Solving partial differential equations

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SUMMARY

The discussion centers on the application of the sign function in the context of solving the partial differential equation (PDE) y_tt = 4 y_xx, with boundary conditions y(0,t) = 0 and y(pi,t) = 0, and initial conditions y_t(x,0) = 0 and y(x,0) = sin^2 x. The general solution utilizes d'Alembert's formula, where F(x) is defined as the odd periodic extension of f(x). The inclusion of the sign function, specifically F(x) = sign(sin x) sin^2 x, is necessary to ensure that F(x) maintains the odd function property, which is essential for the solution's validity.

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with d'Alembert's solution for wave equations
  • Knowledge of odd and even functions in mathematics
  • Basic calculus, including derivatives and integrals
NEXT STEPS
  • Study the properties of odd and even functions in detail
  • Learn about the application of d'Alembert's solution in various PDEs
  • Explore the concept of periodic extensions of functions
  • Investigate the role of boundary and initial conditions in solving PDEs
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Mathematicians, physics students, and engineers involved in solving partial differential equations, particularly those interested in wave equations and their properties.

jaejoon89
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Hi, why does the sign function need to be used in the following?

---
The given equation is y_tt = 4 y_xx
0 < x < pi, t>0
where y_tt is the 2nd derivative with respect to t, y_xx is 2nd wrt x

Boundary conditions
y(0,t) = 0 and y(pi,t) = 0

And initial conditions
y_t (x,0) = 0 = g(x)
y(x,0) = sin^2 x = f(x)

---
General solution (d'Alembert's solution):
y(x,t) = 1/2[F(x+at) - F(x-at)] + int[G(s)ds] from x-at to x+at

My teacher wrote that F(x) is the odd periodic extension of f(x), and then wrote

F(x) = sign(sinx)sin^2 x
Why?
 
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jaejoon89 said:
Hi, why does the sign function need to be used in the following?

---
The given equation is y_tt = 4 y_xx
0 < x < pi, t>0
where y_tt is the 2nd derivative with respect to t, y_xx is 2nd wrt x

Boundary conditions
y(0,t) = 0 and y(pi,t) = 0

And initial conditions
y_t (x,0) = 0 = g(x)
y(x,0) = sin^2 x = f(x)

---
General solution (d'Alembert's solution):
y(x,t) = 1/2[F(x+at) - F(x-at)] + int[G(s)ds] from x-at to x+at

My teacher wrote that F(x) is the odd periodic extension of f(x), and then wrote

F(x) = sign(sinx)sin^2 x
Why?

First try to remember what the requirements are in order for a function to be considered odd. Second, ask yourself what the sign function does. See if you can put these two pieces of info together, in conjunction with the fact that F(x) is odd, to figure out your question.
 
Well, I understand that it makes it odd. Except we had a similar example where y(x,0) = 1/(1+x^2) (which, like sin^2, is even) and the sign function wasn't used. So there must be something else to consider. What is the reason?

y_tt = y_xx
x for all real numbers, t less than or equal to 0
y_t (x,0) = 0
 
Last edited:

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