- •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
12) Method of variation of arbitrary constants.
The method of variation of parameters with arbitrary constants (Lagrange's method) is used to construct the general solution of the nonhomogeneous equation, when we know the general solution of the associated homogeneous equation. Suppose that the general solution of the second order homogeneous equation is expressed through the fundamental system of solutions y1(x) and y2(x): y0(x)=C1y1(x)+ C2y2(x) where C1, C2 are arbitrary constants. The idea of this method is to replace the constants C1 and C2 by functions C1(x) andC2(x), which are chosen so that the solution satisfies the nonhomogeneous equation. The derivatives of the unknown functions C1(x) and C2(x) can be determined from the system of equations
The main determinant of this system is the Wronskian of the functions y1 and y2, which is not equal to zero due to linear independence of the solutions y1 and y2. Therefore, this system of equations always has a unique solution. The final formulas for C1' (x) and C2' (x) have the form
C1`(x)=
; C2`(x)=
When using the method of variation of parameters, it is important to remember that the function f(x) must correspond tothe differential equation in the standard form, i.e. the coefficient a0(x) at the second derivative must be equal to 1. Then the general solution of the original nonhomogeneous equation will be expressed by the formula y(x)= C1(x)y1(x)+ C2(x)y2(x) =
[
-
dx+A1
] y1(x) + [ -
dx+A2
]y2(x) =
A 1y1(x)+A 2y2(x)+Y(x)
Where Y(x) denotes a particular solution of the nonhomogeneous equation.
13) Integration of linear equations with permanent coefficients.
Euler method which is a method of constructing a fundamental system of solutions for the equation
a0y(n)+a1y(n-1)+…+any=0 (1)
Following Euler we find solutions of equation (1) in the form y = eλx , where λ is a constant.
We prove that equation (1) has a solution of the form y = eλx , if λ satisfies to the equation l(λ ) = 0 , (2) where l(λ ) = λn+a1λn−1+ ...+ an
Equation (2) is called characteristic for the differential equation (1).
It is considered separately the different cases.
1) The roots of the characteristic polynomial l(λ ) are real and different.
2) The roots of the characteristic polynomial are different, but among of them there are complex roots.
3) The roots of the characteristic equation are real, but among of them there are multiple. To multiple root λ =λ* multiplicity "k"
corresponding to " k " linearly independent solutions of the form
y1=e λ*x, y2=xe λ* ,..,yk=xk-1e λ*
4) In the general case can also be multiple complex roots. Note that if the multiplicity of the root α + iβ is e , that multiplicity of the adjoint root as well e . Therefore, such pair of roots
corresponding to the following linearly independent solutions
eαxcosβx, xeαxcosβx,...,xl-1eαxcosβ x,
eαxsinβx, xeαxsinβx,...,xl-1eαxsinβ x,
The method of undetermined coefficients
This
method of selection of a particular solution for inhomogeneous linear
equation with constant coefficients, when the in-homogeneity of
quasi-polynomial. Quasi-polynomial are called functions of the form
f(x)=
where μj are constants (not necessarily real), and Pj ( x ) are polynomials of x .
For selecting of particular solutions, the following theorem is used.
Theorem 9. Equation a0y(n)+a1y(n-1)+…+any=P(x)eμx
where P ( x ) is a polynomial of degree l , has a particular solution of the form Yr(x)=xsQ(x) eμx
where s is equal to zero, if μ is not the root of the characteristic equation of the operator L , otherwise s is equal to the multiplicity of the root μ , and Q( x ) is polynomial of the same
degree l as P ( x ).
