Solution to Linear First Order Ordinary Differential Equation/Solution by Integrating Factor
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Proof Technique
The technique to solve a linear first order ordinary differential equation in the form:
- $\dfrac {\d y} {\d x} + \map P x y = \map Q x$
It immediately follows from Integrating Factor for First Order ODE that:
- $e^{\int \map P x \rd x}$
is an integrating factor for $(1)$.
Multiplying it by:
- $e^{\int \map P x \rd x}$
to reduce it to a form:
- $\dfrac {\d y} {\d x} e^{\int \map P x \rd x} y = e^{\int \map P x \rd x} \map Q x$
is known as Solution by Integrating Factor.
It is remembered by the procedure:
- Multiply by $e^{\int \map P x \rd x}$ and integrate.
Examples
Example: $y' - 3 y = \sin x$
- $\dfrac {\d y} {\d x} - 3 y = \sin x$
has the general solution:
- $y = \dfrac 1 {10} \paren {3 \sin x - \cos x} + C e^{3 x}$
Example: $y' + y = \dfrac 1 x$
Consider the linear first order ODE:
- $(1): \quad \dfrac {\d y} {\d x} + y = \dfrac 1 x$
with the initial condition $\tuple {1, 0}$.
This has the particular solution:
- $y = \ds e^{-x} \int_1^x \dfrac {e^\xi \rd \xi} \xi$
Sources
- 1972: George F. Simmons: Differential Equations ... (previous) ... (next): $\S 2.10$