Interactive Rendering with Coherent Ray Tracing
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
SGI® Octane III®
Making ® ® Supercomputing SGI Octane III Personal™ KEY FEATURES Supercomputing Gets Personal Octane III takes high-performance computing out Office Ready of the data center and puts it at the deskside. It A pedestal, one foot by two combines the immense power and performance broad HPC application support and arrives ready foot form factor and capabilities of a high-performance cluster with the for immediate integration for a smooth out-of-the- quiet operation portability and usability of a workstation to enable box experience. a new era of personal innovation in strategic science, research, development and visualization. Octane III allows a wide variety of single and High Performance dual-socket node choices and a wide selection of Up to 120 high- In contrast with standard dual-processor performance, storage, integrated networking, and performance cores and workstations with only eight cores and moderate graphics and compute GPU options. The system nearly 2TB of memory memory capacity, the superior design of is available as an up to ten node deskside cluster Broad HPC Application Octane III permits up to 120 high-performance configuration or dual-node graphics workstation Support cores and nearly 2TB of memory. Octane III configurations. Accelerated time-to-results significantly accelerates time-to-results for over with support for over 50 50 HPC applications and supports the latest Supported operating systems include: ® ® ® HPC applications Intel processors to capitalize on greater levels SUSE Linux Enterprise Server and Red Hat of performance, flexibility and scalability. Pre- Enterprise Linux. All configurations are available configured with system software, cluster set up is with pre-loaded SGI® Performance Suite system Ease of Use a breeze. -
OCTANE Technical Report
OCTANE Technical Report Silicon Graphics, Inc. ANY DUPLICATION, MODIFICATION, DISTRIBUTION, PUBLIC PERFORMANCE, OR PUBLIC DISPLAY OF THIS DOCUMENT WITHOUT THE EXPRESS WRITTEN CONSENT OF SILICON GRAPHICS, INC. IS STRICTLY PROHIBITED. THE RECEIPT OR POSSESSION OF THIS DOCUMENT DOES NOT CONVEY ANY RIGHTS TO REPRODUCE, DISCLOSE OR DISTRIBUTE ITS CONTENTS, OR TO MANUFACTURE, USE, OR SELL ANYTHING THAT IT MAY DESCRIBE, IN WHOLE OR IN PART. Cop VED Table of Contents Section 1 Introduction .....................................................................................................1-1 1.1 Manufacturing.............................................................................................................. 1-3 1.1.1 Industrial Design .....................................................................................1-3 1.1.2 CAD/CAM Solid Modeling ....................................................................1-4 1.1.3 Analysis...................................................................................................1-5 1.1.4 Digital Prototyping..................................................................................1-6 1.2 Entertainment............................................................................................................... 1-8 1.2.1 3D Animation..........................................................................................1-8 1.2.2 Film/Video/Audio ...................................................................................1-9 1.2.3 Publishing..............................................................................................1-10 -
The Shallow Water Wave Ray Tracing Model SWRT
The Shallow Water Wave Ray Tracing Model SWRT Prepared for: BMT ARGOSS Our reference: BMTA-SWRT Date of issue: 20 Apr 2016 Prepared for: BMT ARGOSS The Shallow Water Wave Ray Tracing Model SWRT Document Status Sheet Title : The Shallow Water Wave Ray Tracing Model SWRT Our reference : BMTA-SWRT Date of issue : 20 Apr 2016 Prepared for : BMT ARGOSS Author(s) : Peter Groenewoud (BMT ARGOSS) Distribution : BMT ARGOSS (BMT ARGOSS) Review history: Rev. Status Date Reviewers Comments 1 Final 20 Apr 2016 Ian Wade, Mark van der Putte and Rob Koenders Information contained in this document is commercial-in-confidence and should not be transmitted to a third party without prior written agreement of BMT ARGOSS. © Copyright BMT ARGOSS 2016. If you have questions regarding the contents of this document please contact us by sending an email to [email protected] or contact the author directly at [email protected]. 20 Apr 2016 Document Status Sheet Prepared for: BMT ARGOSS The Shallow Water Wave Ray Tracing Model SWRT Contents 1. INTRODUCTION ..................................................................................................................... 1 1.1. MODEL ENVIRONMENTS .............................................................................................................. 1 1.2. THE MODEL IN A NUTSHELL ......................................................................................................... 1 1.3. EXAMPLE MODEL CONFIGURATION OFF PANAMA ......................................................................... -
General Optics Design Part 2
GENERAL OPTICS DESIGN PART 2 Martin Traub – Fraunhofer ILT [email protected] – Tel: +49 241 8906-342 © Fraunhofer ILT AGENDA Raytracing Fundamentals Aberration plots Merit function Correction of optical systems Optical materials Bulk materials Coatings Optimization of a simple optical system, evaluation of the system Seite 2 © Fraunhofer ILT Why raytracing? • Real paths of rays in optical systems differ more or less to paraxial paths of rays • These differences can be described by Seidel aberrations up to the 3rd order • The calculation of the Seidel aberrations does not provide any information of the higher order aberrations • Solution: numerical tracing of a large number of rays through the optical system • High accuracy for the description of the optical system • Fast calculation of the properties of the optical system • Automatic, numerical optimization of the system Seite 3 © Fraunhofer ILT Principle of raytracing 1. The system is described by a number of surfaces arranged between the object and image plane (shape of the surfaces and index of refraction) 2. Definition of the aperture(s) and the ray bundle(s) launched from the object (field of view) 3. Calculation of the paths of all rays through the whole optical system (from object to image plane) 4. Calculation and analysis of diagrams suited to describe the properties of the optical system 5. Optimizing of the optical system and redesign if necessary (optics design is a highly iterative process) Seite 4 © Fraunhofer ILT Sequential vs. non sequential raytracing 1. In sequential raytracing, the order of surfaces is predefined very fast and efficient calculations, but mainly limited to imaging optics, usually 100..1000 rays 2. -
Computing @SERC Resources,Services and Policies
Computing @SERC Resources,Services and Policies R.Krishna Murthy SERC - An Introduction • A state-of-the-art Computing facility • Caters to the computing needs of education and research at the institute • Comprehensive range of systems to cater to a wide spectrum of computing requirements. • Excellent infrastructure supports uninterrupted computing - anywhere, all times. SERC - Facilities • Computing - – Powerful hardware with adequate resources – Excellent Systems and Application Software,tools and libraries • Printing, Plotting and Scanning services • Help-Desk - User Consultancy and Support • Library - Books, Manuals, Software, Distribution of Systems • SERC has 5 floors - Basement,Ground,First,Second and Third • Basement - Power and Airconditioning • Ground - Compute & File servers, Supercomputing Cluster • First floor - Common facilities for Course and Research - Windows,NT,Linux,Mac and other workstations Distribution of Systems - contd. • Second Floor – Access Stations for Research students • Third Floor – Access Stations for Course students • Both the floors have similar facilities Computing Systems Systems at SERC • ACCESS STATIONS *SUN ULTRA 20 Workstations – dual core Opteron 4GHz cpu, 1GB memory * IBM INTELLISTATION EPRO – Intel P4 2.4GHz cpu, 512 MB memory Both are Linux based systems OLDER Access stations * COMPAQ XP 10000 * SUN ULTRA 60 * HP C200 * SGI O2 * IBM POWER PC 43p Contd... FILE SERVERS 5TB SAN storage IBM RS/6000 43P 260 : 32 * 18GB Swappable SSA Disks. Contd.... • HIGH PERFORMANCE SERVERS * SHARED MEMORY MULTI PROCESSOR • IBM P-series 690 Regatta (32proc.,256 GB) • SGI ALTIX 3700 (32proc.,256GB) • SGI Altix 350 ( 16 proc.,16GB – 64GB) Contd... * IBM SP3. NH2 - 16 Processors WH2 - 4 Processors * Six COMPAQ ALPHA SERVER ES40 4 CPU’s per server with 667 MHz. -
OCTANE® Workstation Owner's Guide
OCTANE® Workstation Owner’s Guide Document Number 007-3435-003 CONTRIBUTORS Written by Charmaine Moyer Production by Linda Rae Sande Illustrated by Kwong Liew Engineering contributions by Jim Bergman, Brian Bolich, Bob Cook, Mark Glusker, John Hahn, Steve Manzi, Ted Marsh, Donna McMaster, Jim Pagura, Michael Poimboeuf, Brad Reger, Jose Reinoso, Bob Sanders, Chris Wheaton, Michael Wright, and many others on the OCTANE engineering and business team. St. Peter’s Basilica image courtesy of ENEL SpA and InfoByte SpA. Disk Thrower image courtesy of Xavier Berenguer, Animatica. © 1997 - 1999, Silicon Graphics, Inc.— All Rights Reserved The contents of this document may not be copied or duplicated in any form, in whole or in part, without the prior written permission of Silicon Graphics, Inc. LIMITED AND RESTRICTED RIGHTS LEGEND Use, duplication, or disclosure by the Government is subject to restrictionsas set forth in the Rights in Data clause at FAR 52.227-14 and/or in similar orsuccessor clauses in the FAR, or in the DOD, DOE or NASA FAR Supplements.Unpublished rights reserved under the Copyright Laws of the United States.Contractor/manufacturer is Silicon Graphics, Inc., 2011 N. Shoreline Blvd., Mountain View, CA 94043-1389. Silicon Graphics, IRIS, IRIX, and OCTANE are registered trademarks and the Silicon Graphics logo, IRIX Interactive Desktop, Power Fortran Accelerator, IRIS InSight, and Stereoview are trademarks of Silicon Graphics, Inc. ADAT is a registered trademark of Alesis Corporation. Centronics is a registered trademark of Centronics Data Computer Corporation. Envi-ro-tech is a trademark of TECHSPRAY. Macintosh is a registered trademark of Apple Computer, Inc. -
Light Refraction with Dispersion Steven Cropp & Eric Zhang
Light Refraction with Dispersion Steven Cropp & Eric Zhang 1. Abstract In this paper we present ray tracing and photon mapping methods to model light refraction, caustics, and multi colored light dispersion. We cover the solution to multiple common implementation difficulties, and mention ways to extend implementations in the future. 2. Introduction Refraction is when light rays bend at the boundaries of two different mediums. The amount light bends depends on the change in the speed of the light between the two mediums, which itself is dependent on a property of the materials. Every material has an index of refraction, a dimensionless number that describes how light (or any radiation) travels through that material. For example, water has an index of refraction of 1.33, which means light travels 33 percent slower in water than in a vacuum (which has the defining index of refraction of 1). Refraction is described by Snell’s Law, which calculates the new direction of the light ray based on the ray’s initial direction, as well as the two mediums it is exiting and entering. Chromatic dispersion occurs when a material’s index of refraction is not a constant, but a function of the wavelength of light. This causes different wavelengths, or colors, to refract at slightly different angles even when crossing the same material border. This slight variation splits the light into bands based on wavelength, creating a rainbow. This phenomena can be recreated by using a Cauchy approximation of an object’s index of refraction. 3. Related Work A “composite spectral model” was proposed by Sun et al. -
Bright-Field Microscopy of Transparent Objects: a Ray Tracing Approach
Bright-field microscopy of transparent objects: a ray tracing approach A. K. Khitrin1 and M. A. Model2* 1Department of Chemistry and Biochemistry, Kent State University, Kent, OH 44242 2Department of Biological Sciences, Kent State University, Kent, OH 44242 *Corresponding author: [email protected] Abstract Formation of a bright-field microscopic image of a transparent phase object is described in terms of elementary geometrical optics. Our approach is based on the premise that image replicates the intensity distribution (real or virtual) at the front focal plane of the objective. The task is therefore reduced to finding the change in intensity at the focal plane caused by the object. This can be done by ray tracing complemented with the requirement of conservation of the number of rays. Despite major simplifications involved in such an analysis, it reproduces some results from the paraxial wave theory. Additionally, our analysis suggests two ways of extracting quantitative phase information from bright-field images: by vertically shifting the focal plane (the approach used in the transport-of-intensity analysis) or by varying the angle of illumination. In principle, information thus obtained should allow reconstruction of the object morphology. Introduction The diffraction theory of image formation developed by Ernst Abbe in the 19th century remains central to understanding transmission microscopy (Born and Wolf, 1970). It has been less appreciated that certain effects in transmission imaging can be adequately described by geometrical, or ray optics. In particular, the geometrical approach is valid when one is interested in features significantly larger than the wavelength. Examples of geometrical description include explanation of Becke lines at the boundary of two media with different refractive indices (Faust, 1955) or the axial scaling effect (Visser et al, 1992). -
Reflections and Refractions in Ray Tracing
Reflections and Refractions in Ray Tracing Bram de Greve ([email protected]) November 13, 2006 Abstract materials could be air (η ≈ 1), water (20◦C: η ≈ 1.33), glass (crown glass: η ≈ 1.5), ... It does not matter which refractive index is the greatest. All that counts is that η is the refractive When writing a ray tracer, sooner or later you’ll stumble 1 index of the material you come from, and η of the material on the problem of reflection and transmission. To visualize 2 you go to. This (very important) concept is sometimes misun- mirror-like objects, you need to reflect your viewing rays. To derstood. simulate a lens, you need refraction. While most people have heard of the law of reflection and Snell’s law, they often have The direction vector of the incident ray (= incoming ray) is i, difficulties with actually calculating the direction vectors of and we assume this vector is normalized. The direction vec- the reflected and refracted rays. In the following pages, ex- tors of the reflected and transmitted rays are r and t and will actly this problem will be addressed. As a bonus, some Fres- be calculated. These vectors are (or will be) normalized as nel equations will be added to the mix, so you can actually well. We also have the normal vector n, orthogonal to the in- calculate how much light is reflected or transmitted (yes, it’s terface and pointing towards the first material η1. Again, n is possible). At the end, you’ll have some usable formulas to use normalized. -
Efficient Ray-Tracing Algorithms for Radio Wave Propagation in Urban Environments
Efficient Ray-Tracing Algorithms for Radio Wave Propagation in Urban Environments Sajjad Hussain BSc. MSc. Supervisor: Dr. Conor Brennan School of Electronic Engineering Dublin City University This dissertation is submitted for the degree of Doctor of Philosophy September 2017 To my parents for their love and encouragement, my loving and supportive wife Akasha for always standing beside me and our beautiful son Muhammad Hashir. Declaration I hereby certify that this material, which I now submit for assessment on the programme of study leading to the award of PhD is entirely my own work, and that I have exercised reasonable care to ensure that the work is original, and does not to the best of my knowl- edge breach any law of copyright, and has not been taken from the work of others save and to the extent that such work has been cited and acknowledged within the text of my work. Signed: ID No.: 13212215 Date: 05/09/2017 Acknowledgements I would like to express special appreciation and thanks to my supervisor, Dr. Conor Brennan, for his continuous support and confidence in my work. His patience and encouragement were invaluable to me throughout the course of my PhD. He pushed me to perform to the best of my abilities. I would also like to thank my examiners, Dr. Jean-Frédéric and Dr. Prince Anandarajah for their brilliant comments and suggestions that has really improved the quality of this thesis. I would especially like to thank my colleagues including Ian Kavanagh, Vinh Pham-Xuan and Dung Trinh-Xuan for their help and support. -
More Ray Tracing
i i i i 13 More Ray Tracing A ray tracer is a great substrate on which to build all kinds of advanced rendering effects. Many effects that take significant work to fit into the object-order ras- terization framework, including basics like the shadows and reflections already presented in Chapter 4, are simple and elegant in a ray tracer. In this chapter we discuss some fancier techniques that can be used to ray-trace a wider variety of scenes and to include a wider variety of effects. Some extensions allow more gen- eral geometry: instancing and constructive solid geometry (CSG) are two ways to make models more complex with minimal complexity added to the program. Other extensions add to the range of materials we can handle: refraction through transparent materials, like glass and water, and glossy reflections on a variety of surfaces are essential for realism in many scenes. This chapter also discusses the general framework of distribution ray trac- ing (Cook et al., 1984), a powerful extension to the basic ray-tracing idea in which multiple random rays are sent through each pixel in an image to produce images with smooth edges and to simply and elegantly (if slowly) produce a wide range of effects from soft shadows to camera depth-of-field. If you start with a brute- force ray intersection loop, The price of the elegance of ray tracing is exacted in terms of computer time: you’ll have ample time to most of these extensions will trace a very large number of rays for any non-trivial implement an acceleration scene. -
AVS on UNIX WORKSTATIONS INSTALLATION/ RELEASE NOTES
_________ ____ AVS on UNIX WORKSTATIONS INSTALLATION/ RELEASE NOTES ____________ Release 5.5 Final (50.86 / 50.88) November, 1999 Advanced Visual Systems Inc.________ Part Number: 330-0120-02 Rev L NOTICE This document, and the software and other products described or referenced in it, are con®dential and proprietary products of Advanced Visual Systems Inc. or its licensors. They are provided under, and are subject to, the terms and conditions of a written license agreement between Advanced Visual Systems and its customer, and may not be transferred, disclosed or otherwise provided to third parties, unless oth- erwise permitted by that agreement. NO REPRESENTATION OR OTHER AFFIRMATION OF FACT CONTAINED IN THIS DOCUMENT, INCLUDING WITHOUT LIMITATION STATEMENTS REGARDING CAPACITY, PERFORMANCE, OR SUI- TABILITY FOR USE OF SOFTWARE DESCRIBED HEREIN, SHALL BE DEEMED TO BE A WARRANTY BY ADVANCED VISUAL SYSTEMS FOR ANY PURPOSE OR GIVE RISE TO ANY LIABILITY OF ADVANCED VISUAL SYSTEMS WHATSOEVER. ADVANCED VISUAL SYSTEMS MAKES NO WAR- RANTY OF ANY KIND IN OR WITH REGARD TO THIS DOCUMENT, INCLUDING BUT NOT LIMITED TO, THE IMPLIED WARRANTIES OF MERCHANTABILITY AND FITNESS FOR A PARTICULAR PUR- POSE. ADVANCED VISUAL SYSTEMS SHALL NOT BE RESPONSIBLE FOR ANY ERRORS THAT MAY APPEAR IN THIS DOCUMENT AND SHALL NOT BE LIABLE FOR ANY DAMAGES, INCLUDING WITHOUT LIMI- TATION INCIDENTAL, INDIRECT, SPECIAL OR CONSEQUENTIAL DAMAGES, ARISING OUT OF OR RELATED TO THIS DOCUMENT OR THE INFORMATION CONTAINED IN IT, EVEN IF ADVANCED VISUAL SYSTEMS HAS BEEN ADVISED OF THE POSSIBILITY OF SUCH DAMAGES. The speci®cations and other information contained in this document for some purposes may not be com- plete, current or correct, and are subject to change without notice.