| Physics M-files
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User contributed physics m-files from the MATLAB Central File Exchange.
Submitted Apr 18, 2000
Updated Apr 30, 2004
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| L. Kocbach: MATLAB in Physics
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Matlab in Physics Teaching
Submitted Nov 11, 2001
Updated Apr 30, 2004
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Total Visits: 2010
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| AOTOOLS Toolbox
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The Adaptive Optics Toolbox is a collection of functions and graphical user interfaces designed for analysis tasks related to adaptive optics systems. By providing these tools in the MATLAB environment the features offered by AOTools are significantly enhanced by the computing and graphics power of MATLAB. Most functions are provided in source code and can be studied or extended by the user. MATLAB also provides a high level of platform independence.
Submitted Jul 07, 1999
Updated Jun 28, 2004
by kazumine
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(1 Ratings)
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| OSLO
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Users of OSLO can simulate and optimize the performance of a wide range of optical systems by using OSLO's design features which help to determine the optimum size, shape and location of the individual optical components in a system.
Submitted Oct 07, 2004
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Total Visits: 800
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| Grating Diffraction Calculator (GD-Calc™)
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GD-Calc, the Grating Diffraction Calculator, computes optical diffraction efficiencies of biperiodic grating structures comprising linear, isotropic, and non-magnetic optical media, based on a generalized variant of rigorous coupled-wave (RCW) diffraction theory. Engineers, scientific programmers, researchers, and students with an interest in optics will find GD-Calc and the accompanying documentation to be a very useful resource for diffraction grating analysis.
Submitted Sep 23, 2005
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| Dielectric Resonator
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Solver for an isolated dielectric resonator.
Submitted Mar 18, 2005
by S. Makarov
Updated Mar 21, 2005
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(3 Ratings)
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| Problems for MATLAB Fundamentals
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Wind chill calculation and non-ideal gas problems from Gustavus Adolphus College.
Submitted Jun 07, 2005
by MATLAB Central Admin
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(9 Ratings)
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| rotsolve.m
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Solve solid body rotation problem.
[A,b] = ROTSOLVE(R1,R2) solves the matrix equation A*R1 + b(:,[1 1 1]) = R2, where A is a 3 by 3 rotation matrix for which: inv(A)=A', b is a 3 by 1 vector (translation),and R1 and R2 are 3 by 3 matrices of initial and final coordinates of 3 points (a,b,c) of a solid body.
Submitted Jul 18, 1999
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| Viscosity of Water and Silicon Oil
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Kinematic viscosities of pure water and Rhodorsil 47 silicon oils as a function of temperature.
Submitted Oct 06, 2005
by F. Moisy
Updated Oct 07, 2005
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(3 Ratings)
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| TIP
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TIP - Toolbox for Identification of the Physical Parameters of Linear Multibody Systems, by Thorsten Schmidt.
Submitted Jul 19, 1999
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(2 Ratings)
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Physical Modeling
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Accelerate system-level analysis and control design with accurate and intuitive models of your physical system
The design of engineering systems requires tight integration of many engineering disciplines. To be successful, teams of engineers must collaborate using a wide array of diverse technologies. Software, in the form of control algorithms and signal processing algorithms, plays an ever increasing role in these systems. Developing software alongside the physical system results in optimized designs and the detection of errors earlier in the design process.
Submitted Mar 19, 2008
by Steve Miller
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Total Visits: 245
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