To solve Partial Differential Equations (PDEs) like the Heat Equation or the Wave Equation , you use the method of separation of variables to turn a multivariable equation into several Ordinary Differential Equations (ODEs). Fourier Series are then used to combine these individual solutions to satisfy the initial and boundary conditions of the original problem. Assume the solution can be written as a product of two independent functions, . Substitute this into the PDE to isolate all terms on one side and all
terms on the other. Because they depend on different variables but are equal, both sides must equal a constant, typically denoted as −λnegative lambda This yields two separate ODEs: one for space ( ) and one for time (
so when we get to that point I we'll explain all of these things one after the other but here I'm just trying to give an overview. YouTube·Emmanuel Jesuyon Dansu Heat Equation and Fourier Series
An=2L∫0Lf(x)sin(nπxL)dxcap A sub n equals the fraction with numerator 2 and denominator cap L end-fraction integral from 0 to cap L of f of x sine open paren the fraction with numerator n pi x and denominator cap L end-fraction close paren d x
), which you solve using the given boundary conditions (like ) to find specific values for and their corresponding eigenfunctions .
. This often involves calculating a Fourier Sine or Cosine Series for the function using orthogonality integrals . For a sine series on , the formula is:
Plug the calculated coefficients back into your general series solution. For the Heat Equation with zero-temperature boundary conditions, the solution typically looks like:
