First-Order Equations
* Existence theorems: A differential
equation y' = g(x,y),
with g continuously
differentiable in a region R
R2,
admits an infinity of solutions f(x,y,C)
= 0, such that for all (x,y)
R there
passes 1! solution.
* Example: The Langevin
equation for brownian motion.
* Non-linear: May have
more arbitrary constants than one expects; For example, y' = y2/3/3,
or the Riccati equation below, have 2.
* Riccati equation: The
non-linear equation y' = a y2
+ b y + c; Can be reduced
wlog to y' = y2 + c, whose
solution is y = –
–1
',
where
'' = –c
;
The latter is to be solved, a linear second-order equation; (Note: c may
not be constant!).
- Example: y' =
(y2–c),
with c constant; The 2-parameter
family of solutions reduces to 1-parameter; The solution of
'' = c
with c a constant is
= A exp{–c1/2x}
+ B exp{c1/2x},
so
![]()
- Blow-up in finite time: The
solutions of dx/dt = x^{1+
},
for
> 0.
@ Riccati: Cariñena & Ramos IJMPA(99)
[and groups]; Rosu et al JPA(03)mp/01 [generalization];
> s.a. Quaternions.
@ Other types, solutions: Kosovtsov mp/02 [operator
method], mp/02 [rational],
mp/02 [integrating factors].
Second-Order Equations > s.a.
integrable systems; Special
Functions; Sturm-Liouville Theory;
WKB Method.
* Methods for solution:
- u''(x)
+ p(x) u'(x)
= r(x), substitute v(x):= u'(x);
- u''(x)
+ p(x) u'(x)
+ q(x) u(x) = , {see #581};
- u''(x)
+ p(x) u'(x) + q(x) u(x)
= r(x), can be reduced to the form without
the q(x) term by u(x) =: v(x) h(x),
where h(x) solves the homogeneous equation.
* Eigenvalue problems: –y''(x)
+ x2N+2y(x)
= xNE y(x),
for –
< x <
,
can be
solved in closed form [@ Bender & Wang mp/01].
* Non-linear example: u'' =
u2,
one solution is u =
6/(x+c)2.
@ General references: Crampin & Saunders JGP(05)
[Cartan theory, duality]; Rafiq et al PLA(08) [homotopy perturbation method].
@ Books: Ayres 52; Coddington & Levinson 55; Nemytskii & Stepanov
60; Pontrjagin 70; Arnold 73, 83; Braun 83; Stroud 74.
@ Eigenvalue problems: Ciftci et al JPA(05)mp/04 [asymptotic
iteration method].
@ Delay-differential equations: in Kaplan & Glass 95 [II]; Simmendinger
et al PRE(99)mp/01.
@ Non-linear equations: Asch et al mp/01 [h3(h''+h')
= 1 as t →
];
Cornejo-Pérez & Rosu PTP(05)mp;
Chandrasekar et al JPA(06)
[linearization]; Ying & Candès JCP(06) [phase flow method for constructing
phase maps].
@ Rational ode's: Avellar et al mp/05,
mp/05 [elementary
first-order integrals].
Different Types and Other Topics > s.a.
differential equations.
* Order reduction: Linear
ode's with non-constant coefficients can be reduced in order if one knows any
single
solution; If u(x) = f(x)
is a particular solution, use the ansatz u(x) = f(x) v(x),
and the ode becomes an
equation of one order less for v'(x).
@ General references: Sakovich PLA(03)
[3rd-order, non-linear].
* Linear homogeneous:
Can be reduced to an eigenvalue problem.
@
Symmetries: Govinder & Leach JPA(95)
[non-local]; Abraham-Shrauner et al JPA(95)
[hidden contact symmetries]; Athorne JPA(97)
[linear, homogeneous equations].
@ Systems of ode's: Gaeta LMP(97)
[normal form]; Mennicken & Moller
03
[boundary eigenvalue problems].
@ Approaches:
Diver JPA(93)
[genetic algorithm]; Bagarello IJTP(04),
same
as IJTP(05)??
[non-commutative strategy].
Main page – Abbreviations – Journals – Comments – Other
sites – Acknowledgements
Send feedback and suggestions to bombelli at olemiss.edu – Modified
12 jul 2008