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Meissner equation : ウィキペディア英語版
Meissner equation
The Meissner equation is a linear ordinary differential equation that is a special case of Hill's equation with the periodic function given as a square wave.〔 〕 〔
〕 There are many ways to write the Meissner equation. One
is as
: \frac + (\alpha^2 + \omega^2 \sgn \cos(t))y = 0
or
: \frac + ( 1 + r f(t;a,b) ) y = 0
where
: f(t;a,b) = -1 + 2 H_a( t \mod (a+b) )
and H_c(t) is the Heaviside function shifted to c. Another version is
: \frac + \left( 1 + r \frac \right) y = 0.
The Meissner equation was first studied as a toy problem for certain resonance problems. It is also useful for understand resonance problems in evolutionary biology.
Because the time-dependence is piecewise linear, many calculations can be performed exactly, unlike for the Mathieu equation. When a = b = 1, the Floquet exponents are roots of the quadratic equation
: \lambda^2 - 2 \lambda \cosh(\sqrt) \cos(\sqrt) + 1 = 0 .
The determinant of the Floquet matrix is 1, implying that origin is a center if |\cosh(\sqrt) \cos(\sqrt)| < 1
and a saddle node otherwise.
== References ==


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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