What is the Green's function for this specific problem?

Click For Summary
SUMMARY

The discussion focuses on finding the Green's function for the differential operator $$K(\phi(s)) = \phi''(s)+\cot(s)\phi'(s)+\left(2-\frac{1}{\sin(s)^2}\right)\phi(s)$$ with boundary conditions $$\phi|_{s=0} < \infty$$ and $$\phi|_{s=\alpha} = 0$$. The correct Green's function is derived using variation of parameters, with solutions $$G_1(s,y)$$ and $$G_2(s,y)$$ defined in terms of Legendre polynomials. The Wronskian is calculated as $$W(s) = -2\csc(s)$$, and the continuity and jump conditions of the Green's function are confirmed. The discussion clarifies that the problem is not self-adjoint, leading to $$G(s,y) \neq G(y,s)$$.

PREREQUISITES
  • Understanding of Green's functions in differential equations
  • Familiarity with Legendre polynomials, specifically $$P_1^1$$ and $$Q_1^1$$
  • Knowledge of Wronskian and its application in linear differential equations
  • Basic concepts of boundary value problems and self-adjoint operators
NEXT STEPS
  • Study the derivation and applications of Green's functions in various boundary value problems
  • Learn about the properties of Legendre polynomials and their role in solving ODEs
  • Explore the implications of self-adjointness in differential equations and Green's functions
  • Investigate the use of Mathematica for solving differential equations and verifying solutions
USEFUL FOR

Mathematicians, physicists, and engineering students involved in solving differential equations, particularly those working with boundary value problems and Green's functions.

member 428835

Homework Statement


Find Green's function of $$K(\phi(s)) = \phi''(s)+\cot(s)\phi'(s)+\left(2-\frac{1}{\sin(s)^2}\right)\phi(s):s\in[0,\alpha]$$
subject to boundary conditions: $$\phi|_{s=0} < \infty\\
\phi|_{s=\alpha} = 0.$$

Homework Equations


Green's function ##G## is found via variation of parameters: $$
G_1(s,y) = \frac{v_1(s)v_2(y)}{W(s)}:0<s<y<\alpha\\
G_2(s,y) = \frac{v_1(y)v_2(s)}{W(s)}:0<y<s<\alpha$$
where ##W## is the Wronskian of ##v_1,v_2## and ##v_i## is a linearly independent solution satisfying a boundary condition.

The Attempt at a Solution


Legendre polynomials of first and second kind (##P_1^1(\cos(s)),Q_1^1(\cos(s))##) solve this ODE, so we construct ##v_1## and ##v_2## from these. To satisfy the finite domain at ##s=0## we take ##v_1 = P_1^1(\cos(s))## and to satisfy ##\phi(\alpha)=0## we take the solution $$v_2(s) = \frac{\tau_2}{\tau_1}(P_1^1(\cos(s))-Q_1^1(\cos(s))):\\
\tau_1 = P_1^1(\cos(\alpha));\,\,\tau_2 = Q_1^1(\cos(\alpha)).$$
Then we find ##W(s) = -2\csc(s)##. Then we know the Green's function from above. However, when I substitute these results into the proposed method, Mathematica is suggesting the ODE is not solved. Any help is much appreciated!

Edit: Evidently the problem is solved when I take solutions of the form $$
G_1(s,y) = \frac{v_1(s)v_2(y)}{W(y)}:0<s<y<\alpha\\
G_2(s,y) = \frac{v_1(y)v_2(s)}{W(y)}:0<y<s<\alpha
$$
since now the boundaries are satisfied ##G1(s=0,y)<\infty;\, G2(s=\alpha,y)=0##. Also, ##G## is continuous: ##G2(s,y)|_{s=y}-G1(s,y)|_{s=y} = 0##, and ##G## exhibits the jump discontinuity at ##s=y##: ##G2'(s,y)|_{s=y}-G1'(s,y)|_{s=y} = 1##.

However, I should note that ##G(s,y)## satisfies the above conditions, but ##G(y,s)## does not. Can anyone comment here?
 
Last edited by a moderator:
Physics news on Phys.org
Your problem isn't self adjoint, so in general ##G(s,y)\neq G(y,s)##. By the way, given that your problem is not self adjoint, are you sure that your formulae,
joshmccraney said:
$$
G_1(s,y) = \frac{v_1(s)v_2(y)}{W(s)}:0<s<y<\alpha\\
G_2(s,y) = \frac{v_1(y)v_2(s)}{W(s)}:0<y<s<\alpha$$

are correct?

jason
 
jasonRF said:
Your problem isn't self adjoint, so in general ##G(s,y)\neq G(y,s)##. By the way, given that your problem is not self adjoint, are you sure that your formulae,are correct?

jason
Thanks for replying Jason! Good to know that fact about Green's functions. Regarding the formula, I think it's slightly incorrect. I in fact think if you evaluate the Wronskian at ##y## instead of ##s## you get the correct solution. Then I'm pretty sure the edited solution in post 1 is valid fro this problem.

Taking the proposed ##v##'s from post 1 and their Wronskian, the Green's function suggested in post 1 edit satisfies ##K(G) = 0## for ##s\neq y##, ##G## is continuous, ##G'## has a unit jump at ##s=y##, and boundary conditions are satisfied by ##G1## and ##G2##. What do you think?
 

Similar threads

  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 18 ·
Replies
18
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
9
Views
2K
Replies
3
Views
2K
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
7
Views
2K