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Say the solution is
                                                                   1/2
                                                            x      t
                                                  u(x, t) =   sin         .
                                                            t      x 1/2
                   Making the change of variables ξ = x/t, f(ξ) = u(x, t), we could rewrite this equation
                   as

                                                                  −1/2
                                                    f(ξ) = ξ sin ξ      .
                   We see now that if we had guessed that the solution of this partial differential equation
                   was only dependent on powers of x/t we could have changed variables to ξ and f and
                   instead solved the ordinary differential equation

                                                         df
                                                     G      , f, ξ  = 0.
                                                         dξ

                   By using similarity methods one can reduce the number of independent variables in some
                   PDE’s.

                   Example 2.5 Consider the partial differential equation

                                                     ∂u     ∂u
                                                    x    + t    − u = 0.
                                                      ∂t    ∂x
                   One way to find a similarity variable is to introduce a transformation to the temporary
                                    0
                                 0
                              0
                   variables u , t , x , and the parameter λ.
                                                                0
                                                          u = u λ
                                                               0 m
                                                          t = t λ
                                                                0 n
                                                          x = x λ
                   where n and m are unknown. Rewriting the partial differential equation in terms of
                   the temporary variables,

                                               ∂u 0            ∂u 0
                                                                            0
                                                           0 m
                                            0 n
                                           x λ     λ 1−m  + t λ    λ 1−n  − u λ = 0
                                               ∂t 0            ∂x 0
                                               ∂u 0           ∂u 0
                                                                           0
                                             x 0  λ −m+n  + t 0  λ m−n  − u = 0
                                               ∂t 0           ∂x 0
                   There is a similarity variable if λ can be eliminated from the equation. Equating the
                   coefficients of the powers of λ in each term,
                                                   −m + n = m − n = 0.


                   This has the solution m = n. The similarity variable, ξ, will be unchanged under the
                   transformation to the temporary variables. One choice is

                                                               0 n
                                                         t    t λ     t 0
                                                    ξ =    =       =    .
                                                               0 m
                                                        x    x λ      x 0



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