- •Differential equation of first order. Separable Equations
- •2. Homogeneous Equations. Linear de of first order.
- •3. Bernoulli Equation. Singular Solution
- •4. Ricatti Equation.
- •5. Exact Equations
- •Using an Integrating Factor
- •Existence and uniqueness of solution of Cauchy problem for de of first order and system of equations.
- •Lagrange and Clairaut Equations.
- •Implicit Equation. Introducing the parameter.
- •Singular Solutions.
- •Reduction of Order.
- •Linear homogeneous and non-homogeneous de of n-th order
- •The theorem of existence and uniqueness of the solution for Linear de
- •Linear independent system of functions.
- •Wronskian.
- •Liouville's formula
- •Structure of the General Solution
- •Reduction of order
- •Characteristic equation. The roots of the Characteristic Equation are Real and Multiple, Complex and Distinct, Complex and Multiple.
- •Method of Variation of Parameters
- •Method of Undetermined Coefficients
- •Linear Homogeneous Systems of de with variable coefficients
- •26) Fundamental System of Solutions and Fundamental Matrix
- •27. Wronskian and Liouville’s Formula.
- •28. Method of Variation of Constants (Lagrange Method)
- •29. Linear nonhomogeneous systems of differential equations with constant coefficients.
Implicit Equation. Introducing the parameter.
An equation of type
where F is a continuous function, is called the first order implicit differential equation. If this equation can be solved for y', we get one or several explicit differential equations of type
that can be solved by methods covered in other sections.
The main techniques for solving an implicit differential equation is the method of introducing a parameter.
Case 1. Implicit Differential Equation of Type x=f(y,y').
Case 2. Implicit Differential Equation of Type y=f(x,y').
Case 3. Implicit Differential Equation of Type x=f(y').
Case 4. Implicit Differential Equation of Type y=f(y').
Singular Solutions.
A function φ(x) is called the singular solution of the differential equation F(x,y,y') = 0, if uniqueness of solution is violated at each point of the domain of the equation. Geometrically this means that more than one integral curve with the common tangent line passes through each point (x0,y0). Note: Sometimes the weaker definition of the singular solution is used, when the uniqueness of solution of differential equation may be violated only at some points. A singular solution of a differential equation is not described by the general integral, that is it can not be derived from the general solution for any particular value of the constant C. We illustrate this by the following example: Suppose that the following equation is required to be solved: (y')2 − 4y = 0. It is easy to see that the general solution of the equation is given by the function y = (x + C)2. Graphically, it's represented by the family of parabolas (Figure 1).
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Fig.1 |
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Besides this, the function y = 0 also satisfies the differential equation. However, this function is not contained in the general solution! Since more than one integral curve passes through each point of the straight line y = 0, the uniqueness of solution is violated on this line, and hence it is a singular solution of the differential equation.
p-discriminant
One
of the ways to find a singular solution is investigation of the
so-called p-discriminant of
the differential equation. If the function F(x,y,y') and
its partial derivatives
and
are
continuous in the domain of the differential equation, the singular
solution can be found from the system of equations:
Lagrange and Clairaut Equations.
Lagrange Equation
A differential equation of type
where φ(y') and ψ(y') are known functions differentiable on a certain interval, is called the Lagrange equation. By setting y' = p and differentiating with respect to x, we get the general solution of the equation in parametric form:
under condition of
where p is a parameter. Lagrange equation may also have a singular solution if the condition φ(p) − p ≠ 0 is failed. The singular solution is given by the expression:
where c is the root of the equation φ(p) − p = 0.
Clairaut Equation
The Clairaut equation has the form:
where ψ(y') is a nonlinear differentiable function. The Clairaut equation is a particular case of the Lagrange equation whenφ(y') = y'. It is solved in the same way by introducing a parameter. The general solution is given by
where C is an arbitrary constant. Similarly to the Lagrange equation, the Clairaut equation may have a singular solution that is expressed parametrically in the form:
where p is a parameter.
