- •Basic concepts and definitions of differential equations.
- •Equations with separated variables.
- •Linear equations of the first order.
- •Equations of the first order unsolved by derivatives.
- •6) Method of introducing a parameter. Lagrange and Clairaut equations.
- •7) Theorem about existence and uniqueness of Cauchy problem.
- •8) General properties of solutions. Continuity, differentiation of solutions of parameter axis and initial data.
- •9) Linear equations of the n-th order. Basic properties.
- •11) Linear inhomogeneous equations
- •12) Method of variation of arbitrary constants.
- •13) Integration of linear equations with permanent coefficients.
- •14) Euler method.
- •16) Fundamental system of solutions.
- •18) Integration of linear inhomogeneous system with quasi-polynomial right side.
- •20.Boundary problem for system of the second order. Green function.
- •Local properties of solutions.
- •Global properties of solutions.
- •26) Transformation of solutions and system.
- •27. Basic concepts. Stability by Lyapunov. Geometric means.
- •28. The main Lyapunov theorems.
- •30) Studying stability by Lyapunov function.
- •31.Differential equations in full differentials .Integral multiplier.
- •32.Integration methods. Homogeneous and linear differential equations of the first order.
- •33.Incomplete equations . Equations assuming reduction of order.
- •34) Local and global theorems.
- •35) Analyticity and differentiation of solutions.
- •36) Solution continuity of parameters and initial data.
- •37. Fundamental system of solutions
- •38. Wronskian determinant. Liouville formula.
- •39. Homogeneous and inhomogeneous linear equations. Liouville formula.
- •40 Integration of linear inhomogeneous equation with quasipolinomial right side.
- •41) Cauchy function. Fundamental solutions.
- •42. Systems of linear differential equations with constant coefficients
- •43. Linear systems of differential equations. Basic systems
- •44. Some methods of the system integration (leading to one equation etc)
- •45.Method of variation of constants
45.Method of variation of constants
The
general form of system of differential equations:
(1)
Let`s
introduce a linear operator L(y)=
,
then (1) we can write in the following form: L[y]=F (2). If F=0
,
then the operator equation (2) is called homogeneous and has the
form: L[y]=0 (3)
Let
Y=
- the general solution of homogeneous sytem (3). Let`s find a
solution of (2) in following way: Y(x)=
,
where Ci(x - unknown functions. Substituting the solution
into (2):
,
and tak into a consideration that Yi - solutions of (3), it means
.
We get,
-
vector equation. The last correspondence can be written in the form
of n-equations with n-indeterminates Ci(x). Meanwhile W≠0 on [a,b],
because Yi - fundamental system of solutions of (3) and, hence, we
can explicitly determine unknown functions: Ci’(x)=
i=
,
Ci’(x)=
And
then the general solution of (2) has a form:Y(x)=
.
