Deprecated: $wgMWOAuthSharedUserIDs=false is deprecated, set $wgMWOAuthSharedUserIDs=true, $wgMWOAuthSharedUserSource='local' instead [Called from MediaWiki\HookContainer\HookContainer::run in /var/www/html/w/includes/HookContainer/HookContainer.php at line 135] in /var/www/html/w/includes/Debug/MWDebug.php on line 372
The existence and stability of periodic solutions of inhomogeneous hyperbolic equation - MaRDI portal

The existence and stability of periodic solutions of inhomogeneous hyperbolic equation (Q2703862)

From MaRDI portal





scientific article
Language Label Description Also known as
English
The existence and stability of periodic solutions of inhomogeneous hyperbolic equation
scientific article

    Statements

    0 references
    0 references
    2 July 2001
    0 references
    telegraph equation
    0 references
    viscous friction
    0 references
    forced transverse vibrations of a stretched string in a potential field
    0 references
    The existence and stability of periodic solutions of inhomogeneous hyperbolic equation (English)
    0 references
    This paper concerns classical time-periodic solutions to the problem NEWLINE\[NEWLINEu_{tt}- u_{xx}+ bu_t+ cu= f(x,t),\quad x\in [0,\pi],NEWLINE\]NEWLINE NEWLINE\[NEWLINEu(0, t)= u(\pi, t)= 0,NEWLINE\]NEWLINE where \(b> 0\) and \(c\geq 0\) are constants and \(f(x,\cdot)\) is \(T\)-periodic. The following is proved: If \(f\) is continuous with respect to \(x\), \(C^2\)-smooth with respect to \(t\), and if NEWLINE\[NEWLINEf(t,x)= f_0(x)+ \sum^\infty_{n=1} f_n(x)\sin{2\pi_n\over T} t,NEWLINE\]NEWLINE then there exists exactly one (\(T\)-periodic with respect to time) solution, this solution is globally asymptotically stable, and NEWLINE\[NEWLINEu(t,x)= u_0(x)+ \sum^\infty_{n=1} \Biggl(v_n(x)\sin {2\pi_n\over T} t+ w_n(x)\cos{2\pi_n\over T} t\Biggr)NEWLINE\]NEWLINE with \(-u''_0+ cu_0= f_0\), \(v''_n+ [({2\pi_n\over T})^2- c] v_n+ b{2\pi_n\over T} w_n= f_n\), \(w''_n+ [({2\pi_n\over T})^2- c] w_n- b{2\pi_n\over T} v_n= 0\) and \(u_0(0)= u_0(\pi)= v_n(0)= v_n(\pi)= w_n(0)= w_n(\pi)= 0\).
    0 references
    0 references

    Identifiers

    0 references
    0 references
    0 references
    0 references