- •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
14) Euler method.
Given
a complex- valued solution. It is proved that the real and
imaginary parts of the complex - valued solution are solutions . the
Euler method which is a method of constructing a fundamental system
of solution for the equation
Following
Euler we find solution of the equation
in the form
,
where
is a constant. We prove that equation
has a solution of the form
,
if
satisfies to the equation
Where
Equation
is called characteristic for
.
It is considered separately the different cases.
The roots of characteristic polynomial
are real and different.The roots of characteristic polynomial are different , but among of them there are complex roots
The roots of characteristic equation are real, but among of them there multiple.
In
the 3rd
case a theorem is proved. To multiple roots
multiplicity ‘”k” corresponding to “k” linearly independent
solution of the form
In the general case can also be multiple complex roots. Note that is the multiplicity of the roots
, that multiplicity of the adjoint root as well e. therefore, such
pair of roots corresponding to the following linearly independent
solutions
15) Basic properties of linear systems. Vector and matrix form.
Linear System Matrix-Vector Form: given an nxn matrix A(t) and nx1 vector valued function f(t):
=
aik(t)xk+fi(t)
i=1….n (pustoi
kvadrattyn ornynda ewtene jok)
where aik(t),fi(t) are given functions, xi(t)is unknown functions called a linear system of differential equations.
We denote
Then
(1) takes the form
=A(t)
+
(t)
If f(t)=0, the system is homogeneous.if not-it’ll be inhomogeneous
Basic properties of linear system:
Homogeneous System Solution Properties :
-Linear combinations of solutions: if x1(t),x2(t),…xk()t,are solutions to x’=Ax,where x’=dx/dt, then x(t)=C1x1(t)+….+Ckxk(t), is also solution for any constants C1,…Ck .
-independence:suppose y1(t),y2(t),…yk(t), are solutions to y’=Ay,for tє I=(a,b)
a)if
y1(t0)..yk(to)
are dependent for some t0
є
I,then there is exist C1,C2…Ck,not all 0,so that
C1y1(t)+C2y2(t)+….+Ck
yk
(t)=0
t
€ I
(the yi(t)'s are dependent any t є I );
b) if y1(t0)..yk(to) are dependent for some t0 є I,then yi(t)'s are dependent any t є I ).
-Solution Structure: if y1(t)….yn(t),are linearly independent solutions to the n-dimensioanl system y’=Ay, then any solution has the form y(t)= C1y1(t)+C2y2(t)+….+Cnyn (t) for some constants C1,C2….Cn.
The n yi's form a fundamental set of solutions.
- Solution Strategy:
a)find n independent yi's to form general solution;
b) if initial value y(t0) is given,
solve Y(to)C=y(t0) for C=(C1,C2….Cn)T, using nxn matrix we have Wronskian
y11…..
y1n this
expression called
y21….. y2n the wronskian
….
Yn1….. ynn
