spring system Pendulum Methods Euler and Euler-Cromer Verlet and friends Runge-Kutta Predictor-Corrector etc. 15

16 Differential Equations 2 Pendulum Differential Equations 16

17 Differential Eqs Poincare-cut instead of x-t-plot view: v-x-plot attractors/chaos Differential Equations - summary Physical examples Mass-spring system Pendulum Methods Euler and Euler-Cromer Verlet and friends Runge-Kutta Predictor-Corrector etc. 17

18 Questions? 08:45h 10:30h room: OH112! 10:45h 12:30h room: OH112! Advanced Programming in Engineering ! Saurabh Srivastava, Thomas Weinhart, Martin Robinson, Stefan Luding 18

Simulation in Computer Graphics. Particles. Matthias Teschner. Computer Science Department University of Freiburg

Simulation in Computer Graphics. Particles. Matthias Teschner. Computer Science Department University of Freiburg Simulation in Computer Graphics Particles Matthias Teschner Computer Science Department University of Freiburg Outline introduction particle motion finite differences system of first order ODEs second

More information

SPH: Towards the simulation of wave-body interactions in extreme seas

SPH: Towards the simulation of wave-body interactions in extreme seas SPH: Towards the simulation of wave-body interactions in extreme seas Guillaume Oger, Mathieu Doring, Bertrand Alessandrini, and Pierre Ferrant Fluid Mechanics Laboratory (CNRS UMR6598) Ecole Centrale

More information

Mass-Spring Systems. Last Time?

Mass-Spring Systems. Last Time? Mass-Spring Systems Last Time? Implicit Surfaces & Marching Cubes/Tetras Collision Detection & Conservative Bounding Regions Spatial Acceleration Data Structures Octree, k-d tree, BSF tree 1 Today Particle

More information

CS205b/CME306. Lecture 9

CS205b/CME306. Lecture 9 CS205b/CME306 Lecture 9 1 Convection Supplementary Reading: Osher and Fedkiw, Sections 3.3 and 3.5; Leveque, Sections 6.7, 8.3, 10.2, 10.4. For a reference on Newton polynomial interpolation via divided

More information

Homework 4: (GRADUATE VERSION)

Homework 4: (GRADUATE VERSION) Homework 4: Wavefront Path Planning and Path Smoothing (GRADUATE VERSION) Assigned: Thursday, October 16, 2008 Due: Friday, October 31, 2008 at 23:59:59 In this assignment, you will write a path planner

More information

Thermal Coupling Method Between SPH Particles and Solid Elements in LS-DYNA

Thermal Coupling Method Between SPH Particles and Solid Elements in LS-DYNA Thermal Coupling Method Between SPH Particles and Solid Elements in LS-DYNA INTRODUCTION: Jingxiao Xu, Jason Wang LSTC Heat transfer is very important in many industrial and geophysical problems. Many

More information

over The idea is to construct an algorithm to solve the IVP ODE (8.1)

over The idea is to construct an algorithm to solve the IVP ODE (8.1) Runge- Ku(a Methods Review of Heun s Method (Deriva:on from Integra:on) The idea is to construct an algorithm to solve the IVP ODE (8.1) over To obtain the solution point we can use the fundamental theorem

More information

CMPE110 - EXPERIMENT 1 * MICROSOFT VISUAL STUDIO AND C++ PROGRAMMING

CMPE110 - EXPERIMENT 1 * MICROSOFT VISUAL STUDIO AND C++ PROGRAMMING CMPE110 - EXPERIMENT 1 * MICROSOFT VISUAL STUDIO AND C++ PROGRAMMING Aims 1. Learning primary functions of Microsoft Visual Studio 2008 * 2. Introduction to C++ Programming 3. Running C++ programs using

More information

#include <iostream> #include <algorithm> #include <cmath> using namespace std; int f1(int x, int y) { return (double)(x/y); }

#include <iostream> #include <algorithm> #include <cmath> using namespace std; int f1(int x, int y) { return (double)(x/y); } 1. (9 pts) Show what will be output by the cout s in this program. As in normal program execution, any update to a variable should affect the next statement. (Note: boolalpha simply causes Booleans to

More information

Acknowledgements. Prof. Dan Negrut Prof. Darryl Thelen Prof. Michael Zinn. SBEL Colleagues: Hammad Mazar, Toby Heyn, Manoj Kumar

Acknowledgements. Prof. Dan Negrut Prof. Darryl Thelen Prof. Michael Zinn. SBEL Colleagues: Hammad Mazar, Toby Heyn, Manoj Kumar Philipp Hahn Acknowledgements Prof. Dan Negrut Prof. Darryl Thelen Prof. Michael Zinn SBEL Colleagues: Hammad Mazar, Toby Heyn, Manoj Kumar 2 Outline Motivation Lumped Mass Model Model properties Simulation

More information

SPH: Why and what for?

SPH: Why and what for? SPH: Why and what for? 4 th SPHERIC training day David Le Touzé, Fluid Mechanics Laboratory, Ecole Centrale de Nantes / CNRS SPH What for and why? How it works? Why not for everything? Duality of SPH SPH

More information

MATLAB. Advanced Mathematics and Mechanics Applications Using. Third Edition. David Halpern University of Alabama CHAPMAN & HALL/CRC

MATLAB. Advanced Mathematics and Mechanics Applications Using. Third Edition. David Halpern University of Alabama CHAPMAN & HALL/CRC Advanced Mathematics and Mechanics Applications Using MATLAB Third Edition Howard B. Wilson University of Alabama Louis H. Turcotte Rose-Hulman Institute of Technology David Halpern University of Alabama

More information

Scientific Computing

Scientific Computing Scientific Computing Martin Lotz School of Mathematics The University of Manchester Lecture 1, September 22, 2014 Outline Course Overview Programming Basics The C++ Programming Language Outline Course

More information

Scientific Computing for Physical Systems. Spring semester, 2018

Scientific Computing for Physical Systems. Spring semester, 2018 Scientific Computing for Physical Systems Spring semester, 2018 Course Goals Learn a programming language (Python) Learn some numerical algorithms (e.g., for solving differential equations) Explore some

More information

Topic 8: Lazy Evaluation

Topic 8: Lazy Evaluation Topic 8: Lazy Evaluation 1 Recommended Exercises and Readings From Haskell: The craft of functional programming (3 rd Ed.) Exercises: 17.1, 17.2, 17.4, 17.8, 17.23, 17.25, 17.28, 17.29 Readings: Chapter

More information

CS 103 Unit 14 - Streams

CS 103 Unit 14 - Streams CS 103 Unit 14 - Streams 1 2 I/O Streams '>>' operator used to read data from an input stream Always skips leading whitespace ('\n', ' ', '\t') and stops at first trailing whitespace '

More information

MATH2071: LAB 2: Explicit ODE methods

MATH2071: LAB 2: Explicit ODE methods MATH2071: LAB 2: Explicit ODE methods 1 Introduction Introduction Exercise 1 Euler s method review Exercise 2 The Euler Halfstep (RK2) Method Exercise 3 Runge-Kutta Methods Exercise 4 The Midpoint Method

More information

C++ For Science and Engineering Lecture 12

C++ For Science and Engineering Lecture 12 C++ For Science and Engineering Lecture 12 John Chrispell Tulane University Monday September 20, 2010 Comparing C-Style strings Note the following listing dosn t do what you probably think it does (assuming

More information

PROGRAMMING AND ENGINEERING COMPUTING WITH MATLAB Huei-Huang Lee SDC. Better Textbooks. Lower Prices.

PROGRAMMING AND ENGINEERING COMPUTING WITH MATLAB Huei-Huang Lee SDC. Better Textbooks. Lower Prices. PROGRAMMING AND ENGINEERING COMPUTING WITH MATLAB 2018 Huei-Huang Lee SDC P U B L I C AT I O N S Better Textbooks. Lower Prices. www.sdcpublications.com Powered by TCPDF (www.tcpdf.org) Visit the following

More information

Lagrangian methods and Smoothed Particle Hydrodynamics (SPH) Computation in Astrophysics Seminar (Spring 2006) L. J. Dursi

Lagrangian methods and Smoothed Particle Hydrodynamics (SPH) Computation in Astrophysics Seminar (Spring 2006) L. J. Dursi Lagrangian methods and Smoothed Particle Hydrodynamics (SPH) Eulerian Grid Methods The methods covered so far in this course use an Eulerian grid: Prescribed coordinates In `lab frame' Fluid elements flow

More information

http://miccom-center.org Topic: Continuum-Particle Simulation Software (COPSS-Hydrodynamics) Presenter: Jiyuan Li, The University of Chicago 2017 Summer School 1 What is Continuum-Particle Simulation?

More information

A SHORT COURSE ON C++

A SHORT COURSE ON C++ Introduction to A SHORT COURSE ON School of Mathematics Semester 1 2008 Introduction to OUTLINE 1 INTRODUCTION TO 2 FLOW CONTROL AND FUNCTIONS If Else Looping Functions Cmath Library Prototyping Introduction

More information

Final Report. Discontinuous Galerkin Compressible Euler Equation Solver. May 14, Andrey Andreyev. Adviser: Dr. James Baeder

Final Report. Discontinuous Galerkin Compressible Euler Equation Solver. May 14, Andrey Andreyev. Adviser: Dr. James Baeder Final Report Discontinuous Galerkin Compressible Euler Equation Solver May 14, 2013 Andrey Andreyev Adviser: Dr. James Baeder Abstract: In this work a Discontinuous Galerkin Method is developed for compressible

More information

Project 1: Convex hulls and line segment intersection

Project 1: Convex hulls and line segment intersection MCS 481 / David Dumas / Spring 2014 Project 1: Convex hulls and line segment intersection Due at 10am on Monday, February 10 0. Prerequisites For this project it is expected that you already have CGAL

More information

Navier-Stokes & Flow Simulation

Navier-Stokes & Flow Simulation Last Time? Navier-Stokes & Flow Simulation Optional Reading for Last Time: Spring-Mass Systems Numerical Integration (Euler, Midpoint, Runge-Kutta) Modeling string, hair, & cloth HW2: Cloth & Fluid Simulation

More information

Partitioning and Divide-and-Conquer Strategies

Partitioning and Divide-and-Conquer Strategies Chapter 4 Slide 125 Partitioning and Divide-and-Conquer Strategies Slide 126 Partitioning Partitioning simply divides the problem into parts. Divide and Conquer Characterized by dividing problem into subproblems

More information

CS Software Engineering for Scientific Computing. Lecture 5: More C++, more tools.

CS Software Engineering for Scientific Computing. Lecture 5: More C++, more tools. CS 294-73 Software Engineering for Scientific Computing Lecture 5: More C++, more tools. Let s go back to our build of mdarraymain.cpp clang++ -DDIM=2 -std=c++11 -g mdarraymain.cpp DBox.cpp -o mdarraytest.exe

More information

The American University in Cairo Department of Computer Science & Engineeringt CSCI &09 Dr. KHALIL Exam-I Fall 2009

The American University in Cairo Department of Computer Science & Engineeringt CSCI &09 Dr. KHALIL Exam-I Fall 2009 The American University in Cairo Department of Computer Science & Engineeringt CSCI 106-05&09 Dr. KHALIL Exam-I Fall 2009 Last Name :... ID:... First Name:... Form I Section No.: EXAMINATION INSTRUCTIONS

More information

Lecture Notes CPSC 224 (Spring 2012) Today... Java basics. S. Bowers 1 of 8

Lecture Notes CPSC 224 (Spring 2012) Today... Java basics. S. Bowers 1 of 8 Today... Java basics S. Bowers 1 of 8 Java main method (cont.) In Java, main looks like this: public class HelloWorld { public static void main(string[] args) { System.out.println("Hello World!"); Q: How

More information

ODEs occur quite often in physics and astrophysics: Wave Equation in 1-D stellar structure equations hydrostatic equation in atmospheres orbits

ODEs occur quite often in physics and astrophysics: Wave Equation in 1-D stellar structure equations hydrostatic equation in atmospheres orbits Solving ODEs General Stuff ODEs occur quite often in physics and astrophysics: Wave Equation in 1-D stellar structure equations hydrostatic equation in atmospheres orbits need workhorse solvers to deal

More information

Multiple Choice Questions (20 questions * 5 points per question = 100 points)

Multiple Choice Questions (20 questions * 5 points per question = 100 points) EECS 183 Winter 2014 Exam 1 Closed Book Closed Notes Closed Electronic Devices Closed Neighbor Turn off Your Cell Phones We will confiscate all electronic devices that we see including cell phones, calculators,

More information

DYNAMIC ARRAYS; FUNCTIONS & POINTERS; SHALLOW VS DEEP COPY

DYNAMIC ARRAYS; FUNCTIONS & POINTERS; SHALLOW VS DEEP COPY DYNAMIC ARRAYS; FUNCTIONS & POINTERS; SHALLOW VS DEEP COPY Pages 800 to 809 Anna Rakitianskaia, University of Pretoria STATIC ARRAYS So far, we have only used static arrays The size of a static array must

More information

Overview. - General Data Types - Categories of Words. - Define Before Use. - The Three S s. - End of Statement - My First Program

Overview. - General Data Types - Categories of Words. - Define Before Use. - The Three S s. - End of Statement - My First Program Overview - General Data Types - Categories of Words - The Three S s - Define Before Use - End of Statement - My First Program a description of data, defining a set of valid values and operations List of

More information

Huei-Huang Lee. Programming with MATLAB2016 SDC ACCESS CODE. Better Textbooks. Lower Prices. UNIQUE CODE INSIDE

Huei-Huang Lee. Programming with MATLAB2016 SDC ACCESS CODE. Better Textbooks. Lower Prices.   UNIQUE CODE INSIDE Programming with Huei-Huang Lee MATLAB2016 SDC P U B L I C AT I O N S Better Textbooks. Lower Prices. www.sdcpublications.com ACCESS CODE UNIQUE CODE INSIDE Powered by TCPDF (www.tcpdf.org) Visit the following

More information

Week4. Huayi Li

Week4. Huayi Li Week4 Huayi Li 2011-9-15 1. Summary of Quiz1 2. An example of if-else statement Recall that, given a Quadratic ax 2 + bx + c = 0 if a = 0, then problem reduces to linear equation. x = -c /b if b 0 x is

More information

Programming in Engineering

Programming in Engineering Faculty of Engineering Technology Programming in Engineering Stefan Luding, Anthony Thornton, Thomas Weinhart edition: 2012 Contents Contents i Preface vii Acknowledgement vii History vii Preliminaries

More information

Partitioning and Divide-and-Conquer Strategies

Partitioning and Divide-and-Conquer Strategies Partitioning and Divide-and-Conquer Strategies Chapter 4 slides4-1 Partitioning Partitioning simply divides the problem into parts. Divide and Conquer Characterized by dividing problem into subproblems

More information

Modelling and Simulation for Engineers

Modelling and Simulation for Engineers Unit T7: Modelling and Simulation for Engineers Unit code: F/503/7343 QCF level: 6 Credit value: 15 Aim This unit gives learners the opportunity to develop their understanding of Ordinary Differential

More information

Navier-Stokes & Flow Simulation

Navier-Stokes & Flow Simulation Last Time? Navier-Stokes & Flow Simulation Pop Worksheet! Teams of 2. Hand in to Jeramey after we discuss. Sketch the first few frames of a 2D explicit Euler mass-spring simulation for a 2x3 cloth network

More information

Errata for C++ and Algorithmic Thinking for the Complete Beginner

Errata for C++ and Algorithmic Thinking for the Complete Beginner Errata for C++ and Algorithmic Thinking for the Complete Beginner 12 What it Hardware? The Central Processing Unit (CPU) This is the part of a computer that actually performs all the tasks defined in a

More information

Linked List using a Sentinel

Linked List using a Sentinel Linked List using a Sentinel Linked List.h / Linked List.h Using a sentinel for search Created by Enoch Hwang on 2/1/10. Copyright 2010 La Sierra University. All rights reserved. / #include

More information

Parallelization of Scientific Applications (II)

Parallelization of Scientific Applications (II) Parallelization of Scientific Applications (II) Parallelization of Particle Based Methods Russian-German School on High Performance Computer Systems, June, 27 th until July, 6 th 2005, Novosibirsk 4. Day,

More information

A brief description of the particle finite element method (PFEM2). Extensions to free surface

A brief description of the particle finite element method (PFEM2). Extensions to free surface A brief description of the particle finite element method (PFEM2). Extensions to free surface flows. Juan M. Gimenez, L.M. González, CIMEC Universidad Nacional del Litoral (UNL) Santa Fe, Argentina Universidad

More information

Example 13 - Shock Tube

Example 13 - Shock Tube Example 13 - Shock Tube Summary This famous experiment is interesting for observing the shock-wave propagation. Moreover, this case uses the representation of perfect gas and compares the different formulations:

More information

Euler s Methods (a family of Runge- Ku9a methods)

Euler s Methods (a family of Runge- Ku9a methods) Euler s Methods (a family of Runge- Ku9a methods) ODE IVP An Ordinary Differential Equation (ODE) is an equation that contains a function having one independent variable: The equation is coupled with an

More information

Exercise 1.1 Hello world

Exercise 1.1 Hello world Exercise 1.1 Hello world The goal of this exercise is to verify that computer and compiler setup are functioning correctly. To verify that your setup runs fine, compile and run the hello world example

More information

CS 103 Unit 14 - Streams

CS 103 Unit 14 - Streams CS 103 Unit 14 - Streams 1 2 I/O Streams '>>' operator reads from a stream (and convert to the desired type) Always skips leading whitespace ('\n', ' ', '\t') and stops at first trailing whitespace '

More information

Example problem: Solution of the 2D unsteady heat equation with restarts

Example problem: Solution of the 2D unsteady heat equation with restarts Chapter 1 Example problem: Solution of the 2D unsteady heat equation with restarts Simulations of time-dependent problem can be very time consuming and it is important to be able to restart simulations,

More information

2.29 Numerical Marine Hydrodynamics Spring 2007

2.29 Numerical Marine Hydrodynamics Spring 2007 Numerical Marine Hydrodynamics Spring 2007 Course Staff: Instructor: Prof. Henrik Schmidt OCW Web Site: http://ocw.mit.edu/ocwweb/mechanical- Engineering/2-29Spring-2003/CourseHome/index.htm Units: (3-0-9)

More information

Thursday 1/8 1 * syllabus, Introduction * preview reading assgt., chapter 1 (modeling) * HW review chapters 1, 2, & 3

Thursday 1/8 1 * syllabus, Introduction * preview reading assgt., chapter 1 (modeling) * HW review chapters 1, 2, & 3 Topics and Syllabus Class # Text Reading I. NUMERICAL ANALYSIS CHAPRA AND CANALE A. INTRODUCTION AND MATLAB REVIEW :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::Week

More information

Skåne University Hospital Lund, Lund, Sweden 2 Deparment of Numerical Analysis, Centre for Mathematical Sciences, Lund University, Lund, Sweden

Skåne University Hospital Lund, Lund, Sweden 2 Deparment of Numerical Analysis, Centre for Mathematical Sciences, Lund University, Lund, Sweden Volume Tracking: A New Method for Visualization of Intracardiac Blood Flow from Three-Dimensional, Time-Resolved, Three-Component Magnetic Resonance Velocity Mapping Appendix: Theory and Numerical Implementation

More information

BITG 1113: Files and Stream LECTURE 10

BITG 1113: Files and Stream LECTURE 10 BITG 1113: Files and Stream LECTURE 10 1 LEARNING OUTCOMES At the end of this lecture, you should be able to: 1. Describe the fundamentals of input & output files. 2. Use data files for input & output

More information

Parallel Summation of Inter-Particle Forces in SPH

Parallel Summation of Inter-Particle Forces in SPH Parallel Summation of Inter-Particle Forces in SPH Fifth International Workshop on Meshfree Methods for Partial Differential Equations 17.-19. August 2009 Bonn Overview Smoothed particle hydrodynamics

More information

CME 345: MODEL REDUCTION

CME 345: MODEL REDUCTION CME 345: MODEL REDUCTION Parameterized Partial Differential Equations Charbel Farhat Stanford University cfarhat@stanford.edu 1 / 19 Outline 1 Initial Boundary Value Problems 2 Typical Parameters of Interest

More information

Application 7.6A The Runge-Kutta Method for 2-Dimensional Systems

Application 7.6A The Runge-Kutta Method for 2-Dimensional Systems Application 7.6A The Runge-Kutta Method for -Dimensional Systems Figure 7.6. in the text lists TI-85 and BASIC versions of the program RKDIM that implements the Runge-Kutta iteration k (,, ) = f tn xn

More information

Quad Doubles on a GPU

Quad Doubles on a GPU Quad Doubles on a GPU 1 Floating-Point Arithmetic floating-point numbers quad double arithmetic quad doubles for use in CUDA programs 2 Quad Double Square Roots quad double arithmetic on a GPU a kernel

More information

Lab: Supplying Inputs to Programs

Lab: Supplying Inputs to Programs Steven Zeil May 25, 2013 Contents 1 Running the Program 2 2 Supplying Standard Input 4 3 Command Line Parameters 4 1 In this lab, we will look at some of the different ways that basic I/O information can

More information

ANSI C. Data Analysis in Geophysics Demián D. Gómez November 2013

ANSI C. Data Analysis in Geophysics Demián D. Gómez November 2013 ANSI C Data Analysis in Geophysics Demián D. Gómez November 2013 ANSI C Standards published by the American National Standards Institute (1983-1989). Initially developed by Dennis Ritchie between 1969

More information

Programming Fundamentals. With C++ Variable Declaration, Evaluation and Assignment 1

Programming Fundamentals. With C++ Variable Declaration, Evaluation and Assignment 1 300580 Programming Fundamentals 3 With C++ Variable Declaration, Evaluation and Assignment 1 Today s Topics Variable declaration Assignment to variables Typecasting Counting Mathematical functions Keyboard

More information

More on Func*ons Command Line Arguments CS 16: Solving Problems with Computers I Lecture #8

More on Func*ons Command Line Arguments CS 16: Solving Problems with Computers I Lecture #8 More on Func*ons Command Line Arguments CS 16: Solving Problems with Computers I Lecture #8 Ziad Matni Dept. of Computer Science, UCSB Announcements Homework #7 due today Lab #4 is due on Monday at 8:00

More information

Overloading Functions & Command Line Use in C++ CS 16: Solving Problems with Computers I Lecture #6

Overloading Functions & Command Line Use in C++ CS 16: Solving Problems with Computers I Lecture #6 Overloading Functions & Command Line Use in C++ CS 16: Solving Problems with Computers I Lecture #6 Ziad Matni Dept. of Computer Science, UCSB A reminder about Labs Announcements Please make sure you READ

More information

Realtime Water Simulation on GPU. Nuttapong Chentanez NVIDIA Research

Realtime Water Simulation on GPU. Nuttapong Chentanez NVIDIA Research 1 Realtime Water Simulation on GPU Nuttapong Chentanez NVIDIA Research 2 3 Overview Approaches to realtime water simulation Hybrid shallow water solver + particles Hybrid 3D tall cell water solver + particles

More information

Cloth Simulation. Tanja Munz. Master of Science Computer Animation and Visual Effects. CGI Techniques Report

Cloth Simulation. Tanja Munz. Master of Science Computer Animation and Visual Effects. CGI Techniques Report Cloth Simulation CGI Techniques Report Tanja Munz Master of Science Computer Animation and Visual Effects 21st November, 2014 Abstract Cloth simulation is a wide and popular area of research. First papers

More information

Data-Driven Modeling. Scientific Computation J. NATHAN KUTZ OXPORD. Methods for Complex Systems & Big Data

Data-Driven Modeling. Scientific Computation J. NATHAN KUTZ OXPORD. Methods for Complex Systems & Big Data Data-Driven Modeling & Scientific Computation Methods for Complex Systems & Big Data J. NATHAN KUTZ Department ofapplied Mathematics University of Washington OXPORD UNIVERSITY PRESS Contents Prolegomenon

More information

Ordinary Differential Equations

Ordinary Differential Equations Next: Partial Differential Equations Up: Numerical Analysis for Chemical Previous: Numerical Differentiation and Integration Subsections Runge-Kutta Methods Euler's Method Improvement of Euler's Method

More information

FEMLAB Exercise 1 for ChE366

FEMLAB Exercise 1 for ChE366 FEMLAB Exercise 1 for ChE366 Problem statement Consider a spherical particle of radius r s moving with constant velocity U in an infinitely long cylinder of radius R that contains a Newtonian fluid. Let

More information

Example problem: Solution of the 2D unsteady heat equation.

Example problem: Solution of the 2D unsteady heat equation. Chapter 1 Example problem: Solution of the 2D unsteady heat equation. This is our first time-dependent example problem. We will demonstrate that, compared to the solution of steady problems, the solution

More information

CHAPTER 1. Introduction

CHAPTER 1. Introduction ME 475: Computer-Aided Design of Structures 1-1 CHAPTER 1 Introduction 1.1 Analysis versus Design 1.2 Basic Steps in Analysis 1.3 What is the Finite Element Method? 1.4 Geometrical Representation, Discretization

More information

Search Algorithms. Linear Search Binary Search

Search Algorithms. Linear Search Binary Search Search Algorithms Linear Search Binary Search Searching The process used to find the location of a target among a list of objects Searching an array finds the index of first element in an array containing

More information

METU Mechanical Engineering Department ME 582 Finite Element Analysis in Thermofluids Spring 2018 (Dr. C. Sert) Handout 12 COMSOL 1 Tutorial 3

METU Mechanical Engineering Department ME 582 Finite Element Analysis in Thermofluids Spring 2018 (Dr. C. Sert) Handout 12 COMSOL 1 Tutorial 3 METU Mechanical Engineering Department ME 582 Finite Element Analysis in Thermofluids Spring 2018 (Dr. C. Sert) Handout 12 COMSOL 1 Tutorial 3 In this third COMSOL tutorial we ll solve Example 6 of Handout

More information

3D Simulation of Dam-break effect on a Solid Wall using Smoothed Particle Hydrodynamic

3D Simulation of Dam-break effect on a Solid Wall using Smoothed Particle Hydrodynamic ISCS 2013 Selected Papers Dam-break effect on a Solid Wall 1 3D Simulation of Dam-break effect on a Solid Wall using Smoothed Particle Hydrodynamic Suprijadi a,b, F. Faizal b, C.F. Naa a and A.Trisnawan

More information

Reading from and Writing to Files. Files (3.12) Steps to Using Files. Section 3.12 & 13.1 & Data stored in variables is temporary

Reading from and Writing to Files. Files (3.12) Steps to Using Files. Section 3.12 & 13.1 & Data stored in variables is temporary Reading from and Writing to Files Section 3.12 & 13.1 & 13.5 11/3/08 CS150 Introduction to Computer Science 1 1 Files (3.12) Data stored in variables is temporary We will learn how to write programs that

More information

BOOLEAN EXPRESSIONS CONTROL FLOW (IF-ELSE) INPUT/OUTPUT. Problem Solving with Computers-I

BOOLEAN EXPRESSIONS CONTROL FLOW (IF-ELSE) INPUT/OUTPUT. Problem Solving with Computers-I BOOLEAN EXPRESSIONS CONTROL FLOW (IF-ELSE) INPUT/OUTPUT Problem Solving with Computers-I Announcements HW02: Complete (individually)using dark pencil or pen, turn in during lab section next Wednesday Please

More information

Module1: Numerical Solution of Ordinary Differential Equations. Lecture 6. Higher order Runge Kutta Methods

Module1: Numerical Solution of Ordinary Differential Equations. Lecture 6. Higher order Runge Kutta Methods Module1: Numerical Solution of Ordinary Differential Equations Lecture 6 Higher order Runge Kutta Methods Keywords: higher order methods, functional evaluations, accuracy Higher order Runge Kutta Methods

More information

FILE IO AND DATA REPRSENTATION. Problem Solving with Computers-I

FILE IO AND DATA REPRSENTATION. Problem Solving with Computers-I FILE IO AND DATA REPRSENTATION Problem Solving with Computers-I Midterm next Thursday (Oct 25) No class on Tuesday (Oct 23) Announcements I/O in programs Different ways of reading data into programs cin

More information

Lab #5 Ocean Acoustic Environment

Lab #5 Ocean Acoustic Environment Lab #5 Ocean Acoustic Environment 2.S998 Unmanned Marine Vehicle Autonomy, Sensing and Communications Contents 1 The ocean acoustic environment 3 1.1 Ocean Acoustic Waveguide................................

More information

Thermal Coupling Method Between SPH Particles and Solid Elements in LS-DYNA

Thermal Coupling Method Between SPH Particles and Solid Elements in LS-DYNA Thermal Coupling Method Between SPH Particles and Solid Elements in LS-DYNA Jingxiao Xu 1, Jason Wang 2 1 LSTC 2 LSTC 1 Abstract Smooth particles hydrodynamics is a meshfree, Lagrangian particle method

More information

Debojyoti Ghosh. Adviser: Dr. James Baeder Alfred Gessow Rotorcraft Center Department of Aerospace Engineering

Debojyoti Ghosh. Adviser: Dr. James Baeder Alfred Gessow Rotorcraft Center Department of Aerospace Engineering Debojyoti Ghosh Adviser: Dr. James Baeder Alfred Gessow Rotorcraft Center Department of Aerospace Engineering To study the Dynamic Stalling of rotor blade cross-sections Unsteady Aerodynamics: Time varying

More information

Fluid-structure Interaction by the mixed SPH-FE Method with Application to Aircraft Ditching

Fluid-structure Interaction by the mixed SPH-FE Method with Application to Aircraft Ditching Fluid-structure Interaction by the mixed SPH-FE Method with Application to Aircraft Ditching Paul Groenenboom ESI Group Delft, Netherlands Martin Siemann German Aerospace Center (DLR) Stuttgart, Germany

More information

Exam 1. CSI 201: Computer Science 1 Fall 2018 Professors: Shaun Ramsey

Exam 1. CSI 201: Computer Science 1 Fall 2018 Professors: Shaun Ramsey Exam 1 CSI 201: Computer Science 1 Fall 2018 Professors: Shaun Ramsey I understand that this exam is closed books and closed notes and is to be completed without a calculator, phone, or other computer.

More information

EL2310 Scientific Programming

EL2310 Scientific Programming Lecture 14: Object Oriented Programming in C++ (ramviyas@kth.se) Overview Overview Lecture 14: Object Oriented Programming in C++ Classes (cont d) More on Classes and Members Group presentations Last time

More information

Sample Final Exam. 1) (24 points) Show what is printed by the following segments of code (assume all appropriate header files, etc.

Sample Final Exam. 1) (24 points) Show what is printed by the following segments of code (assume all appropriate header files, etc. Name: Sample Final Exam 1) (24 points) Show what is printed by the following segments of code (assume all appropriate header files, etc. are included): a) int start = 10, end = 21; while (start < end &&

More information

CSCE 206: Structured Programming in C++

CSCE 206: Structured Programming in C++ CSCE 206: Structured Programming in C++ 2017 Spring Exam 2 Monday, March 20, 2017 Total - 100 Points B Instructions: Total of 13 pages, including this cover and the last page. Before starting the exam,

More information

CFD in COMSOL Multiphysics

CFD in COMSOL Multiphysics CFD in COMSOL Multiphysics Christian Wollblad Copyright 2017 COMSOL. Any of the images, text, and equations here may be copied and modified for your own internal use. All trademarks are the property of

More information

Workpackage 5 - Ordinary Differential Equations

Workpackage 5 - Ordinary Differential Equations Mathematics for I Workpackage 5 - Ordinary Differential Equations Introduction During this laboratory you will be introduced to some of Matlab s facilities for solving ordinary differential equations (ode).

More information

CE221 Programming in C++ Part 1 Introduction

CE221 Programming in C++ Part 1 Introduction CE221 Programming in C++ Part 1 Introduction 06/10/2017 CE221 Part 1 1 Module Schedule There are two lectures (Monday 13.00-13.50 and Tuesday 11.00-11.50) each week in the autumn term, and a 2-hour lab

More information

Object-Oriented Programming, Iouliia Skliarova

Object-Oriented Programming, Iouliia Skliarova Object-Oriented Programming, Iouliia Skliarova CBook a = CBook("C++", 2014); CBook b = CBook("Physics", 1960); a.display(); b.display(); void CBook::Display() cout

More information

Welcome to Microsoft Excel 2013 p. 1 Customizing the QAT p. 5 Customizing the Ribbon Control p. 6 The Worksheet p. 6 Excel 2013 Specifications and

Welcome to Microsoft Excel 2013 p. 1 Customizing the QAT p. 5 Customizing the Ribbon Control p. 6 The Worksheet p. 6 Excel 2013 Specifications and Preface p. xi Welcome to Microsoft Excel 2013 p. 1 Customizing the QAT p. 5 Customizing the Ribbon Control p. 6 The Worksheet p. 6 Excel 2013 Specifications and Limits p. 9 Compatibility with Other Versions

More information

Introduction. Lecture 5 Files and Streams FILE * FILE *

Introduction. Lecture 5 Files and Streams FILE * FILE * Introduction Lecture Files and Streams C programs can store results & information permanently on disk using file handling functions These functions let you write either text or binary data to a file, and

More information

ODE IVP. An Ordinary Differential Equation (ODE) is an equation that contains a function having one independent variable:

ODE IVP. An Ordinary Differential Equation (ODE) is an equation that contains a function having one independent variable: Euler s Methods ODE IVP An Ordinary Differential Equation (ODE) is an equation that contains a function having one independent variable: The equation is coupled with an initial value/condition (i.e., value

More information

Lab # 02. Basic Elements of C++ _ Part1

Lab # 02. Basic Elements of C++ _ Part1 Lab # 02 Basic Elements of C++ _ Part1 Lab Objectives: After performing this lab, the students should be able to: Become familiar with the basic components of a C++ program, including functions, special

More information

PHYSICALLY BASED ANIMATION

PHYSICALLY BASED ANIMATION PHYSICALLY BASED ANIMATION CS148 Introduction to Computer Graphics and Imaging David Hyde August 2 nd, 2016 WHAT IS PHYSICS? the study of everything? WHAT IS COMPUTATION? the study of everything? OUTLINE

More information

pointers + memory double x; string a; int x; main overhead int y; main overhead

pointers + memory double x; string a; int x; main overhead int y; main overhead pointers + memory computer have memory to store data. every program gets a piece of it to use as we create and use more variables, more space is allocated to a program memory int x; double x; string a;

More information

Parallel implicit ordinary differential equation solver for cuda. Tomasz M. Kardaś

Parallel implicit ordinary differential equation solver for cuda. Tomasz M. Kardaś Parallel implicit ordinary differential equation solver for cuda Tomasz M. Kardaś August 11, 2014 Chapter 1 Parallel Implicit Ordinary Differential Equations Solver A simplest definition of stiffness,

More information

Lecture 5 Files and Streams

Lecture 5 Files and Streams Lecture 5 Files and Streams Introduction C programs can store results & information permanently on disk using file handling functions These functions let you write either text or binary data to a file,

More information

The Jello Cube Assignment 1, CSCI 520. Jernej Barbic, USC

The Jello Cube Assignment 1, CSCI 520. Jernej Barbic, USC The Jello Cube Assignment 1, CSCI 520 Jernej Barbic, USC 1 The jello cube Undeformed cube Deformed cube The jello cube is elastic, Can be bent, stretched, squeezed,, Without external forces, it eventually

More information

CVEN Computer Applications in Engineering and Construction. Programming Assignment #2 Random Number Generation and Particle Diffusion

CVEN Computer Applications in Engineering and Construction. Programming Assignment #2 Random Number Generation and Particle Diffusion CVE 0-50 Computer Applications in Engineering and Construction Programming Assignment # Random umber Generation and Particle Diffusion Date distributed: 0/06/09 Date due: 0//09 by :59 pm (submit an electronic

More information

Computational modeling

Computational modeling Computational modeling Lecture 3 : Random variables Theory: 1 Random variables Programming: 1 Implicit none statement 2 Modules 3 Outputs 4 Functions 5 Conditional statement Instructor : Cedric Weber Course

More information

Call-by-Type Functions in C++ Command-Line Arguments in C++ CS 16: Solving Problems with Computers I Lecture #5

Call-by-Type Functions in C++ Command-Line Arguments in C++ CS 16: Solving Problems with Computers I Lecture #5 Call-by-Type Functions in C++ Command-Line Arguments in C++ CS 16: Solving Problems with Computers I Lecture #5 Ziad Matni Dept. of Computer Science, UCSB Administrative CHANGED T.A. OFFICE/OPEN LAB HOURS!

More information

over The idea is to construct an algorithm to solve the IVP ODE (9.1)

over The idea is to construct an algorithm to solve the IVP ODE (9.1) Runge- Ku(a Methods Review of Heun s Method (Deriva:on from Integra:on) The idea is to construct an algorithm to solve the IVP ODE (9.1) over To obtain the solution point we can use the fundamental theorem

More information