Ordinary differential equations Proof
Proof of the reduction of a higher-order equation to a first-order system
Builds on Solution of an ordinary differential equationOrdinary differential equation
Proof
- By the definition of a solution of the equation, solves on when three things hold. The function is times differentiable on . For each , the point lies in . For each , .
- In the same way, solves the system on when three things hold. The function is differentiable on . For each , , and the equations of the system hold at .
- Let solve the equation on , and set for . Since , each is differentiable on , with .
- For , this gives .
- For , step 1 gives on .
- Also for each . By step 2, solves the system on .
- Conversely, let solve the system on , and set . We show by induction on that is times differentiable with , for .
- For this is the definition .
- Let and assume . The function is differentiable with . So is differentiable and . This completes the induction.
- In particular , and is differentiable. So is times differentiable on , and .
- By the last equation of the system, on .
- By steps 7 to 9, for each . So solves the equation on , and for .
Idea
The new unknowns are names for the derivatives . The first equations of the system say exactly that each name is the derivative of the previous one. The last equation is the original equation, written in the new names.
Reading path
To understand this page from the ground up, read these 6 pages in order. The foundations come first.
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- no evidence level
- Differential equation concept
- Function concept
- Interval concept
- Ordinary differential equation definition
- Solution of an ordinary differential equation definition
- Proof of the reduction of a higher-order equation to a first-order system proof
Where this leads
56 pages build on this one.
- Reduction of order
- Eigenvalue method for linear systems
- Liouville's formula
- Solutions for complex conjugate roots
- General solution of an inhomogeneous linear equation
- Solution space of a homogeneous linear equation has dimension n
- Fundamental system of solutions
- Solutions for distinct real roots
- Solutions for repeated roots
- Underdamped
- Wronskian test for linear independence of solutions
- Fundamental matrix
- Damped harmonic oscillator
- Variation of constants formula for linear systems
- Pendulum equation
- Reduction of a higher-order equation to a first-order system
- Forced oscillation and resonance
- Method of undetermined coefficients
- Variation of parameters
- Harmonic oscillator
- Simple harmonic motion
- Anharmonic oscillator
- Proof of the Wronskian test for linear independence of solutions
- Proof that the solution space of a homogeneous linear equation has dimension n
- Phonon dispersion in lattices
- Brunt–Väisälä frequency
- Damping
- Lorentz oscillator model
- Euler's elastica
- Real solutions from a complex eigenpair of a real matrix
- Inverted pendulum
- Liénard equation
- RLC circuit
- Proof of the general solution of an inhomogeneous linear equation
- Floquet theory
- Parametric oscillator
- Furuta pendulum
- Q factor
- Proof of the variation of constants formula for linear systems
- Random vibration
- Random vibration
- Parametric oscillator
- Duhamel's principle
- Anharmonic oscillator
- Annihilator method
- Elastic pendulum
- Proof of the solutions for repeated roots
- Proof of the solutions for distinct real roots
- Mild solution
- Kapitza's pendulum
- Magnus expansion
- Bertrand's theorem
- Spherical pendulum
- Duhamel's principle for heat conduction
- Van der Pol oscillator
- Hill differential equation
Further reading
- Web https://en.wikipedia.org/wiki/Ordinary_differential_equation, Reduction to a first-order system
About this page
| Tag | PGAEBXP9WZ |
|---|---|
| URI | m2://PGAEBXP9WZ |
| Kind | proof |
| Writing | W0 stub |
| MSC | 34A99 |
| Proves | Reduction of a higher-order equation to a first-order system |
| Uses | Solution of an ordinary differential equation, Ordinary differential equation |
| Changed | 4 November 2026 |
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