Discussion Overview
The discussion revolves around finding a complete orthogonal system for boundary value problems involving $C^{\infty}$ functions defined on the interval $[0, \pi]$ with specific boundary conditions. Participants explore the use of Fourier series as a method for constructing this orthogonal system.
Discussion Character
- Exploratory
- Technical explanation
- Conceptual clarification
- Debate/contested
Main Points Raised
- Some participants propose using Fourier series to find the coefficients and establish an orthogonal system for the given function.
- It is noted that the Fourier series is an orthogonal system, and under the boundary conditions, the coefficients for cosine terms ($a_k$) are zero, leading to a representation involving only sine terms.
- Participants discuss the resulting orthogonal system as the set of functions $\{ x \mapsto \sin(kx) \mid k \in \mathbb Z_{>0} \}$.
- There is a question about whether the complete orthogonal system consists of eigenfunctions, leading to further inquiry about which eigenfunctions are relevant.
- Some participants express that the approach holds only if an initial value problem is provided, suggesting a dependency on the specific function and boundary conditions.
- There is a suggestion that the orthogonal complete system may include functions like $1$, $\sin(kx)$, and $\cos(kx)$, depending on the application of boundary conditions.
Areas of Agreement / Disagreement
Participants generally agree on the use of Fourier series to find an orthogonal system, but there is uncertainty regarding the specific eigenfunctions involved and the conditions under which the proposed system applies. The discussion remains unresolved regarding the complete characterization of the orthogonal system.
Contextual Notes
The discussion highlights limitations related to the assumptions about the initial value problem and the specific boundary conditions that influence the orthogonal system's composition. There are unresolved questions about the nature of the eigenfunctions and their roles in the complete orthogonal system.