How to Install and Uninstall levmar.x86_64 Package on Fedora 36

Last updated: October 05,2024

1. Install "levmar.x86_64" package

Please follow the guidance below to install levmar.x86_64 on Fedora 36


    
        
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                sudo dnf update
            
                    
    
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            $
        

        
            
                sudo dnf install
            
                        
                levmar.x86_64
            
                    
    
    Copied

2. Uninstall "levmar.x86_64" package

Please follow the guidance below to uninstall levmar.x86_64 on Fedora 36:


    
        
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                sudo dnf remove
            
                        
                levmar.x86_64
            
                    
    
    Copied


    
        
            $
        

        
            
                sudo dnf autoremove
            
                    
    
    Copied

3. Information about the levmar.x86_64 package on Fedora 36

Last metadata expiration check: 5:07:46 ago on Thu Sep 8 02:05:26 2022.
Available Packages
Name : levmar
Version : 2.6
Release : 10.fc36
Architecture : x86_64
Size : 62 k
Source : levmar-2.6-10.fc36.src.rpm
Repository : fedora
Summary : Levenberg-Marquardt nonlinear least squares algorithm
URL : http://www.ics.forth.gr/~lourakis/levmar/
License : GPLv2+
Description : levmar is a native ANSI C implementation of the Levenberg-Marquardt
: optimization algorithm. Both unconstrained and constrained (under linear
: equations, inequality and box constraints) Levenberg-Marquardt variants are
: included. The LM algorithm is an iterative technique that finds a local
: minimum of a function that is expressed as the sum of squares of nonlinear
: functions. It has become a standard technique for nonlinear least-squares
: problems and can be thought of as a combination of steepest descent and the
: Gauss-Newton method. When the current solution is far from the correct on,
: the algorithm behaves like a steepest descent method: slow, but guaranteed
: to converge. When the current solution is close to the correct solution, it
: becomes a Gauss-Newton method.