61. Geometry And General Principles Envisat Home, 05 Nov 2002. Characteristics. Instruments and Systems. geometryand general Principles. News on geometry and general Principles. http://envisat.esa.int/instruments/mipas/descr/charact/geo-princip.html

You must have a javascript-enabled browser and javacript and stylesheets must be enabled to use some of the functions on this site. Mission and System Instruments Product Handbook User Services ... Envisat Home 08 Apr 2003 Characteristics Instruments and Systems Geometry and General Principles News on... ERS Mission Envisat Mission Images Applications User Services NEWS ARCHIVE Search: Advanced Search Glossary Sitemap FAQ ... Contact us Help on... Geometry and General Principles MIPAS is designed for limb observations to perform maximum sensitivity and good vertical resolution. The instantaneous field of view is only 3 km high to achieve a good vertical resolution, but 30-km-wide to collect sufficient radiance. The instrument is capable of performing measurements in two pointing regimes The instrument is capable of performing measurements in two pointing regimes: rearwards within a 35° wide range in the anti-flight direction, and sideways within a 30° wide area in the anti-sun direction. The rearward viewing range is used for most measurements, as it provides a good Earth coverage, including the polar regions. The sideways range is important for observation of special events, like volcano eruptions, trace-gas concentrations above major air traffic routes, or concentration gradients along the dusk/dawn lines. As a result of the limb viewing geometry, the distance between instrument and tangent point is about 3,300 km. Thus, in order to measure at a predetermined limb height, the pointing of instrument and satellite in elevation direction must be excellent. It is a goal to determine the geometric limb height by pointing information from the spacecraft with a standard deviation below 600 m. Thus, line-of-sight-pointing knowledge with respect to nadir of better than 0.01° (1-sigma) is required. A very high stability of all assemblies affecting the pointing is a design driver for MIPAS as well as for the Envisat satellite.

62. Spacetime And Geometry: An Introduction To General Relativity - Addison Wesley / Features. Appropriate Courses. About the Author(s). RELATED TITLES. Relativity (Physics/Astronomy).Spacetime and geometry An Introduction to general Relativity. http://www.aw.com/catalog/academic/product/1,4096,0805387323,00.html

Find Your Rep Publish with Us Customer Service Careers ... Statistics ABOUT THIS PRODUCT Description Table of Contents Features Appropriate Courses About the Author(s) RELATED TITLES Relativity (Physics/Astronomy) Spacetime and Geometry: An Introduction to General Relativity View Larger Image Sean Carroll University of Chicago ISBN: 0-8053-8732-3 Publisher: Benjamin Cummings Format: Cloth; 750 pp Status: Not Yet Published; Estimated Availability: US: $80.00 You Save: $8.00 (10% off) Our Price: $72.00 Instructor Exam Copy Description Spacetime and Geometry: An Introduction to General Relativity provides a lucid and thoroughly modern introduction to general relativity for advanced undergraduates and graduate students. It introduces modern techniques and an accessible and lively writing style to what can often be a formal and intimidating subject. Readers are led from physics of flat spacetime (special relativity), through the intricacies of differential geometry and Einstein's equations, and on to exciting applications such as black holes, gravitational radiation, and cosmology. Subtle points are illuminated throughout the text by careful and entertaining exposition. A straightforward and lucid approach, balancing mathematical rigor and physical insight, are hallmarks of this important text. AW Higher Education Group , a division of Pearson Education , a Pearson . E-mail webmaster@awl.com

63. Applications To Engineering Design Of The General Geometry, Applications To Engineering Design Of The general geometry, Grid Analysis (GGA) Object In DT_NURBS. leaps Naval Surface Warfare http://ocean.dt.navy.mil/dtnurbs/gga_ms.htm

leaps Naval Surface Warfare Center, Carderock Div., David Taylor Model Basin David Ferguson Boeing Information and Support Services Abstract The DT_NURBS spline geometry subroutine library is a Non-Uniform Rational B-spline library developed with the goal of providing a common mathematical base for integrating geometrically dependent analysis tools with design geometry; and as a tool for use in the development of multi-disciplinary applications. In this paper we will describe the approach taken with the DT_NURBS library, the basic library entities themselves and how they can be used to affect the integration of diverse geometries and analyses. Introduction The basic assumption for using the DT_NURBS math model for the integration of multi-disciplinary analysis is that design and the exchange of information between design disciplines are fundamentally dependent on geometry. That assumption is particularly true for non-empirical, first principle based design. Complicating integration is the fact that analysis processes are unique to each design discipline and consequently the integration of information between disciplines is at best an afterthought and often is considered too difficult to implement. It is also argued that individual disciplines require too much unique methodology to allow for integration without compromise. It is true that individual disciplines need to make use of the best methods for its problems but it will be shown that integration is possible through the use of new and expanded mathematical modeling techniques without compromising solution methods.

64. Double Precision Geometry: A General Technique For Calculating Line And Segment Double Precision geometry A general Technique for Calculating Line and SegmentIntersections Using Rounded Arithmetic (1989) (Make Corrections) (34 citations http://citeseer.nj.nec.com/milenkovic89double.html

Double Precision Geometry: A General Technique for Calculating Line and Segment Intersections Using Rounded Arithmetic (1989) (Make Corrections) (34 citations) Victor Milenkovic IEEE Symposium on Foundations of Computer Science Home/Search Context Related View or download: miami.edu/~vjm/Papers/focs89.ps.gz Cached: PS.gz PS PDF DjVu ... Help From: miami.edu/~vjm/papers (more) Homepages: V.Milenkovic HPSearch (Update Links) Rate this article: (best) Comment on this article (Enter summary) Abstract: This paper describes part of such a theory and its expected payoff, robust approximate geometric algorithms with faster running times than the best exact versions. A theory of robust geometry requires an understanding of the precision requirements of exact algorithms: the number of bits P of arithmetic precision required for each arithmetic operation, expressed as a function of the arithmetic precision N of the input. For a line, N is the number of bits used to express each of the coefficients... (Update) Context of citations to this paper: More ...the fuzzy term quasi robust, which I apply to any algorithm whose output is somehow provably distinguishable from nonsense.

65. The General Relativity And Geometry Phil.spacetime. The general Relativity and geometry. Third Assignment, dueDecember 4 (Tue.). ? http://www.bun.kyoto-u.ac.jp/~suchii/GRgeometry.html

Phil.spacetime The General Relativity and Geometry Third Assignment, due December 4 (Tue.) In classical mechanics, as well as in the special theory of relativity, the coordinates of space and time have a direct physical meaning. To say that a point-event has the X_1 coordinate x_1 means that the projection of the point-event on the axis of X_1, determined by rigid rods and in accordance with the rules of Euclidean geometry, is obtained by measuring off a given rod (the unit length) x_1 times from the origin of coordinates along the axis of X_1. To say that a point-event has the X_4 coordinate x_4 = t, means that a standard clock, made to measure time in a definite unit period, and which is stationary relatively to the system of co-ordinates and practically coincident in space with the point-event, will have measured off x_4 = t periods at the occurrence of the event. (Einstein 1916, 773-4) Einstein (1916), "Die Grundlage der allgemeinen Relativitaetstheorie", Annalen der Physik 49 (1916), 769-822. [English translation

66. P4 PARALLELIZATION OF GENERAL GEOMETRY RAY TRACING IN COMPUTATIONAL PHYSICS P4 PARALLELIZATION OF general geometry RAY TRACING IN COMPUTATIONAL PHYSICS.Steve M. Slater and Jasmina L. Vujic Department of Nuclear http://www.nuc.berkeley.edu/neutronics/papers/hpc94/hpc94.html

P4 PARALLELIZATION OF GENERAL GEOMETRY RAY TRACING IN COMPUTATIONAL PHYSICS Steve M. Slater and Jasmina L. Vujic Department of Nuclear Engineering University of California Berkeley, California 94720 ABSTRACT INTRODUCTION The solution of the Boltzmann transport equation for the neutron distribution in a nuclear reactor remains one of the most computationally-intensive applications in engineering and science. A three-dimensional (3D) transport analysis of the entire reactor core is still beyond the capability of current machines (and algorithms), but with the use of workstations as nodes in a distributed computing environment, we are getting ready to attack this large-scale problem. Although in this paper we present results for two-dimensional (2D) single assembly problems, the methodology can be naturally extended to 3D large-scale applications. The exact collision probability formalism is used in the GTRAN2 code (Vujic 1993) to solve the multigroup integral transport equation in general 2D geometries. Combinatorial geometry (CG) is used to describe complex and irregular configurations in one, two, or three dimensions. A modified CG processor is used to perform ray tracing needed for numerical calculation of the collision/transfer probability (CTP) matrices. Thus, GTRAN2 is a unique combination of the computational efficiency of the deterministic code and the geometric flexibility of Monte Carlo codes. To obtain the discretized integral transport equations for two-dimensional geometry, the area A and boundary L are partitioned into Nr subareas (zones) and Nb subboundaries, respectively, such that

67. The Geometry Of Optimal Control 1. Title page. 2. Model. 3. Optimising cost. 4. general problem. 5. Assumptions.6. Questions. 7. Optimal values. 8. Topviews. 11. Topview animated. 12. Uniqueness.13. http://www.enm.bris.ac.uk/staff/hinke/Talks/Bath/general.html

Title page Model Optimising cost General problem ... 5D visualisation Problem formulation J x inf u q x t x u t d t x' t f x t x u t x x x Assumptions Vector field f is C and linearly controllable about Incremental cost q is C and quadratically positive definite Linear quadratic approximation is nice Optimal value function V lin x x T P x where P

68. Geometry Topology Mathematics Topics In General Topology Kiiti Morita geometry Topology Mathematics Topics in general Topology Kiiti Morita. Subjectgeometry Topology Mathematics Title Topics in general Topology http://www.lyricsbox.co.uk/Kiiti-Morita-Topics-in-General-Topolog-0444704558.htm

Geometry Topology Mathematics Topics in General Topology Kiiti Morita Subject: Geometry Topology Mathematics Title: Topics in General Topology Author: Kiiti Morita Murat R Sertel Workers' Enterp... Jeffrey H Bergstrand Changing ... Gordon W Arbuthnott Chemical S... A Knoester Tinbergen Lectures ... ... Jammers Antonius, Klemp Egon...

69. XIII Geometry Festival - Connections In Modern Mathematics And Physics Much of Simons' work can be collected under the general rubric of the theory of connections.Over this century, connections in differential geometry have come http://www.math.sunysb.edu/events/simons/general.html

Speakers Schedule Registration Accommodations ... Transportation Connections in Modern Mathematics and Physics Stony Brook, April 2-5, 1998 GENERAL INFORMATION This special year of the Geometry Festival will be concerned with the theory of connections and its role in recent developments in mathematics and physics. Topics to be covered will include: Developments in gauge theory such as Seiberg-Witten theory and Floer cohomology. Secondary invariants in topology including the perturbative invariants for 3-manifolds and links arising from the Chern-Simons functional. Secondary invariants in geometry - Index Theory including higher eta-invariants, adiabatic limits, holomorphic torsion, etc. Secondary Invariants in algebra and number theory including the refined Riemann-Roch Theorem in Arakelov theory.

70. Geometry Festival Home Page -- GENERAL INFORMATION SUPPORT general INFORMATION. The 12th geometry Festival will be heldMarch 1416, 1997 at Duke University, Durham, North Carolina. http://www.math.duke.edu/conferences/geomfest97/geomfest_1.html

Go up to Top Go forward to REGISTRATION, FEES, and SUPPORT GENERAL INFORMATION The 12th Geometry Festival will be held March 14-16, 1997 at Duke University, Durham, North Carolina. The conference will survey some recent developments in Geometry, with the goal of communicating these ideas to a broad mathematical audience. PLEASE NOTE THAT THE REGISTRATION DEADLINE IS MARCH 7. You must register before March 7 if you wish to attend the pizza supper or the banquet, to receive support, or to receive assistance in making hotel arrangements. An informal supper, pizza and beer (and soft drinks, of course), will be available at the hotel after the last talk on Friday evening. A banquet is scheduled for the evening of Saturday, March 15. A light breakfast Saturday and Sunday mornings, lunch on Saturday, as well as refreshments during breaks will be provided. The Friday afternoon talk will be held at the Regal University Hotel, as will the supper that evening. The Saturday and Sunday talks will be held in Physics 114 on the Duke campus (The mathematics department is in the Physics building). The banquet on Saturday night will be held at the Regal University Hotel. THE SPEAKERS Jeanne Nielsen Clelland (IAS)

71. CM334Z   -   Space-Time Geometry And General Relativity CM334Z SpaceTime geometry and general Relativity. Semester 2. LecturerDr GMT Watts. The files are in ACROBAT (.pdf) form. Just click http://www.mth.kcl.ac.uk/courses/cm334z.html

CM334Z Space-Time Geometry and General Relativity Semester 2 Lecturer: Dr G M T Watts The files are in ACROBAT (.pdf) form. Just click on the item which interests you to open the acrobat reader, with which you can view and print the file. Information Sheet Course information and outline syllabus Guidelines for the course and tutorials/problem classes Lecture Notes Section 1 All of section 1 Lecture 1 Lecture 2 Lecture 3 ... Lecture 4 Section 2 All of section 2 Lecture 5 Lecture 6 Lecture 7 ... Lecture 10 (part 1) Section 3 All of section 3 Lecture 10 (part 2) Lecture 11 Lecture 12 Section 4 All of section 4 Revised version Section 5 All of section 5 Section 6 All of section 6 Exercises Exercise sheet 1 and the solutions Exercise sheet 2 and the solutions Exercise sheet 3 and the solutions Exercise sheet 4 Exercise sheet 5 Exercise sheet 6 Extra information Past exam papers: Gravitational Lenses: Some colour pictures of the slide shown in class: gif format (179 kb) or jpg format (75 kb) and the text to go with it. A Hubble space telescope site , where these pictures came from. A site specialising in gravitational lenses Edit this page [Return to: List of courses Dept. home page

72. GRTensorII Demonstrations-General Relativity & Geometry. Classical Problems In Computer Algebra; general Relativity; geometry in ThreeDimensions; geometry in Five Dimensions. Classical Problems In Computer Algebra. http://grtensor.phy.queensu.ca/NewDemo/demo.html

Page Index Introduction to GRTensorII mws html pdf (restricted to the Schwarzschild spacetime) Classical Problems In Computer Algebra General Relativity Geometry in Three Dimensions Geometry in Five Dimensions Classical Problems In Computer Algebra Bondi Metric The Bondi metric ( Proc. Roy. Soc. 21) plays an interesting role in the history of algebraic computing in general relativity (see d'Invero in General Relativity and Gravitation ed. A. Held ISBN 0-306-40265-3 (v. 1)). Demonstration 1 (bondi): One step calculation of the covariant Riemann, Ricci and Einstein tensors for the Bondi metric. (This calculation, which once took from 10 to 1000 seconds of computation time on mainframe computers, now runs in less than 1 second on a common PC in many, but not all, computer algebra systems.) bondig1.mpl bondi.mws bondi.html bondi.pdf Ricci Tensor-Number of terms. The idea is to calculate the number of terms in the covariant Ricci tensor in n dimensions. The most general form of the metric tensor is used, that is n(n+1)/2 functions of n variables. The number of terms grows rapidly with n (see G.J. Fee, R.G. McLenaghan and R. Pavelle GR12 Contributed Papers Dimension Diagonal components Off-diagonal components In the following examples the same worksheet is used in each dimension. Whereas n=4 can now be handled on most PCs

73. Kerr Newman Geometry (was Re: General Relativity Vs Flat Minkowski Space Date PrevDate NextThread PrevThread NextDate IndexThread Index KerrNewman geometry (was Re general relativity vs flat Minkowski spacetime). http://www.lns.cornell.edu/spr/1999-10/msg0018904.html

Date Prev Date Next Thread Prev Thread Next ... Thread Index Kerr Newman Geometry (was Re: General relativity vs flat Minkowski spacetime) Subject : Kerr Newman Geometry (was Re: General relativity vs flat Minkowski spacetime) From Date : 22 Oct 1999 00:00:00 GMT Approved : baez@math.ucr.edu Newsgroups : sci.physics.research Organization : University of Cambridge, England References Pine.OSF.4.02A.9910150334230.14136-100000@goedel1.math.washington.edu 380e1907.58323799@news.gte.net Pine.OSF.4.02A.9910202028180.1553-100000@goedel1.math.washington.edu http://www.mrao.cam.ac.uk/~clifford/publications/ However, in higher dimensions, there is no Kerr-Schild form for the Kerr-Newman solution whereas there is one for the higher dimensional Kerr found by Myers and Perry. The reason is because the Kerr Newman solution possess no-known symmetries that is similar to the one in 4d. The Kerr Newman in 4 dimensions is very unique because it can be cast in the Kerr-Schild form. For 13 years, till now, no one has found the Kerr Newman solution in higher dimensions in classical GR, so if anyone thinking of solving a big time problem, I will be happy to discuss this problem, since I have tried many methods to deal with the problem and failed. Thank you and best regards. yours sincerely, Bernard Leong http://www.geocities.com/bleongcw

74. Re: Kerr Newman Geometry (was Re: General Relativity Vs Flat Re Kerr Newman geometry (was Re general relativity vs flat. Prev by thread KerrNewman geometry (was Re general relativity vs flat Minkowski spacetime); http://www.lns.cornell.edu/spr/1999-10/msg0018956.html

Date Prev Date Next Thread Prev Thread Next ... Thread Index Re: Kerr Newman Geometry (was Re: General relativity vs flat Subject : Re: Kerr Newman Geometry (was Re: General relativity vs flat From Date : 25 Oct 1999 00:00:00 GMT Approved : spr@rosencrantz.stcloudstate.edu (sci.physics.research) Minkowski spacetime) Newsgroups : sci.physics.research Organization : University of Washington References Pine.OSF.4.02A.9910150334230.14136-100000@goedel1.math.washington.edu 380e1907.58323799@news.gte.net Pine.OSF.4.02A.9910202028180.1553-100000@goedel1.math.washington.edu Pine.SO4.4.05.9910221327550.18173-100000@mraos.ra.phy.cam.ac.uk ... http://www.math.washington.edu/~hillman/personal.html References Re: General relativity vs flat Minkowski spacetime From: Re: General relativity vs flat Minkowski spacetime From: dmorgan@suenet.qa.net.astro.rug.nl (Dale Morgan) Re: General relativity vs flat Minkowski spacetime From: Kerr Newman Geometry (was Re: General relativity vs flat Minkowski spacetime) From: Prev by Date: Re: How It Might Affect Me Next by Date: Q: Color of neutron stars Prev by thread: Kerr Newman Geometry (was Re: General relativity vs flat Minkowski spacetime) Next by thread: Re: General relativity vs flat Minkowski spacetime Index(es): Date Thread

75. Geometry - General Triangle Solver The general TriangleApplet is a simple triangle solver that is easy to use. general Triangles.......METools Mechanical Engineering Tools Version 1.0. http://www.metools.com/index_page0039.htm

Contact Us: METools - Mechanical Engineering Tools Version 1.0 Description: The General Triangle Applet is a simple triangle solver  that is easy to use. Just supply the knowns and press solve and if you have provided enough information, the unknowns appear. Links: None Details: In order to solve a triangle, you must supply three knows and one of those must be a side. Theory: Angles are solved using trigonometric identities and law of sines, sides are solved using law of cosines. Last Update: Build 1450, 02/20/2002 Known Bugs: Suggestions: No suggestions since last update. Remember that METools is a constantly evolving program where applets are added and modified regularly. If you do not see anything you are interested in, check back in a few weeks or send your suggestion to METools@att.net METools Directory General Triangles The General Triangle Applet is a dynamic applet that updates the conversion whenever a key is pressed or new unit selected. Where am I? Home Applet Directory Geometry        General Triangles Email: METools@att.net

76. Qt-interest Archive - General Question About Geometry Management Qtinterest Archive, April 1998 general question about geometry management.Message 1 in thread Subject general question about geometry http://lists.trolltech.com/qt-interest/1998-04/thread00126-0.html

Trolltech Home Qt-interest Home Recent Threads All Threads ... All threads index page 1 Qt-interest Archive, April 1998 General question about geometry management Message 1 in thread Subject : General question about geometry management From Date : Thu, 16 Apr 1998 20:33:02 -0500 (CDT) To qt-interest@xxxxxxxx http://www2.msstate.edu/~dmi1/index.html Message 2 in thread Subject : Re: General question about geometry management From Date : 17 Apr 1998 08:21:56 +0200 Cc qt-interest@xxxxxxxx To >>>>> "dmi1" == dmi1 <dmi1@Ra.MsState.Edu> writes: dmi1> If you create a dialog with geometry management, does it dmi1> automatically resize the individual widgets with the dialog is dmi1> resized? I need to make one of my widgets capable of resizing dmi1> horizontally and I'd rather not implement the resizing stuff dmi1> on my own (lazy). Yes. Marius Message 3 in thread Subject : Re: General question about geometry management From : "Daniel Solaz" < Date : Fri, 17 Apr 1998 05:09:59 +0200 Organization : (setq dsolaz NIL) Sender : "" <

77. NonEuclid - Hyperbolic Geometry Article + Software Applet NonEuclid is a Software Simulation offering Straightedge and Compass Constructionsin Hyperbolic geometry (a geometry of Einstein's general Relativity and http://www.rice.edu/projects/NonEuclid/NonEuclid.html

NonEuclid NonEuclid is a Software Simulation offering Straightedge and Compass Constructions in Hyperbolic Geometry (a geometry of Einstein's General Relativity Theory and Curved Hyperspace) for use in High School and Undergraduate Education. This web site provides the platform independent, NonEuclid software (written in 100% pure Java) together with a 25 page, illustrated, hypertext introductory explanation of Hyperbolic Geometry. NonEuclid has moved. The new site is: http://math.rice.edu/~joel/NonEuclid/

78. Advances In Differential Geometry And General Relativity The Beemfest Advances in Differential geometry and general Relativity.May 1011, 2003. University of Missouri-Columbia. On the occasion http://www.math.missouri.edu/~staff/conference/beem-conf.html

The Beemfest: Advances in Differential Geometry and General Relativity May 10-11, 2003 University of Missouri-Columbia On the occasion of Professor John Beem's Retirement INVITED SPEAKERS Lilia del Riego (Universidad Autonoma de San Luis Potosi) Tevian Dray (Oregon State University) Paul Ehrlich (University of Florida) Greg Galloway (University of Miami, Florida) Steve Harris (Saint Louis University) Ralph Howard (University of South Carolina) Andrzej Krolak (Polish Academy of Sciences) Phil Parker (Wichita State University) For information about Columbia, Missouri, accommodations, and how to get here: To travel to Columbia, please link to Canterbury Travel , the official travel agents of the conference. For directions on how to get to Columbia, follow this link Information: There is no formal application to attend the conference and there will be no registration fee. For more information e-mail Stamatis Dostoglou (University of Missouri at Columbia) stamatis@math.missouri.edu

79. Development Of A General Geometry Large Eddy Simulation Code, CB.01 Development of a general geometry Large Eddy Simulation Code,.Julia S. Mullen, Paul F. Fischer (Brown University). We present http://flux.aps.org/meetings/YR9596/BAPSDFD96/abs/S330001.html

Next abstract Session CB - L.E.S. ORAL session, Sunday afternoon, November 24 Ballroom W, OnCenter [CB.01] Development of a General Geometry Large Eddy Simulation Code, Julia S. Mullen, Paul F. Fischer (Brown University) We present a general geometry large eddy simulation (LES) code based upon three-dimensional spectral elements. We employ a two parameter PDE-motivated filter which can be tuned for both order and cut-off wave number, and which satisfies boundary conditions appropriate for complex geometry flows. The SGS terms are treated by the Lilly version of the dynamic subgrid scale model. The filter has been tested for complex geometry flows, including a horseshoe vortex flow in a flat-plate/appendage configuration. We have observed that the filter is capable of retaining the large structures, such as hairpin vortices, while removing the high energy ``noise'' in under-resolved regions. The SGS model and the filter described above have been combined into a full LES code. We are currently validating the code against 3-D channel flow benchmark results. Part C of program listing

80. User Documentation - General Geometry general geometry. Normal classes FAffineC, generalaffine transformation. Normal functions http://ravl.sourceforge.net/share/doc/RAVL/Auto/Basic/Tree/Ravl.Math.Geometry.ht

User Documentation RAVL, Recognition And Vision Library DEVELOP HOME PAGE CLASS LIST CONTENTS ... Math Geometry SUBTOPICS General geometry Normal classes: FAffineC General affine transformation. Normal functions: operator Advanced classes: FMatrixC Real Matrix with templated size. FVectorC Real Vector with templated size FPointC Real point with templated size Advanced functions: SolveIP(FMatrixC Solve a general linear system A*x = b Solve(const FMatrixC Solve a general linear system A*x = b SVD(const FMatrixC SVD_IP(FMatrixC SVD(const FMatrixC SVD_IP(FMatrixC ... EigenValues(FMatrixC Calculate the eigen values of a real symmetric matrix. EigenValuesIP(FMatrixC Calculate the eigen values of a real symmetric matrix. EigenVectors(FMatrixC Calculate the eigen values and vectors of a real symmetric matrix. EigenVectorsIP(FMatrixC Calculate the eigen values and vectors of a real symmetric matrix. MaxEigenValue(FMatrixC Get the maximum eigen value and its vector. Documentation by CxxDoc : Tue Aug 13 10:00:52 2002

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